Part of JWAVE-01 — Simple Harmonic Motion

SHM Overview

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Simple Harmonic Motion is the foundational oscillatory motion in physics, defined by the condition that acceleration is proportional to displacement and directed toward the equilibrium position: a=ω2xa = -\omega^2 x. This arises whenever a restoring force obeys Hooke's law F=kxF = -kx. The motion is completely described by three parameters: amplitude AA, angular frequency ω=k/m\omega = \sqrt{k/m}, and initial phase ϕ\phi.

The displacement follows x=Asin(ωt+ϕ)x = A\sin(\omega t + \phi), with velocity v=Aωcos(ωt+ϕ)v = A\omega\cos(\omega t + \phi) and acceleration a=Aω2sin(ωt+ϕ)a = -A\omega^2\sin(\omega t + \phi). The time period T=2π/ωT = 2\pi/\omega is independent of amplitude — a hallmark of SHM that distinguishes it from general oscillatory motion. Two canonical systems dominate JEE problems: the spring-mass system (T=2πm/kT = 2\pi\sqrt{m/k}, gravity-independent) and the simple pendulum (T=2πl/gT = 2\pi\sqrt{l/g}, mass-independent). Understanding SHM is essential because it appears across mechanics (springs, pendulums), waves (standing waves), electromagnetism (LC circuits), and even modern physics (vibrating atoms). The mathematical framework — sinusoidal functions, phase relationships, and energy conservation — forms the backbone of wave physics.

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