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NEET PHYSICSEasy

The phase difference between displacement and acceleration of a particle in a simple harmonic motion is:

A

\frac{3\pi}{2} \text{ rad}

B

\frac{\pi}{2} \text{ rad}

C

zero

D

\pi \text{ rad}

Step-by-Step Solution

  1. Displacement Equation: Let the displacement of a particle executing Simple Harmonic Motion (SHM) be given by: x=Asin(ωt)x = A \sin(\omega t) where AA is the amplitude and ω\omega is the angular frequency.
  2. Velocity Equation: Velocity vv is the time derivative of displacement: v=dxdt=Aωcos(ωt)=Aωsin(ωt+π2)v = \frac{dx}{dt} = A\omega \cos(\omega t) = A\omega \sin(\omega t + \frac{\pi}{2}) (Phase difference between displacement and velocity is π/2\pi/2).
  3. Acceleration Equation: Acceleration aa is the time derivative of velocity: a=dvdt=ddt[Aωcos(ωt)]=Aω2sin(ωt)a = \frac{dv}{dt} = \frac{d}{dt}[A\omega \cos(\omega t)] = -A\omega^2 \sin(\omega t) Using the trigonometric identity sinθ=sin(θ+π)-\sin \theta = \sin(\theta + \pi), we can write: a=Aω2sin(ωt+π)a = A\omega^2 \sin(\omega t + \pi)
  4. Phase Difference: Comparing the phase of displacement (ωt)(\omega t) and acceleration (ωt+π)(\omega t + \pi), the difference is: Δϕ=(ωt+π)(ωt)=π rad\Delta \phi = (\omega t + \pi) - (\omega t) = \pi \text{ rad}
  5. Conclusion: The acceleration is always in opposite phase (180180^\circ or π\pi radians) to the displacement .
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