DQ1D_solution - of the motion and the radius R of the form:...

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Discussion Question 1D P212, Week 1 P211 Review: Uniform Circular Motion page 1 2 1 ˆ r 12 r 12 , F 1 2 =− G m 1 m 2 r 12 2 ˆ r 12 In P112 you will encounter problems where charged particles move in uniform circular motion. The forces involved may be electric or magnetic in nature. The answer to part(e) contains the secret of the cyclotron. Kepler’s Third Law (K-III) for planetary motion about the sun for circular orbits is T 2 = CR 3 where T is the period, R is the radius of the planet’s orbit and C is a constant. (a) Derive K-III for a circular orbit and in the process find an algebraic expression for C in terms the mass of the sun M S , the universal gravitational constant G , and numerical factors. F = -G m M S / R 2 F = ma = -m v 2 / R Set equal to each other and substitute period for velocity. T 2 = 4 π 2 R 3 / (G M S ) (b) Using your answer from part (b), re-express K-III as a relationship between the angular frequency
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Unformatted text preview: of the motion and the radius R of the form: 2 = f( R , G , M S ). 2 = G M S / R 3 R v m M s page 2 (c) Consider uniform circular motion of a body of mass m about a central force which depends on velocity: F = Dv a R b where D is a constant and a and b are known exponents. Derive K-III for this force, again expressing your answer as a relationship between and R, (The constant D will necessarily appear in your final expression, but v must not.) 2-a = D R a + b 1 /m (d) For the case a = 0 and b = 2, verify that your answer to part(c) collapses to that for part (b) (this is an excellent limiting behavior check). (e) Evaluate your answer to part (c) for the case a = 1 and b = 0. How does the angular frequency depend on radius for a force of this nature? = D/m, angular frequency independent of radius....
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DQ1D_solution - of the motion and the radius R of the form:...

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