Copyright © 2009 Pearson Addison-Wesley 4.5-1 4 Graphs of the Circular Functions.

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Copyright © 2009 Pearson Addison-Wesley Graphs of the Circular Functions

Copyright © 2009 Pearson Addison-Wesley Graphs of the Sine and Cosine Functions 4.2 Translations of the Graphs of the Sine and Cosine Functions 4.3 Graphs of the Tangent and Cotangent Functions 4.4 Graphs of the Secant and Cosecant Functions 4.5Harmonic Motion 4 Graphs of the Circular Functions

Copyright © 2009 Pearson Addison-Wesley Harmonic Motion 4.5 Simple Harmonic Motion ▪ Damped Oscillatory Motion

Copyright © 2009 Pearson Addison-Wesley Simple Harmonic Motion The position of a point oscillating about an equilibrium position at time t is called simple harmonic motion.

Copyright © 2009 Pearson Addison-Wesley Simple Harmonic Motion The position of a point oscillating about an equilibrium position at time t is modeled by either where a and are constants, with The amplitude of the motion is |a|, the period is and the frequency is oscillations per time unit.

Copyright © 2009 Pearson Addison-Wesley Example 1 MODELING THE MOTION OF A SPRING Suppose that an object is attached to a coiled spring. It is pulled down a distance of 5 in. from its equilibrium position and then released. The time for one complete oscillation is 4 seconds. (a)Give an equation that models the position of the object at time t. When the object is released at t = 0, the object is at distance −4 in. from equilibrium.

Copyright © 2009 Pearson Addison-Wesley Example 1 MODELING THE MOTION OF A SPRING (continued) Since the time needed to complete one oscillation is 4 sec, P = 4, so The motion is modeled by

Copyright © 2009 Pearson Addison-Wesley Example 1 MODELING THE MOTION OF A SPRING (continued) (b)Determine the position at t = 1.5 sec. At t = 1.5 seconds, the object is about 3.54 in. above the equilibrium position. (c)Find the frequency. The frequency is the reciprocal of the period.

Copyright © 2009 Pearson Addison-Wesley Example 2 ANALYZING HARMONIC MOTION Suppose that an object oscillates according to the model s(t) = 8 sin 3t, where t is in seconds and s(t) is in feet. Analyze the motion. a = 8, so the object oscillates 8 feet in either direction from the starting point. The motion is harmonic because the model is of the form = time (in seconds) for one complete oscillation

Copyright © 2009 Pearson Addison-Wesley Damped Oscillatory Motion Most oscillatory motions are damped by the effect of friction which causes the amplitude of the motion to diminish gradually until the weight comes to rest. This motion can be modeled by

Copyright © 2009 Pearson Addison-Wesley Damped Oscillatory Motion