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Solutions to the third exam of the phy2049 course offered in spring 2007. It covers topics such as electrostatics, oscillating lc circuits, gaussian surfaces, and optics. The exam includes problems on calculating the electric field, maximum charge on a capacitor, charge enclosed in a gaussian surface, speed of light in a medium, and more.
Typology: Exams
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Prof. Darin Acosta Prof. Greg Stewart April 25, 2007
y-axis ↑ ↑ ↑→→→ x-axis
a.) 18 b.) 0 c.) 9 d.) 27 e.) 36
Solution: From symmetry, the field from the pair q 1 q 4 (which is directed from q 1 along the dotted line towards q 4 ) and the field from the pair q 2 q 5 (which is directed from q 2 along the dotted line towards q 5 ) sum to give a zero component in the x-direction. Thus, the x-component of the net force at point P is just E = Efrom q3 + Efrom q6 = (1/4πε 0 )[ (10 -9^ C/1m 2 )(-e (^) x ) + (10-9^ C/1m 2 )(-ex ) ] where ex is a unit vector in the x-direction and the two minus signs indicate that both Efrom q and Efrom q6 point to the left, i. e. in the negative x-direction. Thus, the magnitude of E at point P from all the charges is just [8.99 10^9 Nm 2 /C^2 ]*(2 * 10 -9^ C/m 2 ) = 17.98 N/C
This is like a homework problem in chapter 31. Eq. 31-14 tells use that the amplitude of the current in an oscillating LC circuit is ωQ, where ω, the frequency, is just 1/(LC) 1/2^ and Q is the maximum charge on the capacitor. Q=I (^) max /ω = I (^) max (LC) 1/2^ = 0.1(2x10 -3^ * 3x10-6^ ) 1/2^ = 7.7μC
a. 142 b. 8.85 c. 17. d. 283 e. 0
Solution: Use Gauss’ law (eq. 23-7 in the text). (This problem is similar to sample problem 23-2)
the vector dot product between the electric field vector and the dA over each surface of the cube shown. Since E is entirely in the x-direction, any surface on the cube whose dA vector is perpendicular to x will give a zero dot product. Thus, only the left face (at x=1.0 m and parallel to the yz plane) and the right face (at x=3.0 m and also parallel to the yz plane) will have non-zero contributions to the integral.
E=2.0xi, the minus sign is because dA for the left face points in the minus x-direction and E, the electric field vector, points in the +x-direction. All over the left face, x=1.0 m, and the integral of dA is just the area of the face, 4 m 2. Thus, the integral at the left face is -8 Nm 2 /C. Similarly, for the right face, x=3.0 m, dA points to the right in the same direction as the E field so the dot product is positive and the integral at the right face is +2.0(3.0)(+)4m^2 = +24 Nm 2 /C. So we have
solution: the frequency of light in matter remains the same, however the wavelength is reduced from the freespace value of the wavelength by n, the index of refraction, i. e. λ in glass = λ vacuum/n = 520 nm/1.4. The speed of the propagation of the light in the glass is λ in glass *freq. Since the frequency is unchanged, the speed in glass is just reduced by the same factor that λ is, i. e. speed = 2.998 x 10 8 m/s / 1.4 = 2.14 x 10 8 m/s.
Solution: The focal length of the mirror is f = R/2 = 30 cm. The image is found by solving: 1 1 1
120 cm
p i f
i f p i
Image distance is positive, so image is real and is thus in front of mirror.
0
v
− z (2) 0 0
v
z (3) 0 0
v
− y (4) E v 0 0 (^) zˆ (3) − E v 0 0 yˆ
Solution: The forces must balance:
0 0 0 0
where ˆ^ and ˆ
ˆ
q E v E v
F E v B E v B E y v x
B z
Solution: Use Kirchoff’s junction and loop rules after you define current directions: Junction: i 1 (^) = i 2 (^) + i 3 Outer loop counterclockwise:
i (^2) i (^1)
i (^3)
1 1 1 2 1 2 1 1 1
i R 0
i R R
(1) 25pF (2) 225pF (3) 75pF (4) 100pF (5) 300pF
Solution: The total charge is conserved, as it cannot be removed. The capacitance and potential difference does change, however:
1 1 2 2
2
25pF
q C V C C V
V C C V