t3s3

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z R σ R→∞ z R R σ(θ,φ)= σ 0 cos θ z z z<R z>R R 2 + z 2 - 2Rz =(R - z) R>z (z - R) R<z ˆ r = z ˆ z r 0 = R sin θ 0 cos φ 0 ˆ x + sin θ 0 sin φ 0 ˆ y + cos θ 0 ˆ z dS 0 = R 2 sin θ 0 0 0 r - r 0 = R 2 + z 2 - 2Rz cos θ 0 1/2 E(z ˆ z) = 1 4π 0 ˆ S σ(r 0 )(r - r 0 ) |r - r 0 | 3 dS = σ 0 4π 0 ˆ S cos θ 0 (-R sin θ 0 cos φ 0 ˆ x - R sin θ 0 sin φ 0 ˆ y +(z - R cos θ 0 z) (R 2 + z 2 - 2Rz cos θ 0 ) 3/2 R 2 sin θ 0 0 0 = σ 0 R 2 2 0 ˆ z ˆ 1 -1 u(z - Ru) (R 2 + z 2 - 2Rzu) 3/2 du = 2σ 0 R 3 3 0 z 3 ˆ z z>R

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Page 1: t3s3

CYK\2009\PH102\Tutorial 3 Physics II

1. [G 2.6] Find the electric �eld a distance z above the center of a �at circular disk of radius R (see �gure),which carries a uniform surface charge σ. What does your formula give in the limit R→∞? Also check thecase z � R.

2. A spherical surface of radius R and center at origin carries a surface charge σ(θ, φ) = σ0 cos θ. Find theelectric �eld at z on z-axis. Treat the case z < R (inside) as well as z > R (outside). [Hint: Be sure totake the positive square root:

√R2 + z2 − 2Rz = (R− z) if R > z, but its (z −R) if R < z.]

Let r = zz and r′= R

(sin θ

′cosφ

′x + sin θ

′sinφ

′y + cos θ

′z).

dS′= R2 sin θ

′dθ

′dφ

′∣∣∣r− r′∣∣∣ =

(R2 + z2 − 2Rz cos θ

′)1/2

E(zz) =1

4πε0

ˆS

σ(r′)(r− r

′)

|r− r′ |3dS

=σ0

4πε0

ˆS

cos θ′(−R sin θ

′cosφ

′x−R sin θ

′sinφ

′y + (z −R cos θ

′)z)

(R2 + z2 − 2Rz cos θ′)3/2R2 sin θ

′dθ

′dφ

=σ0R

2

2ε0zˆ 1

−1

u(z −Ru)(R2 + z2 − 2Rzu)3/2

du

=2σ0R

3

3ε0z3z z > R

(a) Problem 1 (b) Problem 4 (c) Problem 5

Figure 1

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= − σ0

3ε0z z < R

Note: E is constant inside sphere.

3. [G 2.9] Suppose the electric �eld in some region is found to be E = kr3r, in spherical coordinates (k issome constant).

(a) Find the charge density ρ.

(b) Find the total charge contained in the sphere of radius R, centered at the origin. (Do it two di�erentways.)

4. [G 2.12] Use Gauss's law to �nd the electric �eld inside a uniformly charged sphere (charge density ρ). [G2.18] Two spheres each of radius R and carrying uniform charge densities +ρ and −ρ, respectively, areplaced so that they partially overlap (See Figure). Call the vector from the positive center to the negativecenter d. Show that the �eld in the region of overlap is constant, and �nd its value.

[G 2.12]

[G 2.18]

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5. [G 2.16] A long coaxial cable (see �gure) carries a uniform volume charge density ρ on the inner cylinder(radius a), and a uniform surface charge density on the outer cylindrical shell (radius b). This surfacecharge is negative and of just the right magnitude so that the cable as a whole is electrically neutral. Findthe electric �eld in each of the three regions: (a) inside the inner cylinder (s < a), (b) between the cylinders(a < s < b), (c) outside the cable (s > b). Plot |E| as a function of s.

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6. [G 2.20] One of these is an impossible electrostatic �eld. Which one?

(a) E = k [xyx + 2yzy + 3xzz]

(b) E = k[y2x + (2xy + z2)y + 2yzz

].

Here k is a constant with the appropriate units. For the possible one, �nd the potential, using the originas your reference point. Check your answers by computing ∇V . [Hint: You must select a speci�c pathto integrate along. It does not matter what path you choose, since the answer is path-independent, butyou simply cannot integrate unless you have a particular path in mind.]

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7. [G 2.21] Find the potential inside and outside a uniformly charged solid sphere whose radius is R and whosetotal charge is q. Use in�nity as your reference point. Compute the gradient of V in each region, and checkthat it yields the correct �eld. Sketch V (r).

8. [G 2.22] Find the potential a distance s from an in�nitely long straight wire that carries a uniform linecharge λ. Compute the gradient of your potential, and check that it yields the correct �eld.

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9. [G 2.26] A conical surface (an empty ice-cream cone) carries a uniform surface charge σ. The height ofthe cone is h, as is the radius of the top. Find the potential di�erence between points a (the vertex) and b(the center of the top).

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10. [G2.27] Find the potential on the axis of a uniformly charged solid cylinder, a distance z from the center.The length of the cylinder is L and its radius is R, and the charge density is ρ. Use your result to calculatethe electric �eld at this point. (Assume that z > L/2.)

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