MASSACHUSETTS INSTITUTE OF TECHNOLOGY Physics Department Physics 8.033 September 11, 2003 Problem Set 2 Due: Thursday, September 18 (by 4:30 pm) Reading: Chapter 2 of Resnick & Halliday. Parallel reading: Chapters 3 & 4 in French. Problem 1 Consider a general wave equation of the form: ∂2y 1 ∂2y = 2 2 ∂x2 V ∂t . (a) Show that any function of the quantity (x ± V t) will satisfy this equation. (b) Make an argument to show why V represents the propagation speed of waves or other disturbances described by this equation. Problem 2 Maxwell’s wave equation for the z­component of an electric field propagating in the x­ direction is: ∂ 2 Ez 1 ∂ 2 Ez = . ∂x2 c2 ∂t2 Show that this equation is not invariant under a Galilean transformation to a reference frame moving with relative speed v in the x direction. (See problem #16, chapter 1, page 35, in Resnick & Halliday.) Optional: Show that any function Ez (x− V t) is a solution to the transformed wave equation, where V = v ± c. Problem 3 “Michelson­Morley Experiment With a Real Wind” Resnick & Halliday, problem #19, chapter 1, page 35. Problem 4 “Not Much of a Contraction” Resnick & Halliday, problem #21, chapter 1, page 35. 1 Problem 5 In Special Relativity we will often want to evaluate the relativistic factor γ = (1 − v /c2 )−1/2 for (1) small values of speed, v, and (2) for values of v close to the speed of light. While this can be done with a calculator, it is often more instructive to derive an approximate analytic result explicitly in terms of powers of (v/c)2 for case (1), and powers of 1/γ 2 for case (2). a) Expand γ in a Taylor series in powers of (v/c)2 , keeping the first 3 terms (constant plus next two terms). (If you have not yet learned about Taylor series, simply adopt the expression given on page 334 of Resnick & Halliday.) Check your answers with those given at the bottom of page 17 in Resnick & Halliday. Evaluate your expression for γ with values of v/c = 0.1, 0.001, and 10−5 . Compare to the values you get by evaluating the full expression for γ with a calculator. b) Show that for large γ, 1 − β � 1/(2γ 2 ). Use this expression to find the values of β when γ = 2, 10, and 103 . Compare the approximate results with those obtained from the full expression using a calculator. 2 Problem 6 “Aberration and Relativity” Resnick & Halliday, problem #27, chapter 1, page 36. Problem 7 “The Speed of Light Really is the Same in All Frames” Resnick & Halliday, problem #6, chapter 2, page 82. (Start with equation 2.4 and apply the Lorentz­Einstein transformations to yield equation 2.5) Problem 8 “A Moving Clock” Resnick & Halliday (2nd edition), problem #9, chapter 2, page 82. Problem 9 “A Moving Rod” Resnick & Halliday (2nd edition), problem #10, chapter 2, page 82. Problem 10 “Hidden Symmetry in the Lorentz Equations” Resnick & Halliday (2nd edition), problem #11, chapter 2, page 82. Show that the variables x and w are completely interchangeable. 2 Optional Problem A “Michelson­Morley, Generalized” Resnick & Halliday (2nd edition), problem #18, chapter 1, page 35. Optional Problem B “A Fascinating “Thought Experiment” Resnick & Halliday (2nd edition), problem #25, chapter 1, page 36. 3