,,lightning1 ,,thunder ,,and ,,lightning ,,conductors4 ,,with ,,an ,,appendix ,,on ,,the ,,recent ,,controversy ,,on ,,lightning ,,conductors4 ,,by ,,gerald ,,molloy1 ,d4 ,d41 ,d4 ,sc4 ,,illustrated4 ,illustration ,,new ,,york3 ,,the ,,humboldt ,,publishing ,,co41 #bh ,,lafayette ,,place4 ,,lightning1 ,,thunder1 ,,and ,,lightning ,,conductors4 ,,contents4 ,,lecture ,i4 ,pages #e-bf ,,lightning ,,and ,,thunder4 ,identity of ,lightning and ,electricity--,franklin's ,experiment--,fatal ,experiment of ,richman--,immediate ,cause of ,lightning--,illustration from ,electric ,spark--,what a ,flash of ,lightning ,is--,duration of a ,flash of ,lightning--,experiments of ,professor ,rood--,wheatstone's ,experiments--,experiment with ,rotating ,disc--,brightness of a ,flash of ,lightning--,various ,forms of ,lightning--,forked ,lightning1 ,sheet ,lightning1 ,globe ,lightning--,st4 ,elmo's ,fire--,experimental ,illustration--,origin of ,lightning--,length of a ,flash of ,lightning--,physical ,cause of ,thunder--,rolling of ,thunder--,succession of ,peals--,variation of ,intensity--,distance of a ,flash of ,lightning ,,lecture ,,ii4 ,pages #bf-ec ,,lightning ,,conductors4 ,destructive ,effects of ,lightning--,destruction of ,buildings--,destruction of ,ships at ,sea--,destruction of ,powder ,magazines--,experimental ,illustrations--,destruction of ,life by ,lightning--,the ,return ,shock--,franklin's ,lightning ,rods--,introduction of ,lightning ,rods into ,england--,the ,battle of ,balls and ,points--,functions of a ,lightning ,conductor--,conditions of a ,lightning ,conductor--,mischief ,done by ,bad ,conductors--,evil ,effects of a ,bad ,earth ,contact--,danger from ,rival ,conductors--,insulation of ,lightning ,conductors--,personal ,safety in a ,thunder ,storm--,practical ,rules--,security ,afforded by ,lightning ,rods ,,appendix4 ,pages #ee-fb ,,recent ,,controversy ,,on ,,lightning ,,conductors4 ,theory of ,lightning ,conductors ,challenged--,lectures of ,professor ,lodge--,short ,account of his ,views and ,arguments--,effect of ,self-,induction on a ,lightning ,rod--,experiment on the ,discharge of a ,leyden ,jar--,outer ,shell only of a ,lightning ,rod ,acts as a ,conductor--,discussion at the ,meeting of the ,british ,association1 ,september1 #ahhh--,statement by ,mr4 ,preece--,lord ,rayleigh and ,sir ,william ,thomson--,professor ,rowland and ,professor ,forbes--,m4 de ,fonvielle1 ,sir ,james ,douglass1 and ,mr4 ,symons--,reply of ,professor ,lodge--,concluding ,remarks of ,professor ,fitzgerald1 ,president of the ,section--,summary ,showing the ,present ,state of the ,question ,,list ,,of ,,illustrations4 ,,page ,,the ,,electric ,,spark3 ,a ,,type ,,of ,a ,,flash ,,of ,,lightning1 #h ,,cardboard ,,disc ,,with ,,black ,,and ,,white ,,sectors2 ,,as ,,seen ,,when ,,at ,,rest1 #ab ,,same ,,disc2 ,,as ,,seen ,,when ,,in ,,rapid ,,rotation1 #ab ,,the ,,brush ,,discharge1 ,,illustrating ,,st4 ,,elmo',s ,,fire1 #ag ,,origin ,,of ,,successive ,,peals ,,of ,,thunder1 #bb ,,variations ,,of ,,intensity ,,in ,a ,,peal ,,of ,,thunder1 #bd ,,discharge ,,of ,,leyden ,,jar ,,battery ,,through ,,thin ,,wires1 #bg ,,glass ,,vessel ,,broken ,,by ,,discharge ,,of ,,leyden ,,jar ,,battery1 #cb ,,gun ,,cotton ,,set ,,on ,,fire ,,by ,,electric ,,spark1 #cc ,,volta',s ,,pistol2 ,,explosion ,,caused ,,by ,,electric ,,spark1 #cd ,,the ,,return ,,shock ,,illustrated1 #ce ,,protection ,,from ,,lightning ,,by ,a ,,closed ,,conductor1 #dh ,,induction ,,effect ,,of ,,leyden ,,jar ,,discharge1 #ef ,,lecture ,i4 ,,lightning ,,and ,,thunder4 ,the electricity produced by an ordinary electric machine exhibits1 under certain conditions1 phenomena which bear a striking resemblance to the phenomena attendant on lightning4 ,in both cases there is a flash of light2 in both there is a report1 which1 in the case of lightning1 we call thunder2 and1 in both cases1 intense heat is developed1 which is capable of setting fire to combustible bodies4 ,further1 the spark from an electric machine travels through space with extraordinary rapidity1 and so does a flash of lightning2 the spark follows a zig-zag course1 and so does a flash of lightning2 the spark moves silently and harmlessly through metal rods and stout wires1 while it forces its way1 with destructive effect1 through bad conductors1 and it is so1 too1 with a flash of lightning4 ,lastly1 the electricity of a machine is capable of giving a severe shock to the human body2 and we know that lightning gives a shock so severe as usually to cause immediate death4 ,for these reasons it was long conjectured by scientific men that lightning is1 in its nature1 identical with electricity2 and that it differs from the electricity of our machines only in this1 that it exists in a more powerful and destructive form4 ,identity of ,lightning and ,electricity4--,but it was reserved for the celebrated ,benjamin ,franklin to demonstrate the truth of this conjecture by direct experiment4 ,he first conceived the idea of drawing electricity from a thundercloud in the same way as it is drawn from the conductor of an electric machine4 ,for this purpose he proposed to place a kind of sentry-box on the summit of a lofty tower1 and to erect1 on the sentry-box1 a metal rod1 projecting twenty or thirty feet upward into the air1 pointed at the end1 and having no electrical communication with the earth4 ,he predicted that when a thundercloud would pass over the tower1 the metal rod would become charged with electricity1 and that an observer1 stationed in the sentry-box1 might draw from it1 at pleasure1 a succession of electric sparks4 ,with the magnanimity of a really great man1 ,franklin published this project to the world2 being more solicitous to extend the domain of science by new discoveries1 than to secure for himself the glory of having made them4 ,the project was set forth in a letter to ,mr4 ,collinson1 of ,london1 which bears date ,july #bi1 #agej1 and which1 in the course of a year or two1 was translated into the principal languages of ,europe4 ,two years later the experiment suggested by ,franklin was made by ,monsieur ,dalibard1 a wealthy man of science1 at his villa near ,marly-la-,ville1 a few miles from ,paris4 ,in the middle of an elevated plain ,monsieur ,dalibard erected an iron rod1 forty feet in length1 one inch in diameter1 and ending above in a sharp steel point4 ,the iron rod rested on an insulating support1 and was kept in position by means of silk cords4 ,in the absence of ,monsieur ,dalibard1 who was called by business to ,paris1 this apparatus was watched by an old dragoon1 named ,coiffier2 and on the afternoon of the tenth of ,may1 #ageb1 he drew sparks from the lower end of the rod at the time that a thundercloud was passing over the neighborhood4 ,conscious of the importance that would be attached to this phenomenon1 the old dragoon summoned1 in all haste1 the prior of ,marly to come and witness it4 ,the prior came without delay1 and he was followed by some of the principal inhabitants of the village4 ,in the presence of the little group1 thus gathered together1 the experiment was repeated--electric sparks were again drawn1 in rapid succession1 from the iron rod2 the prediction of ,franklin was fulfilled to the letter2 and the identity of lightning and electricity was1 for the first time1 demonstrated to the world4 ,franklin's ,experiment4--,meanwhile ,franklin had been waiting1 with impatience1 for the completion of the tower of ,christchurch1 in ,philadelphia1 on which he intended to make the experiment himself4 ,he even collected money1 it is said1 to hasten on the building4 ,but1 notwithstanding his exertions1 the progress of the tower was slow2 and his active mind1 which could ill brook delay1 hit upon another expedient1 remarkable alike for its simplicity and for its complete success4 ,he constructed a boy's kite1 using1 however1 a silk pockethandkerchief1 instead of paper1 that it might not be damaged by rain4 ,to the top of the kite he attached a pointed iron wire about a foot long1 and he provided a roll of hempen twine1 which he knew to be a conductor of electricity1 for flying it4 ,this was the apparatus with which he proposed to explore the nature of a thundercloud4 ,the thundercloud came late in the afternoon of the fourth of ,july1 #ageb1 and ,franklin sallied out with his kite1 accompanied by his son1 and taking with him a common door-key and a ,leyden jar4 ,the kite was soon high in air1 and the philosopher awaited the result of his experiment1 standing1 with his son1 under the lee of a cowshed1 partly to protect himself from the rain that was coming1 and partly1 it is said1 to shield himself from the ridicule of passers-by1 who1 having no sympathy with his philosophical speculations1 might be inclined to regard him as a lunatic4 ,to guard against the danger of receiving a flash of lightning through his body1 he held the kite by means of a silk ribbon1 which was tied to the door-key1 the door-key being itself attached to the lower end of the hempen string4 ,a flash of lightning soon came from the cloud1 and a second1 and a third2 but no sign of electricity could be observed in the kite1 or the hempen cord1 or the key4 ,franklin was almost beginning to despair of success1 when suddenly he noticed that the little fibres of the cord began to bristle up1 just as they would if it were placed near an electric machine in action4 ,he presented the door-key to the knob of the ,leyden jar1 and a spark passed between them4 ,presently a shower began to fall2 the cord1 wetted by the rain1 became a better conductor than it had been before1 and sparks came more freely4 ,with these sparks he now charged the ,leyden jar1 and found1 to his intense delight1 that he could exhibit all the phenomena of electricity by means of the lightning he had drawn from the clouds4 ,in the following year a similar experiment1 with even more striking results1 was carried out1 in ,france1 by de ,romas4 ,though it is said he had no knowledge of what ,franklin had done in ,america1 he1 too1 used a kite2 and1 with a view of making the string a better conductor1 he interlaced with it a thin copper wire4 ,then1 flying his kite in the ordinary way1 when it had risen to a height of about #eej feet1 he drew sparks from it which1 we are told1 were upwards of nine feet long1 and emitted a sound like the report of a pistol4 ,fatal ,experiment of ,richman4--,there can be no doubt that experiments of this kind1 made with the electricity of a thundercloud1 were extremely dangerous2 and this was soon proved by a fatal accident4 ,professor ,richman1 of ,st4 ,petersburgh1 had erected on the roof of his house a pointed iron rod1 the lower end of which passed into a glass vessel1 intended1 as we are informed1 to measure the strength of the charge which he expected to receive from the clouds4 ,on the sixth of ,august1 #agec1 observing the approach of a thunderstorm1 he hastened to his apparatus2 and as he stood near it1 with his head bent down1 to watch the effect1 a flash of lightning passed through his body and killed him on the spot4 ,this catastrophe served to fix public attention on the danger of such experiments1 and gave occasion to the saying of ,voltaire3 8,there are some great lords whom we should always approach with extreme precaution1 and lightning is one of them40#a ,from this time the practice of making experiments directly with the lightning of the clouds seems to have been1 by common consent1 abandoned4 ,immediate ,cause of ,lightning4--,and now1 having set before you some of the most memorable experiments by which the identity of lightning and electricity has been demonstrated1 ,i will try to give you a clear conception regarding the immediate cause of lightning1 so far as the subject is understood at the present day by scientific men4 ,you know that there are two kinds of electricity1 which are called positive and negative2 and that each of them repels electricity of the same kind as itself1 while it attracts electricity of the opposite kind4 ,now1 every thundercloud is charged with electricity of one kind or the other1 positive or negative2 and1 as it hovers over the earth1 it develops1 by what is called induction1 or influence1 electricity of the opposite kind in that part of the earth which is immediately under it4 ,thus we have two bodies--the cloud and the earth--charged with opposite kinds of electricity1 and separated by a stratum of the atmosphere4 ,the two opposite electricities powerfully attract each other2 but for a time they are prevented from rushing together by the intervening stratum of air1 which is a non-conductor of electricity1 and acts as a barrier between them4 ,as the electricity1 however1 continues to accumulate1 the attraction becomes stronger and stronger1 until at length it is able to overcome the resistance of this barrier2 a violent disruptive discharge then takes place between the cloud and the earth1 and the flash of lightning is the consequence of the discharge4 ,illustration3 ,,the ,,electric ,,spark2 ,a ,,type ,,of ,a ,,flash ,,of ,,lightning4 ,the whole phenomenon may be illustrated1 on a small scale1 by means of this electric machine of ,carr's which you see before you4 ,when my assistant turns the handle of the machine negative electricity is developed in that large brass cylinder1 which in our experiment will represent the thundercloud4 ,at a distance of five or six inches from the cylinder ,i hold a brass ball1 which is in electrical communication with the earth through my body4 ,the electrified brass cylinder acts by induction1 or influence on the brass ball1 and develops in it1 as well as in my body1 a charge of positive electricity4 ,now1 the positive electricity of the ball and the negative electricity of the cylinder are mutually attracting each other1 but the intervening stratum of air offers a resistance which prevents a discharge from taking place4 ,my assistant1 however1 continues to work the machine2 the two opposite electricities rapidly accumulate on the cylinder and the ball2 at length their mutual attraction is strong enough to overcome the resistance interposed between them2 a disruptive discharge follows1 and at the same moment a spark is seen to pass1 accompanied by a sharp snapping report4 ,this spark is a miniature flash of lightning2 and the snapping report is a diminutive peal of thunder4 ,furthermore1 at the moment the spark passes you may observe a slight convulsive movement in my hand and wrist4 ,this convulsive movement represents1 on a small scale1 the violent shock1 generally fatal to life1 which is produced by a flash of lightning when it passes through the body4 ,i can continue to take sparks from the conductor as long as the machine is worked2 and it is interesting to observe that these sparks follow an irregular zig-zag course1 just as lightning does4 ,the reason is the same in both cases3 a discharge between two electrified bodies takes place along the line of least resistance2 and1 owing to the varying condition of the atmosphere1 as well as of the minute particles of matter floating in it1 the line of least resistance is almost always a zig-zag line4 ,what a ,flash of ,lightning is4--,lightning1 then1 may be conceived as an electrical discharge1 sudden and violent in its character1 which takes place1 through the atmosphere1 between two bodies highly charged with opposite kinds of electricity4 ,sometimes this electrical discharge passes1 as ,i have said1 between a cloud and the earth2 sometimes it passes between one cloud and another2 sometimes1 on a smaller scale1 it takes place1 between the great mass of a cloud and its outlying fragments4 ,but1 if you ask me in what the discharge itself consists1 ,i am utterly unable to tell you4 ,it is usual to speak and write on this subject as if electricity were a material substance1 a very subtle fluid1 and as if1 at the moment the discharge takes place1 this fluid passes like a rapid stream1 from the body that is positively electrified to the body that is negatively electrified4 ,but we must always remember that this is only a conventional mode of expression1 intended chiefly to assist our conceptions1 and to help us to talk about the phenomena4 ,it does not even profess to represent the objective truth4 ,all that we know for certain is this3 that immediately before the discharge the two bodies are highly electrified with opposite kinds of electricity2 and1 that immediately after the discharge1 they are found to have returned to their ordinary condition1 or1 at least1 to have become less highly electrified than they were before4 ,the flash of light that accompanies an electric discharge is often supposed to be the electricity itself1 passing from one body to the other4 ,but it is not2 it is simply an effect produced by the discharge4 ,heat is generated by the expenditure of electrical energy1 in overcoming the resistance offered by the atmosphere2 and this heat is so intense1 that it produces a brilliant incandescence along the path of the discharge4 ,when a spark appears1 for example1 between the conductor of the machine and this brass ball1 it can be shown1 by very satisfactory evidence1 that minute particles of these solid bodies are first converted into vapor1 and then made to glow with intense heat4 ,the gases1 too1 of which the air is composed1 and the solid particles floating in the air1 are likewise raised to incandescence4 ,so1 too1 with lightning2 the flash of light is due to the intense heat generated by the electrical discharge1 and owes its character to the composition and the density of the atmosphere through which the discharge passes4 ,duration of a ,flash of ,lightning4--,how long does a flash of lightning last8 ,you are aware1 ,i dare say1 that when an impression of light is made on the eye1 the impression remains for a sensible interval of time1 not less than the tenth of a second1 after the source of light has been extinguished or removed4 ,hence we continue1 in fact1 to see the light1 for at least the tenth of a second1 after the light has ceased4 ,now1 if you reflect how brief is the moment for which a flash of lightning is visible1 and if you deduct the tenth of a second from that brief moment1 you will see1 at once1 that the period of its actual duration must be very short indeed4 ,the exact duration of a flash of lightning is a question on which no settled opinion has yet been accepted generally by scientific men4 ,indeed1 the most widely different statements have been made on the subject1 quite recently1 by the highest authorities1 each speaking apparently with unhesitating confidence4 ,thus1 for example1 ,professor ,mascart describes an experiment1 which he says was made by ,wheatstone1 and which showed that a flash of lightning lasts for less than one-thousandth of a second2#b ,professor ,everett describes the same experiment1 without saying by whom it was made1 and gives1 as the result1 that 8the duration of the illumination produced by lightning is certainly less than the ten-thousandth of a second20#c ,professor ,tyndall1 in his own picturesque way1 tells us that 8a flash of lightning cleaves a cloud1 appearing and disappearing in less than the hundred-thousandth of a second20#d and according to ,professor ,tait1 of ,edinburgh1 8,wheatstone has shown that lightning certainly lasts less than the millionth of a second40#e ,experiments of ,professor ,rood4--,i cannot say which of these statements is best supported by actual observation2 for none of the writers ,i have quoted gives any reference to the original memoir from which his statement is derived4 ,as far as my own reading goes1 ,i have only come across one original record of experiments1 made directly on the flash of lightning itself1 with a view to determine the period of its duration4 ,these experiments were carried out by ,professor ,ogden ,rood1 of ,columbia ,college1 ,new ,york1 between the years #ahgj and #ahgc1 and are recorded in the ,american ,journal of ,science and ,arts4#f ,for the description of his apparatus1 and for the details of his observations1 ,i must refer you to the memoir itself2 but ,i may tell you briefly that the results at which he arrived1 if they be accepted1 must lead to a considerable modification of the views previously entertained on the subject4 ,in the first place1 he satisfied himself that what appears to the eye a single flash of lightning is usually1 if not always1 multiple in its character2 consisting1 in fact1 of a succession of distinct flashes1 which follow one another with such rapidity as to make a continuous impression on the retina4 ,next1 he proceeded to measure approximately the duration of these several component flashes2 and he found that it varied over a wide range1 amounting sometimes to fully the twentieth of a second1 and being sometimes less than the sixteen-hundredth of a second4 ,wheatstone's ,experiments4--,these results are extremely interesting2 but we can hardly regard them as finally established1 until they have been confirmed by other observers4 ,i may remark1 however1 that they fit in very well with the experiments made by ,professor ,wheatstone1 many years ago1 on the duration of the electric spark1 which1 as ,i told you1 is a miniature flash of lightning4 ,in these classical experiments1 which leave nothing to be desired in point of accuracy1 ,professor ,wheatstone showed that a spark taken directly from a ,leyden jar1 or a spark taken from the conductor of a powerful electric machine1 that is1 just such a spark as you have seen here to-day1 lasts for less than the millionth of a second4 ,but he also showed that the duration of the spark is greatly increased1 when a resisting wire is introduced into the path of the discharge4 ,thus1 for example1 when the discharge from a ,leyden jar was made to pass through half a mile of copper wire1 with breaks at intervals1 the sparks that appeared at these breaks were found to last for of a second4#g ,hence we should naturally expect that the period of illumination would be still further increased1 in the case of a flash of lightning1 where the resistance interposed is enormously greater than in either of the experiments made by ,wheatstone4#h ,experiment of the ,rotating ,disk4--,it would be tedious1 on an occasion like the present1 to enter into an account of ,wheatstone's beautiful and ingenious method of investigation1 by which the above facts have been established2 but ,i will show you a much more simple experiment which brings home very forcibly to the mind how exceedingly short must be the duration of the electric spark4 ,here is a circular disk of cardboard1 the outer part of which1 as you see1 is divided into sectors1 black and white alternately1 while the space about the centre is entirely white4 ,the disk is mounted on a stand1 by means of which ,i can make it rotate with great velocity4 ,when it is put in rotation1 the effect on the eye is very striking--the central space remains white as before1 but in the outer rim the distinction of black and white absolutely disappears and gives place to a uniform gray4 ,this color is due to the blending together of black and white in equal proportions2 the blending being effected1 not on the cardboard disk1 but on the retina of the eye4 ,illustration3 ,,cardboard ,,disk ,,as ,,seen ,,when ,,at ,,rest4 ,illustration3 ,,same ,,disk ,,as ,,seen ,,when ,,in ,,rapid ,,rotation4 ,i mentioned just now that an impression made on the retina lasts for the tenth of a second after the cause of it has been removed4 ,now1 when this disk is in rotation1 the sectors follow one another so rapidly that the particular part of space occupied at any moment by a white sector will be occupied by a black sector within a time much less than the tenth of a second4 ,it follows that the impression made by each white sector remains on the retina until the following black sector comes into the same position2 and1 in like manner1 the impression made by each black sector remains until the following white sector takes up the position of the black4 ,therefore1 the impression made by the whole outer rim is the impression of black and white combined--that is1 the impression of gray4 ,so far1 ,i dare say1 the phenomenon is already familiar to you all4 ,but ,i propose now to show you the revolving disk illuminated by the electric spark2 and you will observe that1 at the moment of illumination1 the black and white sectors come out as clearly and distinctly as if the disk were standing still4 ,for the success of this experiment it is desirable1 not only to have a brilliant spark in order to secure a good illumination of the disk1 but also to have a succession of such sparks1 that you may see the phenomenon frequently repeated1 and thus be able to observe it at your leisure4 ,to attain these two objects1 ,i have made the arrangement which is here before you4 ,in front of the disk is a large and very powerful ,leyden jar4 ,the rod connected with the inner coating rises well above the mouth of the jar1 and ends in a brass ball nearly opposite the centre of the disk4 ,connected with the outer coating of the jar is another rod which likewise ends in a brass ball1 and which is so adjusted that the distance between the two balls is about an inch4 ,the two rods are connected respectively with the two conductors of a ,holtz machine1 so that1 when the machine is worked1 the jar is first quickly charged1 and then it discharges itself1 with a brilliant spark1 between the two brass balls4 ,thus1 by continuing to work the machine1 we can get1 as long as we choose1 a succession of sparks following one another at short and regular intervals right in front of the disk4 ,everything being now ready1 and the room partially darkened1 the disk is put in rapid rotation2 and you can see1 by the twilight that remains1 the outer rim a uniform gray1 and the central space white4 ,but when my assistant begins to turn the ,holtz machine1 and brilliant sparks leap out at intervals1 the revolving disk1 illuminated for a moment at each discharge1 seems to be standing still1 and shows the black and white sectors distinctly visible4 ,the reason of this is clear3 ,so brief is the moment for which the spark endures1 that the disk1 though in rapid motion1 makes no sensible advance during that small fraction of time2 therefore1 in the image on the retina1 the impression made by the white sectors remains distinct from the impression made by the black1 and the eye sees the disk as it really is4 ,i may notice1 in passing1 a very interesting consideration1 suggested by this experiment4 ,a cannon ball is now commonly discharged with a velocity of about #a1fjj feet a second4 ,moving with this velocity it is1 as you know1 under ordinary circumstances1 altogether invisible to the eye4 ,but suppose it were illuminated1 in the darkness of night1 by this electric spark1 which lasts1 we will say1 for the millionth of a second4 ,during the moment of illumination1 the cannon ball moves through the millionth part of #a1fjj feet1 which is a little less than the fiftieth of an inch4 ,practically1 we may say that the cannon ball does not sensibly change its place while the spark lasts4 ,further1 the impression it makes on the eye1 from the position it occupies at the moment of illumination1 remains on the retina for at least the tenth of a second4 ,therefore1 if we are looking toward that particular part of space where the cannon ball happens to be at the moment the spark passes1 we must see the cannon ball hanging motionless in the air1 though we know it is traveling at the rate of #a1fjj feet a second1 or about #a1jjj miles an hour4 ,brightness of a ,flash of ,lightning4--,i should like to say one word about the brightness of a flash of lightning4 ,somewhat more than thirty years ago1 ,professor ,swan1 of ,edinburgh1 showed that the eye requires a sensible time--about the tenth of a second--to perceive the full brightness of a luminous object4 ,further1 he proved1 by a series of interesting experiments1 that when a flash of light lasts for less than the tenth of a second1 its apparent brilliancy to the eye is proportional to the time of its duration4#i ,now consider the consequence of these facts in reference to the brightness of our electric spark4 ,if the spark lasted for the tenth of a second1 we should perceive its full brightness2 if it lasted for the tenth part of that time1 we should see only the tenth part of its brightness2 if it lasted for the hundredth part1 we should see only the hundredth part of its brightness2 and so on4 ,but we know1 in point of fact1 that it lasts for less than the millionth of a second1 that is1 less than the hundred-thousandth part of the tenth of a second4 ,therefore we see only the hundred-thousandth part of its real brightness4 ,here is a startling conclusion1 and one1 ,i may say1 fully justified by scientific evidence4 ,that electric spark1 brilliant as it appears to us1 is really a hundred thousand times as bright as it seems to be4 ,we cannot speak with the same precision of a flash of lightning2 because its duration has not yet been so exactly determined4 ,but if we suppose that a flash of lightning1 in a particular case1 lasts for the thousandth of a second1 it would follow1 from the above experiments1 that the flash is a hundred times as bright1 in fact1 as it appears to the eye4 ,various ,forms of ,lightning4--,the lightning of which ,i have spoken hitherto is commonly called forked lightning2 a name which seems to have been derived from the zig-zag line of light it presents to the eye4 ,but there are other forms under which the electricity of the clouds often makes itself manifest2 and to these ,i would now invite your attention for a few moments4 ,the most common of them all1 at least in this country1 is that which is familiarly known by the name of sheet lightning4 ,this is1 probably1 nothing else than the lighting up of the atmosphere1 or of the clouds1 by forked lightning1 which is not itself directly visible4 ,generally speaking1 after a flash of sheet lightning1 we hear the rolling of distant thunder4 ,but it sometimes happens1 especially in summer time1 that the atmosphere is again and again lit up by a sudden glow of light1 and yet no thunder is heard4 ,this phenomenon is commonly called summer lightning1 or heat lightning4 ,it is probably due1 in many cases1 to electrical discharges in the higher regions of the atmosphere1 where the air is greatly rarified2 and1 in these cases1 it would seem to resemble the discharges obtained by means of an induction coil in glass tubes containing rarified gases4 ,but there is little doubt that in many cases1 too1 summer lightning1 like ordinary sheet lightning1 is due to forked lightning1 which is so remote that we can neither see the flash itself directly1 nor hear the rolling of the thunder4 ,perhaps the most distinct and satisfactory evidence on this subject1 derived from actual observation1 is contained in the following letter of ,professor ,tyndall1 written in ,may1 #ahhc3 8,looking to the south and south-east from the ,bel ,alp1 the play of silent lightning among the clouds and mountains is sometimes very wonderful4 ,it may be seen palpitating for hours1 with a barely appreciable interval between the thrills4 ,most of those who see it regard it as lightning without thunder--,blitz ohne ,donner1 ,wetterleuchten1 ,i have heard it named by ,german visitors4 ,the ,monte ,generoso1 overlooking the ,lake of ,lugano1 is about fifty miles from the ,bel ,alp1 as the crow flies4 ,the two points are connected by telegraph2 and frequently when the ,wetterleuchten1 as seen from the ,bel ,alp1 was in full play1 ,i have telegraphed to the proprietor of the ,monte ,generoso ,hotel and learned1 in every instance1 that our silent lightning co-existed in time with a thunderstorm more or less terrific in upper ,italy40#aj ,another form of lightning1 described by many writers1 is called globe lightning4 ,it is said to appear as a ball of fire1 about the size of a child's head1 or even larger1 which moves for a time slowly about1 and then1 after the lapse of several seconds1 explodes with a terrific noise1 sending forth flashes of fire in all directions1 which burn whatever they strike4 ,many accounts are on record of such phenomena2 but they are derived1 for the most part1 from the evidence of persons who were not specially competent to observe1 and to describe with precision1 the facts that fell under their observation4 ,hence these accounts1 while they are accepted by some1 are rejected by others2 and it seems to me1 in the present state of the question1 that the existence of globe lightning can hardly be regarded as a demonstrated fact4 ,at all events1 if phenomena of this kind have really occurred1 ,i can only say that nothing we know about electricity1 at present1 will enable us to account for them4#aa ,st4 ,elmo's ,fire4--,a much more authentic and1 at the same time1 very interesting form1 under which the electricity of the clouds sometimes manifests its presence1 is known by the name of ,st4 ,elmo's fire4 ,this phenomenon at one time presents the appearance of a star1 shining at the points of the lances or bayonets of a company of soldiers2 at another1 it takes the form of a tuft of bluish light1 which seems to stream away from the masts and spars of a ship at sea1 or from the pointed spire of a church4 ,it was well known to the ancients4 ,csar1 in his ,commentaries1 tells us that1 after a stormy night1 the iron points of the javelins of the fifth legion seemed to be on fire2 and ,pliny says that he saw lights1 like stars1 shining on the lances of the soldiers1 keeping watch by night upon the ramparts4 ,when two such lights appeared at once1 on the masts of a ship1 they were called ,castor and ,pollux1 and were regarded by sailors as a sign of a prosperous voyage4 ,when only one appeared1 it was called ,helen1 and was taken as an unfavorable omen4 ,in modern times ,st4 ,elmo's fire has been witnessed by a host of observers1 and all its various phases have been repeatedly described4 ,in the memoirs of ,forbin we read that1 when he was sailing once1 in #afif1 among the ,balearic ,islands1 a sudden storm came on during the night1 accompanied by lightning and thunder4 8,we saw on the vessel10 he says1 8more than thirty ,st4 ,elmo's fires4 ,among the rest there was one on the vane of the mainmast more than a foot and a half high4 ,i sent a man up to fetch it down4 ,when he was aloft he cried out that it made a noise like wetted gunpowder set on fire4 ,i told him to take off the vane and come down2 but1 scarcely had he removed it from its place1 when the fire left it and reappeared at the end of the mast1 so that it was impossible to take it away4 ,it remained for a long time1 and gradually went out40 ,on the #adth of ,january1 #ahbd1 ,monsieur ,maxadorf happened to look at a load of straw in the middle of a field just under a dense black cloud4 ,the straw seemed literally on fire--a streak of light went forth from every blade2 even the driver's whip shone with a pale-blue flame4 ,as the black cloud passed away1 the light gradually disappeared1 after having lasted about ten minutes4 ,again1 it is related that on the #hth of ,may1 #ahca1 in ,algiers1 as the ,french artillery officers were walking out after sunset without their caps1 each one saw a tuft of blue light on his neighbor's head2 and1 when they stretched out their hands1 a tuft of light was seen at the end of every finger4 ,not infrequently a traveler in the ,alps sees the same luminous tuft on the point of his alpenstock4 ,and quite recently1 during a thunderstorm1 a whole forest was observed to become luminous just before each flash of lightning1 and to become dark again at the moment of the discharge4#ab ,this phenomenon may be easily explained4 ,it consists in a gradual and comparatively silent electrical discharge between the earth and the cloud2 and generally1 but not always1 it has the effect of preventing such an accumulation of electricity as would be necessary to produce a flash of lightning4 ,i can illustrate this kind of discharge with the aid of our machine4 ,if ,i hold a pointed metal rod toward the large conductor1 you can see1 when the machine is worked and the room darkened1 how the point of the rod becomes luminous and shines like a faint blue star4 ,i substitute for the pointed rod the blunt handles of a pair of pliers1 and a tuft of blue light is at once developed at the end of each handle1 and seems to stream away with a hissing noise4 ,i now put aside the pliers1 and open out my hand under the conductor--and observe how ,i can set up1 at pleasure1 a luminous tuft at the tips of my fingers4 ,now and then a spark passes1 giving me a smart shock1 and showing how the electricity may sometimes accumulate so fast that it cannot be sufficiently discharged by the luminous tuft4 ,lastly1 ,i present a small bushy branch of a tree to the conductor1 and all its leaves and twigs are aglow with bluish light1 which ceases for a moment when a spark escapes1 to be again renewed when electricity is again developed by the working of the machine4 ,illustration3 ,,the ,,brush ,,discharge1 ,,illustrating ,,st4 ,,elmo',s ,,fire4 ,now1 if you put a thundercloud in the place of that conductor1 you can easily realize how1 through its influence1 the lance and bayonet of the soldier1 the alpenstock of the traveler1 the pointed spire of a church1 the masts of a ship at sea1 the trees of a forest1 can all be made to glow with a silent electrical discharge which may or may not1 according to circumstances1 culminate at intervals in a genuine flash of lightning4 ,origin of ,lightning4--,when we seek to account for the origin of lightning1 we are confronted at once with two questions of great interest and importance--first1 ,what are the sources from which the electricity of the thundercloud is derived8 and1 secondly1 ,how does this electricity come to be developed in a form which so far transcends in power the electricity of our machines8 ,these questions have long engaged the attention of scientific men1 but ,i cannot say that they have yet received a perfectly satisfactory solution4 ,nevertheless1 some facts of great scientific value have been established1 and some speculations have been put forward1 which are well deserving of consideration4 ,in the first place1 it is quite certain that the atmosphere which surrounds our globe is almost always in a state of electrification4 ,further1 the electrical condition of the atmosphere would seem to be as variable as the wind4 ,it changes with the change of season2 it changes from day to day2 it changes from hour to hour4 ,the charge of electricity is sometimes positive1 sometimes negative2 sometimes it is strong1 sometimes feeble2 and the transition from one condition to another is sometimes slow and gradual1 sometimes sudden and violent4 ,as a general rule1 in fine1 clear weather1 the electricity of the atmosphere is positive1 and not very strongly developed4 ,in wet weather the charge may be either positive or negative1 and is generally strong1 especially when there are sudden heavy showers4 ,in fog it is also strong1 and almost always positive4 ,in a snowstorm it is very strong1 and most frequently positive4 ,finally1 in a thunderstorm it is extremely strong1 and generally negative2 but it is subject to a sudden change of sign1 when a flash of lightning passes or when rain begins to fall4 ,so far ,i have simply stated facts1 which have been ascertained by careful observations1 made at different stations by competent observers1 and extending over a period of many years4 ,but as regards the process by which the electricity of the atmosphere is developed1 we have1 up to the present time1 no certain knowledge4 ,it has been said that electricity may be generated in the atmosphere by the friction of the air itself1 and of the minute particles floating in it1 against the surface of the earth1 against trees and buildings1 against rocks1 cliffs1 and mountains4 ,but this opinion1 however probable it may be1 has not yet been confirmed by any direct experimental investigation4 ,the second theory is that the electricity of the atmosphere is due1 in great part at least1 to the evaporation of salt water4 ,many years ago1 ,pouillet1 a ,french philosopher1 made a series of experiments in the laboratory1 which seemed to show that evaporation is generally attended with the development of electricity2 and1 in particular1 he satisfied himself that the vapor which passes off from the surface of salt water is always positively electrified4 ,now1 the atmosphere is everywhere charged1 more or less1 with vapor which comes1 almost entirely1 from the salt water of the ocean4 ,hence ,pouillet inferred that the chief source of atmospheric electricity is the evaporation of sea water4 ,this explanation would certainly go far to account for the presence of electricity in the atmosphere1 if the fact on which it rests were established beyond dispute4 ,but there is some reason to doubt whether the development of electricity1 in the experiments of ,pouillet1 was due simply to the process of evaporation1 and not rather to other causes1 the influence of which he did not sufficiently take into account4 ,a conjecture has recently been started that electricity may be generated by the mere impact of minute particles of water vapor against minute particles of air4#ac ,if this conjecture could be established as a fact1 it would be amply sufficient to account for all the electricity of the atmosphere4 ,from the very nature of a gas1 the molecules of which it is composed are forever flying about with incredible velocity2 and therefore the particles of water vapor and the particles of air1 which exist together in the atmosphere1 must be incessantly coming into collision4 ,hence1 however small may be the charge of electricity developed at each individual impact1 the total amount generated over any considerable area1 in a single day1 must be very great indeed4 ,it is evident1 however1 that this method of explaining the origin of atmospheric electricity can only be regarded as1 at best1 a probable hypothesis1 until the assumption on which it rests is supported by the evidence of observation or experiment4 ,length of a ,flash of ,lightning4--,it would seem1 then1 that we are not yet in a position to indicate with certainty the sources from which the electricity of the atmosphere is derived4 ,but whatever these sources may be1 there can be little doubt that the electricity of the atmosphere is intimately associated with the minute particles of water vapor of which the thundercloud is eventually built up4 ,this consideration is of great importance when we come to consider the special properties of lightning1 as compared with other forms of electricity4 ,the most striking characteristic of lightning is the wonderful power it possesses of forcing its way through the resisting medium of the air4 ,in this respect it incomparably surpasses all forms of electricity that have hitherto been produced by artificial means4 ,the spark of an ordinary electric machine can leap across a space of three or four inches2 the machine we have employed in our experiments to-day can give1 under favorable circumstances1 a spark of nine or ten inches2 the longest electric spark ever yet produced artificially is probably the spark of ,mr4 ,spottiswoode's gigantic induction coil2 and it does not exceed three feet six inches4 ,but the length of a flash of lightning is not to be measured in inches1 or in feet or in yards2 it varies from one or two miles1 for ordinary flashes1 to eight or ten miles in exceptional cases4 ,this power of discharging itself violently through a resisting medium1 in which the thundercloud so far transcends the conductor of an electric machine1 is due to the property commonly known among scientific men as electrical potential4 ,the greater the distance to which an electrified body can shoot its flashes through the air1 the higher must be its potential4 ,hence the potential of a thundercloud must be exceedingly high1 since its flashes can pierce the air to a distance of several miles4 ,and what ,i want to point out is1 that we are able to account for this exceedingly high potential1 if we may only assume that the minute particles of water vapor in the atmosphere have1 from any cause1 received ever so small a charge of electricity4 ,the number of such particles that go to make up an ordinary drop of rain are to be counted by millions of millions2 and it is capable of scientific proof that1 as each new particle is added1 in the building up of the drop1 a rise of potential is necessarily produced4 ,it is clear1 therefore1 that there is practically no limit to the potential that may be developed by the simple agglomeration of very small cloud particles1 each carrying a very small charge of electricity4#ad ,this explanation1 which traces the exceedingly high potential of lightning to the building up of rain drops in the thundercloud1 suggests a reason why it so often happens that immediately after a flash of lightning 8the big rain comes dancing to the earth40 ,the potential has been steadily rising as the drops have been getting larger and larger1 until at length the potential has become so high that the thundercloud is able to discharge itself1 and almost at the same moment the drops have become so large that they can no longer be held aloft against the attracting force of gravity4 ,physical ,cause of ,thunder4--,let us now proceed to consider the phenomenon of thunder1 which is so intimately associated with lightning1 and which1 though perfectly harmless in itself1 and though never heard until the real danger is past1 often excites more terror in the mind than the lightning flash itself4 ,the sound of thunder1 like that of the electric spark1 is due to a disturbance caused in the air by the electric discharge4 ,the air is first expanded by the intense heat that is developed along the line of discharge1 and then it rushes back again to fill up the partial vacuum which its expansion has produced4 ,this sudden movement gives rise to a series of sound waves1 which reach the ear in the form of thunder4 ,but there are certain peculiar characteristics of thunder which are deserving of special consideration4 ,rolling of ,thunder4--,they may be classified1 ,i think1 under two heads4 ,first1 the sound of thunder is not an instantaneous report like the sound of the electric spark--it is a prolonged peal lasting1 sometimes1 for several seconds4 ,secondly1 each flash of lightning gives rise1 not to one peal only1 but to a succession of peals following one another at irregular intervals4 ,these two phenomena1 taken together1 produce that peculiar effect on the ear which is commonly described as the rolling of thunder2 and both of them1 ,i think1 may be sufficiently accounted for in accordance with the well-established properties of sound4 ,to understand why the sound of thunder reaches the ear as a prolonged peal1 we have only to remember that sound takes time to travel4 ,since a flash of lightning is practically instantaneous1 we may assume that the sound is produced at the same moment all along the line of discharge4 ,but the sound waves1 setting out at the same moment from all points along the line of discharge1 must reach the ear in successive instants of time1 arriving first from that point which is nearest to the observer1 and last from that point which is most distant4 ,suppose1 for example1 that the nearest point of the flash is a mile distant from the observer1 and the farthest point two miles--the sound will take about five seconds to come from the nearest point1 and about ten seconds to come from the farthest point2 and moreover1 in each successive instant from the time the first sound reaches the ear1 sound will continue to arrive from the successive points between4 ,therefore the thunder1 though instantaneous in its origin1 will reach the ear as a prolonged peal extending over a period of five seconds4 ,succession of ,peals4--,the succession of peals produced by a single flash of lightning is due to several causes1 each one of which may contribute more or less1 according to circumstances1 toward the general effect4 ,first1 if we accept the results arrived at by ,professor ,ogden ,rood1 of ,columbia ,college1 what appears to the eye as a single flash of lightning1 consists1 in fact1 as a general rule1 of a succession of flashes1 each one of which must naturally produce its own peal of thunder2 and although the several flashes1 if they follow one another at intervals of the tenth of a second1 will make one continuous impression on the eye1 the several peals of thunder1 under the same conditions1 will impress the ear as so many distinct peals4 ,the next cause that ,i would mention is the zigzag path of the lightning discharge4 ,to make clear to you the influence of this circumstance1 ,i must ask your attention for a moment to the diagram on next page4 ,let the broken line represent the path of a flash of lightning1 and let ,o represent the position of an observer4 ,the sound will reach him first from the point ,a1 which is nearest to him1 and then it will continue to arrive in successive instants from the successive points along the line ,a ,n and along the line ,a ,m1 thus producing the effect of a continuous peal4 ,meanwhile the sound waves have been traveling from the point ,b1 and in due time will reach the observer at ,o4 ,coming as they do in a different direction from the former1 they will strike the ear as the beginning of a new peal which1 in its turn1 will be prolonged by the sound waves arriving1 in successive instants1 from the successive points along the line ,b ,m and ,b ,h4 ,a little later1 the sound will arrive from the more distant point ,c1 and a third peal will begin4 ,and so there will be several distinct peals proceeding1 so to speak1 from several distinct points in the path of the lightning flash4 ,illustration3 ,,origin ,,of ,,successive ,,peals ,,of ,,thunder4 ,a third cause to which the succession of peals may be referred is to be found in the minor electrical discharges that must often take place within the thundercloud itself4 ,a thundercloud is not a continuous mass like the metal cylinder of this electric machine--it has many outlying fragments1 more or less imperfectly connected with the principal body4 ,moreover1 the material of which the cloud is composed is only a very imperfect conductor as compared with our brass cylinder4 ,for these two reasons it must often happen1 about the time a flash of lightning passes1 that different parts of the cloud will be in such different electrical conditions as to give rise to electrical discharges within the cloud itself4 ,each of these discharges produces its own peal of thunder2 and thus we may have a number of minor peals1 sometimes preceding and sometimes following the great crash which is due to the principal discharge4 ,lastly1 the influence of echo has often a considerable share in multiplying the number of peals of thunder4 ,the waves of sound1 going forth in all directions1 are reflected from the surfaces of mountains1 forests1 clouds1 and buildings1 and coming back from different quarters1 and with varying intensity1 reach the ear like the roar of distant artillery4 ,the striking effect of these reverberations in a mountain district has been described by a great poet in words which1 ,i daresay1 are familiar to most of you3 8,far along1 ,from peak to peak1 the rattling crags among1 ,leaps the live thunder6 ,not from one lone cloud1 ,but every mountain now has found a tongue1 ,and ,jura answers from her misty shroud ,back to the joyous ,alps1 that call to her aloud60 ,variations of ,intensity in ,thunder4--,from what has been said1 it is easy to understand how the general roar of thunder is subject to great changes of intensity1 during the time it lasts1 according to the number of peals that may be arriving at the ear of an observer in each particular moment4 ,but every one must have observed that even an individual peal of thunder often undergoes similar changes1 swelling out at one moment with great power1 and the next moment rapidly dying away4 ,to account for this phenomenon1 ,i would observe1 first1 that there is no reason to suppose that the disturbance caused by lightning is of exactly the same magnitude at every point of its path4 ,on the contrary1 it would seem very probable that the amount of this disturbance is1 in some way1 dependent on the resistance which the discharge encounters4 ,hence the intensity of the sound waves sent forth by a flash of lightning is probably very different at different parts of its course2 and each individual peal will swell out on the ear or die away1 according to the greater or less intensity of the sound waves that reach the ear in each successive moment of time4 ,but there is another influence at work which must produce variations in the loudness of a peal of thunder1 even though the sound waves1 set in motion by the lightning1 were everywhere of equal intensity4 ,this influence depends on the position of the observer in relation to the path of the lightning flash4 ,at one part of its course the lightning may follow a path which remains for a certain length at nearly the same distance from the observer2 then all the sound produced along this length will reach the observer nearly at the same moment1 and will burst upon the ear with great intensity4 ,at another part1 the lightning may for an equal length go right away from the observer2 and it is evident that the sound produced along this length will reach the observer in successive instants1 and consequently produce an effect comparatively feeble4 ,with a view to investigate this interesting question a little more closely1 let me suppose the position of the observer taken as a centre1 and a number of concentric circles drawn1 cutting the path of the lightning flash1 and separated from one another by a distance of #aaj feet1 measured along the direction of the radius4 ,it is evident that all the sound produced between any two consecutive circles will reach the ear within a period which must be measured by the time that sound takes to travel #aaj feet1 that is1 within the tenth of a second4 ,hence1 in order to determine the quantity of sound that reaches the ear in successive periods of one-tenth of a second1 we have only to observe how much is produced between each two consecutive circles4 ,but on the supposition that the sound waves1 set in motion by the flash of lightning1 are of equal intensity at every point of its path1 it is clear that the quantity of sound developed between each two consecutive circles will be simply proportional to the length of the path enclosed between them4 ,with these principles established1 let us now follow the course of a peal of thunder1 in the diagram before us4 ,this broken line1 drawn almost at random1 represents the path of a flash of lightning2 the observer is supposed to be placed at ,o1 which is the centre of the concentric circles2 these circles are separated from one another by a distance of #aaj feet1 measured in the direction of the radius2 and we want to consider how any one peal of thunder may vary in loudness in the successive periods of one-tenth of a second4 ,illustration3 ,,variations ,,of ,,intensity ,,in ,a ,,peal ,,of ,,thunder4 ,let us take1 for example1 the peal which begins when the sound waves reach the ear from the point ,a4 ,in the first unit of time the sound that reaches the ear is the sound produced along the lines ,a ,b and ,a ,c2 in the second unit1 the sound produced along the lines ,b ,d and ,c ,e2 in the third unit1 the sound produced along ,d ,f and ,e ,g4 ,so far the peal has been fairly uniform in its intensity2 though there has been a slight falling off in the second and third units of time1 as compared with the first4 ,but in the fourth unit there is a considerable falling away of the sound2 for the line ,f ,k is only about one-third as long as ,d ,f and ,e ,g taken together2 therefore the quantity of sound that reaches the ear in the fourth unit of time is only one-third of that which reaches it in each of the three preceding units2 and consequently the sound is only one-third as loud4 ,in the fifth unit1 however1 the peal must rise to a sudden crash2 for the portion of the lightning path inclosed between the fifth and sixth circles is about six times as great as that between the fourth and fifth2 therefore the intensity of the sound will be suddenly increased about six-fold4 ,after this sudden crash1 the sound as suddenly dies away in the sixth unit of time2 it continues feeble as the path of the lightning goes nearly straight away from the observer2 it swells again slightly in the ninth unit of time2 and then continues without much variation to the end4 ,this is only a single illustration1 but it seems quite sufficient to show that the changes of intensity in a peal of thunder must be largely due to the position of the spectator in relation to the several parts of the lightning flash4 ,distance of a ,flash of ,lightning4--,i need hardly remind you that1 by observing the interval that elapses between the flash of lightning and the peal of thunder that follows it1 we may estimate approximately the distance of the nearest point of the discharge4 ,light travels with such amazing velocity that we may assume1 without any sensible error1 that we see the flash of lightning at the very moment in which the discharge takes place4 ,but sound1 as we have seen1 takes a sensible time to travel even short distances2 and therefore a measurable interval almost always elapses between the moment in which the flash is seen and the moment in which the peal of thunder first reaches the ear4 ,and the distance through which sound travels in this interval will be the distance of the nearest point through which the discharge has passed4 ,now1 the velocity of sound in air varies slightly with the temperature2 but1 at the ordinary temperature of our climate1 we shall not be far astray if we allow #a1ajj feet for every second1 or about one mile for every five seconds4 ,you will observe also that1 by repeating this observation1 we can determine whether the thundercloud is coming toward us1 or going away from us4 ,so long as the interval between each successive flash and the corresponding peal of thunder1 continues to get shorter and shorter1 the thundercloud is approaching2 when the interval begins to increase1 the thundercloud is receding from us1 and the danger is passed4 ,the crash of thunder is terrific when the lightning is close at hand2 but it is a curious fact1 that the sound does not seem to travel as far as the report of an ordinary cannon4 ,we have no authentic record of thunder having been heard at a greater distance than from twelve to fifteen miles1 whereas the report of a single cannon has been heard at five times that distance2 and the roar of artillery1 in battle1 at a greater distance still4 ,on the occasion of the ,queen's visit to ,cherbourg1 in ,august1 #aheh1 the salute fired in honor of her arrival was heard at ,bonchurch1 in the ,isle of ,wight1 a distance of sixty miles4 ,it was also heard at ,lyme ,regis1 in ,dorsetshire1 which is eighty-five miles from ,cherbourg1 as the crow flies2 and we are told that1 not only was it audible in its general effect1 but the report of individual guns was distinctly recognized4 ,the artillery of ,waterloo is said to have been heard at the town of ,creil1 in ,france1 #aae miles from the field of battle2 and the cannonading at the siege of ,valenciennes1 in #agic1 was heard1 from day to day1 at ,deal1 on the coast of ,england1 a distance of #abj miles4#ae ,so far1 ,i have endeavored to set forth some general ideas on the nature and origin of lightning1 and of the thunder that accompanies it4 ,in my next ,lecture ,i propose to give a short account of the destructive effects of lightning1 and to consider how these effects may best be averted by means of lightning conductors4 ,,note ,,to ,,page #bj4 ,,on ,,the ,,high ,,potential ,,of ,a ,,flash ,,of ,,lightning4 ,the potential of an electrified sphere is equal to the quantity of electricity with which the sphere is charged1 divided by the radius of the sphere4 ,now the minute cloud particles1 which go to make up a drop of rain1 may be taken to be very small spheres2 and if v represent the potential of each one1 q the quantity of electricity with which it is charged1 and r the radius of the sphere1 we have v q_/r4 ,suppose #a1jjj of these cloud particles to unite into one2 the quantity of electricity in the drop1 thus formed1 will be #a1jjjq2 and the radius1 which increases in the ratio of the cube root of the volume1 will be #ajr4 ,therefore the potential of the new sphere will be #ajjjq_/#ajr1 or #ajjq_/r2 that is to say1 it will be #ajj times as great as the potential of each of the cloud particles which compose it4 ,when a million of cloud particles are blended into a single drop1 the same process will show that the potential has been increased ten thousandfold2 and when a drop is produced by the agglomeration of a million of millions of cloud particles1 the potential of the drop will be a hundred million times as great as that of the individual particles4#af ,,footnotes3 #a 8,il y a des grands seigneurs dont il ne faut approcher qu'avec d'extrmes prcautions4 ,le tonnerre est de ce nombre40--,dict4 ,philos4 art4 ,foudre4 #b ,electricit ,statique1 ii41 #efa4 #c ,deschanel's ,natural ,philosophy1 ,sixth ,edition1 p4 #fda4 #d ,fragments of ,science1 ,fifth ,edition1 p4 #caa4 #e ,lecture on ,thunderstorms1 ,nature1 vol4 xxii41 p4 #cda4 #f ,third ,series1 vol4 v41 p4 #afa4 #g ,phil4 ,trans4 ,royal ,society1 #ahcd1 vol4 cxxv41 pp4 #ehc-eia4 #h ,in experiments with a ,leyden jar1 ,feddersen has shown that the duration of the discharge is increased1 not only by increasing the striking distance1 but also by increasing the size of the jar4 ,now1 a flash of lightning may be regarded as the discharge of a ,leyden jar of immense size1 with an enormous striking distance2 and therefore we should expect that the duration of the discharge should be greatly prolonged4 ,see ,american ,journal of ,science and ,arts1 ,third ,series1 vol4 i41 p4 #ae4 #i ,see original paper by ,swan1 ,trans4 ,royal ,society1 ,edinburgh1 #ahdi1 vol4 xvi41 pp4 #eha-fjc2 also1 a second paper1 ib4 #ahfa1 vol4 xxii41 pp4 #cc-ci4 #aj ,nature1 vol4 xxviii41 p4 #ed4 #aa ,see1 however1 an attempt to account for this phenomenon in ,de ,larive's ,treatise on ,electricity1 ,london1 #ahec-h1 vol4 iii41 pp4 #aii1 #bjj2 and another1 quite recently1 by ,mr4 ,spottiswoode1 in a ,lecture on the ,electrical ,discharge1 delivered before the ,british ,association at ,york1 in ,september1 #ahha1 and published by ,longmans1 ,london1 p4 #db4 ,see also1 for recent evidence regarding the phenomenon itself1 ,scott's ,elementary ,meteorology1 pp4 #age-h4 #ab ,see ,jamin1 8,cours de ,physique10 i41 #dhj-a2 ,tomlinson1 8,the ,thunderstorm10 ,third ,edition1 pp4 #ie-ajc2 8,thunderstorms10 a ,lecture by ,professor ,tait1 ,nature1 vol4 xxii41 p4 #cef4 #ac ,professor ,tait1 ,on ,thunderstorms1 ,nature1 vol4 xxii41 pp4 #dcf-g4 #ad ,see note at the end of this ,lecture1 p4 #bf4 #ae ,see ,tomlinson1 ,the ,thunderstorm1 pp4 #hg-i4 #af ,see ,tait on ,thunderstorms1 ,nature1 vol4 xxii41 p4 #dcf4 ,,lecture ,,ii4 ,,lightning ,,conductors4 ,the effects of lightning1 on the bodies that it strikes1 are analogous to those which may be produced by the discharge of our electric machines and ,leyden jar batteries4 ,when the discharge of a battery traverses a metal conductor of sufficient dimensions to allow it an easy passage1 it makes its way along silently and harmlessly4 ,but if the conductor be so thin as to offer considerable resistance1 then the conductor itself is raised to intense heat1 and may be melted1 or even converted into vapor1 by the discharge4 ,on opposite page is shown a board on which a number of very thin wires have been stretched1 over white paper1 between brass balls4 ,the wires are so thin that the full charge of the battery before you1 which consists of nine large ,leyden jars1 is quite sufficient to convert them in an instant into vapor4 ,i have already1 on former occasions1 sent the charge through two of these wires1 and nothing remains of them now but the traces of their vapor1 which mark the path of the electric discharge from ball to ball4 ,at the present moment the battery stands ready charged1 and ,i am going to discharge it through a third wire1 by means of this insulated rod which ,i hold in my hand4 ,the discharge has passed2 you saw a flash1 and a little smoke2 and now1 if you look at the paper1 you will find that the wire is gone1 but that it has left behind the track of its incandescent vapor1 marking the path of the discharge4 ,illustration3 ,,discharge ,,of ,,leyden ,,jar ,,battery ,,through ,,thin ,,wires4 ,destruction of ,buildings by ,lightning4--,we learn from this experiment that the electricity stored up in our battery passes1 without visible effect1 through the stout wire of a discharging rod1 but that it instantly converts into vapor the thin wire stretched across the spark board4 ,and so it is with a flash of lightning4 ,it passes harmlessly1 as every one knows1 through a stout metal rod1 but when it comes across bell wires or telegraph wires1 it melts them1 or converts them into vapor4 ,on the sixteenth of ,july1 #agei1 a flash of lightning struck a house in ,southwark1 on the south side of ,london1 and followed the line of the bell wire4 ,after the lightning had passed1 the wire was no longer to be found2 but the path of the lightning was clearly marked by patches of vapor which were left1 here and there1 adhering to the surface of the wall4 ,in the year #aged1 the lightning fell on a bell tower at ,newbury1 in the ,united ,states of ,america1 and having dashed the roof to pieces1 and scattered the fragments about1 it reached the bell4 ,from this point it followed an iron wire1 about as thick as a knitting needle1 melting it as it passed along1 leaving behind a black streak of vapor on the surface of the walls4 ,again1 the electric discharge1 passing through a bad conductor1 produces mechanical disturbance1 and1 if the substance be combustible1 often sets it on fire4 ,so1 too1 as you know1 the lightning flash1 falling on a church spire1 dashes it to pieces1 knocking the stones about in all directions1 while it sets fire to ships and wooden buildings2 and more than once it has caused great devastation by exploding powder magazines4 ,let me give you one or two examples3 ,in ,january1 #agfb1 the lightning fell on a church tower in ,cornwall1 and a stone--three hundred-weight--was torn from its place and hurled to a distance of #ahj feet1 while a smaller stone was projected as far as #a1bjj feet from the building4 ,again1 in #ahji1 the lightning struck a house not far from ,manchester1 and literally moved a massive wall twelve feet high and three thick to a distance of several feet4 ,you may form some conception of the enormous force here brought into action1 when ,i tell you that the total weight of mason-work moved on this occasion was not less than twenty-three tons4 ,the church of ,st4 ,george1 at ,leicester1 was severely damaged by lightning on the #ast of ,august1 #ahdf4 ,about #h o'clock in the evening the rector of the parish saw a vivid streak of light darting with incredible velocity against the upper part of the spire4 8,for the distance of forty feet on the eastern side1 and nearly seventy on the west1 the massive stonework of the spire was instantly rent asunder and laid in ruins4 ,large blocks of stone were hurled in all directions1 broken into small fragments1 and in some cases1 there is reason to believe1 reduced to powder4 ,one fragment of considerable size was hurled against the window of a house three hundred feet distant1 shattering to pieces the woodwork1 and strewing the room within with fine dust and fragments of glass4 ,it has been computed that a hundred tons of stone were1 on this occasion1 blown to a distance of thirty feet in three seconds4 ,in addition to the shivering of the spire1 the pinnacles at the angles of the tower were all more or less damaged1 the flying buttresses cracked through and violently shaken1 many of the open battlements at the base of the spire knocked away1 the roof of the church completely riddled1 the roofs of the side entrances destroyed1 and the stone staircases of the gallery shattered40#ag ,lightning has been at all times the cause of great damage to property by its power of setting fire to whatever is combustible4 ,fuller says1 in his ,church ,history1 that 8scarcely a great abbey exists in ,england which once1 at least1 has not been burned by lightning from heaven40 ,he mentions1 as examples1 the ,abbey of ,croyland twice burned1 the ,monastery of ,canterbury twice1 the ,abbey of ,peterborough twice2 also the ,abbey of ,st4 ,mary's1 in ,yorkshire1 the ,abbey of ,norwich1 and several others4 ,sir ,william ,snow ,harris1 writing about twenty years ago1 tells us that 8the number of churches and church spires wholly or partially destroyed by lightning is beyond all belief1 and would be too tedious a detail to enter upon4 ,within a comparatively few years1 in #ahbb for instance1 we find the magnificent ,cathedral of ,rouen burned1 and1 so lately as #ahej1 the beautiful ,cathedral of ,saragossa1 in ,spain1 struck by lightning during divine service and set on fire4 ,in ,march of last year a dispatch from our ,minister at ,brussels1 ,lord ,howard de ,walden1 dated the #bdth of ,february1 was forwarded by ,lord ,russell to the ,royal ,society1 stating that1 on the preceding ,sunday1 a violent thunderstorm had spread over ,belgium2 that twelve churches had been struck by lightning2 and that three of these fine old buildings had been totally destroyed40#ah ,even in our own day the destruction caused by fires produced through the agency of lightning is very great--far greater than is commonly supposed4 ,no general record of such fires is kept1 and consequently our information on the subject is very incomplete and inexact4 ,i may tell you1 however1 one small fact which1 so far as it goes1 is precise enough and very significant4 ,in the little province of ,schleswig-,holstein1 which occupies an area less than one-fourth of the area of ,ireland1 the ,provincial ,fire ,assurance ,association has paid in sixteen years1 for damage caused by lightning1 somewhat over #ajj1jjj1 or at the rate of more than #f1jjj a year4 ,the total loss of property every year in this province1 due to fires caused by lightning1 is estimated at not less than #ab1ejj4ai ,destruction of ,ships at ,sea4--,the destructive effects of lightning on ships at sea1 before the general adoption of lightning conductors1 seems almost incredible at the present day4 ,from official records it appears that the damage done to the ,royal ,navy of ,england alone involved an expenditure of from #f1jjj to #aj1jjj a year4 ,we are told by ,sir ,william ,snow ,harris1 who devoted himself for many years to this subject with extraordinary zeal and complete success1 that between the year #ahaj and the year #ahae--that is1 within a period of five years--8no less than forty sail of the line1 twenty frigates1 and twelve sloops and corvettes were placed hors de combat by lightning4 ,in the merchant navy1 within a comparatively small number of years1 no less than thirty-four ships1 most of them large vessels with rich cargoes1 have been totally destroyed--been either burned or sunk--to say nothing of a host of vessels partially destroyed or severely damaged40#bj ,and these statements1 be it observed1 take no account of ships that were simply reported as missing1 some of which1 we can hardly doubt1 were struck by lightning in the open sea1 and went down with all hands on board4 ,a famous ship of forty-four guns1 the ,resistance1 was struck by lightning in the ,straits of ,malacca1 and the powder magazine exploding1 she went to the bottom4 ,of her whole crew only three were saved1 who happened to be picked up by a passing boat4 ,it has been well observed that1 were it not for these three chance survivors1 nothing would have been known concerning the fate of the vessel1 and she would have been simply recorded as missing in the ,admiralty lists4 ,nothing is more fearful to contemplate than the scene on board a ship when she is struck by lightning in the open sea1 with the winds howling around1 the waves rolling mountains high1 the rain coming down in torrents1 and the vivid flashes lighting up the gloom at intervals1 and carrying death and destruction in their track4 ,i will read you one or two brief accounts of such a scene1 given in the pithy but expressive language of the sailor4 ,in ,january1 #aghf1 the ,thisbe1 of thirty-six guns1 was struck by lightning off the coast of ,scilly1 and reduced to the condition of a wreck4 ,here is an extract from the ship's log3 8,four ,a4 ,m41 strong gales2 handed mainsail and main top-sail2 hove to with storm staysails2 blowing very heavy1 ,s4 ,e4 #d4ae1 a flash of lightning1 with tremendous thunder1 disabled some of our people4 ,a second flash set the mainsail1 main-top1 and mizen staysails on fire4 ,obliged to cut away the mainmast2 this carried away mizen top-mast and fore top-sail yard4 ,found foremast also shivered by the lightning4 ,fore top-mast went over the side about #i ,a4 ,m4 ,set the foresail40#ba ,a few years later1 in ,march1 #agif1 the ,lowestoffe was struck in the ,mediterranean1 and we read as follows in the log of the ship3 8,north end of ,minorca2 heavy squalls2 hail1 rain1 thunder1 and lightning4 #ab4ae1 ship struck by lightning1 which knocked three men from the masthead1 one killed4 #ab4cj1 ship again struck2 main top-mast shivered in pieces2 many men struck senseless on the decks4 ,ship again struck1 and set on fire in the masts and rigging2 mainmast shivered in pieces2 fore top-mast shivered2 men benumbed on the decks1 and knocked out of the top2 one man killed on the spot4 #a4cj1 cut away the mainmast2 employed clearing wreck4 #d1 moderate2 set the foresail40#bb ,again1 in #ahaj1 the ,repulse1 a ship of seventy-four guns1 was struck1 off the coast of ,spain4 8,the wind had been variable in the morning--and at #ab4ce there was a heavy squall1 with rain1 thunder1 and lightning4 ,the ship was struck by two vivid flashes of lightning1 which shivered the maintop-gallant mast1 and severely damaged the mainmast4 ,seven men were killed on the spot2 three others only survived a few days2 and ten others were maimed for life4 ,after the second discharge the rain fell in torrents4 ,the ship was more completely crippled than if she had been in action1 and the squadron1 then engaged on a critical service1 lost for a time one of its fastest and best ships40#bc ,destruction of ,powder ,magazines4--,not less appalling is the devastation caused by lightning when it falls on a powder magazine4 ,here is a striking example3 ,on the eighteenth of ,august1 #agfi1 the tower of ,st4 ,nazaire1 at ,brescia1 was struck by lightning4 ,underneath the tower about #bjj1jjj pounds of gunpowder1 belonging to the ,republic of ,venice1 were stored in vaults4 ,the powder exploded1 leveling to the ground a great part of the beautiful city of ,brescia1 and burying thousands of its inhabitants in the ruins4 ,it is said that the tower itself was blown up bodily to a great height in the air1 and came down in a shower of stones4 ,this is1 perhaps1 the most fearful disaster of the kind on record4 ,but we are not without examples in our own times4 ,in the year #ahef the lightning fell on the ,church of ,st4 ,john1 in the ,island of ,rhodes4 ,a large quantity of gunpowder had been deposited in the vaults of the church4 ,this was ignited by the flash2 the building was reduced to a mass of ruins1 a large portion of the town was destroyed1 and a considerable number of the inhabitants were killed4 ,again1 in the following year1 the magazine of ,joudpore1 in the ,bombay ,presidency1 was struck by lightning4 ,many thousand pounds of gunpowder were blown up1 five hundred houses were destroyed1 and nearly a thousand people are said to have been killed4#bd ,experimental ,illustrations4--,and now1 before proceeding further1 ,i will make one or two experiments1 with a view of showing that the electricity of our machines is capable of producing effects similar to those produced by lightning1 though immeasurably inferior in point of magnitude4 ,here is a common tumbler1 about three-quarters full of water4 ,into it ,i introduce two bent rods of brass1 which are carefully insulated below the surface of the water by a covering of india-rubber4 ,the points1 however1 are exposed1 and come to within an inch of one another1 near the bottom of the tumbler4 ,outside the tumbler1 the brass rods are mounted on a stand1 by means of which ,i can send the full charge of this ,leyden jar battery through the water1 from point to point4 ,since water is a bad conductor of electricity1 as compared with metals1 the charge encounters great resistance in passing through it1 and in overcoming this resistance produces considerable mechanical commotion1 which is usually sufficient to shiver the glass to pieces4 ,to charge the battery will take about twenty turns of this large ,holtz machine4 ,observe how the pith ball of the electroscope rises as the machine is worked1 showing that the charge is going in4 ,and now it remains stationary2 which is a sign that the battery is fully charged1 and can receive no more4 ,you will notice that the outside coating of the battery has been already connected with one of the brass rods dipping into the tumbler of water4 ,by means of this discharger ,i will now bring the inside coating into connection with the other rod4 ,and see1 before contact is actually made1 the spark has leaped across1 and our tumbler is violently burst asunder from top to bottom4 ,illustration3 ,,glass ,,vessel ,,broken ,,by ,,discharge ,,of ,,leyden ,,jar ,,battery4 ,this will probably appear to you a very small affair1 when compared with the tearing asunder of solid masonry1 and the hurling about of stones by the ton weight4 ,no doubt it is2 and that is just one of the lessons we have to learn from the experiment we have made4 ,for1 not only does it show us that effects of this kind may be caused by electricity artificially produced1 but it brings home forcibly to the mind how incomparably more powerful is the lightning of the clouds than the electricity of our machines4 ,the property which electricity has of setting fire to combustible substances may be easily illustrated4 ,this india-rubber tube is connected with the gas pipe under the floor1 and to the end of the tube is fitted a brass stop-cock which ,i hold in my hand4 ,i open the cock1 and allow the jet of gas to flow toward the conductor of ,carr's machine1 while my assistant turns the handle2 a spark passes1 and the gas is lit4 ,again1 my assistant stands on this insulating stool1 placing his hand on the large conductor of the machine1 while ,i turn the handle4 ,his body becomes electrified1 and when he presents his knuckle to this vessel of spirits of wine1 which is electrically connected with the earth1 a spark leaps across1 and the spirits of wine are at once in a blaze4 ,once more2 ,i tie a little gun-cotton around one knob of the discharging rod1 and then use it to discharge a small ,leyden jar2 at the moment of the discharge the gun-cotton is set on fire4 ,it would be easy to explode gunpowder with the electric spark1 but the smoke of the explosion would make the lecture-hall very unpleasant for the remainder of the lecture4 ,i propose1 therefore1 to substitute for gunpowder an explosive mixture of oxygen and hydrogen1 with which ,i have filled this little metal flask1 commonly known as ,volta's pistol4 ,by a very simple contrivance1 the electric spark is discharged through the mixture1 when ,i hold the flask toward the conductor of the machine4 ,a cork is fitted tightly into the neck of the flask1 and at the moment the spark passes you hear a loud explosion1 and you see the cork driven violently up to the ceiling4 ,illustration3 ,,gun-,,cotton ,,set ,,on ,,fire ,,by ,,electric ,,spark4 ,destruction of ,life4--,the last effect of lightning to which ,i shall refer1 and which1 perhaps1 more than any other1 strikes us with terror1 is the sudden and utter extinction of life1 when the lightning flash descends on man or on beast4 ,so swift is this effect1 in most cases1 that death is1 in all probability1 absolutely painless1 and the victim is dead before he can feel that he is struck4 ,i cannot give you1 with any degree of exactness1 the number of people killed every year by lightning1 because the record of such deaths has been hitherto very imperfectly kept1 in almost all countries1 and is1 beyond doubt1 very incomplete4 ,but perhaps you will be surprised to learn that the number of deaths by lightning actually recorded is1 on an average1 in ,england about #bb every year1 in ,france #hj1 in ,prussia #aaj1 in ,austria #bab1 in ,european ,russia #ddj4be ,so far as can be gathered from the existing sources of information1 it would seem that the number of persons killed by lightning is1 on the whole1 about one in three of those who are struck4 ,the rest are sometimes only stunned1 sometimes more or less burned1 sometimes made deaf for a time1 sometimes partially paralyzed4 ,on particular occasions1 however1 especially when the lightning falls on a large assembly of people1 the number of persons struck down and slightly injured1 in proportion to the number killed1 is very much increased4 ,an interesting case of this kind is reported by ,mr4 ,tomlinson4 8,on the twenty-ninth of ,august1 #ahdg1 at the parish church of ,welton1 ,lincolnshire1 while the congregation were engaged in singing the hymn before the sermon1 and the ,rev4 ,mr4 ,williamson had just ascended the pulpit1 the lightning was seen to enter the church from the belfry1 and instantly an explosion occurred in the centre of the edifice4 ,all that could move made for the door1 and ,mr4 ,williamson descended from the pulpit1 endeavoring to allay the fears of the people4 ,but attention was now called to the fact that several of the congregation were lying in different parts of the church1 apparently dead1 some of whom had their clothing on fire4 ,five women were found injured1 and having their faces blackened and burned1 and a boy had his clothes almost entirely consumed4 ,a respected old parishioner1 ,mr4 ,brownlow1 aged sixty-eight1 was discovered lying at the bottom of his pew1 immediately beneath one of the chandeliers1 quite dead4 ,there were no marks on the body1 but the buttons of his waistcoat were melted1 the right leg of his trousers torn down1 and his coat literally burnt off4 ,his wife in the same pew received no injury40#bf ,illustration3 ,,volta',s ,,pistol2 ,,explosion ,,caused ,,by ,,electric ,,spark4 ,not less striking is the story told by ,dr4 ,plummer1 surgeon of the ,illinois ,volunteers1 in the ,medical and ,surgical ,reporter of ,june #ai1 #ahfe3 8,our regiment was yesterday the scene of one of the most terrible calamities which it has been my lot to witness4 ,about two o'clock a violent thunderstorm visited us4 ,while the old guard was being turned out to receive the new1 a blinding flash of lightning was seen1 accompanied instantly by a terrific peal of thunder4 ,the whole of the old guard1 together with part of the new1 were thrown violently to the earth4 ,the shock was so severe and sudden that1 in most cases1 the rear rank men were thrown across the front rank men4 ,one man was instantly killed1 and thirty-two men were more or less severely burned by the electric fluid4 ,in some instances the men's boots and shoes were rent from their feet and torn to pieces1 and1 strange as it may appear1 the men were injured but little in the feet4 ,in all cases the burns appear as if they had been caused by scalding-hot water1 in many instances the skin being shriveled and torn off4 ,the men all seem to be doing well1 and a part of them will be able to resume their duties in a few days40 ,the ,return ,shock4--,it sometimes happens that people are struck down and even killed at the moment a discharge of lightning takes place between a cloud and the earth1 though they are very far from the point where the flash is actually seen to pass2 while others1 who are situated between them and the lightning1 suffer very little1 or perhaps not at all4 ,this curious phenomenon was first carefully investigated by ,lord ,mahon in the year #aggi1 and was called by him the 8return shock40 ,his theory1 which is now commonly accepted1 may be easily understood with the aid of the sketch before you4 ,illustration3 ,,the ,,return ,,shock ,,illustrated4 ,let us suppose ,,abc to represent the outline of a thundercloud which dips down toward the earth at ,a and at ,c4 ,the electricity of the cloud develops by inductive action a charge of the opposite kind in the earth beneath it4 ,but the inductive action is most powerful at ,e and ,f1 where the cloud comes nearest to the earth4 ,hence1 bodies situated near these points may be very highly electrified as compared with bodies at a point between them1 such as ,d4 ,now1 when a flash of lightning passes at ,e1 the under part of the cloud is at once relieved of its electricity1 its inductive action ceases1 and1 therefore1 a person situated at ,f suddenly ceases to be electrified4 ,this sudden change from a highly electrified to a neutral state involves a shock to his system which may be severe enough to stun or even to kill him4 ,meanwhile1 people at ,d1 having been also electrified to some extent by the influence of the thundercloud1 must in like manner undergo a change in their electrical condition when the flash of lightning passes1 but this change will be less violent because they were less highly electrified4 ,many experiments have been devised to illustrate this theory of ,lord ,mahon4 ,but the best illustration ,i know is furnished by this electric machine of ,carr's4 ,if you stand near one end of the large conductor when the machine is in action and sparks are taken from the other end1 you will feel a distinct electric shock every time a spark passes4 ,the large conductor here takes the place of the cloud1 the spark that passes at one end represents the flash of lightning1 and the observer at the other end gets the return shock1 though he is at a considerable distance from the point where the flash is seen4 ,an experiment of this kind1 of course1 cannot be made sensible to a large audience like the present4 ,but ,i can give you a good idea of the effect by means of this tuft of colored papers4 ,while the machine is in action ,i hold the tuft of papers near that end of the conductor which is farthest from the point where the discharge takes place4 ,you see the paper ribbons are electrified by induction1 and1 in virtue of mutual repulsion1 stand out from one another 8like quills upon the fretful porcupine40 ,but1 when a spark passes1 the inductive action ceases1 the paper ribbons cease to be electrified1 and the whole tuft suddenly collapses into its normal state4 ,while fully accepting ,lord ,mahon's theory of the return shock as perfectly good so far as it goes1 ,i would venture to point out another influence which must often contribute largely to produce the effect in question1 and which is not dependent on the form of the cloud4 ,it may easily happen1 from the nature of the surface in the district affected by a thundercloud1 that the point of most intense electrification--say ,e in the figure--is in good electrical communication with a distant point1 such as ,f1 while it is very imperfectly connected with a much nearer point1 ,d4 ,in such a case it is evident that bodies at ,f will share largely in the highly-electrified condition of ,e1 and also share largely in the sudden change of that condition the moment the flash of lightning passes2 whereas bodies at ,d will be less highly electrified before the discharge1 and less violently disturbed when the discharge takes place4 ,this principle may be illustrated by a very simple experiment4 ,here is a brass chain about twenty feet long4 ,one end of it ,i hand to any one among the audience who will kindly take hold of it2 the other end ,i hold in my hand4 ,i now stand near the conductor of the machine2 and will ask some one to stand about ten feet away from me1 near the middle of the chain1 but without touching it4 ,now observe what happens when the machine is worked and ,i take a spark from the conductor3 ,my friend at the far end of the chain1 twenty feet away1 gets a shock nearly as severe as the one ,i get myself1 because he is in good electrical communication with the point where the discharge takes place4 ,but my more fortunate friend1 who is ten feet nearer to the flash1 is hardly sensible of any effect1 because he is connected with me only through the floor of the hall1 which is1 comparatively speaking1 a bad conductor of electricity4 ,summary4--,let me now briefly sum up the chief destructive effects of lightning4 ,first1 with regard to good conductors3 though it passes harmlessly through them if they be large enough to afford it an easy passage1 it melts and converts them into vapor if they be of such small dimensions as to offer considerable resistance4 ,secondly1 lightning acts with great mechanical force on bad conductors2 it is capable of tearing asunder large masses of masonry1 and of projecting the fragments to a considerable distance4 ,thirdly1 it sets fire to combustible materials4 ,and lastly1 it causes the instantaneous death of men and animals4 ,franklin's ,lightning ,rods4--,the object of lightning conductors is to protect life and property from these destructive effects4 ,their use was first suggested by ,franklin1 in #agdi1 even before his famous experiment with the kite2 and immediately after that experiment1 in #ageb1 he set up1 on his own house1 in ,philadelphia1 the first lightning conductor ever made4 ,he even devised an ingenious contrivance1 by means of which he received notice when a thundercloud was approaching4 ,the contrivance consisted of a peal of bells1 which he hung on his lightning conductor1 and which were set ringing whenever the lightning conductor became charged with electricity4 ,franklin's lightning rods were soon adopted in ,america2 and he himself contributed very much to their popularity by the simple and lucid instructions he issued every year1 for the benefit of his countrymen1 in the annual publication known as 8,poor ,richard's ,almanac40 ,it is very interesting at this distance of time to read the homely practical rules laid down by this great philosopher and statesman2 and1 though some modifications have been suggested by the experience of a hundred and thirty years1 especially as regards the dimensions of the lightning conductor1 it is surprising to find how accurately the general principles of its construction1 and of its action1 are here set forth4 8,it has pleased ,god10 he says1 8in ,his goodness to mankind1 at length to discover to them the means of securing their habitations and other buildings from mischief by thunder and lightning4 ,the method is this3 ,provide a small iron rod1 which may be made of the rod-iron used by nailors1 but of such a length that one end being three or four feet in the moist ground1 the other may be six or eight feet above the highest part of the building4 ,to the upper end of the rod fasten about a foot of brass wire1 the size of a common knitting needle1 sharpened to a fine point2 the rod may be secured on the house by a few small staples4 ,if the house or barn be long1 there may be a rod and point at each end1 and a middling wire along the ridge from one to the other4 ,a house thus furnished will not be damaged by lightning1 it being attracted by the points and passing through the metal into the ground1 without hurting anything4 ,vessels also having a sharp-pointed rod fixed on the top of their masts1 with a wire from the foot of the rod reaching down round one of the shrouds to the water1 will not be hurt by lightning40 ,introduction of ,lightning ,rods into ,england4--,the progress of lightning conductors was more slow in ,england and on the ,continent of ,europe1 owing to a fear1 not unnatural1 that they might1 in some cases1 draw down the lightning where it would not otherwise have fallen4 ,people preferred to take their chance of escaping as they had escaped before1 rather than invite1 as it were1 the lightning to descend on their houses1 in the hope that an iron rod would convey it harmless to the earth4 ,but the immense amount of damage done every year by lightning1 soon led practical men to entertain a proposal which offered complete immunity from all danger on such easy terms2 and when it was found that buildings protected by lightning conductors were1 over and over again1 struck by lightning without suffering any harm1 a general conviction of their utility was gradually established in the public mind4 ,the first public building protected by a lightning rod in ,england was ,st4 ,paul's ,cathedral1 in ,london4 ,on the eighteenth of ,june1 #agfd1 the beautiful steeple of ,saint ,bride's ,church1 in the city1 was struck by lightning and reduced to ruin4 ,this incident awakened the attention of the dean and chapter of ,st4 ,paul's to the danger of a similar calamity1 which seemed1 as it were1 impending over their own church4 ,after long deliberation1 they referred the matter to the ,royal ,society1 asking for advice and instruction4 ,a committee of scientific men was appointed by the ,royal ,society to consider the question4 ,benjamin ,franklin himself1 who happened to be in ,london at the time1 as the representative of the ,american ,states in their dispute with ,england1 was nominated a member of the committee4 ,and the result of its deliberation was that1 in the year #agfi1 a number of lightning conductors were erected on ,st4 ,paul's ,cathedral4 ,it was on this occasion that arose the celebrated controversy about the respective merits of points and balls4 ,franklin had recommended a pointed conductor2 but some members of the committee were of opinion that the conductor should end in a ball and not in a point4 ,the decision of the committee was in favor of ,franklin's opinion1 and pointed conductors were accordingly adopted for ,st4 ,paul's ,cathedral4 ,but the controversy did not end here4 ,the time was one of great political excitement1 and party spirit infused itself even into the peaceful discussions of science4 ,the weight of scientific opinion was on the side of ,franklin2 but it was hinted1 on the other side1 that the pointed conductors were tainted with republicanism1 and pregnant with danger to the empire4 ,as a rule1 the whigs were strongly in favor of points2 while the ,tories were enthusiastic in their support of balls4 ,for a time the ,tories seemed to prevail4 ,the king was on their side4 ,experiments on a grand scale were conducted in his presence1 at the ,pantheon1 a large building in ,oxford street2 he was assured that these experiments proved the great superiority of balls over points2 and to give practical effect to his convictions1 his majesty directed that a large cannon ball should be fixed on the end of the lightning conductor attached to the royal palace at ,kew4 ,but the committee of the ,royal ,society remained unconvinced4 ,in course of time the heat of party spirit abated2 experience as well as reason was found to be in favor of ,franklin's views2 and the battle of the balls and points has long since passed into the domain of history4#bg ,functions of a ,lightning ,conductor4--,a lightning conductor fulfills two functions4 ,first1 it favors a silent and gradual discharge of electricity between the cloud and the earth1 and thus tends to prevent that accumulation which must of necessity take place before a flash of lightning will pass4 ,secondly1 if a flash of lightning come1 the lightning conductor offers it a safe channel through which it may pass harmless to the earth4 ,these two functions of a lightning conductor may be easily illustrated by experiment4 ,when our machine is in action1 if ,i present my closed hand to the large brass conductor1 a spark passes between them1 and ,i feel1 at the same moment1 a slight electric shock4 ,here the conductor of the machine1 as usual1 holds the place of the electrified cloud2 my closed hand represents1 as it were1 a lofty building that stands out prominently on the surface of the earth2 the spark is the flash of lightning1 and the electric shock just suggests the destructive power of the sudden disruptive discharge4 ,now let me protect this building by a lightning conductor4 ,for this purpose1 ,i take in my hand a brass rod1 which ,i connect with the earth by a brass chain4 ,in the first instance1 ,i will have a metal ball on the end of my lightning conductor4 ,you see the effect2 sparks pass rapidly1 but ,i feel no shock4 ,i can increase the strength of the discharge by hanging this condensing jar on the conductor of the machine4 ,sparks pass now1 much more brilliant and powerful than before1 but still ,i get no shock4 ,it is evident1 therefore1 that my lightning rod does not prevent the flash from passing1 but it conveys it harmless to the ground4 ,i next take a rod which is sharply pointed1 and connecting it as before with the earth by a brass chain1 ,i present the sharp point to the conductor of the machine4 ,observe how different is the result2 there is no disruptive discharge2 no spark passes2 no shock is felt4 ,electricity still continues to be generated in the machine1 and electricity is generated1 by induction1 in the brass rod1 and in my body4 ,but these two opposite electricities discharge themselves silently1 by means of this pointed rod1 and no sensible effect of any kind is exhibited4 ,these experiments are very simple1 but they really put before us1 in the clearest possible way1 the whole theory of lightning conductors4 ,in particular1 they give us ocular demonstration that an efficient lightning rod not only makes the lightning harmless when it comes1 but tends very much to prevent its coming4 ,a remarkable example1 on a large scale1 of this important property1 is furnished by the town of ,pietermaritzburg1 the capital of the colony of ,natal1 in ,south ,africa4 ,this town is subject to the frequent visitation of thunderstorms1 at certain seasons of the year1 and much damage was formerly done by lightning1 but since the erection of lightning conductors on the principal buildings1 the lightning has never fallen within the town4 ,thunderclouds come as before1 but they pass silently over the city1 and only begin to emit their lightning flashes when they reach the open country1 and have passed beyond the range of the lightning conductors4#bh ,but it will often happen1 even in the case of a pointed conductor1 that the accumulation of electricity goes on so fast that the silent discharge is insufficient to keep it in check4 ,a disruptive discharge will then take place1 from time to time1 and a flash of lightning will pass4 ,under these circumstances1 the lightning conductor is called upon to fulfill its second function1 and to convey the lightning harmless to the earth4 ,conditions of a ,lightning ,conductor4--,from the consideration of the functions which it has to fulfill1 we may now infer what are the conditions necessary for an efficient lightning conductor4 ,the first condition is that the end of the conductor1 projecting into the air1 should have1 at least1 one sharp point4 ,our experiments have shown us that a pointed conductor tends1 in a manner1 to suppress the flash of lightning altogether2 whereas a blunt conductor1 or one ending in a ball1 tends only to make it harmless when it comes4 ,it is evident1 therefore1 that the pointed conductor offers the greater security4 ,but a fine point is very liable to be melted when the lightning falls upon it1 and thus to be rendered less efficient for future service4 ,to meet this danger1 it has recently been suggested1 by the ,lightning ,rod ,conference1 that the extreme end of the conductor should be a blunt point1 destined to receive the full force of the lightning flash1 when it comes2 and that1 a little lower down1 a number of very fine points should be provided1 with a view to favor the silent discharge4 ,this suggestion1 which appears admirably fitted to provide for the twofold function of a lightning conductor1 deserves to be recorded in the exact terms of the official report4 8,it seems best to separate the double functions of the point1 prolonging the upper terminal to the very summit1 and merely beveling it off1 so that1 if a disruptive discharge does take place1 the full conducting power of the rod may be ready to receive it4 ,at the same time1 having regard to the importance of silent discharge from sharp points1 we suggest that1 at one foot below the extreme top of the upper terminal1 there be firmly attached1 by screws and solder1 a copper ring bearing three or four copper needles1 each six inches long1 and tapering from a quarter of an inch diameter to as fine a point as can be made2 and with the object of rendering the sharpness as permanent as possible1 we advise that they be platinized1 gilded1 or nickel plated40#bi ,the second condition of a lightning conductor is1 that it should be made of such material1 and of such dimensions1 as to offer an easy passage to the greatest flash of lightning likely to fall on it2 otherwise it might be melted by the discharge1 and the lightning1 seeking for itself another path1 might force its way through bad conductors1 which it would partly rend asunder1 and partly consume by fire4 ,copper is now generally regarded as the best material for lightning conductors1 and it is almost universally employed in these countries4 ,if it is used in the form of a rope1 it should not be less than half an inch in diameter2 if a band of copper is preferred--and it is often found more convenient by builders--it should be about an inch and a half broad and an eighth of an inch thick4 ,in ,france it has been hitherto more usual to employ iron rods for lightning conductors1 but since iron is much inferior to copper in its conducting power1 the iron rod must be of much larger dimensions2 it should be at least one inch in diameter4#cj ,the third condition is that the lightning conductor should be continuous throughout its whole length1 and should be placed in good electrical contact with the earth4 ,this is a condition of the first importance1 and experience has shown that it is the one most likely of all to be neglected4 ,in a large town the best earth connection is furnished by the system of water-mains and gas-mains1 each of which constitutes a great network of conductors everywhere in contact with the earth4 ,two points1 however1 must be carefully attended to--first1 that the electrical contact between the lightning conductor and the metal pipe should be absolutely perfect2 and1 secondly1 that the pipe selected should be of such large dimensions as to allow the lightning an easy passage through it to the principal main4 ,if no such system of water-pipes or gas-pipes is at hand1 then the lightning rod should be connected with moist earth by means of a bed of charcoal or a metal plate not less than three feet square4 ,this metal plate should be always of the same material as the conductor1 otherwise a galvanic action would be set up between the two metals1 which in course of time might seriously damage the contact4 ,dry earth1 sand1 rock1 and shingle are bad conductors2 and1 if such materials exist near the surface of the earth1 the lightning rod must pass through them and be carried down until it reaches water or permanently damp earth4 ,mischief ,done by ,bad ,conductors4--,if the earth contact is bad1 a lightning conductor does more harm than good4 ,it invites the lightning down upon the building without providing for it1 at the same time1 a free passage to earth4 ,the consequence is that the lightning forces a way for itself1 violently bursting asunder whatever opposes its progress1 and setting fire to whatever is combustible4 ,i will give you some recent and striking examples4 ,in the month of ,may1 #ahgi1 the church of ,laughton-en-le-,morthen1 in ,england1 though provided with a conductor1 was struck by lightning and sustained considerable damage4 ,on examination it was found that the lightning followed the conductor down along the spire as far as the roof2 then1 changing its course1 it forced its way through a buttress of massive masonwork1 dislodging about two cartloads of stones1 and leaped over to the leads of the roof1 about six feet distant4 ,it now followed the leads until it came to the cast-iron down-pipes intended to discharge the rain-water1 and through these it descended to the earth4 ,when the earth contact of the lightning conductor was examined1 it was found exceedingly deficient4 ,the rod was simply bent underground1 and buried in dry loose rubbish at a depth not exceeding eighteen inches4 ,this is a very instructive example4 ,the lightning had a choice of two paths--one by the conductor prepared for it1 the other by the leads of the roof and the down-pipes--and1 by a kind of instinct which1 however we may explain1 we must always contemplate with wonder1 it chose the path of least resistance1 though in doing so it had to burst its way at the outset through a massive wall of solid masonry4#ca ,on the #eth of ,june1 in the same year1 a flash of lightning struck the house of ,mr4 ,osbaldiston1 near ,sheffield1 and1 notwithstanding the supposed protection of a lightning conductor1 it did damage to the amount of about five hundred pounds4 ,the lightning here followed the conductor to a point about nine feet from the ground1 then passed through a thick wall to a gas-pipe at the back of the drawing-room mirror4 ,it melted the gas-pipe1 set fire to the gas1 smashed the mirror to atoms1 broke the ,sevres vases on the chimney-piece1 and dashed the furniture about4 ,in this case1 as in the former1 it was found that the earth contact was bad2 and1 in addition1 the conductor itself was of too small dimensions4 ,hence1 the electric discharge found an easier path to earth through the gas-pipes1 though to reach them it had to force for itself a passage through a resisting mass of non-conductors4#cb ,again in the same year1 on the #bhth of ,may1 the house of ,mr4 ,tomes1 of ,caterham1 was struck by lightning1 and some slight damage was done4 ,after a careful examination it was found that the greater part of the discharge left the lightning conductor with which the house was provided1 and passed over the slope of the roof to an attic room1 into which it forced its way through a brick wall1 and reached a small iron cistern4 ,this cistern was connected by an iron pipe of considerable dimensions with two pumps in the basement story2 and through them the lightning found an easy passage to the earth1 and did but little harm on its way4 ,when the earth contact of the lightning conductor was examined1 it was discovered that the end of the rod was simply stuck into a dry chalky soil to a depth of about twelve inches4 ,thus in this case1 as in the two former1 it was made quite clear that the lightning conductor failed to fulfill its functions because the earth contact was bad4#cc ,cases are not uncommon in which builders provide underground a carefully constructed reservoir of water1 into which the lower end of the lightning rod is introduced4 ,the idea seems to prevail that a reservoir of water constitutes a good earth contact2 and this is quite true of a natural reservoir1 such as a lake1 where the water is in contact with moist earth over a considerable area4 ,but an artificial reservoir may have quite an opposite character1 and practically insulate the lightning conductor from the earth4 ,one which came under my notice lately1 in the neighborhood of this city1 consists of a large earthenware pipe set on end in a bed of cement1 and kept half full of water4 ,now1 the earthenware pipe is a good insulator1 and so is the bed of cement in which it rests2 and the whole arrangement is identical1 in all essential features1 with the apparatus of ,professor ,richman1 in which he introduced his lightning rod into a glass bottle1 and by which he lost his life a hundred and thirty years ago4 ,a conductor mounted in this manner will1 probably enough1 draw down lightning from the clouds2 but it is more likely to discharge it1 with destructive effect1 into the building it is intended to guard1 than to transmit it harmlessly to the earth4 ,an example is at hand in the case of ,christ ,church1 in the town of ,clevedon1 in ,somersetshire4 ,this church was provided with a very efficient system of lightning conductors1 five in number1 corresponding to the four pinnacles and the flagstaff1 on the summit of the principal tower4 ,the five conductors consisted of good copper-wire rope2 all were united together inside the tower1 through which they were carried down to earth1 and there ended in an earthenware drain4 ,this kind of earth contact might be pretty good as long as water was flowing in the drain2 but whenever the drain was dry the conductor was practically insulated from the earth4 ,on the fifteenth of ,march1 #ahgf1 the church was struck by lightning1 which for some distance followed the line of the conductor2 then finding its passage barred by the earthenware drain1 which was dry at the time1 it burst through the walls of the church1 displacing several hundredweight of stone1 and making its way to earth through the gas-pipe4#cd ,another very instructive example is furnished by the lightning conductor attached to the lighthouse of ,berehaven1 on the south-west coast of ,ireland4 ,it consists of a half-inch copper-wire rope1 which is carried down the face of the tower 8until it reaches the rock at its base1 where it terminates in a small hole1 three inches by three inches1 jumped out of the rock1 about six inches under the surface40 ,here1 again1 we have a good imitation of ,professor ,richman's experiment1 with only this difference1 that a small hole in the rock is substituted for a glass bottle4 ,a lightning conductor of this kind fulfills two functions3 it increases the chance of the lightning coming down on the building1 and it makes it positively certain that1 having come1 it cannot get to earth without doing mischief4 ,the lightning did come down on the ,berehaven ,lighthouse1 about five years ago4 ,as might have been expected1 it made no use of the lightning conductor in finding a path to earth1 but forced its way through the building1 dealing destruction around as it descended from stage to stage4 ,the ,board of ,irish ,lights furnished a detailed report of this accident to the ,lightning ,rod ,conference1 in ,march1 #ahhj1 from which the above particulars have been derived4#ce ,precaution ,against ,rival ,conductors4--,but it is not enough to provide a good lightning conductor1 which is itself able to convey the electric discharge harmless to the earth2 we must take care that there are no rival conductors near at hand in the building1 to draw off the lightning from the path prepared for it1 and conduct it by another route in which its course might be marked with destruction4 ,this precaution is of especial importance at the present day1 owing to the great extent to which metal1 of various kinds1 is employed in the construction and fittings of modern buildings4 ,i will take a typical case which will bring home this point clearly to your minds4 ,a great part of the roof of many large buildings is covered with lead4 ,the lead1 at one or more points may come near the gutters intended to collect the rain water2 the gutters are in connection with the cast-iron down-pipes into which the water flows1 and these down-pipes often pass into the earth1 which1 under the circumstances1 is generally moist1 and1 therefore1 in good electrical contact with the metal pipes4 ,here1 then1 is an irregular line of conductors1 which1 though it has gaps here and there1 may1 under certain conditions1 offer to the lightning discharge a path not less free than the lightning conductor itself4 ,what is the consequence8 ,the flash of lightning1 or a part of it1 will quit the lightning rod1 and make its way to earth through the broken series of conductors1 doing1 perhaps1 serious mischief1 as it leaps across1 or bursts asunder1 the non-conducting links in the chain4 ,another illustration may be taken from the gas and water-pipes1 with which almost all buildings in great cities are now provided1 and which constitute a network of conductors1 spreading out over the walls and ceilings1 and stretching down into the earth1 with which they have the best possible electrical contact4 ,now1 it often happens that a lightning conductor1 at some point in its course1 comes within a short distance of this network of pipes4 ,in such a case1 a portion of the electrical discharge is apt to leave the lightning conductor1 force its way destructively through masses of masonry1 enter the network of pipes1 melt the leaden gas-pipe1 ignite the gas1 and set the building on fire4 ,these are not merely the speculations of philosophers4 ,all the various incidents ,i have just described have occurred1 over and over again1 during the last few years4 ,you will remember1 in some of the examples ,i have already set before you1 when the electric discharge failed to find a sufficient path to earth through the lightning rod1 it followed some such broken series of chance conductors as we are now considering4 ,but this broken series of conductors seems to bring with it a special danger of its own1 even when the lightning conductor is otherwise in efficient working order4 ,i will give you just one case in point4 ,on the fifth of ,june1 #ahgi1 the ,church of ,saint ,marie1 ,rugby1 was struck by lightning and set on fire1 and narrowly escaped being burned to the ground4 ,a number of workmen were engaged on that day in repairing the spire of the church4 ,about three o'clock they saw a dense black cloud approaching1 and they came down to take shelter within the building4 ,in a few minutes they heard a terrific crash just overhead2 at the same moment the gas was lighted under the organ loft and the woodwork was set in a blaze4 ,the men soon succeeded in putting out the fire1 and the church escaped with very little damage4 ,now1 in this case there was no reason to suppose that the lightning conductor was in any way defective4 ,but about half-way up the spire there was a peal of eight bells4 ,attached to these bells were iron wires1 about the eighth of an inch in diameter1 leading from the clappers down to the organ-loft1 where they came within a short distance of a gas-pipe fixed in the wall4 ,it would seem that a great part of the discharge was carried safely to earth by the lightning conductor4 ,but a part branched off at the bells in the spire1 descended by the iron wires1 and forced its way into the organ loft1 to reach the network of gas-pipes1 through which it passed down to the earth1 melting the soft leaden gas-pipe in its course and lighting the gas4 ,the remedy for this danger is obvious4 ,all large masses of metal used in the structure of a building--the leads and gutters of the roof1 the cast-iron down-pipes1 the iron gas and water mains--should be put in good metallic connection with the lightning conductor1 and1 as far as may be1 with one another4 ,connected in this way they furnish a continuous and effective line of conductors leading safely down to earth2 and1 instead of being a dangerous rival1 they become a useful auxiliary to the lightning rod4 ,i would observe1 however1 that the lightning conductor ought not to be connected directly with the soft leaden pipes which are commonly employed to convey gas and water to the several parts of a building4 ,such pipes1 as we have seen1 are liable to be melted when any considerable part of the lightning discharge passes through them2 and thus much harm might be done1 and the building might even be set on fire by the lighting of the gas4 ,every good end will be attained if the conductor is put in metallic connection with the iron gas and water mains either inside or outside the building4 ,insulation of ,lightning ,conductors4--,it is a question often asked whether a lightning rod should be insulated from the building it is intended to protect4 ,i believe that this practice was formerly recommended by some writers1 and ,i have observed that glass insulators are still employed not infrequently by builders in the erection of lightning conductors2 but1 from the principles ,i have set before you to-day1 it seems clear that any insulation of this kind is1 to say the least1 altogether useless4 ,the building to be protected is itself in electrical communication with the earth1 and the lightning conductor1 if efficient1 is also in electrical communication with the earth--therefore1 the lightning conductor and the building are in electrical communication with each other through the earth1 and any attempt at insulating them from one another above the earth is only labor thrown away4 ,further1 ,i have just shown you that the masses of metal employed in the structure or decoration of a building ought to be electrically connected with each other and with the lightning conductor4 ,now1 if this be done1 the lightning conductor is1 by the fact1 in direct communication with the building1 and the glass insulators are utterly futile4 ,again1 the building itself1 during a thunderstorm1 becomes highly electrified by the inductive action of the cloud1 and needs to be discharged through the conductor just as the surrounding earth needs to be discharged2 therefore1 the more thoroughly it is connected with the conductor1 the more effectively will the conductor fulfill its functions4 ,personal ,safety in a ,thunderstorm4--,i suppose there is hardly any one to whom the question has not occurred1 at some time or another1 what he had best do to secure his personal safety during a thunderstorm4 ,this question is of so much practical interest that ,i think ,i shall be excused if ,i say a few words about it1 though perhaps1 strictly speaking1 it is somewhat beside the subject of lightning conductors4 ,at the outset1 perhaps1 ,i shall surprise you when ,i say that you would enjoy the most perfect security if you were in a chamber entirely composed of metal plates1 or in a cage constructed of metal bars1 or if you were incased1 like the knights of old1 in a complete suit of metal armor4 ,this kind of defense is looked upon as so perfect1 among scientific men1 that ,professor ,tait does not hesitate to recommend his adventurous young friends devoted to the cause of science to provide themselves with a light suit of copper1 and1 thus protected1 take the first opportunity of plunging into a thundercloud1 there to investigate1 at its source1 the process by which lightning is manufactured4#cf ,the reason why a metal covering affords complete protection is that1 when a conductor is electrified1 the whole charge of electricity exists on the outside surface of the conductor2 and therefore1 when a discharge takes place1 it is only the outside surface that is affected4 ,thus1 if you were completely incased in a metal covering1 and then charged with electricity by the inductive action of a thundercloud1 it is only the metal covering that would undergo any change of electrical condition2 and when the lightning flash would pass1 it is only the metal covering that would be discharged4 ,let me show you a very pretty and interesting experiment to illustrate this principle3 ,here is a hollow brass cylinder1 open at the ends1 mounted on an insulating stand4 ,on the outside is erected a light brass rod with two pith balls suspended from it by linen threads4 ,two pith balls are also suspended by linen threads from the inner surface of the cylinder4 ,you know that these pith balls will indicate to us the electrical condition of the surfaces to which they are attached4 ,if the surface be electrified1 the pith balls attached to it will share in its electrical condition1 and will repel each other2 if the surface be neutral1 the pith balls attached to it will be neutral1 and will remain at rest4 ,i now put this apparatus under the influence of our thundercloud1 that is1 the large brass conductor of our machine4 ,the moment my assistant turns the handle1 the electricity begins to be developed on the conductor1 and you see1 at once1 the effect on the brass cylinder4 ,the pith balls attached to the outer surface fly asunder2 those attached to the inner surface remain at rest4 ,and now a spark passes2 our thundercloud is discharged2 the inductive action ceases2 the pith balls on the outside suddenly collapse1 while those on the inside are in no way affected4 ,illustration3 ,,protection ,,from ,,lightning ,,furnished ,,by ,a ,,closed ,,conductor4 ,it is not necessary that the brass cylinder should be insulated4 ,to vary the experiment1 ,i will now connect it with the earth by a chain2 you will observe that the effect is precisely the same as before4 ,flash after flash passes while the machine continues in action2 the outside pith balls fly about violently1 being charged and discharged alternately2 the inside pith balls remain all the time at rest4 ,thus you see clearly that1 if you were sitting inside such a metal chamber as this1 or covered with a complete suit of metal armor1 you would be perfectly secure during a thunderstorm1 whether the chamber were electrically connected with the earth or insulated from it4 ,practical ,rules4--,but it rarely happens1 when a thunderstorm comes1 that an iron hut or a complete suit of armor is at hand1 and you will naturally ask me what you ought to do under ordinary circumstances4 ,first1 let me tell you what you ought not to do4 ,you ought not to take shelter under a tree1 or under a haystack1 or under the lee of a house2 you ought not to stand on the bank of a river1 or close to a large sheet of water4 ,if indoors1 you ought not to stay near the fireplace1 or near any of the flues or chimneys2 you ought not to stand under a gasalier hanging from the ceiling2 you ought not to remain close to the gas pipes or water-pipes1 or any large masses of metal1 whether used in the construction of the building1 or lying loosely about4 ,the necessity for these precautions is sufficiently evident from the principles ,i have already put before you4 ,you want to prevent your body from becoming a link in that broken chain of conductors which1 as we have seen1 the electric discharge between earth and cloud is likely to follow4 ,now a tree is a better conductor than the air2 and your body is a better conductor than a tree4 ,hence1 the lightning1 in choosing the path of least resistance1 would leave the air to pass through the tree1 and would leave the tree to pass through you4 ,a like danger would await you if you stood under the lee of a haystack or of a house4 ,the number of people who lose their lives by taking refuge under trees in thunderstorms is very remarkable4 ,as one instance out of many1 ,i may cite the following case which was reported in the ,times1 ,july #ad1 #ahhg3 8,yesterday the funeral of a negress was being conducted in a graveyard at ,mount ,pleasant1 sixty miles north of ,nashville1 ,tennessee1 when a storm came on1 and the crowd ran for shelter under the trees4 ,nine persons stood under a large oak1 which the lightning struck1 killing everyone1 including three clergymen1 and the mother and two sisters of the girl who had been buried40 ,again1 every large sheet of water constitutes practically a great conductor1 which offers a very perfect medium of discharge between the earth round about and the cloud4 ,therefore1 when a thundercloud is overhead1 the sheet of water is likely to become one end of the line of the lightning discharge2 and if you be standing near it1 the line of discharge may pass through your body4 ,when lightning strikes a building1 it is very apt to use the stack of chimneys in making its way to earth1 partly because the stack of chimneys is generally the most prominent part of the building1 and partly because1 on account of the heated air and the soot within the chimney1 it is usually a moderately good conductor4 ,therefore1 if you be indoors1 you must keep well away from the chimneys2 and for a similar reason1 you must keep as far as you can from large masses of metal of every kind4 ,having pointed out the sources of danger which you must try to avoid in a thunderstorm1 ,i have nearly exhausted all the practical advice that ,i have at my command4 ,but there are some occasions on which it may be possible1 not only to avoid evident sources of danger1 but to make special provision for your own security4 ,thus1 for example1 in the open country1 if you stand a short distance from a wood1 you may consider yourself as practically protected by a lightning conductor4 ,for a wood1 by its numerous branches and leaves1 favors very much a quiet discharge of electricity1 thus tending to suppress altogether the flash of lightning2 and if the flash of lightning does come1 it is much more likely to strike the wood than to strike you1 because the wood is a far more prominent body1 and offers1 on the whole1 an easier path to earth4 ,in like manner1 if you place yourself near a tall solitary tree1 some twenty or thirty yards outside its longest branches1 you will be in a position of comparative safety4 ,if the storm overtake you in the open plain1 far away from trees and buildings1 you will be safer lying flat on the ground than standing erect4 ,in an ordinary dwelling house1 the best situation is probably the middle story1 and the best position in the room is in the middle of the floor2 provided1 of course1 that there is no gasalier hanging from the ceiling above or below you4 ,strictly speaking1 the middle of the room would be a still safer position than the middle of the floor2 and nothing could be more perfect than the plan suggested by ,franklin1 to get into 8a hammock1 or swinging bed1 suspended by silk cords1 and equally distant from the walls on every side1 as well as from the ceiling and floor1 above and below40 ,an interesting case has been recently recorded1 by a resident of ,venezuela1 which illustrates in a remarkable way the excellence of this advice4 8,the lightning10 he says1 8struck a rancho--a small country house1 built of wood and mud1 and thatched with straw or large leaves--where one man slept in a hammock1 another lay under the hammock on the ground1 and three women were busy about the floor2 there were also several hens and a pig4 ,the man in the hammock did not receive any injury whatever1 while the other four persons and the animals were killed40#cg ,but1 as ,i can hardly hope that many of you when the thunderstorm actually comes will find yourselves provided with a hammock1 ,i would recommend1 as more generally useful1 another plan of ,franklin's1 which is simply to sit on one chair in the middle of the floor and put your feet up on another4 ,this arrangement will approach very nearly to absolute security if you take the further precaution1 also mentioned by ,franklin1 of putting a feather bed or a couple of hair mattresses under the chairs4#ch ,security ,afforded by ,lightning ,rods4--,you might1 perhaps1 be inclined to infer hastily1 from the examples ,i have set before you1 in the course of this lecture1 of buildings which were struck and severely injured by lightning though provided with lightning conductors1 that a lightning rod affords a very imperfect protection to life and property4 ,but such an idea would be entirely at variance with the evidence at hand on the subject4 ,in all the cases to which ,i have referred1 and in many others which might easily have been cited1 the damage was done simply because the lightning rods were deficient in one or more of the conditions on which ,i have so much insisted4 ,where these conditions are fulfilled1 the lightning flash will either not come down at all upon the building1 or1 if it do come1 it will be carried harmless to the earth4 ,perhaps there is no one fact that so forcibly brings home to the mind the complete protection afforded by lightning conductors as the change which followed their introduction into the ,royal ,navy4 ,i have already told you that in former times the damage done by lightning to ships of the ,royal ,navy was a regular source of expenditure1 amounting every year to several thousand pounds sterling4 ,but1 after the general adoption of lightning conductors about forty years ago1 through the indefatigable exertions of ,sir ,william ,snow ,harris1 this source of expenditure absolutely disappeared1 and injury to life and property has long been practically unknown in ,her ,majesty's ,fleet4 ,i should say1 however1 that the trial of lightning conductors in the ,navy1 though it lasted long enough to prove their perfect efficiency1 has almost come to an end in our own days4 ,the great iron monsters which in recent times have taken the place of the wooden ships of ,old ,england are quite independent of lightning rods in the common sense of the word4 ,their ponderous masts are virtually lightning rods of colossal dimensions1 and their unsightly hulls are1 so to speak1 earth-plates of enormous size in perfect electrical contact with the ocean4 ,to add to such structures lightning conductors of the common kind would be nothing better than 8wasteful and ridiculous excess40 ,as regards buildings on land1 ,i may refer to the little province of ,schleswig-,holstein1 of which ,i have already spoken to you4 ,from some cause or other this small peninsula is singularly exposed to thunderstorms1 and of late years it has been more abundantly provided with lightning conductors than1 perhaps1 any other district of equal extent in ,europe4 ,now1 as a simple illustration of the protection afforded by these lightning conductors1 ,i may mention that1 on the #bfth of ,may1 #ahgh1 a violent thunderstorm burst over the little town of ,utersen4 ,five several flashes of lightning fell in different parts of the town1 but not the slightest harm was done1 each flash being safely carried to earth by a lightning conductor4 ,further1 it appears from the records of the fire insurance company that1 out of #eeb buildings injured by lightning during a period of eight years--from #ahgj to #ahgh--only four had lightning conductors2 and in these four cases it was found1 on examination1 that the lightning conductors were defective4#ci ,it would be easy to multiply evidence on this subject4 ,but as ,i have already trespassed1 ,i fear1 too far on your patience1 ,i will content myself with saying1 in conclusion1 that according to all the highest authorities1 both practical and theoretical1 any structure provided with a lightning conductor properly fitted up in conformity with the principles ,i have set before you to-day is perfectly secure against lightning4 ,the lightning1 indeed1 may fall upon it1 but it will pass harmless to the earth2 and the experience of more than a hundred years has fully justified the simple and modest words of the great inventor of lightning conductors3 8,it has pleased ,god1 in ,his goodness to mankind1 at length to discover to them the means of securing their habitations and other buildings from mischief by thunder and lightning40 ,,note ,i4 ,,on ,,the ,,lightning ,,conductor ,,at ,,berehaven4#dj ,it is satisfactory to know that the lightning conductor referred to in my lecture as attached to the lighthouse at ,berehaven has been put in good order under the best scientific guidance4 ,the following interesting letter from ,professor ,tyndall1 which appeared in the ,times1 ,august #ca1 #ahhg1 gives the history of the matter very clearly1 and fully bears out the views put forward in my lecture3 8,your recent remarks on thunderstorms and their effects induce me to submit to you the following facts and considerations4 ,some years ago a rock lighthouse on the coast of ,ireland was struck and damaged by lightning4 ,an engineer was sent down to report on the occurrence2 and1 as ,i then held the honorable and responsible post of scientific adviser to the ,trinity ,house and ,board of ,trade1 the report was submitted to me4 ,the lightning conductor had been carried down the lighthouse tower1 its lower extremity being carefully embedded in a stone perforated to receive it4 ,if the object had been to invite the lightning to strike the tower1 a better arrangement could hardly have been adopted4 8,i gave directions to have the conductor immediately prolonged1 and to have added to it a large terminal plate of copper1 which was to be completely submerged in the sea4 ,the obvious convenience of a chain as a prolongation of the conductor caused the authorities in ,ireland to propose it2 but ,i was obliged to veto the adoption of the chain4 ,the contact of link with link is never perfect4 ,i had1 moreover1 beside me a portion of a chain cable through which a lightning discharge had passed1 the electricity in passing from link to link encountering a resistance sufficient to enable it to partially fuse the chain4 ,the abolition of resistance is absolutely necessary in connecting a lightning conductor with the earth1 and this is done by closely embedding in the earth a plate of good conducting material and of large area4 ,the largeness of area makes atonement for the imperfect conductivity of earth4 ,the plate1 in fact1 constitutes a wide door through which the electricity passes freely into the earth1 its disruptive and damaging effects being thereby avoided4 8,these truths are elementary1 but they are often neglected4 ,i watched with interest some time ago the operation of setting up a lightning conductor on the house of a neighbor of mine in the country4 ,the wire rope which formed part of the conductor was carried down the wall and comfortably laid in the earth below without any terminal plate whatever4 ,i expostulated with the man who did the work1 but he obviously thought he knew more about the matter than ,i did4 ,i am credibly informed that this is a common way of dealing with lightning conductors by ignorant practitioners1 and the ,bishop of ,winchester's palace at ,farnham has been mentioned to me as an edifice #8protected' in this fashion4 ,if my informant be correct1 the #8protection' is a mockery1 a delusion1 and a snare40 ,,note ,,ii4 ,,books ,,of ,,reference4 ,as some of my readers may wish to pursue the study of lightning and lightning conductors beyond the limits to which a popular lecture must1 of necessity1 be confined1 ,i subjoin a list of the books which ,i think they would be likely to find most useful for the purpose4 ,among ordinary text-books on physics--,jamin1 ,cours de ,physique1 vol4 i41 pp4 #dgj-did2 ,mascart1 ,trait d',electricit ,statique1 vol4 ii41 pp4 #eee-egi2 ,de ,larive1 ,a ,treatise on ,electricity1 in three volumes1 ,london1 #ahec-h1 vol4 iii41 pp4 #ij-bja2 ,daguin1 ,trait de ,physique1 vol4 iii41 pp4 #bji-bhj2 ,riess1 ,die ,lehre von der ,reibungs-,elektricitt1 vol4 ii41 pp4 #did-efd2 ,mller-,pouillet1 ,lehrbuch der ,physik1 ,braunschweig1 #ahha1 vol4 iii41 pp4 #baj-bbe2 ,scott1 ,elementary ,meteorology1 chap4 x4 ,of the numerous special treatises and detached papers on the subject1 ,i would recommend ,instruction sur les ,paratonnerres adopt par l',acadmie des ,sciences1 ,part i41 #ahbc1 ,part ii41 #ahed1 ,part iii41 #ahfg1 ,paris1 #ahgd2 ,arago1 ,sur le ,tonnerre1 ,paris1 #ahcg2 also his ,meteorological ,essays1 translated by ,sabine1 ,london1 #ahee2 ,sir ,william ,snow ,harris1 ,on the ,nature of ,thunderstorms1 ,london1 #ahdc2 also by the same writer1 ,a ,treatise on ,frictional ,electricity1 ,london1 #ahfg2 and various papers on lightning conductors1 from #ahbb to #ahei2 ,tomlinson1 ,the ,thunderstorm1 ,london1 #ahgg2 ,anderson1 ,lightning ,conductors1 ,london1 #ahhj2 ,holtz1 ,ueber die ,theorie1 die ,anlage1 und die ,prfung der ,blitzableiter1 ,greifswald1 #ahgh2 ,weber1 ,berichte ber ,blitzschlge in der ,provinz ,schleswig-,holstein1 ,kiel1 #ahhj-a2 ,tait1 ,a ,lecture on ,thunderstorms1 delivered in the ,city ,hall1 ,glasgow1 in #ahhj1 ,nature1 vol4 xxii42 ,report of the ,lightning ,rod ,conference1 ,london1 #ahhb4 ,this last-mentioned volume comes to us with very high authority1 representing1 as it does1 the joint labors of several eminent scientific men selected from the following societies3 ,the ,meteorological ,society1 the ,royal ,institute of ,british ,architects1 the ,society of ,telegraph ,engineers and ,electricians1 the ,physical ,society4 ,since the above was in print1 two lectures given before the ,society of ,arts by ,professor ,oliver ,lodge1 ,f4 ,r4 ,s41 have appeared in the ,electrician1 ,june and ,july1 #ahhh1 in which some new views are put forward respecting lightning conductors1 that seem deserving of careful consideration4 ,,footnotes3 #ag ,the ,thunderstorm1 by ,charles ,tomlinson1 ,f4 ,r4 ,s41 ,third ,edition1 pp4 #aec-d4 #ah ,two ,lectures on ,atmospheric ,electricity and ,protection from ,lightning1 published at the end of his ,treatise on ,frictional ,electricity1 p4 #bgc4 #ai ,see ,report of ,lightning ,rod ,conference1 p4 #aai4 #bj ,loco citato4 #ba ,sir ,william ,snow ,harris1 loco citato1 p4 #bgd4 #bb ,id41 p4 #bge4 #bc ,the ,thunderstorm1 by ,charles ,tomlinson1 ,f4,r4,s41 ,third ,edition1 p4 #agb4 #bd ,see for these facts1 ,anderson1 ,lightning ,conductors1 p4 #aig2 ,tomlinson1 ,the ,thunderstorm1 pp4 #afg-i2 ,harris1 loco citato1 pp4 #bgc-d4 #be ,see ,anderson1 ,lightning ,conductors1 pp4 #agj-e4 #bf ,the ,thunderstorm1 pp4 #aeh-i4 ,see also an account of four persons who were struck on the ,matterhorn1 in ,july1 #ahfi1 all of whom were hurt1 and none killed3 ,whymper's ,scrambles ,among the ,alps1 pp4 #dad1 #dae4 #bg ,see ,philosophical ,transactions of the ,royal ,society1 #aggc1 p4 #db1 and #aggh1 part i41 p4 #bcb2 ,anderson's ,lightning ,conductors1 pp4 #dj-b2 ,lighting ,rod ,conference1 pp4 #gf-i4 #bh ,see ,a ,lecture on ,thunderstorms1 by ,professor ,tait of ,edinburgh1 published in ,nature1 vol4 xxii41 p4 #cfe4 #bi ,report of the ,lightning ,rod ,conference1 p4 #d4 #cj ,the dimensions here set forth are greater in some respects than those 8recommended as a minimum0 in the report of the ,lightning ,rod ,conference1 page #f4 ,but it will be observed by those who consult the report that the minimum recommended is just the size which1 in the preceding paragraph of the report1 is said to have been actually melted by a flash of lightning2 and1 therefore1 it seems not to be a very safe minimum4 ,it will be also seen that there is some confusion in the figures given1 and that they contradict one another4 ,for the dimensions of iron rods1 see the instructions adopted by the ,academy of ,science1 ,paris1 ,may #bj1 #ahge2 ,lightning ,rod ,conference1 pp4 #fg-h4 #ca ,see letter of ,mr4 ,r4 ,s4 ,newall1 ,f4 ,r4 ,s41 in the ,times1 ,may #cj1 #ahgi4 #cb ,see ,nature1 ,june #ab1 #ahgi1 vol4 xx41 p4 #adf4 #cc ,see letter of ,mr4 ,tomes in ,nature1 vol4 xx41 p4 #ade2 also ,lightning ,rod ,conference1 pp4 #baj-ae4 #cd ,see ,anderson1 ,lightning ,conductors1 pp4 #bjh-aj4 #ce ,see ,lightning ,rod ,conference1 pp4 #bjh-aj2 see also the note at the end of this ,lecture1 p4 #eb4 #cf ,lecture on ,thunderstorms1 ,nature1 vol4 xxii41 pp4 #cfe1 #dcg4 ,see1 also1 a very interesting paper by the late ,professor ,j4 ,clerk ,maxwell1 read before the ,british ,association at ,glasgow in #ahgf1 and reprinted in the report of the ,lightning ,rod ,conference1 pp4 #aji1 #aaj4 #cg ,nature1 vol4 xxxi41 p4 #dei4 #ch ,see further information on this interesting subject in the ,report of the ,lightning ,rod ,conference1 pp4 #bcc-e4 #ci ,see 8,die ,theorie1 die ,anlage1 und die ,prfung der ,blitzableiter10 von ,doctor ,w4 ,holtz1 ,griefswald1 #ahgh4 #dj ,see page #dd4 ,,appendix4 ,,recent ,,controversy ,,on ,,lightning ,,conductors4 ,the lecture on lightning conductors contained in this volume fairly represents1 ,i think1 the theory hitherto received on the subject4 ,it is1 moreover1 entirely in accord with the report of the ,lightning ,rod ,conference1 brought out in #ahhc1 by a committee of most eminent men1 representing several branches of science1 who were specially chosen to consider this question some ten years ago4 ,lectures of ,professor ,lodge4--,but1 in the month of ,march1 #ahhh1 two lectures were given before the ,society of ,arts1 in ,london1 by ,professor ,oliver ,lodge1 in which this theory was directly challenged1 and attacked with cogent arguments1 supported by striking and original experiments4 ,these lectures gave rise to an animated controversy1 which culminated in a formal discussion at the recent meeting of the ,british ,association in ,bath4 ,the discussion was carried on with great spirit1 and most of the leading representatives of physical and mechanical science took an active part in it4 ,the greater portion of this volume was printed off before the meeting of the ,british ,association took place4 ,but the discussion on the theory of lightning conductors seemed to me so interesting and important that ,i thought it right1 in the form of an ,appendix1 to give some account of the questions at issue1 and of the opinions expressed upon them4 ,professor ,lodge maintains#da that the received theory of lightning rods is open to two objections4 ,first1 it takes account only of the conducting power of the lightning rod1 and takes no account of the phenomenon known as self-induction1 or electrical inertia4 ,secondly1 it assumes that the whole substance of a lightning rod acts as a conductor1 in all cases of lightning discharge2 whereas there is reason to believe that1 in many cases1 it is only a thin outer shell that really comes into action4 ,i will deal with these two points separately4 ,the ,effect of ,self-,induction4--,when an electric discharge begins to pass through a conductor1 a momentary back electro-motive force is developed in the conductor1 which obstructs its passage4 ,this phenomenon is called by some self-induction1 by others electrical inertia2 but its existence is admitted by all4 ,now1 when a flash of lightning1 so to say1 falls on a lightning rod1 the back electro-motive force developed is very considerable2 and it may offer so great an obstruction that the discharge will find an easier passage by some other route1 such as the stone walls and woodwork1 and furniture of the building4 ,according to this view1 the obstruction which a flash of lightning encounters in a conductor consists partly of the resistance of the conductor1 in the ordinary sense of the word resistance1 and partly of the back electro-motive force due to self-induction4 ,the sum of these two ,professor ,lodge calls the impedance of the lightning rod2 and he considers that the impedance may be enormously great1 even when the resistance1 in the ordinary sense1 is comparatively small4 ,in support of this view he has devised the following extremely ingenious and remarkable experiment4 ,a large ,leyden jar1 ,l1 was arranged in such a manner that1 while it received a steady charge from an electrical machine1 it discharged itself1 at intervals1 across the air space at ,a1 between two brass balls4 ,the discharge had then two alternative paths before it2 one through a conducting wire1 ,c1 the other across a second air space1 between two brass balls at ,b4 ,during the experiment1 the two balls at ,a were kept at a fixed distance of one inch apart2 but the distance between the two balls at ,b was varied4 ,the conductor1 ,c1 used in the first instance1 was a stout copper wire1 about forty feet long1 and having a resistance of only one-fortieth of an ohm4 ,illustration3 ,,induction ,,effect ,,of ,,leyden ,,jar ,,discharge4 ,m ,electrical ,machine4 ,l ,leyden ,jar4 ,a ,b ,air ,spaces between ,brass ,knobs4 ,c ,conducting ,wire4 ,it was found that1 so long as the distance between the ,b knobs was less than #a4dc inches1 all the discharges passed across between the knobs1 in the form of a spark4 ,when the distance exceeded #a4dc inches1 all the discharges passed through the conductor1 ,c1 and no spark appeared between the balls at ,b4 ,and when the distance was exactly #a4dc inches1 the discharge sometimes took place between the knobs1 and sometimes followed the conductor1 ,c4 ,the interpretation given to these facts is that the obstruction offered by the conductor ,c was about equal to the resistance of #a4dc inches of air2 and it is proposed to call this distance1 under the conditions of the experiment1 the critical distance4 ,coming now to the application of these results1 ,professor ,lodge argues that the conductor ,c1 in his experiment1 represents a lightning rod of unimpeachable excellence2 and yet1 in certain cases1 the discharge refuses to follow the conductor1 and prefers to leap across a considerable space of air1 notwithstanding the enormous resistance it there encounters4 ,in like manner1 he says1 a flash of lightning may1 in certain cases1 leave a lightning rod fitted up in the most orthodox manner1 and force its way to earth through resisting masses of mason work and such chance conductors as may come across its path4 ,this conclusion1 he admits1 is altogether at variance with the received views on the subject2 but he contends that it is perfectly in accord with the scientific theory of an electrical discharge4 ,the moment the discharge begins to pass in the conductor1 it encounters the obstruction due to self-induction2 and this obstruction is so great that the bad conductors offer1 on the whole1 an easier path to earth4 ,variation of the ,experiment4--,when the experiment was varied by substituting a thin iron wire for the stout copper wire at first employed1 a very curious result was obtained4 ,the wire chosen was of the same length as the copper1 but had a resistance about #a1cjj times as great2 its resistance being1 in fact1 #cc4c ohms4 ,nevertheless1 in this experiment1 when the ,b knobs were at a distance of #a4dc inches1 no spark passed1 which showed that the discharge always followed the line of the conductor1 and therefore that the conductor offered less obstruction than #a4dc inches of air4 ,the knobs were then brought gradually nearer and nearer2 and it was not until the distance was considerably reduced that the sparks began to pass between them4 ,when the distance was exactly #a4jc inches1 the discharge sometimes passed between the knobs1 and sometimes through the conductor2 this was1 therefore1 the critical distance1 in the case of the iron wire4 ,thus it appeared that the obstruction offered to the discharge by the iron wire was much less than that offered by the copper1 the one being equal to a resistance of only #a4jc inches of air1 the other to a resistance of #a4dc inches4 ,it does not appear that ,professor ,lodge undertakes to offer any satisfactory explanation of this result4 ,he has come to the conclusion1 from his various experiments1 that1 in the case of a sudden discharge1 difference of conducting power between fairly good conductors is a matter of practically no account2 and that difference of sectional area is a matter of only trifling account4 ,but he does not see why a thin iron wire should have a smaller impedance than a much thicker wire of copper4 ,he proposes to repeat the experiments so as to confirm or to modify the result1 which for the present seems to him anomalous4#db ,the ,outer ,shell only of a ,lightning ,rod ,acts as a ,conductor4--,as a consequence of self-induction or electrical inertia1 ,professor ,lodge contends that a lightning discharge in a conductor consists of a series of oscillations4 ,these oscillations follow one another with extraordinary rapidity--there may be a hundred thousand in a second1 there may be a million4 ,now it has been shown that1 when a current starts in a conductor1 it does not start at once all through its section2 it begins on the outside1 and then gradually1 but rapidly1 penetrates to the interior4 ,from this he infers that the extremely rapid oscillations of a lightning discharge have not time to penetrate to the interior of a conductor4 ,the electricity keeps surging to and fro in the superficial layer or outer shell1 while the interior substance of the rod remains inert and takes no part in the action4 ,a conductor1 therefore1 will be most efficient for carrying off a flash of lightning if it present the greatest possible amount of surface2 a thin1 flat tape will be more efficient than a rod of the same mass2 and a number of detached wires more efficient than a solid cylinder4 ,as for existing lightning conductors1 the greater part of their mass would1 in many cases1 have no efficacy whatever in carrying off a flash of lightning4 ,the ,discussion4--,the discussion at the meeting of the ,british ,association was opened by ,mr4 ,william ,h4 ,preece1 ,f4,r4,s41 ,electrician to the ,post ,office1 who claimed to have #ejj1jjj lightning conductors under his control4 ,he expressed his conviction that a lightning rod1 properly erected and duly maintained1 was a perfect protection against injury from lightning2 and in support of this conviction he urged very strongly the report of the ,lightning ,rod ,conference4 ,this report represented the mature judgment of the most eminent scientific men1 who had devoted years to the study of the question2 and he wished particularly to bring before the meeting their clear and decisive assertion--an assertion he was there to defend--that 8there is no authentic case on record where a properly constructed conductor failed to do its duty40 ,the new views put forward by ,professor ,lodge were based1 in great measure1 on his theory that a lightning discharge consisted of a series of rapid oscillations4 ,but this theory should be received with great caution4 ,it seemed to be nothing more than a deduction from certain mathematical formulas1 and was not supported by any solid basis of observation or experiment4 ,besides1 there were many facts against it4 ,they all knew that a flash of lightning magnetized steel bars1 deranged the compasses of ships at sea1 and transmitted signals on telegraph wires4 ,but such effects could not be produced by a series of oscillations1 which1 being equal and opposite1 would neutralize each other4 ,it was alleged that these rapid oscillations occurred in the discharge of a ,leyden jar4 ,that might be true1 and probably was true2 but they were not dealing with ,leyden jars1 they were dealing with flashes of lightning4 ,if there was any analogy between the discharge of a ,leyden jar and a flash of lightning1 it was to be found1 not in the external discharge employed by ,professor ,lodge in his experiments1 but in the bursting of the glass cylinder between the two coatings of the jar4 ,lord ,rayleigh thought the experiments of ,professor ,lodge were likely to have important practical applications to lightning conductors4 ,but though these experiments were valuable as suggestions1 they did not furnish a sufficient ground for adopting any new system of protection4 ,it was only by experience with lightning conductors themselves that the question could be finally settled4 ,sir ,william ,thomson hoped for great fruit from the further investigation of self-induction in the case of sudden electrical discharges4 ,he warmly encouraged ,professor ,lodge to continue his researches2 but he expressed no decided opinion on the question at issue4 ,incidentally he observed that the best security for a gun-powder magazine was an iron house2 no lightning conductor at all1 but an iron roof1 iron walls1 and an iron floor4 ,wooden boards should1 of course1 be placed over the floor to prevent the danger of sparks from people walking on sheet-iron4 ,this iron magazine might be placed on a dry granite rock1 or on wet ground2 it might even be placed on a foundation under water2 it might be placed anywhere they pleased2 no matter what the surroundings were1 the interior would be safe4 ,he thought that was an important practical conclusion which might safely be drawn from the consideration of these electrical oscillations and the experiments regarding them4 ,professor ,rowland1 of the ,johns ,hopkins ,university1 ,america1 said that the question seemed to be whether the experiment of ,professor ,lodge actually represented the case of lightning4 ,he was very much disposed to think it did not4 ,in the experiment almost the whole circuit consisted of good conductors2 whereas1 in the case of lightning1 the path of the discharge was1 for the most part1 through the air1 and therefore it might be an entirely different phenomenon4 ,the air being a very bad conductor1 a flash of lightning might1 perhaps1 not consist of oscillations1 but rather of a single swing4 ,moreover1 it was not at all clear that the length of the spark1 in the experiment1 could be taken as a measure of the obstruction offered by the conductor4 ,professor ,george ,forbes was greatly impressed with the beauty and significance of ,professor ,lodge's experiments1 but he did not think the result so clear that they should be warranted in abandoning the principles laid down by the ,lightning ,rod ,conference4 ,m4 de ,fonvielle1 of ,paris1 supported the views of ,mr4 ,preece4 ,he cited the example of ,paris1 where they had erected a sufficient number of lightning conductors1 according to the received principles1 and calamities from lightning were practically unknown4 ,he suggested that the ,eiffel ,tower1 which they were now building1 and which would be raised to the height of a thousand feet1 would furnish an unrivalled opportunity for experiments on lightning conductors4 ,sir ,james ,douglass1 ,chief ,engineer to the ,corporation of ,trinity ,house1 had a large experience with lighthouse towers4 ,the lightning rods on these towers had been erected and maintained during the last fifty years entirely according to the advice of ,faraday4 ,they never had a serious accident2 and such minor accidents as did occur from time to time were always traced to some defect in the conductor4 ,they had now established a more rigid system of inspection1 and he1 for one1 should feel perfectly safe in any tower where this system was carried out4 ,mr4 ,symons1 ,f4,r4,s41 ,secretary to the ,meteorological ,society1 had taken part in a discussion on lightning conductors as long ago as #ahei4 ,it had been a hobby with him all his life to investigate the circumstances of every case he came across in which damage was done by lightning1 and the general impression left by his investigations entirely coincided with the views just expressed by ,sir ,james ,douglass4 ,he had been a member of the ,lightning ,rod ,conference1 and was the editor of their report2 and he wished to enter his protest against the idea of rejecting all that had hitherto been done in connection with lightning conductors on the strength of mere laboratory experiments4 ,professor ,lodge1 in reply1 said he could perfectly understand the position of those who held that a lightning rod properly fitted up never failed to do its duty1 because1 whenever it failed1 they said it was not properly fitted up4 ,the great resource in such cases was to ascribe the failure to bad earth contact4 ,he thought a good earth contact was a very good thing1 but he could not understand why such extraordinary importance should be attached to it4 ,a lightning rod had two ends--an earth end and a sky end--and he did not see why good contact was more necessary at one end than at the other4 ,if a few sharp points sticking out from the conductor were sufficient for a good sky contact1 why were they not sufficient also for a good earth contact8 ,besides1 though a bad earth contact might explain why a certain amount of disruption should take place at the earth where the bad contact existed1 he did not see how it accounted for the flash shooting off sideways half-way down the conductor4 ,again1 what does a bad earth contact mean8 ,if an electrical engineer finds a resistance of a hundred ohms1 he will rightly pronounce the earth contact to be very bad indeed4 ,but why should the lightning flash leave a conductor with a resistance of a hundred ohms in order to follow a line of non-conductors where it encounters a resistance of many thousand ohms8 ,he accepted the statement of ,mr4 ,preece that his whole theory depended on the existence of oscillations in the lightning discharge2 but there was good reason to believe they existed1 because they were proved to exist in the discharge of a ,leyden jar4 ,mr4 ,preece objected that an oscillating discharge could not produce magnetic effects1 as a flash of lightning was known to do4 ,he confessed he was unable to explain how an oscillating discharge produced such effects2#dc but that it could produce them there was no doubt whatever1 for the discharge of a ,leyden jar produces magnetic effects1 and we have ocular demonstration that the discharge of a ,leyden jar is an oscillating discharge4 ,as to the assurances we had received from electrical engineers that a properly fitted lightning conductor never fails1 he should like to ask them how the ,hotel de ,ville1 in ,brussels1 had been set on fire by lightning on the #ast of last ,june4 ,the system of lightning conductors on this building had been erected in accordance with the received theory1 and had been held up by writers on the subject as the most perfect in ,europe4 ,unless some explanation were forthcoming to account for its failure1 we could no longer regard lightning conductors as a perfect security against danger4 ,the ,president of ,section ,a1 ,professor ,fitzgerald1 in bringing the discussion to a close1 observed that one result of this meeting would be to give a new interest to the phenomena of static electricity and its practical applications4 ,he was inclined himself to think that the experiments of ,professor ,lodge were not quite analogous to the case of a flash of lightning4 ,in comparing the discharge of a ,leyden jar with a flash of lightning they should look for the analogy1 not so much in the external discharge through a series of conductors1 but rather1 as ,mr4 ,preece had observed1 in the bursting of the glass between the two coatings of the jar4 ,as regarded the oscillations in a ,leyden jar discharge1 he did not think such oscillations were at all necessary to account for the phenomena observed in the experiments4 ,many of the results which ,professor ,lodge seemed to think would require some millions of oscillations per second would be produced by a single discharge lasting for a millionth of a second4 ,improvements1 perhaps1 were possible in our present system of lightning conductors1 but practical experience had shown1 however we might reason on the matter1 that1 on the whole1 lightning conductors had been a great protection to mankind from the dangers of lightning4 ,summary4--,i will now try to sum up the results of this interesting discussion1 and state briefly the conclusions which1 as it seems to me1 may be deduced from it4 ,first1 ,i would remind my readers that a lightning rod has two functions to fulfill4 ,its first function is to promote a gradual1 but rapid1 discharge of electricity according as it is developed1 and thus to prevent such an accumulation as would lead to a flash of lightning4 ,its second function is to convey the flash of lightning1 when it does come1 harmless to the earth4 ,now1 the new views advanced by ,professor ,lodge in no way impugn the efficiency of lightning rods as regards their first function2 and it is evident that the greater the number of lightning rods distributed over a given area1 the more perfectly will this function be fulfilled4 ,this is a point of great practical importance which seemed to me1 in some degree1 lost sight of during the progress of the discussion4 ,secondly1 it was practically admitted by the highest authorities that the experiments and reasoning of ,professor ,lodge afford good grounds for reconsidering the received theory of lightning conductors as regards their second function--that of carrying the lightning flash harmless to the earth4 ,but there was undoubtedly a general feeling that it would be rash to set aside1 all at once1 the received theory on the strength of laboratory experiments made under conditions widely different from those which actually exist in a lightning discharge4 ,experiments are wanted on a larger scale2 and1 if possible1 experiments with lightning rods themselves4 ,thirdly1 the testimony of electrical engineers who have had large experience with lightning conductors seems almost unanimous that a lightning conductor erected and maintained in accordance with the conditions prescribed by the ,lightning ,rod ,conference gives perfect protection4 ,it was certainly unfortunate that the ,hotel de ,ville1 in ,brussels1 which was reputed the best protected building in ,europe1 should have been damaged by lightning just two months before the discussion took place2 but no certain conclusion can be drawn from this catastrophe until we know exactly the conditions under which it occurred4 ,so the matter stands1 awaiting further investigation4 ,,footnotes3 #da ,see his ,lectures1 published in the ,electrician1 ,june #bb1 ,june #bi1 ,july #f1 and ,july #ac1 #ahhh4 #db ,see paper read at the meeting of the ,british ,association1 in ,bath1 #ahhh1 published in the ,electrician1 page #fjg4 ,september #ad4 #dc ,see a very ingenious hypothesis1 to account for this phenomenon1 suggested by ,professor ,ewing in the ,electrician1 p4 #gab4 ,october #e1 #ahhh4 ,transcriber's ,notes ,errors and omissions in punctuation have been corrected4 ,page #aa3 8continuous inpression0 changed to 8continuous impression0 ,page #da3 8full conconducting power0 changed to 8full conducting power0 ,page #dd3 8it base0 changed to 8its base0 ,page #eh3 8follow one an-another0 changed to 8follow one another0