Theory and Design for Mechanical Measurements
Theory and Design for Mechanical Measurements
6th Edition
ISBN: 9781118881279
Author: Richard S. Figliola, Donald E. Beasley
Publisher: WILEY
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Chapter 2, Problem 2.17P

For the Fourier series given by

Chapter 2, Problem 2.17P, For the Fourier series given by where t is time in seconds: What is the fundamental frequency in

where t is time in seconds:

  1. What is the fundamental frequency in hertz and radians/second?
  2. What is the period T associated with the fundamental frequency?
  3. Express this Fourier series as an infinite series containing sine terms only.

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QUESTION 4 Consider a 2 DOF system shown below. k₁ k₂ non m2 F₁ F kz Find the second natural frequency (in rad/s) for the system shown below. Use scientific notation with 3 significant digits. Omit units. (eg. 2.03e0) Let m1 = 3, m2 = 3, k1 = 4, k2 = 6, and k3 = 8.
Question 3 Find the natural frequency (in rad/sec) of the system in In the figure below: Use: m1= 5 kg, k1 = 53 N/m, k2 65 N/m and k3 18 N/m Write your answer to FOUR significant figures. Don't write the units X1 X2 k1 k2 k3 W ww m1
The one-dimensional harmonic oscillator has the Lagrangian L = mx˙2 − kx2/2. Suppose you did not know the solution of the motion, but realized that the motion must be periodic and therefore could be described by a Fourier series of the form x(t) =∑j=0 aj cos jωt, (taking t = 0 at a turning point) where ω is the (unknown) angular frequency of the motion. This representation for x(t) defines many_parameter path for the system point in configuration space. Consider the action integral I for two points t1 and t2 separated by the period T = 2π/ω. Show that with this form for the system path, I is an extremum for nonvanishing x only if aj = 0, for j ≠ 1, and only if ω2 = k/m.

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Theory and Design for Mechanical Measurements

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