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Solutions to the final exam questions for the physics 2049 spring 2011 course focusing on optics and electromagnetism. Topics covered include mirror and lens equations, compound lenses, young's experiment, interference, soap film, capacitors, current in a magnetic field, electric fields, gauss's law, and rlc circuits.
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PHY2049 Spring 2011 Profs. P. Avery, S. Hershfield
Final Exam Solution
Answer: The image is initially erect, then flips upside down
Solution: For a concave mirror the object distance, p, and image distance, i, are related via 1/p + 1/i = 1/f with the focal length, f , being positive. Near the mirror p is small so 1/p > 1 /f and the image distance is negative (virtual image). Consequently, the magnification, m = −i/p, is positive, and the image is erect. Far from the mirror, 1/p < 1 /f , and the image distance is positive (real image). In this case the magnification, m = −i/p, is negative, and the image is inverted.
Answer: 10
Solution: Because the radius of curvature is 30 cm, the focal length is f = r/2 = 15 cm. An upright image three times the object size corresponds to a magnification of m = −i/p = 3. This implies that i = − 3 p and 1/p+1/i = 1/p− 1 /(3p) = 2 / 3 p = 1/f. The object distance is (2/3)f = 10 cm.
Answer: 120 cm to the right; m = − 1. 0
Solution: This is a compound lens problem. Find the image of the first lens, and use that as the object for the second lens. For the first lens we have 1 30
i 1
The image relative to the first lens is -10 cm, which is 10 cm to the left of the first lens and 40 cm to the left of the second lens. Thus, the object distance for the second lens is 40 cm:
1 40
i 2
The final image is i 2 = 120 cm to the right of the second lens, and the overall magnification is m = (−i 1 /p 1 )(−i 2 /p 2 ) = (10/30)(− 120 /40) = −1.
Answer: the dark fringes get brighter and the bright ones get darker
Solution: If one of the slits in Young’s experiment is covered up, then there will be no interference pattern. Partially covering up a slit reduces the interference: dark fringes get brighter and bright ones get darker.
Answer: 400 nm
Solution: Because the index of refraction of the film is greater than that of air (n = 1) there is an additional phase shift for the reflection inside the soap film. The condition for constructive interference is 2L = (m+ 0.5)λ/ 1 .5 or λ = 3L/(m+ 0.5). The fact that λ = 800 nm and λ = 480 nm are consecutive maximum means that if λ = 800 nm corresponds to m, then λ = 480 nm corresponds to m + 1. Using the m dependence on λ, this implies that 800/480 = (m + 1.5)/(m + 0.5), but 800 /480 = 5/3 = (2 + 1.5)/(1 + 0.5). In other words for m = 1 for λ = 800 nm, and hence L = (m + 0.5)λ/3 = 400 nm.
Answer: Q and V / 2
Solution: The charge on capacitors in series is the same (Q). This in turn implies that the voltage drop across each of the identical capacitors is also the same: Q/C. They each drop half the voltage.
Answer: The resistivity of the copper wire does not depend on its length.
Solution: Resistivity is an intrinsic property of the material. Like density it does not depend on the geometry or dimensions of the wire.
Answer: 4 V
Solution: The net resistance of the three resistors in series is 12 Ω. The current is 24V /12Ω = 2 A, and the voltage drop across the 2 Ω resistor is (2 A)(2 Ω) = 4 V.
Answer: 2 πm/(eB)
Solution: Let the component of the velocity perpendicular to the magnetic field be v⊥. The magnitude of the force on the electron is F = ma = mv^2 ⊥/r = ev⊥B. Eliminating one of the v⊥’s from this equation, the angular frequency of rotation perpendicular to the field is ω = v⊥/r = eB/m. The angular frequency is related to the period via ω = 2π/T.
Answer: 4 × 107 m/s
Solution: Since the electrons are assumed to be accelerated from rest, conservation of energy implies that (1/2)mev^2 = e(5000V ). Solve for v = 4. 19 × 107 m/s ≈ 4 × 107 m/s.
Answer: 0.75 mA clockwise
Solution: The flux is increasing out of the page at a rate dΦB /dt = π(2cm)^2 (3T /s) = 0. 00377 V. To oppose this change in flux the induced current is clockwise. It has magnitude 0. 00377 V /5Ω = 0. 754 mA.
Answer: 420 V
Solution: At resonance the driving angular frequency is ωd = 1/
LC = 70. 7 Hz, and the voltages of the inductor and capacitor cancel one another. The net voltage drop is equal to the voltage drop across the resistor. Consequently, the amplitude of the current oscillations is I = 12V /4Ω = 3A. The voltage across the inductor is Ldi/dt and has amplitude LωI = 424V.
Answer: 3. 0 × 10 −^5 T
Solution: The current of 3A leads to a displacement current of 3A between the plates. This displacement current flows uniformly within the plate radius of 1.0 cm. Using
Bds = μoid,enc for a circular path of radius r = 0.5 cm, the magnetic field is B = μoid,enc/(2πr). Because the circle has radius 0.5 cm, the displacement current enclosed is (3A)(πr^2 )/(π(1cm)^2 ) = 0. 75 A.
Answer: 65.4◦
Solution: At the first interface using Snell’s law we have n 1 sin(θ 1 ) = n 2 sin(θ 2 ). At the second interface where there is total internal reflection n 2 sin(θ 2 ) = n 3 sin(θ 3 ) = n 3. Putting these two together n 1 sin(θ 1 ) = n 3 or θ 1 = sin−^1 (n 3 /n 1 ).
Answer: 3
Solution: 400 rulings/mm corresponds to a separation between slits of d = 0. 001 m/400 = 2500nm. The condition for observing a diffraction line is d sin(θ) = mλ, which implies that d = 2500nm > mλ. For the largest wavelength, 700 nm, the largest m for which this inequality is satisfied is m = 3.
Answer: 25 m
Solution: Rayleigh’s criterion states that two objects are on the verge of resolvability if the central diffraction maximum of one is at the first minimum of the other. This occurs for θ ≈ sin(θ) = 1. 22 λ/d. For this problem λ = 500 nm, d = 50 cm, and θ = ∆x/(20000km), where ∆x is the smallest resolvable distance. Solve for ∆x = 24. 4 m.