Chapter 13 Oscillations About Equilibrium 03/28/05 Dr. Jie Zou PHY 1151G Department of Physics 1 Outline n Oscillations n n Periodic motions n n Basic cause for oscillations Period and frequency Simple harmonic motions n n n 03/28/05 Classical example: A mass attached to a spring Position as a function of time for a simple harmonic motion Period of a mass on a spring Dr. Jie Zou PHY 1151G Department of Physics 2 Oscillations n n 03/28/05 Oscillations: When systems are displaced from equilibrium, it often results in oscillations back and forth from one side of the equilibrium position to the other. Basic cause of oscillations: When an object is displaced from a position of stable equilibrium it experiences a restoring force that is directed back toward the equilibrium position. Dr. Jie Zou PHY 1151G Department of Physics 3 Periodic Motion n n Periodic motion: A motion that repeats itself over and over is referred to as periodic motion. Definition of period, T : time required for one cycle (one oscillation) of a periodic motion. The trace of an n SI unit: second or s. electrocardiogram n Definition of frequency, f : the (ECG or EKG). number of oscillations per unit of time. f = 1/T. n 03/28/05 SI unit: per second = 1/s = Hz. Dr. Jie Zou PHY 1151G Department of Physics 4 Example: Periodic motion n If the processing speed of a personal computer is 1.80 GHz, how much time is required for one processing cycle? ν A tennis ball is hit back and forth between two players warming up for a match. If it takes 2.31 s for the ball to go from one player to the other, what are the period and frequency of the tennis ball’s motion? 03/28/05 Dr. Jie Zou PHY 1151G Department of Physics 5 Simple harmonic motion n n 03/28/05 A classical example of simple harmonic motion: The mass-spring system. Key feature of a massspring system: A spring exerts a restoring force that is proportional to the displacement from equilibrium, F = - kx. Dr. Jie Zou PHY 1151G Department of Physics 6 Position versus time for simple harmonic motion n Position versus time in simple harmonic motion: x = Acos 2π t T n n n 03/28/05 Here we suppose that the cart is released at t = 0 from rest at x = A . Amplitude, A : it represents the maximum displacement of the cart on either side of equilibrium. Period, T : the cart’s motion repeats with a period T. Dr. Jie Zou PHY 1151G Department of Physics 7 Example 13-1 n An air-track cart attached to a spring completes one oscillation every 2.4 s. At t = 0 the cart is released from rest at a distance of 0.10 m from its equilibrium position. What is the position of the cart at (a) 0.30 s, (b) 0.60 s, (c) 2.7 s, and (d) 3.0 s? 03/28/05 Dr. Jie Zou PHY 1151G Department of Physics 8 Period of a mass on a spring n m A horizontal spring: T = 2π k n Unstretched at their n n n 03/28/05 equilibrium position. Here m is the mass (kg), and k is the force constant of the spring (N/m), and T is the period (s). The period, T, increases with the mass and decreases with the spring’s force constant. The period, T, is independent of the amplitude, A . Dr. Jie Zou PHY 1151G Department of Physics 9 A vertical spring n n A vertical spring is in equilibrium at y=-y0. At this equilibrium position, the spring stretches by an amount y0 given by n n n 03/28/05 ky0 = mg or y0 = mg/k A mass on a vertical spring oscillates about the equilibrium point y = -y0. m The period is also T = 2π Dr. Jie Zou PHY 1151G Department of Physics k 10 Active-Example 13-2 ν ν 03/28/05 When a 0.420-kg mass is attached to a spring, it oscillates with a period of 0.350 s. If, instead, a different mass, m2, is attached to the same spring, it oscillates with a period of 0.700 s. Find (a) the force constant of the spring and (b) the mass m2. Real world physics: the relationship between the mass and period is used by NASA to measure the mass of astronauts in orbit - The Body Mass Measurement Device (BMMD) Dr. Jie Zou PHY 1151G Department of Physics 11 Homework #11 (03/28/05) n Chapter 13, Page 413, Problems: # 6, 8, 14, 27, 29. 03/28/05 Dr. Jie Zou PHY 1151G Department of Physics 12