___ __ ___ __ NameSt)L.&) S (1) [25 pointsj Two wide, flat conducting plates are arranged as shown, with inner surfaces (area A) parallel to the x-z plane, at positions y = ±a. Assume that the plates are wide enough to allow edge effects to be neglected, so the fields have y-dependence only. The region between the plates is filled with a non-conducting material having volume charge p = p 0 sin- with p 0 a constant. a , (a) Find a general relationship for the electric field between the plates. (b) If the boundary conditions are set so that the electric field is given by (+p a / e) at y = 0 just inside the surface of each plate, find the potential difference between the two plates. (c) Find the total charge (with sign) on each plate. (d) If the plate on the right is moved to the right, opening a gap between it and the charged region, while maintaining the total charges on the plates unchanged, describe the resulting electric field between the plates. - — (0.7 7E’ c: I_SL C 4- c? J -. o c / 1f ir’ 1. ¶-t 0 4- 64-v V-SE,a =- -c< s:ci-4 — < — r L &k I cr ‘ 13 fy*c E G/ ç, 02 ç A 1p q / f Vfr--- c -y 4 k 0 A hc i% 0 _p 4 Yo r C) A o-, E-F..U c U c-c t -7ô”1L. A-( :144 4A ‘- 2 — VC 4 ) i Name___________ (2) [25 points I An electric field is given (in cylindrical coordinates z, s. ) by E = [AcospJ— IA(sin)/ si in some region of space, where A is a constant. (a) Determine whether this field could be found in an electrostatic situation. (b) If this field is allowed in electrostatics, determine the charge density in this region. (c) Similar to the above, suppose in spherical coordinates, E = O[BsinOI— [BcosOj,in some region with B a constant. Determine whether this field can exist in an electrostatic situation. (d) If the field from (c) is allowed, determine the charge density in the region where it occurs. (e) Choose one of these fields, which is allowed in the static situation, and determine the are potential difference in going from the point (x a, y = 0, = 0) to (x = 0, y = 2a, = 0). These cartesian coordinates; you will need to translate to the appropriate curvilinear coordinates. (q) T kk uuiv.t, f’..cJ% lj-c’rv J+Jo-o÷{o - 1 y (1’) (c) Lô] ÷[o L’ Cqv4E 10t) ruA.fk-(S(-”j AJo+ Cct) ,P — E E ‘ c E rQol4.C E 4b 1 - ) I.s O +Lf- 4-kt’c 2rBc) 1 ( — r (5 0 1 Ce) E/c — fr-4- Cd’ ‘ Càv b (A. ikj=o. E AV Lhc) ) I- 1 J / C%c; E)(5) sl/)(cj o a - ô s r ñrr t a -- — E __ Name S3 L AJS’ inner shell (radius a) (3) [25 points I Two concentric spherical shells are arranged as follows: the a potential is conducting, and is held at a potential V = 0, while the outer shell (radius b) has is vacuum, given in spherical coordinates by ( cosO), with V, a constant. Between the shells with no charges. between a and b. (a) Write the general solutions of the Laplace equation which would apply in this region. (b) State the boundary conditions, and solve to find the potential, V() . (c) Find the surface charge density vs. 0 at r a, on the surface of the inner sphere , 0 cs9 V (ca) \f( r9 ? ,4;J )/ ( C (c-) c r 1, SfJ k± (4+4q4)O —, t+ 1 Y2 V,: &,1 / k ti t? Ac tcAt. (c..iJ) f-tPL ) ‘, 0 — V L? I =+-- V( (c) E ::)! — V o (If- ) çj 4 Name 5a I $ r reflector”, consisting of (4)125 points I A point charge +Q is located close to a grounded “corne distance to three perpendicular metal plates. The charge equidistant from the plates, with Li the the . each plate. The sketch is a cutaway view, but consider the planes to extend to infinity INote, distance of Q to the corner would be d’J .1 (a) Describe the charge distribution used to solve this problem. (b) Find the force on the charge +Q, with direction. tion, but (c) Find the total charge on each of the three surfaces. This does not require a calcula you should explain your reasoning sufficient to show how you got the result. relative to the (d) Find the net force on each plate, with direction. (You can state the magnitude ck.) part (b) answer. Hint--if you are doing a long calculation for this one you are off-tra is (°‘) (‘1€ e £ Th nc- cJ, &rL dYQJkyL 3 F ( ) _j c(2 cA $1’d. (tJ3) 1 ,;j .__j_ °?frv-(-Q)c: 3 .lr Qc.J\ i( 4v kCSA-- f VL FK ‘1 z. Ft — tJ - (‘1r1 ( • lc c.L.,: — . 1FH 4d ( -ji 5 p fs D(2JO{) 2 FQ — Lj fj 4. ((774 Ci2d?- 2 __ 4( 0 )cJ’d: J -Q LQ /- ‘5 FAc( 1-zk; 4W 4 j-L (c) (c L> n-k i-o 9-4 cL>) 1 k%J cAAyz, L- A) ÷) tt i 44 /M 1 co ( (d)LLt fE 4k - • c 2J r 17 ‘ 4 iF! J