,illustration3 ,,first ,,direct-,,connected ,,electric ,,generator ,,unit ,,of ,,large ,,capacity ,,ever ,,constructed ,,up ,,to ,,the ,,time ,,it ,,was ,,made ,,by ,,thomas ,a4 ,,edison ,,in ,,june1 #ahha4 ,,capacity1 #abjj ,,incandescent ,,lamps ,,of #af ,,candle-,,power ,,each ,a-,b-,c ,,of ,,electricity ,,by ,,william ,h4 ,,meadowcroft ,,harper ,,brothers ,,publishers ,,new ,,york ,,london ,a-,b-,c of ,electricity ,,copyright1 #ahhh1 #aiji1 ,,by ,,william ,h4 ,,meadowcroft ,,copyright1 #aiae1 ,,by ,,harper ,,brothers ,,printed ,,in ,,the ,,united ,,states ,,of ,,america ,,published ,,may1 #aiae ,,from ,,the ,,laboratory ,,of ,,thomas ,a4 ,,edison ,,orange1 ,n4 ,j4 ,,mr4 ,w4 ,h4 ,,meadowcroft1 ,new ,york ,city4 ,,dear ,,sir3 ,i have read the ,,ms4 of your ,a-,b-,c of ,electricity1 and find that the statements you have made therein are correct4 ,your treatment of the subject1 and arrangement of the matter1 have impressed me favorably4 ,yours truly1 ,,thos4 ,a4 ,,edison ,,contents ,,chap4 ,,page ,,introduction ,,to ,,new ,,edition viii ,,preface x ,i4 #a ,,ii4 ,,definitions #c ,,iii4 ,,magnetism #af ,,iv4 ,,the ,,telegraph #bc ,v4 ,,wireless ,,telegraphy #cc ,,vi4 ,,the ,,telephone #dj ,,vii4 ,,electric ,,light #ed ,,viii4 ,,electric ,,power #hg ,,ix4 ,,batteries #ie ,x4 ,,conclusion #abg ,,introduction ,,to ,,new ,,edition ,the favor with which this book has been received has brought about the preparation of this new edition4 ,the present volume has been enlarged by the addition of certain new material and it has been entirely reset4 ,some new illustrations have been made1 and in its new dress the book1 it is hoped1 will be found to afford an even larger measure of usefulness4 ,the principles of the science remain the same1 but the author is glad of the opportunity to note certain developments in their application4 ,w4 ,h4 ,m4 ,,edison ,,laboratory1 ,april1 #aiae4 ,,preface ,while there is no lack of most excellent text-books for the study of those branches of ,electricity which are above the elementary stage1 there is a decided need of text-books which shall explain1 in simple language1 to young people of1 say1 fourteen years and upward1 a general outline of the science1 as well as the ground-work of those electrical inventions which are to-day of such vast commercial importance4 ,there is also a need for such a book among a large part of the adult population1 for the reason that there have been great and radical changes in this science since the time they completed their studies1 and they have not the time to follow up the subject in the advanced books4 ,as instances of those changes just spoken of1 the electric light1 telephone1 and storage batteries may be mentioned1 which have been developed during the last ten or twelve years1 with the result of adding very many features that were entirely new to electricians4 ,with these ideas in view ,i have prepared this little volume4 ,it is not intended1 in the slightest degree1 to be put forward as a scientific work1 but it will probably give to many the information they desire without requiring too great a research into books which treat more extensively and deeply of this subject4 ,w4 ,h4 ,m4 ,a-,b-,c ,,of ,,electricity ,a-,b-,c ,,of ,,electricity ,i ,we now obtain so many of our comforts and conveniences by the use of electricity that all young people ought to learn something of this wonderful force1 in order to understand some of the principles which are brought into practice4 ,you all know that we have the telegraph1 the telephone1 the electric light1 electric motors on street-cars1 electric bells1 etc41 besides many other conveniences which the use of electricity gives us4 ,every one knows that1 by the laws of multiplication1 twice two makes four1 and that twice two can never make anything but four4 ,well1 these useful inventions have been made by applying the laws of electricity in certain ways1 just as well known1 so as to enable us to send in a few moments a message to our absent friends at any distance1 to speak with them at a great distance1 to light our houses and streets with electric light1 and to do many other useful things with quickness and ease4 ,but you must remember that we do not know what electricity itself really is4 ,we only know how to produce it by certain methods1 and we also know what we can do with it when we have obtained it4 ,in this little book we will try to explain the various ways by which electricity is obtained1 and how it is applied to produce the useful results that we see around us4 ,we will try and make this explanation such that it will encourage many of you to study this very important and interesting subject more deeply4 ,in the advanced books on electricity there are many technical terms which are somewhat difficult to understand1 but in this book it will only be necessary to use a few of the more simple ones1 which it will be well for you to learn and understand before going further4 ,,ii ,,definitions ,the three measurements most frequently used in electricity are ,the ,volt1 ,the ,ampre1 ,the ,ohm4 ,we will explain these in their order4 ,illustration3 ,fig4 #a ,the ,volt4--,this term may be better understood by making a comparison with something you all know of4 ,suppose we have a tank containing one hundred gallons of water1 and we want to discharge it through a half-inch pipe at the bottom of the tank4 ,suppose1 further1 that we wanted to make the water spout upward1 and for this purpose the pipe was bent upward as in ,fig4 #a4 ,if you opened the tap the water would spout out and upward as in ,fig4 #a4 ,illustration3 ,fig4 #b ,the cause of its spouting upward would be the weight or pressure of the water in the tank4 ,this pressure is reckoned as so many pounds to the square inch of water4 ,now1 if the tank were placed on the roof of the house and the pipe brought to the ground as shown in ,fig4 #b1 the water would spout up very much higher1 because there would be many more pounds of pressure on account of the height of the pipe4 ,so1 you see1 the force or pressure of water is measured in pounds1 and1 therefore1 a pound is the unit of pressure1 or force1 of water4 ,now1 in electricity the unit of pressure1 or force1 is called a volt4 ,this word volt does not mean any weight1 as the word pound weight does4 ,you all know that if you have a pound of water you must have something to hold it1 because it has weight1 and1 consequently1 occupies some space4 ,but electricity itself has no weight and therefore cannot occupy any space4 ,when we desire to carry water into a house or other building we do so by means of hollow pipes1 which are usually made of iron4 ,this is the way that water is brought into houses in cities and towns1 so that it may be drawn and used in any part of a dwelling4 ,now1 the principal supply usually comes from a reservoir which is placed up on high ground so as to give the necessary pounds of pressure to force the water up to the upper part of the houses4 ,if some arrangement of this kind were not made we could get no water in our bedrooms1 because1 as you know1 water will not rise above its own level unless by force4 ,the water cannot escape as long as there are no holes or leaks in the iron pipes1 but if there should be the slightest crevice in them the water will run out4 ,in electricity we find similar effects4 ,the electricity is carried into houses by means of wires which are covered1 or insulated1 with various substances1 such1 for instance1 as rubber4 ,just as the iron of the pipes prevents the water from escaping1 the insulation of the wire prevents the escape of the electricity4 ,now1 if we were to cause the pounds of pressure of water1 in pipes of ordinary thickness1 to be very greatly increased1 the pipes could not stand the strain and would burst and the water escape4 ,so it is with electricity4 ,if there were too many volts of pressure the insulation would not be sufficient to hold it and the electricity would escape through the covering1 or insulation1 of the wire4 ,it is a simple and easy matter to stop the flow of water from an ordinary faucet by placing your finger over the opening4 ,as the water cannot then flow1 your finger is what we will call a non-conductor and the water will be retained in the pipe4 ,we have just the same effects in electricity4 ,if we place some substance which is practically a non-conductor1 or insulator1 such as rubber1 around an electric wire1 or in the path of an electric current1 the electricity1 acted upon by the volts of pressure1 cannot escape1 because the insulation keeps it from doing so1 just as the iron of the pipe keeps the water from escaping4 ,thus1 you see1 the volt does not itself represent electricity1 but only the pressure which forces it through the wire4 ,there are other words and expressions in electricity which are sometimes used in connection with the word volt4 ,these words are pressure and intensity4 ,we might say1 for instance1 that a certain dynamo machine had an electromotive force of #aaj volts2 or that the intensity of a cell of a battery was #b volts1 etc4 ,we might mention1 as another analogy1 the pressure of steam in a boiler1 which is measured or calculated in pounds1 just as the pressure of water is measured4 ,so1 we might say that #ajj pounds steam pressure used through the medium of a steam-engine to drive a dynamo could thus be changed to electricity at #ajj volts pressure4 ,the ,ampre4--,now1 in comparing the pounds pressure of water with the volts of pressure of electricity we used as an illustration a tank of water containing #ajj gallons1 and we saw that this water had a downward force or pressure in pounds4 ,let us now see what this pressure was acting upon4 ,it was forcing the quantity of water to spout upward through the end of the pipe4 ,now1 as the quantity of water was #ajj gallons1 it could not all be forced at once out of the end of the pipe4 ,the pounds pressure of water acting on the #ajj gallons would force it out at a certain rate1 which1 let us say1 would be one gallon per minute4 ,this would be the rate of the flow of water out of the tank4 ,thus1 you see1 we find a second measurement to be considered in discharging the water-tank4 ,the first was the force1 or pounds of pressure1 and the second the rate at which the quantity of water was being discharged per minute by that pressure4 ,this second measurement teaches us that a certain quantity will pass out of the pipe in a certain time if the pressure is steady1 such quantity depending1 of course1 on the size or friction resistance of the pipe4 ,in electricity the volts of pressure act so as to force the quantity of current to flow through the wires at a certain rate per second1 and the rate at which it flows is measured in ampres4 ,for instance1 let us suppose that an electric lamp required a pressure of #ajj volts and a current of one ampre to light it up1 we should have to supply a current of electricity flowing at the rate of one ampre1 acted upon by an electromotive force of #ajj volts4 ,you will see1 therefore1 that while the volt does not represent any electricity1 but only its pressure1 the ampre represents the rate of flow of the current itself4 ,you should remember that there are several words sometimes used in connection with the word ampre--for instance1 we might say that a lamp required a current of one ampre or that a dynamo would give a quantity of #bj ampres4 ,the ,ohm4--,you have learned that the pressure would discharge the quantity of water at a certain rate through the pipe4 ,now1 suppose we were to fix two discharge-pipes to the tank1 the water would run away very much quicker1 would it not8 ,if we try to find a reason for this1 we shall see that a pipe can only1 at a given pressure1 admit so much water through it at a time4 ,therefore1 you see1 this pipe would present a certain amount of resistance to the passage of the total quantity of water1 and would only allow a limited quantity at once to go through4 ,but1 if we were to attach two or more pipes to the tank1 or one large pipe1 we should make it easier for the water to flow1 and1 therefore1 the total amount of resistance to the passage of the water would be very much less1 and the tank would quickly be emptied4 ,now1 as you already know1 water has substance and weight and therefore occupies some space1 but electricity has neither substance nor weight1 and therefore cannot occupy any space2 consequently1 to carry electricity from one place to another we do not need to use a pipe1 which is hollow1 but we use a solid wire4 ,these solid wires have a certain amount of resistance to the passage of the electricity1 just as the water-pipe has to the water1 and 7as it is in the case of the water7 the effect of the resistance to the passage of electricity is greater if you pass a larger quantity through than a smaller quantity4 ,if you wanted to carry a quantity of electricity to a certain distance1 and for that purpose used a wire1 there would be a certain amount of resistance in that wire to the passage of the current through it2 but if you used two or more wires of the same size1 or one large wire1 the resistance would be very much less and the current would flow more easily4 ,suppose that1 instead of emptying the water-tank from the roof through the pipe1 we had just turned the tank over and let the water all pour out at once down to the ground4 ,that would dispose of the water very quickly and by a short way1 would it not8 ,that is very easy to be seen1 because there would be no resistance to its passage to the ground4 ,well1 suppose we had an electric battery giving a certain quantity of current1 say five ampres1 and we should take a large wire that would offer no resistance to that quantity and put it from one side of the battery to the other1 a large current would flow at once and tend to exhaust the battery4 ,this is called a short circuit because there is little or no resistance1 and it provides the current with an easy path to escape4 ,remember this1 that electricity always takes the easiest path4 ,it will take as many paths as are offered1 but the largest quantity will always take the easiest4 ,as the subject of resistance is one of the most important in electricity1 we will give you one more example1 because if you can obtain a good understanding of this principle it will help you to comprehend the whole subject more easily in your future studies4 ,we started by comparison with a tank holding #ajj gallons of water1 discharging through a half-inch pipe1 and showed you that the pounds of pressure would force the quantity of gallons through the pipe4 ,when the tap was first opened the water would spout up very high1 but as the water in the tank became lower the pressure would be less1 and1 consequently1 the water would not spout so high4 ,so1 if it were desired to keep the water spouting up to the height it started with1 we should have to keep the tank full1 so as to have the same pounds of pressure all the time4 ,but1 if we wanted the water to spout still higher we should have to use other means1 such as a force-pump1 to obtain a greater pressure4 ,now1 if we should use too many pounds pressure it would force the quantity of water more rapidly through the pipe and would cause the water to become heated because of the resistance of the pipe to the passage of that quantity acted upon by so great a pressure4 ,this is just the same in electricity1 except that the wire itself would become heated1 some of the electricity being turned into heat and lost4 ,if a wire were too small for the volts pressure and ampres of current of electricity the resistance of such wire would be overcome1 and it would become red-hot and perhaps melt4 ,electricians are therefore very careful to calculate the resistance of the wires they use before putting them up1 especially when they are for electric lighting1 in order to make allowances for the ampres of current to flow through them1 so that but little of the electricity will be turned into heat and thus rendered useless for their purpose4 ,the unit of resistance is called the ohm 7pronounced like home without the h74 ,all wires have a certain resistance per foot1 according to the nature of the metal used and the size of the wire--that is to say1 the finer the wire the greater number of ohms resistance it has to the foot4 ,water and electricity flow under very similar conditions--that is to say1 each of them must have a channel1 or conductor1 and each of them requires pressure to force it onward4 ,water1 however1 being a tangible substance1 requires a hollow conductor2 while electricity1 being intangible1 will flow through a solid conductor4 ,the iron of the water-pipe and the insulation of the electric wire serve the same purpose--namely1 that of serving to prevent escape by reason of the pressure exerted4 ,there is another term which should be mentioned in connection with resistance1 as they are closely related1 and that is opposition4 ,there is no general electrical term of this name1 but1 as it will be most easily understood from the meaning of the word itself1 we have used it4 ,let us give an example of what opposition would mean if applied to water4 ,probably every one knows that a water-wheel is a wheel having large blades1 or paddles1 around its circumference4 ,when the water1 in trying to force its passage1 rushes against one of these paddles it meets with its opposition1 but overcomes it by pushing the paddle away4 ,this brings around more opposition in the shape of another paddle1 which the water also pushes away4 ,and so this goes on1 the water overcoming this opposition and turning the wheel around1 by which means we can get water to do useful work for us4 ,you must remember1 however1 that it is only by putting opposition in the path of a pressure and quantity of water that we can get this work4 ,the same principle holds good in electricity4 ,we make electricity in different ways1 and in order to obtain useful work we put in its path the instruments1 lamps1 or machines which offer the proper amount of resistance1 or opposition1 to its passage1 and thus obtain from this wonderful agent the work we desire to have done4 ,you have learned that three important measurements in electricity are as follows3 ,the volt is the practical unit of measurement of pressure2 ,the ampre is the practical unit of measurement of the rate of flow2 and ,the ohm is the practical unit of measurement of resistance4 ,,iii ,,magnetism ,now we will try to explain to you something about magnets and magnetism4 ,there are very few boys who have not seen and played with the ordinary magnets1 shaped like a horseshoe1 which are sold in all toy-stores as well as by those who sell electrical goods4 ,well1 you know that these magnets will attract and hold fast anything that is made of iron or steel1 but they have no effect on brass1 copper1 zinc1 gold1 or silver1 yet there is nothing that you can see which should cause any such effect4 ,you will notice1 then1 that magnetism is like electricity2 we cannot see it1 but we can tell that it exists1 because it produces certain effects4 ,and here is another curious thing--magnetism produces electricity1 and electricity produces magnetism4 ,this seems to be a very convenient sort of a family affair1 and it is owing to this close relation that we are able to obtain so many wonderful things by the use of electricity4 ,we shall now show you how electricity produces magnetism1 and1 when we come to the subject of electric lighting we will explain how magnetism produces electricity4 ,illustration3 ,fig4 #c ,the easiest way to show how electricity makes magnetism is to find out how magnets are made4 ,suppose we wanted to make a horseshoe magnet1 just mentioned above2 we would take a piece of steel and wind around it some fine copper wire1 commencing on one leg of the horseshoe and winding around until we came to the end of the other leg4 ,then we should have two ends of wire left1 as shown in the sketch4 7,fig4 #c47 ,we connect these two ends with an electric battery1 giving1 say1 two volts1 and then the ampres of current of electricity will travel through the wire1 and in doing so has such an influence on the steel that it is converted into a magnet1 such as you have played with4 ,the current is broken--that is to say1 it is shut off several times in making a magnet of this kind1 and then the wire is taken away from the battery and is unwound from the steel horseshoe1 leaving it free from wire1 just as you have seen it4 ,this horseshoe is now a permanent magnet--that is1 it will always attract and hold pieces of iron and steel4 ,now1 if you were to do the same thing with a horseshoe made of soft iron instead of steel it would not be a magnet after you stopped the current of electricity from going through the wires1 although the piece of iron would be a stronger magnet while the electricity was going through the wire around it4 ,the steel magnet is called a permanent magnet1 and its ends1 or poles1 are named ,north and ,south4 ,there is usually a loose piece of steel or iron1 called an armature1 put across the ends1 which has the peculiar property of keeping the magnetism from becoming weaker1 and thereby retaining the strength of the magnet4 ,the strongest part of the magnet is at the poles1 while1 at the point marked 7which is called the neutral point7 there is scarcely any magnetism4 ,it will be well to remember the object of the armature as we shall meet it again in describing dynamo machines4 ,the magnets made of iron are called electromagnets because they exhibit magnetism only when the ampres of current of electricity are flowing around them4 ,they also have two poles1 north and south1 as have permanent magnets4 ,electromagnets are used in nearly all electrical instruments1 not only because they are stronger than permanent magnets1 but because they can be made to act instantly by passing a current of electricity through them at the most convenient moment1 as you will see when we explain some of the electrical instruments which are used to produce certain effects4 7,fig4 #d47 ,illustration3 ,fig4 #d ,of course there are a great many different shapes in which magnets are made4 ,the simplest is the bar magnet1 which is simply a flat or round piece of iron or steel4 ,suppose you made a magnet of a flat piece of steel and put on top of it a sheet of paper1 and then threw on the paper some iron filings1 you would see them arrange themselves as is shown in the following sketch4 7,fig4 #e47 ,the filings would always arrange themselves in this shape1 no matter how large or small the magnets were4 ,and1 if you were to cut it into two or half a dozen pieces1 each piece would have the same effect4 ,this shows you that each piece would itself become a magnet and would have its poles exactly as the large one had4 ,illustration3 ,fig4 #e ,now1 we have another curious thing to tell you about magnets4 ,if you present the north pole of a magnet to the south pole of another magnet1 they will attract and hold fast to each other1 but if you present a south pole to another south pole1 or a north pole to a north pole1 they will repel each other1 and there will be no attraction4 ,you can perform some interesting experiments by reason of this fact4 ,we will give you one of them4 ,take1 say1 a dozen needles and draw them several times in the same direction across the ends of a magnet so that they become magnetized4 ,now stick each needle half-way through a piece of cork1 and put the corks1 with the needles sticking through them1 into a bowl of water4 ,then take a bar magnet and bring it gradually toward the middle of the bowl and you will see the corks advance or back away from the magnet4 ,if the ends of the needles sticking up out of the water are south poles and the end of the magnet you present is a north pole1 the needles will come to the center2 but will go to the side of the bowl if you present the south pole4 ,you can vary this pretty experiment by turning up the other ends of part of the needles4 ,you will remember that when we explained what resistance meant1 we told you that electricity would always take the easiest path1 and while part of it will flow in a small wire1 the largest portion will take an easier path if it can get to something larger that is a metallic substance4 ,electricity will only flow easily through anything that is made of metal4 ,you will also remember that you learned that when electricity took a short cut to get away from its proper path it was called a short circuit4 ,all this must be taken into consideration when magnets are being made4 ,in the first place1 the wire we wind around steel or iron to make magnets must always be covered with an insulator of electricity4 ,magnet wire is usually covered with cotton or silk4 ,if it were left bare1 each turn of the wire would touch the next turn1 and so we should make such an easy path for the electricity that it would all go back to the battery by a short circuit1 and then we would get no magnetic effect in the steel or iron4 ,the only way we can get electricity to do useful work for us is to put some resistance or opposition in its way4 ,so you see that if we make it travel through the wire around the iron or steel1 there is just enough resistance or opposition in its way to give it work to get through the wire1 and this work produces the peculiar effect of making the iron or steel magnetic4 ,the covering on the wire1 as you will remember1 is called insulation4 ,,iv ,,the ,,telegraph ,every one knows how very convenient the telegraph is1 but there are not many who think how wonderful it is that we can send a message in a few seconds of time to a distant place1 even though it were thousands of miles away4 ,and yet1 though the present system of telegraphing is a wonderful one1 the method of sending a telegram is simple enough4 ,the apparatus that is used in sending a telegram is as follows3 ,the ,battery4 ,the ,wire4 ,the ,telegraph ,key4 ,the ,sounder4 ,the different kinds of electric batteries will be mentioned afterward1 so we will not stop now to describe them1 but simply state that a battery is used to produce the necessary electricity4 ,as you all know what wire is1 there is no necessity of describing it further4 ,the telegraph key is shown in the sketch below4 7,fig4 #f47 ,illustration3 ,fig4 #f ,this instrument is usually made of brass1 except that upon the handle there is the little knob which is of hard rubber4 ,the handle1 or lever1 moves down when this knob is pressed1 and a little spring beneath pushes it up again when let go4 ,you will see a second smaller knob1 the use of which we will explain later4 ,the sounder is shown on the following page4 7,fig4 #g47 ,the part consisting of the two black pillars is an electromagnet1 and across the top of these pillars is a piece of iron called the armature1 which is held up by a spring4 ,illustration3 ,fig4 #g ,now let us see how the battery and wire are placed in connection with these instruments4 ,you have seen that we usually have two wires for the electricity to travel in1 one wire for it to leave the battery1 and the other to return on4 ,but you will easily see that if two wires had to be used in telegraphing it would be a very expensive matter1 especially when they had to be carried thousands of miles4 ,so1 instead of using a second wire1 we use the earth to carry back the electricity to the battery1 because the earth is a better conductor even than wire4 ,although a quantity of ground equal in size to the wire would offer thousands of times greater resistance than the wire1 yet1 owing to the great body of our earth1 its total resistance is even less than any telegraph wire used4 ,when two electric wires are run from a battery and connected together through some instrument1 this is called a circuit1 because the electricity has a path in which it can travel back to the battery4 ,this would be a metallic circuit2 but when one wire only is used1 and the other side of the battery is connected with the earth1 it is called a ground or earth circuit1 because the electricity returns through the earth4 ,illustration3 ,fig4 #h ,if you look at this sketch 7,fig4 #h7 you will see how the telegraph instruments are connected and will then be able to understand how a message can be sent4 ,here we have two sets of telegraph apparatus1 one of which1 let us say1 is in ,new ,york and the other in ,philadelphia4 ,you will see that one wire from the battery is connected with the earth1 and the other wire with the sounder4 ,another wire goes from the sounder to one leg of the key so as to make the brass base of the key part of the circuit4 ,the other leg of the key is insulated from the brass base by being separated therefrom with some substance which will not carry electricity1 such1 for instance1 as hard rubber4 ,we will suppose that there is already a wire strung up on poles between ,new ,york and ,philadelphia1 and that the key1 sounder1 and battery in the latter city are connected in the same way as those in ,new ,york4 ,now1 to enable us to send a message from one city to the other we must connect the ends of the wires to the instruments in each city2 so we connect one end to the insulated leg of the key in ,new ,york1 and the other end to the insulated leg of the key in ,philadelphia4 ,everything is now completed1 and1 as soon as we find out what is the use of that part of the key that has a little round1 black handle1 we shall be ready to start4 ,this is called the switch4 ,if you will look once more at the picture of the key you will see under the long handle 7or lever7 a little point which the lever will touch when it is pressed down4 ,now this little point is part of that insulated leg1 and1 therefore1 this point is also insulated from the base4 ,if a current of electricity were sent along the wire it could not get any farther than this point unless we put in some arrangement to complete the path1 or circuit1 for it to travel in4 ,we therefore put in the switch4 ,one end of the switch 7which is made of brass with a rubber handle7 is fastened on the base of the key1 so that it may be moved to the right or left4 ,the other end1 when the switch is moved to the left 7or closed71 touches a piece of brass fastened to the little point we have mentioned1 and so makes a free path for the electricity to go through the base of the key and through the wire to the sounder1 and from there to the battery1 and so back to the earth4 ,this switch must be opened before the sounder near it will respond to its neighboring key4 ,now we are ready to send a message4 ,suppose we want to send a telegram from ,new ,york to ,philadelphia4 ,the operator in ,new ,york opens his switch and presses down his key several times4 ,the switch on the ,philadelphia key being closed1 the electricity goes through to the sounder1 and1 this being made an electromagnet by the current passing through the wire1 the iron armature is attracted by the magnetism and drawn down to the magnet with a snap4 ,it will stay there as long as the ,new ,york operator keeps his lever pressed down1 but1 when he allows it to spring up1 there is no current passing through the ,philadelphia sounder and there is no magnetism1 consequently the armature springs up again with a click4 ,as often as the operator presses down his key lever and lets it spring up again1 the same action takes place in the sounder1 and it makes that click1 click1 which you have heard if you have ever seen telegraph instruments in operation4 ,let us continue1 however1 to send our message4 ,the ,new ,york operator1 having pressed down his key several times to signal the ,philadelphia operator1 closes his switch to receive the answer from ,philadelphia4 ,the operator in the latter city then opens his switch and presses down his key several times1 which makes the ,new ,york sounder click1 in the same way1 to let the operator there know that he is ready to receive the message4 ,he then closes his switch and receives the telegram which the ,new ,york operator sends after opening his key4 ,telegraphic messages are sent and received in this way and are read by the sound of the clicks4 ,these sounds may be represented on paper by dots1 dashes1 and spaces4 ,for instance1 if you press down the key and let it spring back quickly1 that would represent a dot4 ,if you press down the key and hold it a little longer before letting it spring up again1 it would represent a dash4 ,a space would be represented by waiting a little while before pressing down the key again4 ,we show you below the alphabet in these dots1 dashes1 and spaces1 and these are the ones now used in sending all telegraphic messages4 ,illustration ,thus1 you see1 if you were telegraphing the word and you would press down your key and let it return quickly1 then press down again and return after a longer pause1 which would give the letter ,a2 then slowly and quickly1 which would be ,n2 then slowly and twice quickly1 which would be ,d4 ,any persevering boy can learn to operate a telegraph instrument by a little study and regular practice2 and1 as complete learner's sets can be purchased very cheaply1 this affords a pleasant and useful recreation for boys4 ,there are many cases where two boys living near each other have a set of telegraph instruments in their homes and run a wire from one house to the other1 thus affording many hours of pleasant and profitable amusement4 ,in giving the above explanation of telegraphing we have described only the simple and elementary form4 ,in large telegraph lines1 such as those of the ,western ,union1 there are many more additional instruments used1 which are very complicated and difficult to understand2 such1 for instance1 as the quadruplex1 by which four distinct messages can be sent over the same wire at the same time4 ,we have1 therefore1 described only the simplest form in order to give the general idea of the working of the telegraph by electromagnetism1 which is the principle of all telegraphing4 ,when you study electricity more deeply you will find this subject and the many different instruments very interesting and wonderful4 ,v ,,wireless ,,telegraphy ,if it has seemed extraordinary to you that only one wire should be necessary for sending a message by the electric telegraph1 and that our earth can be used instead of a second wire1 how much more wonderful it is to realize that in these days we can exchange telegraphic messages with different points without any connecting wires at all between them1 even though the places be many hundred miles apart4 ,thus1 two ships on the ocean1 entirely out of sight of each other1 may intercommunicate1 or may telegraph to or receive despatches from a far-distant shore2 indeed1 telegraphy without wires has been accomplished across the ,atlantic ,ocean4 ,in the language of the day1 this is called wireless telegraphy1 although it is more correct to think of it as aerial1 or space1 telegraphy4 ,as you will naturally want to know how this is effected1 we will try to explain the main principles in a simple manner4 ,if you drop a stone into a quiet pond1 you will see the water form into ring-like waves1 or ripples1 which travel on and on until they die away in the far distance4 ,these waves are caused1 as we have seen1 by a disturbance of the body of water4 ,probably you have already learned in school that all known space is said to be filled with a medium called ether1 and that this medium is so exceedingly thin that it penetrates1 or permeates1 everything1 so that it exists in the densest bodies as well as in free space4 ,for the sake of obtaining a clear idea of this theory we may imagine that the ether envelops and permeates every thing in the entire universe4 ,hence we can easily realize that1 although we cannot see or feel the ether1 any disturbance of it will set it in wavelike motion4 ,modern science accounts for light1 radiant heat1 and electrical phenomena by reason of wavelike disturbances1 vibrations1 or pulsations of this ether4 ,thus1 if you should strike a light1 the ether would be disturbed1 causing waves to form1 which1 like the waves in the water1 would travel in every direction4 ,when these waves reached the eyes of another person within seeing distance1 that person's eyes would be so acted upon by the waves that he would see the light which you had made1 and would see it instantly1 for light waves travel about #ahf1jjj miles per second4 ,so1 if you create an electrical disturbance1 the same kind of an effect will be produced2 that is to say1 waves in the ether will be created1 or propagated1 and will travel on and on in every direction4 ,now1 if some form of electrical appliance can be made that will be of the right kind to respond to them 7as the eye responds to light rays71 these electric waves can be made practically useful for transmitting messages through space4 ,this is just what has been done1 and we will now give you a brief general description of one kind of apparatus used4 ,for sending1 or transmitting1 as it is usually termed1 there is used an induction-coil1 having rather large brass balls on the secondary terminals2 suitable batteries1 a condenser1 a ,morse telegraph key1 and an aerial1 or wire which is carried away up into the air vertically1 and is made fast to a pole or special tower4 ,when these are connected properly1 the closing of the circuit with the key will cause sparks to jump between the brass balls4 ,this electrical discharge1 or oscillation1 is carried by the aerial into the upper air and causes intense pulsations in the ether1 which set up waves as already mentioned4 ,if the circuit is opened again the disturbance ceases4 ,so1 by alternately closing and opening the circuit1 the ,morse characters can be imitated4 ,but how can these signals be received by the man for whom they are intended1 who may be a hundred miles or more away8 ,he has a receiving set1 consisting of a sensitive relay1 batteries1 resistance-coils1 a ,morse register1 an aerial1 and a special device called a coherer4 ,this is the important part of the whole set1 because it is sensitive to the electrical waves4 ,it consists of a little glass tube about as large around as an ordinary lead-pencil1 and perhaps two inches long4 ,in the tube are two metallic plugs1 each having a wire attached so that one wire projects from each end of the tube4 ,the plugs are separated inside the tube by a very small space1 and in this space are some metal filings4 ,one wire from the coherer is connected to the aerial and the other to the ground4 ,when there are no electrical ether waves to influence them1 these filings1 being loosely separated1 are at rest and offer high resistance2 but when the ether is disturbed by electrical vibrations and the waves arrive at the coherer 7through the aerial71 these filings are drawn together1 or cohere4 ,this lowers their resistance and they become a better conductor4 ,now1 the coherer wires are also connected through a battery to the relay1 which in turn is connected through another battery to a ,morse register4 ,therefore1 when the filings become a conductor1 the current flows through them and the circuit to the relay is closed4 ,that attracts an armature which closes the circuit of the ,morse register and thus marks the electrical impulse on a strip of paper tape4 ,in the mean time1 a restoring device1 called a decoherer1 operated also by the relay circuit1 has tapped upon the coherer1 thus shaking the filings loose again1 so that they are ready to cohere again and register another impulse1 or character4 ,thus1 by pressing the key at the transmitting end for long or short periods1 to represent ,morse characters1 long and short waves are propagated in the ether and are received and recorded at the receiving end through the coherer and other parts of the receiving set4 ,in this way telegraphic messages are sent and received through space1 between points separated by hundreds or thousands of miles4 ,we have tried to describe to you the general principles underlying the art of wireless telegraphy as plainly as possible1 using for illustration the simplest kind of apparatus employed for the practical sending and receiving of messages4 ,at the present day there are several systems in actual practice1 and with the growth of the art there have been many elaborations of apparatus that have come into use4 ,for instance1 the coherer is not as much used as formerly4 ,in its place there are employed several kinds of wave-detectors as they are now termed1 and in many of the systems the electrical pulsations are generated by a dynamo-machine instead of batteries4 ,then1 again1 instead of the messages being recorded by a ,morse register at the receiving end1 the operator receives them by means of a telephone receiver1 through which he hears the ,morse characters and writes them down in words as he hears them4 ,generally the aerial1 or antenn1 as it is sometimes named1 consists of several wires1 sometimes a large number1 carried to a considerable height4 ,there are a great many other details which might be written to explain all the complicated apparatus which is used in some of the systems1 but it is not intended in this book to offer more than a general explanation of main principles4 ,we must leave it to you to study the details elsewhere if you so desire after you have read these pages4 ,,vi ,,the ,,telephone ,you probably all know that the telephone is an electrical instrument by which one person may talk to another who is at a distance4 ,not only can we talk to a person who is in a different part of the city1 but such great improvements have been made in these instruments that we can talk through the telephone to a person in another city1 even though it be hundreds of miles away4 ,the main principle of the telephone is electromagnetism1 as in the telegraph1 but there are other important points in addition to those we mentioned in describing the latter4 ,let us take first the ,,induction-,,coil ,you will remember that an electromagnet is made by winding many turns of wire around a piece of iron and sending a current of electricity through this wire4 ,now1 suppose this current of electricity was being supplied by two cells of a battery4 ,if you took in your hands the wires coming from these two cells1 giving1 say1 four volts1 you could not feel any shock2 but if you were to take hold of the ends of the wires on the electromagnet and separate them while this same current was going through1 you would get a decided shock4 ,this separation would break the circuit1 and the reason you would get a shock is that1 while the electricity is acting on the wire1 the iron itself is magnetized1 and on breaking the circuit reacts upon the wire1 producing for a moment more volts of pressure in every turn of it4 ,thus1 you see1 this weak pressure of electricity as it travels through the wire can yet produce1 through its magnetism1 strong momentary effects1 but you cannot feel it unless you break the circuit4 ,,how ,,the ,,induction-,,coil ,,is ,,made ,the object of the induction-coil is to produce high intensity1 or pressure1 from a comparatively weak pressure and large current of electricity2 so1 if we add still more wire1 the magnet has a larger number of turns to act upon and thus makes a very strong pressure1 or large number of volts1 but a lesser number of ampres4 ,instead of taking one piece of iron1 as we would for an ordinary electromagnet1 we take a bundle of iron wires in making an induction-coil1 as these give a stronger effect4 ,around this bundle of wires we wrap many turns of insulated copper wire4 ,this is called the primary coil1 and the ends of this wire are to be attached to the battery4 ,illustration3 ,fig4 #i ,on top of1 or over1 this primary coil we wrap a great many turns of very fine wire1 of which1 as it is so fine1 a great length can be used4 ,this is called the secondary coil1 and it is in this coil that the volts1 or pressure1 of electricity become strongest4 ,above we show you a sketch of an induction-coil4 7,fig4 #i47 ,at the left-hand side of the cut is a circuit-breaker1 which is simply a piece of iron 7armature7 on a spring placed opposite the iron core4 ,this armature is made a part of the wire leading to the primary coil4 ,when the current from the battery is sent through the wires1 the core becomes magnetized and draws this armature away from a fixed contact point1 thus breaking the circuit1 but the spring pulls it back1 again completing the circuit1 and so it keeps going back and forth very rapidly with a br-r-r-ing sound4 ,if you were now to take hold of the ends of the secondary coil you would get a continuous series of quick shocks which would feel like pins and needles running into you4 ,perhaps most of you have taken hold of the handles of a medical battery and have had shocks therefrom4 ,in so doing1 you have simply had the current from the secondary of an induction-coil4 ,the current may be made weaker by sliding a metallic cover over part of the iron core and so shutting off part of the magnetic effect4 ,,sparking ,,coils ,while on this subject we may add that these coils will produce sparks from the two ends of the wire of the secondary coil4 ,these sparks vary in length according to the amount of wire in the coil4 ,small ones are made which give a spark a quarter of an inch in length1 while others are made which will give sparks #aj1 #ab1 and #af inches in length4 ,in the latter1 however1 there are many miles of wire in the secondary coil4 ,the largest induction-coil known is one which was made for an ,english scientist4 ,there are #cda1hej turns1 or #bhj miles1 of wire in the secondary coil4 ,with #cj cells of ,grove battery this coil will give a spark #db inches in length4 ,you may form some idea of the effect of this induction-coil when we state that if we desired to produce the same length of spark direct from batteries1 without using an induction-coil1 we should require the combined volts of pressure of #fj1jjj to #ajj1jjj cells of battery4 ,having explained to you briefly the induction-coil--how it is made and its action--we must ask you to bear these principles in mind1 and presently we will tell you how it is used in the telephone4 ,the next thing we shall try to explain will be ,,the ,,vibrating ,,diaphragm ,did you ever take the end of a cane in your hand1 raise it up over your head1 and then bring it down suddenly and sharply1 so that it nearly touched the ground1 as though you were about to strike something8 ,if not1 try it now with a thin walking-cane or with a pine stick about three feet long and one-half inch thick1 and you will find that there is a peculiar sound given out4 ,it is not the stick that makes this sound1 but it is owing to the fact that you have caused the air to vibrate1 or tremble1 and thus give out a sound4 ,illustration3 ,fig4 #aj ,if you strike a tuning-fork sharply you will see the ends vibrate and a sound will be given4 ,if you put your fingers on top of a silk hat and speak near it you will feel vibrations of your voice4 ,every time you speak you cause vibrations of the air2 and the louder and higher you speak the greater the number of vibrations4 ,suppose you take a thin piece of wood in your hands 7say1 for instance1 the lid of a cigar-box cut in the shape shown in the picture1 ,fig4 #aj7 and hold it about two inches from your mouth and then speak4 ,you will feel the wood tremble in your hand4 ,this is because the vibrations of the air cause the wood to vibrate in the same manner4 ,these vibrations are very minute and cannot be seen with the naked eye1 but they actually take place1 and could be measured with a delicately balanced instrument4 ,illustration3 ,fig4 #aa ,now let us try another experiment in further illustration of this principle4 ,we will take a tube about three inches long and one and one-half or two inches in diameter4 ,this tube may be made of cardboard4 ,now cut out a piece of thin cardboard which will just fit over one end of the tube4 ,this piece we will call the diaphragm4 ,fasten the diaphragm by pasting it with two strips of thin paper to the tube4 ,these strips of paper should be fastened only on the ends1 and the middle of the paper allowed to be slack1 as shown in the picture1 so that the diaphragm may work backward and forward easily4 ,take a small shot about the size seen in the sketch and tie it to a single thread of fine silk1 then let it hang as shown in the sketch 7,fig4 #aa71 so that it will only just touch the diaphragm4 ,now1 if you speak into the open end of the tube the diaphragm will vibrate and the shot will be seen to move to and from it according to the strength of the vibrations4 ,if we could by any means make a diaphragm in another tube reproduce these same vibrations1 we should hear the same words respoken1 if the tube were held to the ear4 ,illustration3 ,fig4 #ab ,while the vibrations caused by the human voice are too minute to be seen1 it may seem surprising that they can be made to produce power4 ,this is done by an ingenious mechanism called a ,phonomotor1 perfected by the great inventor ,thomas ,a4 ,edison1 of whom every one has probably heard4 ,this mechanism1 when spoken or sung at 7or into7 immediately responds by causing a wheel to revolve4 ,no amount of blowing will start the wheel1 but it can instantly be set in motion by the vibrations caused by sound4 ,the ,phonomotor 7which is shown in the engraving ,fig4 #ab7 has a diaphragm and mouthpiece4 ,a spring1 which is secured to the bedpiece1 rests on a piece of rubber tubing placed against the diaphragm4 ,this spring carries a pawl that acts on a ratchet or roughened wheel on the fly-wheel shaft4 ,a sound made in the mouthpiece creates vibrations in the diaphragm2 the vibrations of the diaphragm move the spring and pawl with the same impulses1 and as the pawl thus moves back and forth on the ratchet-wheel it is made to revolve4 ,the instrument1 therefore1 is of great value for measuring the mechanical force of sound waves1 or vibrations1 produced by the human voice4 ,,the ,,transmitter ,that part of the telephone into which we speak is called the transmitter4 ,this is usually a piece of hard rubber having a round mouthpiece cut through it4 ,at the other side of this mouthpiece is placed a diaphragm made of a thin piece of metal1 which is held m place by a light spring4 ,behind this diaphragm1 and very close to it1 is placed a carbon button4 ,between this carbon button and the diaphragm is a small piece of platinum1 which is placed so as to touch both the button and diaphragm very lightly4 ,this platinum contact piece is connected with one of the wires running to the primary of the induction-coil1 and the spring attached to the carbon button is connected with the battery to which the other wire of the primary is connected4 ,this is all shown in the sketch of a transmitter4 7,fig4 #ac47 ,illustration3 ,fig4 #ac ,a is the mouthpiece2 ,b1 the diaphragm2 ,c1 the carbon button2 ,d1 the wire at the end of which is the platinum contact2 ,e1 the battery2 and ,f1 the induction-coil2 ,p1 ,p are the wires to the primary1 and ,s1 ,s to the secondary wires4 ,we will now say a few words about the receiver1 and then describe the manner in which the telephone works4 ,,the ,,receiver ,this is that part of the telephone which is held to the ear1 and by which we can hear the words spoken into the transmitter of the telephone at the other end of the line4 ,illustration3 ,fig4 #ad ,the receiver is made of hard rubber1 and contains a permanent bar magnet1 which is wound with wire so as to make it also an electromagnet when desired4 ,in front of this magnet is placed loosely a diaphragm of thin sheet iron4 ,this diaphragm is placed so as to be within the influence of the magnet1 but just so that neither one can touch the other4 ,fig4 #ad is a sketch of the receiver4 ,a and ,b are the wires leading to the magnet1 ,c1 and ,d is the diaphragm4 ,e and ,f are where the wires connect1 one from the secondary of the induction-coil in the other telephone1 and the other connected with the earth4 ,,the ,,carbon ,,button ,the little carbon button plays an important part in the telephone4 ,you will see from the sketch of the transmitter that the current of electricity will flow through the carbon button to the contact point and through the wire to the primary of the induction-coil4 ,now1 carbon has a peculiarity1 which is this1 that if we press this carbon button1 ever so slightly1 against the platinum contact1 there would be less resistance to the flow of the electricity through the wire to the primary1 and the more we press it the less the resistance becomes4 ,the consequence of this would be that more current would go to the primary1 and the secondary would become correspondingly stronger4 ,if the carbon button were left untouched1 and nothing pressed against it1 the flow of current through it would be perfectly even4 ,having examined the inside of the transmitter and receiver1 and understanding the effect of pressure on the carbon button1 let us now see ,,how ,,the ,,telephone ,,works ,when we speak into the mouthpiece of the transmitter1 the vibrations of the air cause the diaphragm to vibrate very rapidly1 and1 of course1 every movement of the diaphragm presses more or less against the carbon button1 in consequence of which the currents passing through the primary of the induction-coil are constantly increased or diminished and thus produce similar effects1 but magnified1 in the secondary4 ,the effect of this is that the magnet in the receiver of the other telephone is receiving a rapidly changing current1 which1 producing corresponding magnetic changes1 makes the magnet alternately weaker or stronger4 ,this influences1 by magnetism1 the iron diaphragm accordingly1 and makes it reproduce the same vibrations that were caused by the speech at the transmitter of the sending telephone4 ,thus1 the same vibrations being reproduced1 the original sounds are given out1 and we can hear what the person at the sending telephone is saying4 ,the action of the telephone illustrates well the wonderfully quick action of the electric current by the reproduction of these sound waves1 or air vibrations1 for they number many thousands in one minute's speech4 ,,vii ,,electric ,,light ,we have now arrived at a very interesting part of the study of electricity1 as well as a more difficult part than we have yet told you of1 but one which you can easily understand if you read carefully4 ,you must all have seen electric lights1 either in the streets or in some large buildings1 for so many electric lights are now used that there are very few people who have not seen them4 ,but perhaps some of you have only seen the large1 dazzling lights that are used in the streets1 and do not know that there is another kind of electric light which is in a globe about the size and shape of a large pear1 and gives about the same light as a good gas-jet4 ,these two kinds of electric lights have different names4 ,the large1 dazzling lights which you see in the streets are called arc-lights1 and the small1 pear-shaped lamps1 which give a soft1 steady light1 are called incandescent lights4 ,we will tell you later why these names are given to them4 ,illustration3 ,fig4 #ae ,the incandescent lights are generally used in houses1 stores1 theaters1 factories1 steamboats1 and other places where a number of small lights are more pleasant to the eyes4 ,the arc-lights 7,fig4 #ae7 are used to light streets and large spaces where a great quantity of light is wanted4 ,it would not be pleasant to have one of these dazzling arc-lamps in your parlor--although it would give a great deal of light--because your eyes would soon become tired4 ,but two or three of the small incandescent lights 7,fig4 #af7 would be very agreeable1 because they would give you a nice1 soft light to read or work by1 and would not tire your eyes4 ,so1 you see1 these two different kinds of lamps are very useful in their proper places4 ,now1 if you will read patiently and carefully1 we will try and explain how both these lights are made4 ,illustration3 ,fig4 #af ,you have seen that the telegraph1 telephone1 electric bells1 etc41 are worked by batteries4 ,electric lights1 however1 require such a large amount of current that it is too expensive to produce them in large quantities by batteries4 ,a small number of lamps could be lighted by batteries1 but if we were to attempt to use them to light #ejj or #a1jjj lamps together1 the expense would be so enormous as to make it entirely out of the question4 ,there are many millions of incandescent lamps in use in the ,united ,states1 but you will easily see that there could not be that number used if we had to depend on batteries to light them4 ,you will understand this more thoroughly when you have finished reading this little book4 ,well1 you will ask1 if we cannot use batteries1 what is used to produce these electric lights8 ,machines called dynamo-electric machines1 or generators1 which are driven by steam-engines or water-power1 are used to produce the electricity which makes these lamps give us light4 ,you will remember that in the chapter on ,magnetism we explained to you how electricity makes magnetism1 and now we will explain how1 in the dynamo1 magnetism makes electricity4 ,illustration3 ,fig4 #ag ,it has been found that the influence of a magnet is very strong at its poles1 and that this influence is always in the same lines4 ,this influence has been described as lines of force1 which you will see represented in the sketch above by the dotted lines 7,fig4 #ag74 ,of course1 these lines of force are only imaginary and cannot be seen in any magnet1 but they are always present4 ,the meaning of this term lines of force1 then1 is used to designate the strength of the magnet4 ,many years ago the great scientist ,faraday made the discovery that1 by passing a closed loop of wire through the magnetic lines of force existing between the poles of a magnet1 the magnetism produced the peculiar effect of creating a current of electricity in the wire4 ,if the closed loop of wire were passed down1 say from ,u to ,d1 the current flowed in the wire in one direction1 and if it were passed upward1 from ,d to ,u1 the current flowed in the other direction4 ,thus1 you see1 magnetism produces electricity in the closed loop of wire as it cuts through the magnetic lines of force4 ,just why or how1 nobody knows2 we only know that electricity is produced in that way1 and to-day we make practical use of this method of producing it by embodying this principle in dynamo-machines1 as we will shortly explain4 ,in carrying this discovery into practice in making dynamo-machines we use copper wire4 ,if iron were used1 there would be a current of electricity generated1 but it would be much less in quantity1 because iron wire has much greater resistance to the passage of electricity than the same size of copper wire4 ,perhaps you can understand it more thoroughly if we state that when a closed loop of wire is passed up and down between the poles of a strong magnet there is a very perceptible opposition felt to the passage of the wire to and fro4 ,this is due to the influence of the magnetism upon the current produced in the wire as it cuts through the lines of force1 and1 inasmuch as these lines of force are always present at the poles of a magnet1 you will see that1 no matter how many times you pass the loop of wire up and down1 there will be created in it a current of electricity by its passage through the lines of force4 ,illustration3 ,fig4 #ah ,suppose that1 instead of using one single loop of copper wire1 you wound upon a spool a long piece of wire like that in ,fig4 #ah1 and that you turned this spool around rapidly between the poles of the magnet1 you would thus be cutting the lines of force by the same wire a great many times1 and every time one length of the wire cut through the lines of force some electricity would be generated in it1 and this would continue as long as the spool was revolved4 ,but1 as each length would only be a part of the one piece of wire1 you will easily see that there would be a great deal of electricity generated in the whole piece of wire4 ,illustration3 ,fig4 #ai ,all we have to do1 then1 is to collect this electricity from the two ends of the wire1 and use it4 ,if we should attach two wires to the two ends of this wire on the spool1 they would be broken off when it turned around1 so we must use some other method4 ,we fix on the end of the spool 7which is called an armature7 two pieces of copper1 so that they will not touch each other 7as in ,fig4 #ai71 and fasten the ends of the wire to these pieces of copper4 ,this is called a commutator1 and1 as you see1 is really the ends of the wire on the spool4 ,now we get two thin1 flat pieces of copper and fix them so that they will rest upon the copper bars of the commutator1 but will not go round with it4 ,these two flat pieces of copper are called the brushes1 and they will collect from the commutator the electricity which is gathered in the wire around the spool4 ,as the brushes stand still1 two wires can be fastened to them1 and thus the ampres of current of electricity1 acted upon by the volts pressure1 can be carried away to be used in the lamps1 for you must remember that as long as the spool turns around it gathers more electricity while there is any magnetism for the wire on the spool to pass through4 ,the constant revolving of the spool creates so much electricity that it is driven out from the wire on the spool1 through the commutator to the brushes1 and there it finds a path to travel away from the pressure of the new electricity which is all the time being made4 ,in this way we get a continuous current of electricity in the two wires leading from the commutator1 and can use it to light electric lamps or for other useful purposes4 ,in explaining this to you1 so far1 we have used as an illustration of the magnet one of the steel permanent magnets in order to make the explanation more simple1 but now that you understand how the electricity is made1 we must explain to you something about the magnets that are used in dynamo-machines4 ,we can perhaps make this more clear by giving another example4 ,suppose you had a dynamo which was lighting up #ajj of the incandescent lamps1 each of #bjj ohms resistance and each requiring #ajj volts pressure4 ,now each lamp would take just a certain quantity of electricity1 say half an ampre2 so1 the #ajj lamps would require one hundred times that quantity4 ,but1 if you turned off #ej of these lamps at once1 the tendency would be for the pressure to rise above the #ajj volts required for the other #ej1 and they would be apt to burn out quicker4 ,it is plainly to be seen1 then1 that we must have some means of regulating the magnetism so as to regulate the lines of force for the wire on the armature to cut through4 ,we can do this with an electromagnet1 but not with a permanent magnet1 because we cannot easily regulate the amount of magnetism which a permanent magnet will give4 ,there is another reason why we cannot use permanent magnets in a dynamo1 and that is because they cannot be made to give as much magnetism as an electromagnet will give4 ,thus you will see that there are very good reasons for using electromagnets in making dynamo-machines4 ,let us see now how these electromagnets and dynamos are made1 and then examine the methods which are followed to operate and use them4 ,you must remember1 to begin with1 that in referring to wire used on magnets and armatures and for carrying the electricity away to the lamps1 we always mean wire that is covered or insulated4 ,in electric lighting1 insulated wire is always used1 except at the points where it is connected with1 the dynamo1 the lamps1 a switch1 or any point where we make what is called a connection4 ,as the shape of the magnets is different in the dynamos of various inventors1 we will take for illustration the one that is nearest the shape of the horseshoe and the shape that is generally used in illustrating the principle of the dynamo4 ,this is the form used by ,mr4 ,edison1 whom we have previously mentioned4 ,this form is shown in ,fig4 #bj4 ,now1 although this magnet appears to be in one piece1 it really consists of five parts screwed together so as to make1 practically1 one piece4 ,the names of the parts are as follows3 ,f1 ,f are the cores2 ,c the yoke1 which binds them together2 and ,p1 ,p the pole pieces1 where the magnetism is the strongest4 ,these pole pieces are rounded out to receive the armature1 which1 as you will remember1 is the part that turns around4 ,illustration3 ,fig4 #bj ,the cores1 ,f1 ,f1 are first wound with a certain amount of wire1 which depends upon the use the dynamo is to be made for4 ,thus1 you will see1 there will be on each core two loose ends of the wire that is wound around it--namely1 the beginning of the wire and the end where we leave off winding1 which on the two cores together will make four ends of wire4 ,we will tell you presently what is done with them4 ,after the cores are wound1 they are screwed firmly to the yoke and to the pole pieces1 so as to make1 for all practical purposes1 one whole piece pretty nearly the shape of a horseshoe magnet4 ,illustration3 ,fig4 #ba ,now1 to make the dynamo complete1 we must put in the armature between the poles1 which are rounded off1 as you will see1 to accommodate it4 ,the armature is held up by two bearings1 which you will see in the sketch of the complete dynamo above4 7,fig4 #ba47 ,the armature in a practical dynamo-machine consists of a large spool made of thin sheets of iron firmly fastened together and having a steel shaft run through the center1 upon which it revolves4 ,this spool1 or armature1 is wound with a number of strands of copper wire4 ,the commutator1 instead of consisting of two bars1 is made in many dynamos with as many bars as there are strands of wire1 and the ends of these wires are fastened to the bars of the commutator so as to make1 practically1 one long piece of wire1 just as we showed you in explaining how the electricity was produced4 ,the brushes1 resting upon the commutator1 carry away the electricity from it into the wires with which they are connected4 ,now we have our dynamo all put together and ready to start as soon as we properly connect these four loose ends of wire on the cores4 ,if you will turn back to ,fig4 #bj you will see that two of the wires are marked ,i1 and the other two ,o4 ,the letter ,i means the inside wire1 or where the winding began1 and the letter ,o means the outside wire1 or where we left off winding4 ,now1 if we fasten together 7or connect7 the two ends of wires1 ,i and ,o1 near the top of the magnet1 we make the two wires round the cores into one wire1 which starts1 say1 at ,i near the poles1 goes all around one core1 crosses over and around the other core down to the other end of the wire to ,o1 near the poles4 ,so far we have called the iron a magnet1 although it is not a magnet until electricity is put into it2 so1 when the dynamo is started for the first time1 these two ends of wire1 ,i and ,o1 are connected to a battery or other source of current for the purpose of sending electricity through the wire on the cores4 ,when the electricity goes into this wire the iron immediately becomes a magnet1 and the lines of force are present at the poles4 ,now1 the armature is turned around rapidly by a steam-engine1 and1 as the wire on the armature cuts the lines of force with great rapidity and so frequently1 there is quickly generated a large quantity of electricity1 which passes out as fast as it is made through the commutator and the brushes to the lamp4 ,and so long as the armature is revolved and the battery attached1 the electricity will be made1 or1 as it is usually termed1 generated4 ,as we stated above1 a battery is used the first time the dynamo is run1 and now we will explain why it is not needed afterward4 ,although iron will not become a permanent magnet1 like steel1 it does not lose all its magnetism after it has been once thoroughly charged4 ,when the dynamo is stopped1 after the first trial1 and the battery is taken away1 you will discover only traces of magnetism about the poles4 ,they will not readily attract even a needle or iron filings2 but there is1 nevertheless1 a very small amount of magnetism left in the iron4 ,small as this magnetism is1 however1 it is enough to make very faint and weak lines of force at the poles of the magnet4 ,after the battery is taken away1 the ends of the wire on the cores1 which were connected to the battery1 are connected1 instead1 to the wires which carry away the electricity from the brushes to the lamps4 ,thus1 you will see1 if any electricity goes from the dynamo to the lamps1 part of it must also find its way through the wires which are around the cores4 ,we will now start up the dynamo without having any battery attached and see what happens4 ,the armature turns around and the wires upon it cut through those very faint lines of force which are always at the poles4 ,this1 as you know1 makes some electricity2 very little1 to be sure1 but it comes out through the brushes to the wires leading to the lamps1 and there it finds the wires leading back to the cores4 ,well1 part of this weak current of electricity goes into these wires and travels back round the cores and so makes the magnetism stronger4 ,the consequence of this is that the lines of force become stronger and1 as the armature keeps turning around1 the electricity naturally becomes stronger1 and so there is more of it going through the wires back to the cores and increasing the strength of the magnet all the time1 until the dynamo becomes strong enough to generate all the current it was intended to give for the lamps4 ,of course1 you understand that the stronger the magnet becomes1 the greater will be the lines of force and the greater the amount of electricity made by the turning of the armature4 ,now1 there is naturally a limit to what can be done with any particular dynamo2 so1 while the electricity continues to strengthen the magnetism and the magnetism increases the electricity1 this cannot go beyond what is called the saturation point of the magnet4 ,saturation means that the iron is full of magnetism1 and will hold that much but no more4 ,you will learn more as to the saturation of magnets when you study electricity more deeply1 and we therefore do not intend to enter into that subject in this book4 ,we will only state1 however1 that the magnets of dynamos are not always charged up to their saturation point4 ,,the ,,lamps ,so far you have learned how the current of electricity is produced1 and now we will follow along the wires to find out how it makes the lamps give out both strong lights and the smaller1 pleasant ones4 ,suppose we take first the large1 dazzling lights we see in the streets1 which1 as you know1 are called ,,arc-,,lights ,those who have seen the arc-lamps will readily recognize them from the picture in ,fig4 #bb4 ,you will see that there are two sticks1 or pencils1 of carbon4 ,now you will remember that in the chapter on ,magnetism we told you that in order to have electricity do work for us we must put some resistance or opposition in its way4 ,when we get light from an electric lamp it is because we make the electricity do some work in the lamp1 and this work is in pushing its way through a resistance or opposition which is in the lamp4 ,illustration3 ,fig4 #bb ,when we generate electricity in the dynamo and put two wires for it to travel in1 the current goes away from the dynamo through one of the wires and will go back to the dynamo through the other one if it can possibly get a chance to get to this other one4 ,now1 the electricity which is constantly being made fills the wires and acts as a pressure to force the current through the wires back to the dynamo1 and1 if we put no resistance or opposition in the way1 it would have a very easy path to travel in and would do no work at all4 ,the wires leading to an electric lamp should have very little resistance1 not sufficient to require any work from the current in passing through4 ,so1 if we bring the two carbons in an arc-lamp together they really form part of the wire1 and do not interrupt the current in its travels1 but1 if we separate the carbons1 we make a gap which the current must jump across if it wants to go on4 ,as the volts1 or pressure1 is so great1 the current must jump1 and this against the resistance or opposition in an arc-lamp is that which gives the current so much work to do4 ,indeed1 so hard is it for the current to jump across this gap that it breaks off from one carbon a shower of tiny particles as fine as the finest dust1 and makes them white hot in passing to the other4 ,this shower of fine carbon dust1 together with the ends of the carbons1 being white hot1 of course makes a light1 and this is the dazzling light which you see in the arc-lamp4 ,of course1 when the electricity has jumped over from one carbon to the other1 it goes through it to the wire1 and so passes on to the next lamp1 where it has to jump again1 and so on until it has gone through the last lamp1 then it has an easy path to get back to the dynamo4 ,now1 we want you to understand more thoroughly how that much resistance or opposition will cause heat1 so we will try to give you a simple example4 ,most of you know that if you were holding a rope tightly in your hands and some one pulled it through them quickly and suddenly1 it would get very hot and your hands would feel as though they were being burned4 ,this is heat caused by your hands resisting or opposing the passage of the rope through them1 and if you could hold on tightly enough and the rope was drawn through quickly enough1 it would take fire4 ,this fire would1 therefore1 cause heat and light4 ,it is just this principle of resistance to the passage of the current which causes the light in an arc-lamp1 as we have shown you4 ,,incandescent ,,lamps ,you have just learned that the light in an arc-lamp is caused by the current forcing off from the carbon sticks tiny particles and heating them up until they give a brilliant light4 ,so1 you see1 in an arc-light there is a wearing away of carbon by electricity1 and therefore these sticks1 or pencils1 of carbon in time are all burned away4 ,in practice the carbon pencils last about eight or ten hours1 and then new ones must be put in4 ,now1 in the incandescent lamp there is also carbon used1 but the light is not produced by the combustion or wasting away of the carbon1 as we will show you4 ,the picture below will show you the appearance of an incandescent lamp4 7,fig4 #bc47 ,illustration3 ,fig4 #bc ,you will see that this lamp consists of a pear-shaped globe1 and inside is a long ,u-shaped strip of carbon no thicker than an ordinary thread4 ,this is a strip of bamboo cane#a which has been carbonized to a thread of charcoal4 ,it is joined to two wires which come through the glass4 ,these two wires come down through the bottom of the globe1 and one is fastened to a brass screw-ring1 while the other wire is fastened to a brass button at the bottom of the lamp4 ,these two 7the ring and button7 must1 as you know1 be separated from each other by something which will not carry electricity1 or they would make a short circuit when the electricity was applied4 ,we separate the ring and the button in various ways4 ,now1 if we took the ends of two wires which were charged with the proper amount of electricity and put one wire on the screw-ring and the other on the button1 the lamp would light up1 because there would be a complete path for the current to travel in4 ,illustration3 ,fig4 #bd ,it will1 however1 be plain to you that it would be awkward to light the lamps in this way1 so we use a socket into which the lamp is screwed4 7,fig4 #bd47 ,the wires from the dynamo carrying the electricity are connected in the socket1 one wire with the screw thread into which the screw-ring fits1 and the other with a button which the button on the lamp touches when the lamp is screwed into the socket4 ,thus we have a connected path for the current to travel in1 or1 as it is termed1 a complete circuit4 ,you will notice that in the incandescent lamp the electricity does not need to jump1 as it does in the arc-light1 because we give it one continuous line to travel in4 ,in order1 however1 to get the current to do work for us1 we put some resistance in its path1 which it must overcome in order to travel back to the dynamo4 ,the resistance in an incandescent lamp is the ,u-shaped carbon strip 7or1 as it is called1 filament74 ,this charcoal filament has so much greater resistance than the wires that it opposes1 or resists1 the passage of the electricity through it2 but the electricity must go through1 and1 as it is strong enough to force its way1 it overcomes this resistance and passes on through the carbon to the wire at the other end4 ,you see it is a struggle between the carbon and the electricity1 the current being determined to go on and the carbon trying to keep it back2 and1 in the end1 the electricity1 being the stronger1 gets the best of it2 but the struggle has been so hard that the carbon has been raised to a white heat1 or incandescence1 and so gives out a beautiful light1 which continues as long as the current of electricity flows4 ,you will remember that in the arc-light the carbons are slowly consumed and new ones must be put in4 ,if the carbon in the incandescent light were consumed1 it would not last many minutes1 because it is only about the size of a horsehair4 ,now1 you will naturally inquire why this fine strip is not burned up when it is raised to so high a heat4 ,well1 we will tell you4 ,you know that if you light a match and let it burn the wood will all be consumed4 ,but did you ever light a match1 put it into a small bottle1 and put the cork in8 ,if you never did1 do so now as an experiment1 and you will see that the match will keep lighted for an instant and then go out without consuming the wood4 ,the reasons for this are very simple4 ,in order to burn anything up entirely it is absolutely necessary to have the gas called oxygen present1 and1 as the air you live in contains a very large amount of oxygen1 there is more than sufficient in your room to cause the wood of the match to be entirely consumed after it is lighted4 ,but there is such a small quantity of oxygen in the bottle that it is not enough to keep the fire going in the match1 and1 consequently1 it will not burn up the wood4 ,the reason the filament in an incandescent lamp is not burned up is because there is no oxygen inside the globe4 ,after the carbon is put in its place all the oxygen is drawn out through a tube1 and the glass is sealed up so that no more oxygen can get in4 ,this is called obtaining a vacuum1 and vacuum means a space without air4 ,there being no oxygen in the globe1 it is impossible for the carbon to burn up2 so the incandescent lamp will continue to give its light for a very long time1 some of them lasting for thousands of hours4 ,some day1 however1 from a great variety of obscure causes1 the filament becomes weak in some particular spot and breaks1 and the light ceases4 ,when this happens1 we unscrew the lamp and put another one in1 and the light goes on as usual4 ,now you have learned how the incandescent lamp is made to give light4 ,we will add that it is a beautiful1 soft1 white light1 almost without heat1 it will not explode1 throws off no poisonous fumes like gas or oil lamps1 and has many other points of comfort and convenience which make it very desirable4 ,,electric-,,light ,,wires ,before closing the subject of electric light you would perhaps like to know something about the way in which we place the wires leading to the lamps4 ,illustration3 ,fig4 #be ,if you remember what we told you about measurements in the beginning of this book1 it will be easy to understand what follows3 ,you know that if you have a very great pressure you can force a quantity through a small conductor4 ,this is the principle upon which the arc-lamps are run4 ,every arc-lamp takes about #dj to #ej volts and from #e to #aj ampres to produce the light1 and they are connected with the wires as shown in ,fig4 #be4 ,this is called running lamps in series1 and1 as you will see from the sketch1 the wire starts out from the dynamo and connects with one carbon of the first arc-lamp1 and to the other carbon is connected another wire which goes on to the next lamp1 and so on until the last lamp is reached1 and then the wire goes back to the dynamo4 ,this forms1 practically1 one continuous loop from one brush to the other of the dynamo4 ,the current starts out1 makes its way through the first lamp1 goes on to the next1 makes its way through that1 and so on till it has jumped the last one2 then it goes back to the dynamo4 ,now1 as each of these jumps requires a pressure of #dj or #ej volts1 you will easily see that the total pressure1 in volts1 of the electricity must be as many times #dj or #ej volts as there are lamps to be lighted2 so1 if there were #fj lamps in circuit1 there would be #b1djj to #c1jjj volts pressure1 which1 while it gives very fine lights1 might cause instant death to any one touching the wires4 ,suppose anything happened to the first lamp1 which stopped the current from jumping through it4 ,there would be no path for the current to travel farther1 and1 consequently1 all the lights would go out4 ,to get over this difficulty there is sometimes used what is called a shunt1 which only acts when the lamp will not light4 ,this shunt carries the current round the lamp to the other wire1 so that it may travel on and light up the other lamps4 ,,wires ,,for ,,incandescent ,,lamps ,the wiring for incandescent lamps is carried out in an entirely different way1 which you can see by comparing ,fig4 #be ,a with ,fig4 #be which shows the wiring for arc-lamps4 ,illustration3 ,fig4 #be ,a ,this is called connecting in multiple arc4 ,you will notice that the two wires running out from the dynamo 7which are called the main wires7 do not form one continuous loop as in the arc-light system1 but that a smaller wire is attached to one of the main wires and then connected with the screw-ring in the lamp-socket2 then another wire is connected with the button in the socket and afterward to the other main wire4 ,every lamp forms an independent path through which the current can travel back to the dynamo4 ,now1 if we turn one of these incandescent lamps out1 we simply shut off one of these paths and the electricity travels through the other lamps1 and1 if we wish1 we can turn out all the lamps but one and there will still be a way for the electricity to go back to the dynamo4 ,in the arc-lamps we must have a very high number of volts pressure1 because the electricity has only one path1 and it all has to pass through the first and other lamps till it comes to the last one4 ,in the incandescent light the electricity has as many paths as there are lamps1 so we only need to keep one certain pressure in volts in the main wires all the time4 ,this pressure is even all the way through the main wires1 and1 therefore1 it is ready to light a lamp the instant it is turned on1 because1 as you have seen1 electricity will always get back to the dynamo if there is a possible chance1 and the lamp opens a path4 ,the volts pressure used to operate any number of incandescent lamps is altogether very much less than for a number of arc-lights4 ,for example1 in the ,edison system the pressure 7sometimes called electromotive force7 is only about #aaj volts1 which is very mild and not at all dangerous4 ,this electromotive force would be the same if there were one lamp or ten thousand lighted4 ,while this ,edison current would not hurt any one1 you should remember that it is much the better plan not to touch any electric-light wires until you have learned a great deal more on this subject4 ,we may add that each of the standard incandescent lamps requires only about one-quarter of an ampre of current to make them give a light of #af candle-power1 which is about the light given by a very good gas-jet1 and while the electromotive force1 or pressure1 would only be about #aaj volts1 whether there were one lamp or ten thousand lighted1 there must be sufficient ampres in the wires to give each lamp its proper quantity4 ,,switches ,we have made mention several times of turning on or off one or more lights1 and now1 perhaps1 you would like to know how this is done4 ,suppose the electricity was traveling through wires to one or several lamps1 it would light up those lamps as long as the wires provided a path to travel in1 but if you were to cut out one of them1 which is called breaking the circuit1 there would be no road for the electricity to follow1 and1 consequently1 its course would be stopped short and the lamps would go out4 ,you will remember that electricity must have a complete circuit or it can do no work1 and in electric lighting it is always a metallic circuit that is used4 ,now1 the switch is simply a device which is used to break the circuit so that the current cannot pass on4 ,the simplest form of switch is seen in the sketch4 7,fig4 #bf47 ,illustration3 ,fig4 #bf ,you will see that there is a wire cut in two1 and to one piece is attached a metallic piece1 ,a1 which turns one way or the other1 and when it is turned so as to touch the other part of the wire the circuit is closed and the electricity goes from the lower part of the wire through the metallic piece ,a to the other part of the wire1 thus making a complete circuit or path for the electricity to travel in4 ,if we turn the piece ,a away from the upper wire this breaks the circuit and cuts off the path1 and1 of course1 the lamps would go out4 ,this is the principle of the switch1 and1 although they are made in thousands of ways1 switches all have the same object--namely1 the closing and breaking of the circuit1 whether it is for one or a hundred lamps4 ,,wire ,,on ,,dynamos ,in explaining to you the construction and working of dynamo-machines1 we did not state anything about the amounts of wire used in winding the machine4 ,it is not our intention to say exactly how much is used on any one dynamo1 because that is among the things you will have to learn when you come to study the subject of electricity more deeply4 ,we simply want to have you understand that upon the number of turns of wire on any one machine depends the effect that that amount of wire1 carrying electricity1 will have upon a certain weight of iron when the armature is revolved a certain number of turns per minute4 ,a certain number of strands of wire on an armature will only do a certain amount of work at the most1 so you will see that a small dynamo will not produce as much electricity as a larger one containing more iron and wire4 ,for high pressure there must be more strands of wire cutting the lines of force more frequently than would be required for low pressure2 and1 to produce a great many ampres1 the armature must be larger and the wire upon it thicker than it would need to be if only a small number of ampres were wanted4 ,this of itself is a very deep and complicated subject1 and many books have been written upon it alone4 ,we shall1 therefore1 not attempt to go more deeply into it in this little book1 but simply content ourselves with giving you the general idea1 which will be sufficient until you make a thorough study of the subject4 ,,viii ,,electric ,,power ,one of the most convenient uses to which electricity is put is in producing motive power for driving all kinds of machines1 from a sewing-machine to a railway train1 and we will now try to explain how we can get this kind of work from electricity4 ,to begin with1 you all know that a piece of machinery is usually made to work by revolving a wheel which is part of the machine1 either by means of a steam-engine or by water-power1 or1 as a sewing-machine1 by foot-power4 ,now1 when we work a piece of machinery by electricity we do just the same thing by using1 instead of the steam-engine or water or foot power1 an electric-engine called an electromotor1 which operates in the same way--namely1 by turning the wheel of the machine it is applied to4 ,foot-power is hard work for the person who is applying the power1 and1 as you can easily see1 one person can make only a very little power by use of the feet4 ,steam and water power can be used for any large amount of work1 but the work must be within a few hundred feet of the engine or the power cannot be used4 ,if there were a factory using steam-power a block or two away from where you lived1 and you had a lathe in your house which you would like to have run by the steam-power in the factory1 it would be practically impossible to do this4 ,now1 if the factory were still farther away from your house1 it would be still more impossible1 and if it were a mile away it would be foolish to dream of taking steam-power from a place so far away4 ,suppose1 however1 that this factory was lighted by electric lights1 it would be a very easy matter to take some of the power over to your house4 ,this could be done1 even if the factory were miles away1 by taking two wires from their electric-light wires and running them into your house to an electromotor connected with your lathe4 ,this electromotor would then run your lathe just as well as if it were belted to a steam-engine4 ,so1 you see1 power can be carried in the form of electricity through two wires over very great distances and made to do work at a long way from the engine which is turning the dynamo to make the electricity4 ,thus1 you may have brought into your house wires which will give lights and1 at the same time1 power to run a sewing-machine1 a lathe1 or any other piece of machinery4 ,having learned so far that a dynamo will make a continuous current of electricity1 and that two wires will carry this current to any place where it is wanted1 let us now see what takes place in the electromotor to transform the electricity into power4 ,an electromotor 7which we will now call by its short name1 motor7 is simply a machine made like a dynamo4 ,curious as it may seem to you1 it is a fact that if you take two dynamo-machines exactly alike1 and run one with the steam-engine so as to produce electricity1 and then take the two main wires and attach them to the brushes of the other dynamo1 the electricity will drive this other dynamo so as to produce a great deal of power which could be used for driving other machines4 ,thus1 the second dynamo would become a motor4 ,in the chapter on dynamos we explained something about the way they were made and how the electricity was produced4 ,,the ,,motor ,you will remember that the armature consists of a spool wound with wire4 ,this spool is made of iron plates fastened together so as to form one solid piece4 ,the armature of a motor may be made in the same way2 in fact1 the whole motor is practically a dynamo-machine4 ,there is something more about magnetism which we will tell you of here1 because you will more easily understand it in its relation to an electromotor4 ,if we take an ordinary piece of iron and bring one end of it near to 7but not touching7 one pole of a magnet1 this piece of iron will itself become a weaker magnet as long as it remains in this position4 ,this is said to be magnetism by induction4 ,the end of the piece of iron nearest to the magnet will be of the opposite polarity4 ,for instance1 if the pole of the magnet were north1 the end of the iron which was nearest to this north pole would be south1 and1 of course1 the other end would be north4 ,to make this more plain we show it in the following sketch4 7,fig4 #bg47 ,this would be the same whether the magnet were a permanent or an electromagnet4 ,you will remember also that the north pole of one magnet will attract the south pole of another magnet1 but will repel a north pole4 ,these are the principles made use of in an electromotor1 and we will now try to show you how this is carried into practice4 ,illustration3 ,,steel ,,permanent ,,magnet ,,iron ,fig4 #bg ,although a motor is made like a dynamo1 we will show a different form of machine from the dynamo already illustrated1 because it will help you to understand more easily4 7,fig4 #bh47 ,here we have an electromagnet with its poles1 and an iron armature wound with wire1 just as in the dynamo we have described1 except that its form is different4 ,illustration3 ,fig4 #bh ,a commutator and brushes are also used1 but the electricity1 instead of being taken away from the brushes1 is taken to them by the wires connected with them4 ,two wires are also connected which take part of the electricity around the magnet1 just as in the dynamo4 ,now1 when the volts pressure and ampres of electricity coming from a dynamo or battery are turned into the wires leading to the brushes of the motor1 they go through the commutator into the armature and round the magnet1 and so create the lines of force at the poles and magnetize the iron of the armature4 ,let us see what the effect of this is4 ,the poles of the magnet become north and south1 and the four ends on the armature also become north and south1 two of each4 ,by referring to ,fig4 #bh again we shall see what takes place4 ,the north pole of the magnet is doing two things3 it is repelling1 or forcing away1 the upper north pole of the armature and at the same time drawing toward itself the lower south pole of the armature4 ,in the mean time the south pole of the magnet is repelling the south pole of the armature and at the same time drawing toward itself the north pole of the armature4 ,this1 of course1 makes the armature turn around1 and the same poles are again presented to the magnet1 when they are acted upon in the same manner1 which makes the armature revolve again1 and this action continues as long as electricity is brought through the wires to the brushes4 ,thus1 the armature turns around with great speed and strength1 and will then drive a machine to which it is attached4 ,the speed and strength of the motor are regulated by the amount of iron and wire upon it1 and by the volts pressure and ampres of electricity supplied to the brushes4 ,motors are made from a small size that will run a sewing-machine up to a size large enough to run a railway train1 and are often operated through wires at a great distance from the place where the electricity is being made1 sometimes miles away4 ,they are also made in a great many different forms1 but the principle is practically the same as we have just described to you4 ,,ix ,,batteries ,so far we have only described one way of producing electricity--namely1 by means of a dynamo-machine driven by steam or water power4 ,the supply of electricity so obtained is regular and constant as long as the steam or water power is applied to the dynamo4 ,there is another and very different way of producing electricity1 and this is by means of a chemical process in what is called a battery4 ,to obtain electricity from the dynamo we must spend money for the coal to make the steam which operates the steam-engine1 or for the water which turns the water-wheel1 as well as for an engineer in both cases4 ,when we obtain electricity from a battery we must spend money for the chemicals and metals which are constantly consumed in the battery4 ,,primary ,,batteries ,an electrical battery is a device in which one or more chemical substances act upon a metal and a carbon1 or upon two different metals1 producing thereby a current of electricity1 which will continue as long as there is any action of the chemicals upon the metal and carbon1 or upon the two metals4 ,batteries for producing electricity may be divided into two classes1 called open circuit batteries and closed circuit batteries4 ,open-circuit batteries are those which are used where the electricity is not required constantly without intermission--for instance1 in telephones1 electric bells1 burglar alarms1 gas-lighting1 annunciators1 etc4 ,closed-circuit batteries are those which are used where the effect produced must be continuous every moment1 as1 for instance1 in electric lights and motors4 ,the open-circuit battery is made in many different ways1 so we only describe two of the principal ones4 ,as we told you in an early part of this book1 we do not know just what electricity is1 nor why it is produced under the conditions existing in a battery4 ,but we do know that by following certain processes and making certain chemical combinations we can make as much electricity and in such proportions as we want4 ,the two metals1 or the metal and carbon1 in a battery are called the elements1 and to these are connected the wires which lead from the battery to the instruments to be worked by it4 ,the ,leclanch ,battery4--,this form of open-circuit battery consists of a glass jar in which is placed the elements4 ,one element consists of a rod of zinc1 and the other element is carbon and powdered black oxide of manganese4 ,these two 7the carbon and black oxide of manganese7 are placed in an earthenware vessel called a porous cup4 ,this is simply a small jar made of clay which is not glazed4 ,thus1 the liquid which is in the glass jar penetrates through the porous cup to the carbon and manganese which it contains1 and so the chemicals affect both these and the zinc at once1 for1 in order to obtain electricity1 you will remember that the chemical action must take place at the same time upon both the elements in the same vessel4 7,fig4 #bi47 ,the chemical substance used in this battery is sal-ammoniac1 or salts of ammonia4 ,a certain quantity of this salt is dissolved in water1 and this solution is poured into the glass jar4 ,when this is done the battery will generate electricity at once4 ,illustration3 ,fig4 #bi ,it should be remembered that the proper term for the chemical mixture which acts upon the elements in any battery is electrolyte4 ,the ,dry ,battery4--,the cleanliness1 convenience1 high efficiency1 and comparatively low internal resistance of the dry cell has brought it into great favor in the last few years4 ,it is now extensively used in preference to the ,leclanch and other open-circuit batteries having liquid electrolyte for light work1 such as bells1 gas-lighting1 burglar alarms1 ignition on motor-boats1 automobiles1 etc4 ,the dry cell is also used in great numbers for pocket flash-lamps1 and in other ways where it would be impossible to employ batteries containing liquids4 ,a dry cell consists of zinc1 carbon1 and the electrolyte1 which is a mixture so made that it is in the form of a gelatinous or semi-solid mass1 so that it will not run or slop over4 ,a piece of sheet zinc is formed into a long tube1 and a round1 flat piece of zinc is soldered at one end1 thus making a cup open at one end4 ,this forms the cell itself1 and at the same time becomes one of the elements4 ,the other element is a piece of battery carbon which is long enough to project out of the top of the cell about half an inch or more4 ,while the cell is being filled with the electrolyte the carbon is held up by a support so that it does not touch the zinc at the bottom of the cup4 ,of course1 the zinc cup and the carbon are provided with proper binding-posts or other attachments1 so that conducting wires can be connected4 ,the electrolyte is packed into the cup and around the carbon in such a way that the cup is entirely filled within about half an inch from the top1 and then some melted tar or pitch is poured over the top of the electrolyte4 ,this seals the cell and binds the contents solidly together4 ,just before the sealing compound hardens1 one or two holes are made in it so that the gases may escape4 ,the composition of the electrolyte itself is not exactly alike in all dry cells1 as the various manufacturers follow their own particular formulas4 ,however1 as you may be curious to know something about it1 we would state that one formula embraces flour1 water1 plaster of ,paris1 granulated carbon1 zinc chloride1 ammonium chloride1 and manganese binoxide4 ,you will remember that the ,leclanch and the dry batteries are purely open-circuit cells1 and that they can be used to advantage for electric bells1 annunciators1 burglar alarms1 gas ignition1 etc41 where the current of electricity is not doing continuous work1 but only for a few seconds at a time4 ,consequently1 the batteries have a little rest in between1 if only for a few seconds4 ,now1 if we were to attempt to use open-circuit batteries for electric lights or motors1 where the electricity must work constantly every second1 the batteries would polarize--that is to say1 they would only work a few minutes and then stop1 because the chemicals used in them are of that kind that they will only allow the battery to do a little work at a time4 ,the batteries we have been describing will do the ordinary work for which they are intended for sometimes a year without requiring any attention1 but if we try to make them do work for which they were not intended1 they would only last a few days4 ,if we should want to operate electric lights or motors continuously from a battery we must1 therefore1 use ,,closed-,,circuit ,,batteries ,there is a great variety of ways in which closed-circuit batteries are made1 but1 as the main principles are very much alike1 we will only describe two general kinds1 those with and those without a porous cup4#b ,in the first place1 we must state that closed-circuit batteries proper usually consist of a glass jar and two elements--carbon and zinc4 ,sometimes a porous cup is used2 for what reason you will soon learn4 ,the chemicals that are used are usually different from those used in the open-circuit batteries and are much stronger4 ,these chemicals are usually sulphuric acid and bichromate of potash 7or chromic acid71 which are mixed with water4 ,we will now examine two of the types of closed-circuit batteries1 taking first the one without the porous cup1 of which the ,grenet is a good example4 ,illustration3 ,fig4 #cj ,this battery1 as you see1 consists of a glass jar1 in which are placed two plates of carbon and one of zinc4 7,fig4 #cj47 ,the latter is between the two carbon plates and is movable up and down1 so that it may be drawn up out of the solution when it is not desired to use the battery4 ,when the zinc is in the solution there is a steady and continuous current of electricity developed1 which can be taken away by wires from the connections on top of the battery4 ,if the zinc were left in the solution when the battery was not in use1 the acid would act upon it almost as much as though the electricity were not being used1 and thus the zinc would be eaten away and the acid would be neutralized1 so that no more action could be had when we wanted more electricity4 ,now1 in the ,grenet battery we can light a lamp or run a motor for several hours continuously1 but at the end of that time the solution would become black and it would do no more work4 ,then we must throw out that solution and put in fresh1 and the battery will do the same work again1 and so on4 ,if you should only want to light your lamp or run your motor for a few minutes1 you could pull the zinc up from the solution and put it down again when you wanted the electricity once more4 ,the carbon element in the battery is not consumed by the acid1 although the zinc is4 ,illustration3 ,fig4 #ca ,now you will see the use of the porous cup4 ,we will take as an illustration of this type an ordinary battery in which a porous cup is used4 7,fig4 #ca47 ,here1 you will see1 the carbon is placed in the porous cup1 while the zinc is outside in the glass jar4 ,in the glass cell with the zinc is usually used water made slightly acid1 and the strong solution of sulphuric acid and bichromate of potash 7or chromic acid7 is poured in the porous cup1 where the carbon is placed4 ,the strong solution penetrates the porous cup very slowly and gets to the zinc1 when it immediately produces a current of electricity4 ,but the acid does not get at the zinc so freely as it does in the battery without a porous cup1 and1 consequently1 neither the acid nor the zinc is so rapidly used up4 ,where porous cups are used1 the batteries will give a continuous current for a very much longer time than without them1 and will1 sometimes1 give many hours' work every day for several months without requiring any change of solution4 ,polarization4--,there is one other reason why a longer working time can be had from a battery with a porous cup1 and that is1 in a battery without a porous cup the action of the acid upon the zinc is so rapid that the carbon plates become covered with gas1 and1 therefore1 the proper action by the acid cannot take place upon them4 ,thus1 the battery ceases to work1 and is said to be polarized4 ,when a porous cup is used1 the action of the acid upon the zinc is slow enough to give off only a small amount of gas1 and thus the acid has a chance to act upon the carbon plates and develop a steady current of electricity4 ,,the ,,work ,,done ,,by ,,batteries ,the pressure and quantity of electricity given off continuously by open and closed circuit batteries is very different4 ,the pressure 7or electromotive force7 of one cell of an ordinary open-circuit battery is only about one volt1 and the current is usually very much less than one ampre1 except in a dry cell1 which may give more4 ,in the closed-circuit batteries described1 the electromotive force of each cell is about two volts1 while the current varies from #a to perhaps #ej ampres1 according to the size of the zinc and carbon plates4 ,it would not matter if you made one cell as big as a barrel1 nor if you put in a dozen carbons and zincs1 the electromotive force would not exceed the volts mentioned for each type of battery1 but the ampre capacity would be greater than in a smaller cell on account of the larger size of the carbon and zinc plates4 ,internal ,resistance4--,there is one other point which affects the number of ampres which can be obtained from a closed-circuit battery1 and that is whether there is a large or small internal resistance in the battery itself4 ,this depends upon the solution which is used and the arrangement of the plates4 ,if there is a high resistance in the battery itself 7called internal resistance71 the electricity must do work to overcome this resistance before it can get out of the battery to do useful work through the wires1 and1 consequently1 the capacity in ampres is limited4 ,if1 on the other hand1 there is very little resistance in the battery1 the current has very little work to flow to the wires leading from the battery1 and we can get a larger quantity1 or greater number of ampres4 ,thus1 you will see that while the closed-circuit battery is the stronger1 and will do all that the open-circuit battery will do1 and even more1 in a short time the latter1 though weaker1 will do about as much work for the same amount of zinc and carbon as the former1 but takes a much longer time4 ,,batteries ,,for ,,electric ,,light ,as we have explained to you1 closed-circuit batteries are used for producing incandescent electric lights in small numbers1 as well as for running motors4 ,to operate incandescent lights1 a number of batteries connected together are used4 ,the number used depends upon the pressure which the lamps require to make them give the required light4 ,we will now explain how the batteries are connected together for this purpose4 ,illustration3 ,fig4 #cb ,suppose you wished to light an incandescent lamp of1 say1 three candle-power1 which required six volts4 ,we would take three closed-circuit batteries which would each give two volts1 and connect by a piece of wire the zinc of the first to the carbon of the second1 and the zinc of the second to the carbon of the third1 as shown in the sketch4 7,fig4 #cb47 ,we would then attach a wire to the carbon of the first and one to the zinc of the third1 and there would be six volts in these two wires1 which would light up one six-volt lamp nicely4 ,this is called connecting in series1 or for intensity4 ,now if each of these cells gave ten ampres alone1 the three will only give ten ampres together when they are connected in series4 ,if our lamp only required one ampre1 you would naturally think that ten similar lamps put on the wires would give as good light as the one1 but that is not so4 ,although you might light up two lamps1 the pressure would drop and the lights would become less brilliant if you put on the whole number4 ,so1 if we wished to put on the whole ten lights we would connect another battery and thus increase the pressure1 which would probably make these ten lamps burn brightly4 ,these rules hold good for connecting any number of batteries for lamps of any number of volts--that is to say1 there should be calculated about two volts for each cell and an allowance made for drop in pressure4 ,,connecting ,,in ,,multiple ,there is another way of connecting batteries1 and that is to obtain a larger number of ampres4 ,this is called connecting in multiple arc1 or for quantity4 ,illustration3 ,fig4 #cc ,let us take again for an illustration the three cells giving each #b volts and #aj ampres4 ,this time we connect the carbon of the first to the carbon of the second1 and the carbon of the second to that of the third2 then we connect the zinc of the first to that of the second1 and the zinc of the second to that of the third1 as shown in the sketch4 7,fig4 #cc47 ,we then attach a wire to the zinc and one to the carbon in the third cell1 and we then can obtain from these two wires only #b volts1 but #cj ampres4 ,there are1 again1 many ways of connecting several of these sets together1 but it is not intended in this book to go into these at length1 for the reason that we only set out to give a simple explanation of the first principles of this subject4 ,we shall therefore only give an illustration of one more method of connecting batteries which will be easy to understand4 ,this is called ,,multiple ,,series ,the sketch we have last given shows three batteries connected in multiple4 ,these we will call set ,no4 #a4 ,now1 suppose we take three more batteries exactly similar and connect them together just in the same manner4 ,let us call this set ,no4 #b4 ,now take the wire leading from the carbon of set ,no4 #b and connect it with the wire leading from the zinc of set ,no4 #a4 ,then take a wire leading from the zinc of set ,no4 #b1 and a wire leading from the carbon of set ,no4 #a1 and connect them with the lamps or motors4 ,these two sets being connected in multiple series1 we shall get #d volts and #cj ampres4 ,this is called connecting in multiple series1 and may be extended indefinitely with any number of batteries4 ,we should add that one of the elements in a battery is called positive1 and the other negative4 ,,the ,,edison ,,primary ,,battery ,as this type of battery will work efficiently on either open or closed circuit1 we have thought best to describe it separately at this place1 in order not to confuse your ideas while reading about batteries generally4 ,the type of cell we will now describe was originated by an inventor named ,lalande1 and was known by that name2 but it has been greatly improved and rendered more efficient by ,edison1 and is now manufactured and sold by him under the name of the ,edison ,primary ,battery4 ,before describing the cell itself1 let us consider the action that takes place in a battery of this kind4 ,if certain metals are placed in a suitable solution1 and are connected together1 outside of the solution1 by wires1 vigorous chemical action will take place at the surfaces of the metals1 and electrical energy will be produced4 ,the plates must be of different metals1 and the solution should be one that will dissolve neither of them except when an electric current is allowed to flow4 ,one of the metals is usually zinc1 which is gradually eaten away or dissolved by the solution while the battery is delivering electrical energy4 ,it is the chemical combination of the zinc and the solution that produces this energy1 which leaves the zinc in the form of an electric current1 and passes through the solution to the other metal1 out of the cell to the wire1 and thence back by another wire to the zinc1 where it is once more started on its circuit4 ,at the surface of the other metal1 which may be1 and frequently is1 copper1 small bubbles of the gas called hydrogen are produced4 ,this gas rises to the surface of the liquid and gradually passes off into the air4 ,but its presence offers resistance to the passage of the current2 so that generally there is associated with the copper a supply of the gas oxygen4 ,oxygen and hydrogen are always very eager to mix with each other1 and1 therefore1 when the hydrogen bubbles appear they are quickly taken up by the oxygen near by4 ,the mixture of these two gases forms water1 which becomes part of the solution4 ,all of this happens so quickly that the hydrogen cannot be perceived so long as there is any oxygen left in the copper-oxide plate4 ,illustration3 ,fig4 #cd ,in the ,edison ,primary ,battery 7,fig4 #cd7 the plates are zinc1 known as the negative1 and copper oxide 7copper and oxygen71 or the positive4 ,these are suspended in a solution of caustic soda and water1 the plates and solution being contained in jars of glass or porcelain4 ,the plates are provided with suitable wires for connecting the cells with one another and with the lamps1 motors1 or other devices which they are to operate4 ,there are usually two zinc plates and one copper-oxide plate1 or multiples thereof4 ,the quantity of current that may be withdrawn depends on the size and number of the plates1 as well as upon their construction and arrangement4 ,the voltage of these cells is low1 being about #j4fe volt each2 but this is more than compensated for by the fact that the internal resistance of the battery is so low that the voltage is not perceptibly affected even at continuous high-discharge rates1 and that the voltage remains practically constant throughout the life of the cell4 ,furthermore1 when the battery is not in use there is practically no local action4 ,consequently1 the cells may remain on open circuit 7that is1 doing no work7 for years and there will be no loss of energy4 ,the cell will then operate with the same practical efficiency as if it were new4 ,in some classes of work this battery remains in service from four to six years without attention4 ,another peculiar advantage of this battery lies in the fact that the plates and the electrolyte are so well proportioned that they are all exhausted at the same time1 and then new plates and solution can be put in the jar1 restoring it to its original condition4 ,these batteries are used in great numbers for railway signal work and for other purposes1 such as fire and burglar alarm systems1 various telephone functions1 operation of electric self-winding and programme clock systems1 small electric-motor work1 for low candle-power electric lamps1 gas-engine ignition1 electro-plating1 telegraph systems1 chemical analysis1 and other experimental work where batteries are required that will remain in use for long periods of time without requiring any attention or renewal4 ,the remarks that have been made on previous pages about connecting up batteries in series1 multiple1 and multiple series apply also to these ,edison ,primary ,cells4 ,fig4 #ce shows a battery of four of these cells connected in series4 ,,secondary1 ,,or ,,storage1 ,,batteries ,the open and closed circuit batteries we have so far described are used to produce electricity by the action of the chemicals upon the elements contained in them4 ,they are called primary batteries4 ,illustration3 ,fig4 #ce ,the batteries which we will now tell you of are called secondary1 or storage1 batteries1 and do not of themselves make any primary current1 but simply act as reservoirs1 so to speak1 to hold the energy of the electric current which is led into them from a dynamo or primary battery4 ,at the proper time and under proper conditions these secondary batteries will give back a large percentage of the energy of the electric current which has been stored in them4 ,this class of battery has been called by these three names3 secondary battery1 accumulator1 and storage battery2 but as the latter name is used almost exclusively in this country1 we shall use it in the following description4 ,,two ,,types ,there are two distinct types of storage battery4 ,one is called the lead or acid storage battery1 and the other the alkaline or nickel-iron storage battery4 ,each of them simply acts as a reservoir to hold the energy of the electric current which is led into it1 and each of them1 under proper conditions1 will give back that energy4 ,as the lead storage battery is the oldest in point of discovery and invention1 we will describe it first4 ,,the ,,lead ,,storage ,,battery ,a lead storage battery usually consists of a glass or hard-rubber jar containing lead plates and a solution consisting of water and sulphuric acid4 ,a single unit is usually called a cell4 7,fig4 #cf47 ,there are always at least two lead plates in a storage-battery cell of this kind1 although there may be any number above that4 ,for the sake of making a clearer explanation to you1 we will take as an illustration a cell containing only two plates4#c ,illustration3 ,fig4 #cf ,we have1 then1 a glass or hard-rubber jar containing two lead plates and a solution consisting of water and sulphuric acid4 ,these plates are called the elements1 and one is called the positive and the other the negative element4 ,the solution is called the electrolyte4 ,the positive element is a sheet of lead upon which is spread a paste made of red-lead4 ,the negative element is a similar sheet of lead upon which is spread a paste made of litharge4 ,now1 when these plates are thus prepared1 they are put into the acid solution in the jar1 and a wire attached to each plate is connected with the two wires from a dynamo or other source of electric current1 just as a lamp would be connected4 ,the electric current then goes into the storage-battery cell1 entering by the positive plate and coming out by the negative4 ,these plates and the paste upon them offer some resistance1 or opposition1 to the passage of the current1 so the electricity must do some work to get from one to the other4 ,the work it does in this case is to so act upon the paste that its chemical nature is changed4 ,so1 after the primary current has been passed from one plate to the other for some time1 and after several discharges1 the storage battery may be disconnected1 being now formed4 ,the paste on the lead plates is now found to have changed its chemical nature1 the paste on the positive plate having been transformed into peroxide of lead1 and that on the negative plate into spongy lead4 ,on arriving at this condition1 the paste on the plates is called active material4 ,this process of formation is absolutely essential before the lead storage battery is ready to be used for actual work4 ,so1 when the plates have been fully formed1 the storage battery may be again connected with a source of electric current which again enters by the positive plate and leaves by the negative4 ,this current so acts on the active material that it combines with the acid solution and1 through the energy of the charging current1 forms other chemical compounds which may for convenience be called sulphates4 ,when the charging current has flowed through the battery long enough to produce these changes in the active material the battery is said to be charged1 and is ready for useful work4 ,if the two wires attached to the plates are now connected with electric lamps1 or a motor1 or other device1 the active material will develop energy in the effort to again change its nature4 ,this energy takes the form of an electric current1 which leaves the battery and passes through the conductors and operates the lamps1 motors1 or other devices in its passage4 ,in this way the battery is said to be discharged1 and at the end of its discharge it can again be charged and discharged in a similar manner for a long time1 until the active material is either used up or drops off the plates4 ,so far as the actual details of construction are concerned1 lead storage batteries are made in a great many different ways1 but the materials are1 in general1 of the same nature as those we have mentioned above4 ,,the ,,alkaline ,,storage ,,battery ,we shall now describe an entirely different type of storage battery1 which contains neither lead nor acid4 ,it is one of the many inventions of ,thomas ,a4 ,edison4 ,in the alkaline storage battery the gas called oxygen plays a very important part1 and we will try to make it clear to you what this part is4 ,you are well aware of the fact that if you leave your pocket-knife out in the air it will get rusty4 ,the reason for this is that iron or steel quickly tends to combine with the oxygen of the air1 and this combination of oxygen and iron is rust1 otherwise called oxide of iron1 or iron oxide4 ,this iron oxide1 or rust1 is therefore the result of a chemical action between the iron and the oxygen4 ,now as all chemical actions require the expenditure of energy1 there has been developed either heat or electricity in the process4 ,the oxygen may be taken away from the iron oxide1 chemically2 but here again would be another chemical action which would require energy to be once more expended4 ,iron oxide may be made chemically in many different ways4 ,it is frequently made in the form of a powder4 ,therefore1 we do not have to depend upon iron rust for a supply of this material4 ,before going further we must consider another oxide--namely1 nickel oxide4 ,it is characteristic of nickel that when it is combined with oxygen to a certain degree so as to form the compound known as nickel oxide1 it will receive still more oxygen4 ,now1 if under proper conditions we compel iron oxide to give up its oxygen to some other kind of chemical compound1 such as nickel oxide1 we must expend energy4 ,but1 on the other hand1 if this nickel oxide gives back the oxygen to the iron--which it will do if opportunity is given--there is energy produced again in receiving the oxygen4 ,in other words1 the energy previously expended1 or part of it1 is now returned4 ,this action and reaction are practically those that take place in the ,edison alkaline storage battery4 ,for simplicity of illustration we will consider a cell containing only two plates1 one positive and one negative4 ,the negative plate is made up of a number of small1 flat1 perforated pockets containing iron oxide in the form of a fine powder4 ,the positive plate is made up of small1 perforated tubes containing nickel oxide mixed with very thin flakes of metallic nickel4 7,fig4 #cg illustrates these plates1 the positive being in front47 ,illustration3 ,fig4 #cg ,these two elements1 positive and negative1 having wires or conductors attached1 are placed in a nickeled-steel can containing the electrolyte1 which consists of a potash solution4 ,you will see that this differs from a lead storage battery1 in which the electrolyte is sulphuric acid and water4 ,if we were to put this acid solution into a metallic can 7except one made of lead7 the can would not last long1 as the acid would quickly eat holes through it4 ,now let us see what takes place in the ,edison alkaline storage battery4 ,if an electric current from a dynamo or other source of electricity is caused to pass through the positive to the negative plate the oxygen present in the iron oxide passes to and remains with the nickel oxide4 ,during all the time this is going on the battery is said to be charging1 and when all the oxygen has been removed from the iron oxide and is taken up by the nickel oxide1 then the battery is said to be charged1 and the flow of current into the battery is stopped4 ,a change has now taken place4 ,the powder in the negative plate is no longer iron oxide1 but has been reduced to metallic iron1 because the oxygen has been removed4 ,the powder in the positive plate is now raised to a higher or super oxide of nickel1 because it has taken the oxygen that was in the iron4 ,but the nickel oxide will readily give up its excess of oxygen1 and the iron will receive it back freely if permitted4 ,if the proper conditions are established1 this transfer of oxygen will take place1 but the iron cannot receive it without delivering energy4 ,illustration3 ,fig4 #ch ,the proper conditions are established by providing a conducting circuit between the two elements1 in which lamps1 motors1 or other electrical devices are placed4 ,as soon as this circuit is provided1 the opportunity is given to the iron to receive the oxygen4 ,this it does1 and in so doing develops electrical energy4 ,this energy is in the form of electric current which is then delivered by the battery on what is called the discharge1 and this current may be used for lighting lamps or for operating motors or other electrical devices4 ,the battery is said to be discharging as long as the iron is receiving oxygen from the nickel oxide4 ,as soon as it becomes iron oxide once more1 the giving out of energy ceases and the battery is said to be discharged1 and must again be charged to obtain further work from it4 ,such a battery can be charged and discharged an indefinite number of times4 ,this type of battery is very rugged1 and its combinations are not self-destructive4 ,it is very simple1 as it provides chiefly for the movement of the oxygen back and forth2 besides1 it gives much more current for its weight than the lead type of storage battery4 7,fig4 #ch shows the plates of a standard ,edison cell removed from container47 ,,connecting ,,storage ,,batteries ,on the discharge1 one cell of a lead storage battery gives an average of about #b volts1 and a cell of alkaline storage battery about #a4b volts1 no matter what its size or the number of plates may be4 ,when there are more than two plates in one cell1 all the positives in that cell are connected together by metallic strips or bands1 and all negatives in the cell are connected together in a similar way4 ,although we cannot obtain more than the above-named electromotive force from one cell of either type of storage battery1 we can obtain a greater ampre capacity by using large plates instead of small ones1 or by using a larger number of small size4 ,the same effects are produced by connecting the cells in series1 or multiple1 or multiple series1 as we showed you in regard to primary batteries2 and the storage batteries may be charged as well as discharged when connected in any one of these ways4 ,,charging ,,current ,the current which is used for charging must always be greater in pressure than that of the storage batteries which are being charged4 ,if it is not1 the storage batteries will be the stronger of the two and will overpower the charging current and so discharge themselves4 ,x ,,conclusion ,we will now bring this little volume to a close1 having given you a brief outline of the simplest rudiments of that wonderful power of nature1 ,electricity4 ,we may compare this subject to a beautiful house the inside of which you would like to examine from top to bottom4 ,we have opened the door for you2 now walk in and examine everything4 ,there may be a great many stairs to climb1 but what you see and learn will repay for all the trouble4 ,,the ,,end ,,footnotes3 #a ,the filaments in modern ,mazda lamps1 as made at the ,edison ,lamp ,works1 are strips of metallic tungsten4 #b ,the batteries we will now describe are for closed-circuit work only1 and they are never used for open-circuit work4 ,but there is a type of battery made that is available for either open or closed circuit operation4 ,this is the ,edison ,primary ,battery1 which will be described later on4 #c ,practically1 there is always one more negative plate than positive plates in a regular storage-battery cell4 ,consequently1 a standard cell always contains an odd number of plates4 ,,transcriber',s ,,note -,plain print and punctuation errors fixed4