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Material Type: Assignment; Class: CLASSICAL DYNAMICS I; Subject: Physics; University: University of Alabama - Huntsville; Term: Fall 2008;
Typology: Assignments
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University of Alabama in Huntsville Department of Physics Fall 2008
Deadline: 13 October, 2008
Problem 21: Two identical and massless rods of length ` are connected to a horizontal bar at a distance a from each other. The gravitational acceleration is g. Two identical masses m are connected to the lower ends of the rods, and are connected to each other by a spring of equilibrium length a and spring con- stant k. Show that the matrix formed from the eigenvectors simultaneously diagonalizes both the kinetic energy matrix and the potential energy matrix.
Problem 22: A mass M is constrained to move along a horizontal and frictionless wire. A second mass m is connected to M through a massless rod of length b. The gravitational acceleration is g. The system can move and oscillate only in the plane of the wire and the direction of the gravitational acceleration. Find the normal modes and the normal coordinates.
Problem 23: Two identical masses m are connected by identical and massless rods of length b, so that the second rod is connected to the mass at the end of the first rod and the second mass is connected at the end of the second rod. (Same setup at that of problem 12.) Find the normal frequencies and the normal modes. Assume two dimensional motion.
Problem 24: Three identical masses m are connected by four identical springs of spring
constant k. The masses move along a circular wire, so that one of the masses (say mass A) is fixed, and the other three are free to move along the wire. Find the eigenfrequencies and the normal modes.
Problem 25: A simple pendulum of length ` and mass m is pivoted at a point O on a block of mass 2m. The block can slide without friction on a horizontal surface. The gravitational acceleration is g. Assuming plane motion, obtain the equations of motion and the normal modes. Use the displacement of the block x and the angle of the pendulum’s arm from the vertical direction θ (such that θ = 0 is directed downward) as generalized coordinates. Solve the equations of motion for the initial conditions x(t = 0) = 0, x˙(0) = 1, θ(0) = 0.1, θ˙(0) = 0.