Recall from last lecture: Simple Harmonic Motion

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Kinematics of Circular MotionTime for one complete revolution:

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Kinematics of Circular MotionLet's write : F c = F , T = Tx-components:y-components:c( F )cx⇒Fc⇒F( F )c= Tx+ mgx= Tsinα+ 0= Tsinα= T+ mg⇒ 0 = T cosα− mgmg⇒ T =cosαsubstituting value for T abovecyyyNewton's 2 nd lawbut:

Kinematics of Circular MotionTime for one complete revolution:

Page 2 and 3: Kinematic of Simple Harmonic Motion
Page 6 and 7: Uniform circular motionDefinition:
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Recall from last lecture: Simple Harmonic Motion

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