Simple Harmonic Motion - Experiment 1 | PHYSICS 289, Lab Reports of Physics

Download Simple Harmonic Motion - Experiment 1 | PHYSICS 289 and more Lab Reports Physics in PDF only on Docsity! PHYSICS 289 Experiment 1 Fall 2004 SIMPLE HARMONIC MOTION − I (A short report is required for this lab: worksheet, graphs and answers to all the questions.) Simple Harmonic Motion (SHM) is a special type of periodic motion that is described by a single sine/cosine function with a unique frequency. It occurs whenever there is a linear restoring force, i.e., when the magnitude of the restoring force is directly proportional to the displacement of the system from equilibrium. In this case, the magnitude of the acceleration a will also be proportional to the displacement x from equilibrium, but they are always opposite in direction. Let C be the proportionality constant between acceleration and displacement, i.e., a = −Cx. Then it is easy to see that the solution for x is simply Acos(ωt+φ) where A is the amplitude of the oscillation and ω the angular frequency, with C = ω2. The period of the motion, T, is related to C by the equation CfT /2/2/1 πωπ === (1) For many systems this is strictly true only for small amplitude oscillations. For a mass m attached to a spring moving in one dimension without friction, we have a = F/m, where F is the spring force. A hookean spring obeys F = − kx, where k is called the spring constant. So a = − (k/m)x, i.e., C = k/m..Hence k/m = C = 4π2/T2 (2) In this experiment we will use masses and springs to study simple harmonic motion. Please refer to your text or lecture notes the full derivation of the above equations. A. Spring Constant from Hooke’s Law (5 points) We want to first find out if springs obey Hooke’s law: F = − kx. This can be done by measuring the extension of a spring x as a function of the force applied to the spring. However, we shall use two stretched springs on opposite sides of the mass instead of just one spring on one side. The two spring may be considered identical. Attach a spring between each end of the air track and the cart. Turn on the air and observe the equilibrium position of the mass. Since the air track is nearly frictionless, even the tiniest disturbance will set the cart into oscillation. This should not prevent you from obtaining the equilibrium position. (Why?) Turn off the air so that the mass stays still. Attach a fine string to the one end of the cart, and pass it over the pulley. Suspend a mass at the other end of the string. Its weight is the applied force F. Turn on the air again and find the new equilibrium position of the cart due to this force. Repeat this for several masses, recording the mass and the position of the cart, as determined from the attached pin. Also record the uncertainty in your measurement of the position each time. Note that if the air tracks have air pulleys, a light weight ribbon (a recording tape) is used in place of the string. Make a plot of your mass vs. position data. In equilibrium the magnitude of the force exerted by the stretched springs is equal to the suspended weight mg, so a hookean spring would obey. mg = F = − kx , i.e., the graph of m vs. x should be linear and the slope is given by −k/g. Draw the “best” straight line through the data points, and measure the slope of the line. From the slope calculate the effective spring constant k for the two springs combined. From the uncertainty in the slope determine the uncertainty in the spring constant. Part A Questions 1. Is your data in the graph of mass as a function of position consistent with a straight line? 2. What is your value and uncertainty for the spring constant k for two springs? B. Spring Constant from Period (5 points) Gently remove one spring from the apparatus in part (A) and gently hang it on the horizontal small “finger” of the vertical stand. Position the stand such that the spring hang over the edge of the lab bench. (The key word here is GENTLE because the springs are very delicate and they are IRREPLACEABLE.) Suspend different masses M on the spring and measure the period T for small vertical oscillations with the stop clock. In order to not over-stretch the spring, keep the mass M under 25 g, make sure the amplitude of oscillation is small and vertical. Do not let the spring swing like a pendulum. The period of oscillation is given by Eq. (2), which can be rewritten as M = (k/4π2)T2 Thus, the graph of M versus T2 is expected to have a slope equal to k/4π2. Measure the period of oscillation for several cart masses M, and plot M as a function of T2. Draw the “best” straight line through the data. Determine the slope of the line (k/4π2). Find k and its uncertainty. Part B Questions: 1. To measure T, you might let the mass go up and down 10 cycles. Although it is natural to use the top or bottom positions to mark the beginning and end, it is actually more accurate to use the midpoint. Why? 2. What is the value and uncertainty for the spring constant, as determined from the period?