This preview has intentionally blurred sections. Sign up to view the full version.
View Full Document
Unformatted text preview: Adam S. Bolton March 6, 2002
[email protected] MIT 8.02 Spring 2002
Exam #1 Solutions Problem 1 (a) No bulbs glowing: no closed circuit anywhere and hence no current anywhere. (b) A and B glow with equal brightness, as they are connected in series to the battery and
thus the same current passes through each. C is still off. (c)A, B, and C all glow. A is brightest, for all current ﬂows through it. B and C glow with
equal but lesser brightness, as the current through A is split equally between B and C. (d) Bulb A in case (c) is brightest of all: effective resistance of the bulb combination is
decreased from that of part (b) by the addition of bulb C in parallel with bulb B. By Ohm’s law, more current is then drawn from the battery in case (c) as compared to case (b), leading
to a brighter bulb A. Bulbs B and C in case (c) are faintest of all. Let V be the battery voltage and R be the
resistance of each bulb. The effective resistance of the circuit as a whole is 2R in case (b)
and 1.5R in case Thus the current through A is V/2R in case (b) and V/1.5R = 2V/3R
in case Therefore in case (b) the current through B is also V/ 2R, but in case (c) the
current through B (and C) is half of 2V/ 3R, which is V/ 3R. This latter current is less than
V/ 2R, and so B and C in case (c) are fainter than A and B in case (e—b) B glowing, C off. (e—c) B and C glowing with equal brightness. (e—d) All on—bulb brightnesses are equal, for all bulbs have the full battery voltage across
themselves, and therefore the same current goes through each. Problem 2
(a) Q 2 CV, and C & V are the same for both capacitors. So each has a charge +CV on
its upper plate and —CV on its lower plate. (b) For both capacitors, electric ﬁeld has magnitude E = V/d and is directed downwards
(from + charge to —). (c) Right capacitor: C & V unchanged, so +CV on upper plate and —CV on lower plate
still. Left capacitor: V unchanged, but 0 —> K30 = 30, giving charges +30V on upper plate
and —30V on lower. (d) Same answer as part (b), for V and d remain unchanged. MIT 8.02 Spring 2002 7 Exam #1 Solutions 2 Problem 3 (a) Since there is no current inside the conductor, the E—ﬁeld is zero everywhere inside.
Therefore Gauss’s law dictates that there cannot be any net charge inside the conductor,
so none of the charge will be found in the region 71 < 7“ < m. Now suppose some of the
net positive charge +q remained on the inner surface of the pipe. We could enclose this
charge with a Gaussian surface lying entirely within the conducting material (ignoring end
effects), and since E = 0 everywhere within a conductor, Gauss’s law would tell us that our
Gaussian surface contained no net charge. This would only be possible if there were some
negative charge within the cavity to balance the positive charge on the inner pipe wall. But
this cavity is empty. So we may conclude that none of the charge will stay on the inner wall.
Since we have found that it cannot go anywhere else, all charge +q must go to the outer
surface. Symmetry of the system dictates that the charge will be distributed evenly over this
surface, with surface charge density a = +q/27rr2L. (See the solution to homework problem
2.1 for discussion of a related situation.) (b) Symmetry requires that E be in the radial direction and depend only upon 7“. (By
“radial” here we mean perpendicularly away from the pipe axis, not radial in the sense of
spherical coordinates. Unfortunately there is no good terminology to distinguish between
“cylindrical—radial” and “spherical—radial” Application of Gauss’s law to a cylindrical Gaus—
sian surface of length l and radius 7“ coaxial with the pipe leads to (27rrl)E = Qencl/eo. For
7“ < r1, Qencl = 0 and hence E = 0. (ii) We already know that E = 0 inside the conductor
(r1 < 7“ < 73). (iii) For 7“ > 7‘2, Qencl = +ql/L, and thus E = +q/(27reorL) radially outward
(i.e. cylindrical—radially). (c) AV 2 0: potential difference is the line integral of the electric ﬁeld, and the electric ﬁeld
is zero everywhere between the axis and the outer surface. (d) Nothing changes from part (b): there was no E—ﬁeld in the pipe cavity to begin with, so
there is nothing to induce a polarization charge in the dielectric. END ...
View
Full
Document
 Spring '08
 Turner
 Physics

Click to edit the document details