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Solutions to Additional Conceptual Practice Problems for PHYS 1112 Final Exam

PHYS 1112 – Exam 4 w Solutions (2010) – Intro to Physics 2

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Physics <strong>1112</strong>Spring 2009University of GeorgiaInstruc<strong>to</strong>r: HBSchüttlerof Φ m , with final values of flux Φ ′ m = B ′ A cos Θ ′ , magnetic field strength B ′ and angleΘ ′ ≡ ̸ ( A ⃗′ , B ⃗ ′ ), after changing the field/circuit configuration, as follows:(A) Φ ′ m = −BA < +BA = Φ m with Θ ′ = 180 o and B ′ = B;(B): Φ ′ m = 0 < BA = Φ m with Θ ′ = 90 o and B ′ = B;(C): Φ ′ m = B ′ A < BA = Φ m with Θ ′ = 0 o and B ′ < B;(D): Φ ′ m = BA = Φ m with Θ ′ = 0 o = Θ and B ′ = B;(E): Φ ′ m = B ′ A > BA = Φ m with Θ ′ = 0 o and B ′ > B;(F): Φ ′ m = 0 < BA = Φ m with Θ ′ = 90 o and B ′ = B.There<strong>for</strong>e, the time-dependent change of flux ∆Φ m ≡ Φ ′ m − Φ m and the resulting inducedEMF E = −∆Φ m /∆t (with ∆t > 0 here) have the following signs:∆Φ m < 0 and hence E > 0 <strong>for</strong> processes (A), (B), (C) and (F). By the sign convention <strong>for</strong>Faraday’s law, a positive EMF E > 0 drives the current I in the loop in right-hand (RH)direction around A ⃗ (i.e., point RH thumb in A-direction; ⃗ then 4 RH fingers will point inI-direction). Since A ⃗ was chosen <strong>to</strong> point in<strong>to</strong> the paper, ”RH direction around A” ⃗ means:clockwise. So, current I flows clockwise around the loop and there<strong>for</strong>e deposits positivecharge on the upper capaci<strong>to</strong>r plate (and an equal amount of negative charge on the lowercapaci<strong>to</strong>r plate) in processes (A), (B), (C) and (F).∆Φ m > 0 and hence E < 0 <strong>for</strong> process (E). By the sign convention <strong>for</strong> Faraday’s law, anegative EMF E < 0 drives the current I in the loop against RH direction around ⃗ AHence, current I flows counter-clockwise around the loop and there<strong>for</strong>e deposits negativecharge on the upper capaci<strong>to</strong>r plate (and an equal amount of positive charge on the lowercapaci<strong>to</strong>r plate) in process (E).∆Φ m = 0 and hence E = 0 <strong>for</strong> process (D). Hence, there is no induced EMF and no inducedcurrent I in the loop and there<strong>for</strong>e zero charge being deposited on the either capaci<strong>to</strong>r plate.For an alternative way of solving this, using Lenz’s rule, see posted solution of HomeworkProblem P08.01 <strong>for</strong> details.10

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