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Simple Harmonic Motion. Ideal Springs F Applied =kx k = spring constant x = displacement of the spring +x  pulled displacement -x  compressed displacement.

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Presentation on theme: "Simple Harmonic Motion. Ideal Springs F Applied =kx k = spring constant x = displacement of the spring +x  pulled displacement -x  compressed displacement."— Presentation transcript:

1 Simple Harmonic Motion

2 Ideal Springs F Applied =kx k = spring constant x = displacement of the spring +x  pulled displacement -x  compressed displacement

3 Hooke’s Law Describes the restoring force of an ideal spring F = -kx Negative sign indicates that this force always goes in the opposite direction of displacement

4 Hooke’s Law This type of restoring force will create a back and forth or up and down type of motion This type of friction-free motion is designated simple harmonic motion The maximum excursion from equilibrium is the amplitude  A

5 Period Mass-Spring Complex T = 2π√(m/k) Pendulum T = 2π√(L/g)

6 The Reference Circle Simply  a ball moving in uniform circular motion The shadow cast by the ball on a film creates the same type of sinusoidal pattern It makes another model of simple harmonic motion

7 Displacement x = A cos  = A cos  t  = 2  / T f = 1 / T  = 2  f (  is often called angular frequency)

8 Velocity & Acceleration v = -A  sin  = -A  sin  t v max = A  a = -A  2 cos  = -  2 cos  t a max = A  2

9 Frequency of Vibration  = (k / m) 1/2  must be in radians per second k  spring constant m  mass

10 Energy & Simple Harmonic Motion W elastic = ½ kx o 2 – ½ kx f 2 PE elastic = ½ kx 2 E Total = ½ mv 2 + ½  2 + mgh + ½ kx 2


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