Page:A Treatise on Electricity and Magnetism - Volume 1.djvu/38

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2

ERRATA. VOL. I.


p. 159, 1. 3, for F read f.

,, 1. 2 from bottom, for M read M_2 .

p. 163, 1. 20, for \lambda_{i-s+1} read \lambda_{i-\sigma+1}.

p. 164, equation (34), for (-1)^{i-s} \frac {\left | \underline{2s} \right .}{2^2s \left | \underline{i} \right . \left | \underline{s} \right . } read (-1)^{i-\sigma} \frac {\left | \underline{2\sigma} \right .}{2^2\sigma \left | \underline{i} \right . \left | \underline{\sigma} \right .}

p. 179, equation (76), for i+l read 2i+1.

p. 185, equation (24), for \frac{x^2}{b^2}-\frac{z^2}{c^2}=1 read \frac{x^2}{b^2}-\frac{z^2}{c^2-b^2}=1

p. 186, 1. 5 from bottom, for 'The surface-density on the elliptic plate' read The surface-density on either side of the elliptic plate

p. 186, equation (30), for 2\pi read 4\pi.

p. 188, equation (38), for \pi^2 read 2\pi^2.

p. 196, 1. 27, for e..e read e_1..e_2 .

p. 197, equation (10) should be M = \frac{E \,e}{f}-\frac{1}{2}\frac{e^2 a^3}{f^2(f^2-a^2)}

p. 204, 1. 15 from bottom, dele either.

p. 215, 1. 4, for \sqrt{2k} read \sqrt{2} k.

p. 234, equation (13), for 2E read \frac{E}{2\pi}.

p. 335, dele last 14 lines.

p. 336, 1. 1, dele therefore.

" 1. 2, for 'the potential at C to exceed that at D by P,' read a current, C, from X to Y .

" 1. 4, for 'C to D will cause the potential at A to exceed that at B by the same quantity P,' read X to Y will cause an equal current G from A to B.

p. 351, 1. 3, for R_1^2 u^2 + R_2^2 v^2 + R_3^2 w^2 read R_1 u^2+R_2 v^2+R_3 w^2 \,

1. 5, read +2\iiint (u \frac{dV}{dx} +v \frac{dV}{dy} + w \frac{dV}{dz}) \, dx\, dy\, dz

p. 355, last line, for S' read S.

p. 356, equation (12), for  {\overline {\left . \frac {db}{d} \right |}}^2 read {\overline {\left . \frac {db}{dx} \right |}}^2

p. 365, in equations (12), (15), (16), for A read Ar. E E

p. 366, equation (3), for \frac{E_2}{r_1} read \frac{E_2}{r_2}

p. 367, 1. 5, for 2k_1 S read 2k_2 S.

p. 368, equation (14), for J_2^' read I_2^'.

p. 397, 1. 1, for \frac {D'}{E} \delta' read \frac {D'}{E'} \delta '.

p. 404, at the end of Art. 350 insert as follows:—

When \gamma, the resistance to be measured, a, the resistance of the battery, and \alpha, the resistance of the galvanometer, are given, the best values of the other resistances have been shewn by Mr. Oliver Heaviside (Phil. Mag., Feb. 1873) to be

c=\sqrt {a \alpha}, b=\sqrt {a \gamma \frac{\alpha + \gamma}{a + \gamma}}, \beta=\sqrt {\alpha \gamma\ \frac {a+\gamma}{\alpha +\gamma} }