This preview shows pages 1–3. Sign up to view the full content.
This preview has intentionally blurred sections. Sign up to view the full version.View Full Document
Unformatted text preview: Chapter 13 Vibrations and Waves This chapter covers oscillatory motion and wave propagation. Hookes Law The behavior of many springs approximates Hookes Law : F = -kx x is the amount by which the spring is stretched or compressed from its equilibrium position and F is the restoring force exerted by the spring. The negative sign means that the force is opposite to the direction of the stretch or compression. k is the force constant of the spring (N/m) and is a measure of the spring stiffness. Example : A mass, m = 500 g, is hung from the end of a spring attached to a support. In its equilibrium position, the mass stretches the spring by 5 cm. What is the force constant of the spring? k = F/x = mg/x = (0.5 kg)(9.8 m/s 2 )/(0.05 m) = 98/m Elastic Potential Energy In a previous chapter, it was shown that the potential energy associated with the stretch or compression of a Hookes law spring is U = kx 2 In the above example, the potential energy stored in the spring is U = (98/m)(0.1 m) 2 = 0.49 J Spring oscillation Assume that one end of a horizontal spring is anchored to a support and a mass is attached to the other end. The mass is pulled a distance x = A from its equilibrium position and allowed to oscillate back and forth on a frictionless surface. The position of the mass will be given as a function of time is given by ) 2 cos( ft A x = where the frequency of oscillation is given by m k f 2 1 = 1 The period T of oscillation is 1/f, so k m T 2 = The oscillation of a Hookes law spring is called Simple Harmonic Motion (SHM)....
View Full Document
- Spring '09