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The displacement of a particle executing simple harmonic motion is given by y=A0+Asinωt+Bcosωty = A_0 + A \sin \omega t + B \cos \omega t. Then the amplitude of its oscillation is given by:

A

A+BA + B

B

A0+A2+B2A_0 + \sqrt{A^2 + B^2}

C

A2+B2\sqrt{A^2 + B^2}

D

A02+(A+B)2\sqrt{A_0^2 + (A+B)^2}

Step-by-Step Solution

  1. Analyze the Equation: The given displacement equation is y=A0+Asinωt+Bcosωty = A_0 + A \sin \omega t + B \cos \omega t.
  2. Identify Components:
  • The term A0A_0 is a constant, representing the shift of the equilibrium position from the origin. It does not affect the amplitude of the oscillation.
  • The oscillating part consists of two simple harmonic motions: y1=Asinωty_1 = A \sin \omega t and y2=Bcosωty_2 = B \cos \omega t.
  1. Determine Phase Difference: We know that cosωt=sin(ωt+π2)\cos \omega t = \sin(\omega t + \frac{\pi}{2}). Therefore, the second wave leads the first by a phase angle of ϕ=π2\phi = \frac{\pi}{2}.
  2. Apply Superposition Principle: The resultant amplitude RR of two SHMs with amplitudes AA and BB and phase difference ϕ\phi is given by the formula : R=A2+B2+2ABcosϕR = \sqrt{A^2 + B^2 + 2AB \cos \phi}
  3. Calculate Amplitude: Substituting ϕ=π2\phi = \frac{\pi}{2}: R=A2+B2+2ABcos(90)R = \sqrt{A^2 + B^2 + 2AB \cos(90^\circ)} R=A2+B2+0R = \sqrt{A^2 + B^2 + 0} R=A2+B2R = \sqrt{A^2 + B^2}
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