(c) (1 POINT) At point C , what is the direction of the electric field vector ?
Indicate this direction with an arrow at that point.
(d ) ( 1 POINT) At point B , what is the direction of the electric field vector ?
Indicate this direction with an arrow at that point.
(e) (2 POINTS) Given that point D is at the surface of the sphere, then what is
the magnitude E of the electric field at point D ? Use symbols.
(f ) (1 POINT) At point D , what is the direction of the electric field vector ?
Indicate this direction with an arrow at that point.
(g) (2 POINTS) Suppose the magnitude of the electric field at point F is one-
half the magnitude of the electric field at D. What is the distance of point F
from the center ? Use symbols.
Now for the "real deal." We're talking 24 points, so proceed
carefully. Use symbols always:
(h) (12 POINTS) Suppose the distance of point B from the center is
R/4. What is the magnitude E of the electric field at point B ?
(i) (12 POINTS) Suppose the distance of point C from the center
is 3R/2. What is the magnitude E of the electric field at point C ?
(b) (13 points) What is the potential V at the point P shown in fig.1 ?
Derive this. Show all calculus steps !!
Now look at fig. 2. One of the ions in the tube is a point charge q of mass m. Let's say it starts from rest at a distance 2b from the end of the rod, and accelerates to a distance b/2 from that end. Pretend that gravity has been turned off !
(c) (3 points) What must be the sign of q , positive or negative?
(d) (12 points) What is the speed of the point charge q when it reaches the distance b/2 ?
(a) (2 points) What is the magnitude E of the electric field at a distance r from the central axis of the capacitor if b < r ? Explain.
(b) (3 points) What is the magnitude E of the electric field at a distance r from the central axis of the capacitor if a < r < b? Derive E. Show all steps.
(c) (4 points) Derive the capacitance per unit length of the system.
Solution: (a) E = 0 since zero net charge is enclosed by any Gaussian surface larger than b in radius. (b) E = 2·k·lambda/r. You better derive this ! Remember that for cylindrical symmetry, (E·2·pi·r·L) = qenc /e0 = lambda·L/e0; thus, E = lamba/( 2·pi·e0.r ) = 2·k·lambda/r. Note qenc =lambda·L, since the radius of the Gaussian surface is between a and b and only encloses lambda·L on the inner sphere ! (c) For a length L of the capacitor, the capacitance is Q/V = (lamba·L)/[2·k·lambda·ln(b/a)] = L/[2·k·ln(b/a)]. Note that V = 2·k·lambda·ln(b/a) is obtained by integrating 2·k·lambda/r from a to b. To get the capacitance per unit length, divide by L to get 1/[2kln(b/a)] . See the derivation on page 808, example 26.2. |