Elements of Natural Philosophy Ii Acoustics Iii Optics
Elements of Natural Philosophy Ii Acoustics Iii Optics
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In our eReader you can find the full English version of the book. Read Elements of Natural Philosophy Ii Acoustics Iii Optics Online - link to read the book on full screen. Our eReader also allows you to upload and read Pdf, Txt, ePub and fb2 books. In the Mini eReder on the page below you can quickly view all pages of the book - Read Book Elements of Natural Philosophy Ii Acoustics Iii Optics
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The effect of the reciprocal action of the two waves being to fix the point 0, these waves will both be totally reflected there, will return to the ends, be again reflected, return to the centre, from which they will be thrown back towards on. The ends, and so on till the living force of the cord is totally expended upon the air. Thus the two portions M and N of the cord may vibrate as though the point had been originally fixed.
If the finger be ap- ^ Finger applied at plied but for an in- one ...third the start at 0, at a dis- ^ ^ ^^ ^ ^~ tance from M equal to one-third of the jy, .. -^ . ..^^ {J[r whole length M N, while the wave is pro- jr\ . R~~^ ^ ^ gressing from JLC to- wards 0, the latter will be resolved, as before, into two component waves, Primitive pulse one of which will continue to move towards N on the two; same side of the cord, the other will return to M on the opposite side. The distance MO being equal to one- half of N, the return component will be wholly re- flected and change sides at M, and come back to the point by the time the direct component arrives at N, where the latter will be totally reflected and pass to the opposite side of the cord.
What to read after Elements of Natural Philosophy Ii Acoustics Iii Optics?
You can find similar books in the "Read Also" column, or choose other free books by W H C William Holms Chambers Bartlett to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
The effect of the reciprocal action of the two waves being to fix the point 0, these waves will both be totally reflected there, will return to the ends, be again reflected, return to the centre, from which they will be thrown back towards on. The ends, and so on till the living force of the cord is totally expended upon the air. Thus the two portions M and N of the cord may vibrate as though the point had been originally fixed.
If the finger be ap- ^ Finger applied at plied but for an in- one ...third the start at 0, at a dis- ^ ^ ^^ ^ ^~ tance from M equal to one-third of the jy, .. -^ . ..^^ {J[r whole length M N, while the wave is pro- jr\ . R~~^ ^ ^ gressing from JLC to- wards 0, the latter will be resolved, as before, into two component waves, Primitive pulse one of which will continue to move towards N on the two; same side of the cord, the other will return to M on the opposite side. The distance MO being equal to one- half of N, the return component will be wholly re- flected and change sides at M, and come back to the point by the time the direct component arrives at N, where the latter will be totally reflected and pass to the opposite side of the cord.
What to read after Elements of Natural Philosophy Ii Acoustics Iii Optics?
You can find similar books in the "Read Also" column, or choose other free books by W H C William Holms Chambers Bartlett to read onlineMoreLess
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