The Diffusion of Gases Through Liquids And Allied Experiments
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For large values of V there is no point of intersection, or the disk passes without interruption from the lower to the upper plate of the condenser. The same result may be brought about by decreasing D for a fixed V, and on this principle I have based the following method of measurement.
If we differentiate equations (i) and (2) with respect to / the results are dl 2. 262 Xio\D-iy ~dl = l? P8 ^ If these slopes are identical F 2 = - 2. 262 X io 6 -=5 pg(D-l) 3 (6) Now, when there is but a single... point of intersection (tangency of equations (i) and (2)), equations (3) and (6) correspond to the same value of l = l c, whence after canceling superfluous quantities D = & (7) In other words, if the electrical forces are sufficiently strong to raise the disk e more than one-third of the distance D between the plates of the condenser, it will pass all the way to the upper disk cc. Hence under these circumstances equation (3) gives F 2 = o. 5 02 7 XioVZ) 2 AK 2 (8) Thus in case of the first method of measurement the upper plate cc, fig.
What to read after The Diffusion of Gases Through Liquids And Allied Experiments?
You can find similar books in the "Read Also" column, or choose other free books by Carl Barus to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
For large values of V there is no point of intersection, or the disk passes without interruption from the lower to the upper plate of the condenser. The same result may be brought about by decreasing D for a fixed V, and on this principle I have based the following method of measurement.
If we differentiate equations (i) and (2) with respect to / the results are dl 2. 262 Xio\D-iy ~dl = l? P8 ^ If these slopes are identical F 2 = - 2. 262 X io 6 -=5 pg(D-l) 3 (6) Now, when there is but a single... point of intersection (tangency of equations (i) and (2)), equations (3) and (6) correspond to the same value of l = l c, whence after canceling superfluous quantities D = & (7) In other words, if the electrical forces are sufficiently strong to raise the disk e more than one-third of the distance D between the plates of the condenser, it will pass all the way to the upper disk cc. Hence under these circumstances equation (3) gives F 2 = o. 5 02 7 XioVZ) 2 AK 2 (8) Thus in case of the first method of measurement the upper plate cc, fig.
What to read after The Diffusion of Gases Through Liquids And Allied Experiments?
You can find similar books in the "Read Also" column, or choose other free books by Carl Barus to read onlineMoreLess
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