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Question

In SHM, what is true about the particle’s acceleration when its kinetic energy is at its maximum?

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Explanation

**Damped oscillations** occur when resistive forces dissipate energy, amplitude decays exponentially as A(t) = A₀ e^(-b t/2m), b damping coefficient (kg/s), frequency slightly reduced ω' = √(ω₀² - (b/2m)²). Damping arises from friction or viscosity, energy loss per cycle proportional to velocity squared, motion eventually stops. Kinetic energy is maximum at the mean position ( x = 0 ), where acceleration ( a = -ω² x ) is zero, as the restoring force vanishes. Applying x = A cos(ωt + φ), v = -ωA sin(ωt + φ), a = -ω²x and E = ½kA² = ½mω²A², result It is zero follows, reflecting SHM dependence on

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