Exercise 4.4 A pendulum is made of a bob of mass m but the string is replaced by a spring of constant k. Write the Lagrangian in terms of the length of the spring and the angle it makes with the vertical. Let the unstretched length of the spring be lo. Answer: 1 L = mi? +ml-6* + mgl cos 0 – k(l – lo)².
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- Problem 2.5 A particle in the infinite square well has as its initial wave function an even mixture of the first two stationary states: Y (x, 0) = A [Y1(x)+ ¥2(x)]. (a) Normalize ¥ (x, 0). (That is, find A. This is very easy, if you exploit the orthonor- mality of y1 and ý2. Recall that, having normalized ¥ at t = 0, you can rest assured that it stays normalized–if you doubt this, check it explicitly after doing part (b).) (b) Find ¥ (x, t) and |4 (x, t)|². Express the latter as a sinusoidal function of time, as in Example 2.1. To simplify the result, let w = 7²h/2ma². (c) Compute (x). Notice that it oscillates in time. What is the angular frequency of the oscillation? What is the amplitude of the oscillation? (If your amplitude is greater than a/2, go directly to jail.) (d) Compute (p). (As Peter Lorre would say, “Do it ze kveek vay, Johnny!") (e) If you measured the energy of this particle, what values might you get, and what is the probability of getting each of them? Find the…Problem 2.13 A particle in the harmonic oscillator potential starts out in the state ¥ (x. 0) = A[3¥o(x)+ 4¼1(x)]. (a) Find A. (b) Construct ¥ (x, t) and |¥(x. t)P. (c) Find (x) and (p). Don't get too excited if they oscillate at the classical frequency; what would it have been had I specified ¥2(x), instead of Vi(x)? Check that Ehrenfest's theorem (Equation 1.38) holds for this wave function. (d) If you measured the energy of this particle, what values might you get, and with what probabilities?Assistance with last two questions
- Problem 2 Consider the block of mass m, connected to a spring of spring constant k and placed on a inclined plane of angle a. Let la be the length of the spring at equili brium, and r be the elongation. The block oscillates and at the same time is rotating around origin 0, in the plane of the inclined, by a variable angular velocity . 1. Calculate the degrees of freedom of the block 2. What is the kinetic energy of the block 3. What is the potential energy of the block 4. Write the Lagrangian function (don't derive the Euler Lagrange equa- tions) k reference plane m o'I just need help for part a. Question 3. (Hamilton and Lagrange formalism)Calculate the constants b₁ and b2 in the the following equation 1 Imax d²x(t) for the condition (0) ) = xmax, the maximum extension of the oscillator. What is v(0) for this condition? Match the items in the left column to the appropriate blanks in the equations on the right. Make certain each equation is complete before submitting your answer. ?). dt² ∞ b₂ 0 t=0 dx (t) (da)₁-0 dt t=0 b₁ x(t) v(0) = xmax = b₁ co Therefore, b₁ = 0 + b₂ sin and b₂ = (√5.0) k μl • (√) +0 k COS 00 (√5-0) x(t) = b₁ cos Reset t + b₂ sin 2 sin (√) Help
- Exercise 6.4 Consider an anisotropic three-dimensional harmonic oscillator potential acy = { m (w² x ² + w} y² + w? 2²). V (x, y, z) = = m(o² x² + @z. (a) Evaluate the energy levels in terms of wx, @y, and (b) Calculate [Ĥ, Î₂]. Do you expect the wave functions to be eigenfunctions of 1²? (c) Find the three lowest levels for the case @x = @y= = 2002/3, and determine the degener- of each level.Introduction to Classical Dynamics The Lagrangian Method Please I need a complete solution of this, thank you.Two blocks and three springs are configured as shown in the figure. All motion is horizontal. When the blocks are at rest, all springs are unstretched. 6. k1 kiz ell m1 m2 a. . ] Choose as generalized coordinates the displacement of each block from its equilibrium position and write the Lagrangian. b. . c. :. -] Find the T and V. ] Suppose m, = 2m, k, = 4k, m2 = m, k2 = k, kz = 2k Find the frequencies of small oscillations. d. -] Find the normal modes of oscillation. ..] At time t = 0, mass #1 is displaced by a distance b relative to its equilibrium position. i.e. x, (0) = b. The other initial conditions are x,(0) = 0, *1(0) = 0, and xz(0) = 0. Find t , the next time at which x2 vanishes. е.