Springs, pendulums, wave properties, and sound
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Simple Harmonic Motion (SHM) is the repetitive, oscillatory motion exhibited by systems where the restoring force is directly proportional to the displacement from equilibrium and oppositely directed. This unit focuses on two canonical examples: a mass attached to an ideal spring and a simple pendulum swinging through small angles. For the spring, Hooke's Law (F = -kx) provides the linear restoring force that drives the oscillation. The resulting motion is sinusoidal, described by x(t) = A cos(ωt + φ), where A is the amplitude, ω is the angular frequency, and φ is the phase constant determined by initial conditions. A crucial insight is that the period of a spring-mass system depends on the mass and the spring constant but is completely independent of the amplitude. This isochronism means a mass oscillating with a large amplitude takes exactly the same time per cycle as one with a small amplitude, assuming small enough displacement that the spring remains ideal. For the simple pendulum, the restoring force is a component of gravity, and the period T = 2π√(L/g) depends only on length and gravitational acceleration—not on the mass of the bob. However, this formula is only valid for small angles (typically θ < 15°) where sinθ ≈ θ in radians. Energy analysis in SHM reveals a continuous exchange between kinetic and potential energy. At maximum displacement, all energy is potential; at equilibrium, all energy is kinetic. The total mechanical energy E = ½kA² is constant if damping is negligible. The AP Exam frequently tests your ability to sketch x-t, v-t, and a-t graphs, to identify points of maximum speed or acceleration, and to use energy conservation to find speed at any position. You will also encounter the concepts of frequency, period, and angular frequency, and you must keep them distinct: ω = 2πf = 2π/T. Resonance—the dramatic increase in amplitude when a system is driven at its natural frequency—appears conceptually, explaining phenomena from bridge collapses to molecular vibrations.
F = -k*x (Hooke's Law)a = -(k/m)*xx(t) = A*cos(ω*t + φ)ω = sqrt(k/m) (spring)T = 2π*sqrt(m/k) (spring)T = 2π*sqrt(L/g) (simple pendulum, small angles)E = ½*k*A² (total mechanical energy)v_max = A*ωAnswer each question one at a time. Click an option to select your answer.
Watch these unit review videos directly on our site.
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Quick reference for Simple Harmonic Motion. Print this out and review before the exam!
F = -k*xx(t) = A*cos(ω*t + φ)ω = sqrt(k/m); T = 2π*sqrt(m/k) (spring)T = 2π*sqrt(L/g) (simple pendulum, small angle)E = ½*k*A² = ½*k*x² + ½*m*v²v_max = A*ω; a_max = A*ω²ω = 2π*f = 2π/Tsqrt(9.8/2.5) requires parentheses around the fraction.y1 = A*cos(ω*x) to visualize motion and find intercepts.