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Advanced Calculus fi..

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I348 <strong>Advanced</strong> <strong>Calculus</strong>, Fifth Edition4. a) Write out in detail the steps leading from the Maxwell equations (5.120) to the partialdifferential equations (5.129), (5.130).b) Show from Eqs. (5.120), . . . , (5.130) that each component of E satis<strong>fi</strong>es the wave1equation in each domain free of charge.5. Find the temperature distribution in a solid whose boundaries are two parallel planes, dunits apart, kept at temperatures TI, T2, respectively. (Hint: Take the boundaries to be theplanes x = 0, x = d and note that, by symmetry, T must be independent of y and z.)6. Show that on the basis of the laws of thermodynamics, the line integralis independent of the path in the T V plane. The integrand is minus the differential of thefree energy F.7. Consider a fluid motion in space. A particle occupying position (xo, yo. zo) at time t = 0occupies position (x , y , z) at time t . Thus x , y , z become functions of xo, yo, 20, t :Let the V symbol be used as follows:x = ~ (xo, YO, 20, t), 2y = @(xo, yo* ZO. t), (*)z = x(x0, yo, zo, t).and let J denote the JacobianLet v denote the velocity vector:a(x, Y, Z) 41a(xo7 yo, ZO).ax ay az a4 a@ axv=-i+-j+-k=-i+-j+-k.at at at at at ata) Show that J = V x . V y x Vz.b) Show thataxo vy x vz ay0 v y x- = i. -vz az0=j. - = k. V y x vzax J ' ax J ' ax J 'and obtain similar expressions for(Hint: See Problem 5 following Section 2.12).C) Show thata J--=vv,.vy xvz+vv,.vzxVx+vv,.vxxvy.at 4d) Show that1 aJdivv = --.J at

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