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Transcript
Oscillations and Waves Energy Changes During Simple Harmonic Motion Energy in SHM energy velocity Energy-time graphs KE PE Total Note: For a spring-mass system: KE = ½ mv2 KE is zero when v = 0 PE = ½ kx2 PE is zero when x = 0 (i.e. at vmax) Energy–displacement graphs energy KE PE Total -xo displacement +xo Note: For a spring-mass system: KE = ½ mv2 KE is zero when v = 0 (i.e. at xo) PE = ½ kx2 PE is zero when x = 0 Kinetic energy in SHM We know that the velocity at any time is given by… v = ω √ (xo2 – x2) So if Ek = ½ mv2 then kinetic energy at an instant is given by… Ek = ½ mω2 (xo2 – x2) Potential energy in SHM If a = - ω2 x then the average force applied trying to pull the object back to the equilibrium position as it moves away from the equilibrium position is… F = - ½ mω2x Work done by this force must equal the PE it gains (e.g in the springs being stretched). Thus.. Ep = ½ mω2x2 Total Energy in SHM Clearly if we add the formulae for KE and PE in SHM we arrive at a formula for total energy in SHM: ET = ½ mω2xo2 Summary: Ek = ½ mω2 (xo2 – x2) Ep = ½ mω2x2 ET = ½ mω2xo2 Subtitle Text Subtitle Text Subtitle Text Subtitle Text Subtitle Text Subtitle Text Subtitle Text Subtitle Text Subtitle Text Subtitle Text Subtitle Text
