Bridge swing lesson
The Tacoma Narrows Bridge collapse in 1940 wasn’t from high winds alone—it was wind energy locking onto the bridge’s torsional natural frequency, feeding the oscillation every cycle.
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Resonance is a universal phenomenon that links physics, engineering, and everyday life. A playground swing, a tuning fork, and a tuned radio all rely on the same mathematics of oscillation. Whenever energy can slosh back and forth between two forms—kinetic vs. potential, electric vs. magnetic—the system has a natural frequency at which it prefers to vibrate. At that frequency, even small inputs can build to large responses. Understanding resonance is essential for designing safe mechanical systems, efficient circuits, and everything from skyscrapers to smartphone antennas.
In mechanics, the simplest model is the mass–spring–damper. With mass m, stiffness k, and viscous damping c, the natural angular frequency is ωₙ = √(k/m), corresponding to fₙ = ωₙ/(2π). The damping ratio ζ = c / (2√(km)) determines whether the system is underdamped (oscillatory), critically damped (fastest non-oscillatory return), or overdamped (slow return). The quality factor Q = 1/(2ζ) measures sharpness: high-Q systems ring for many cycles, low-Q systems die out quickly. Engineers also track the decay constant α = c/(2m) and the damped natural frequency ωd = ωₙ√(1 − ζ²), which is slightly less than the undamped value.
Electrical engineers see the same formulas in RLC circuits. With inductance L, capacitance C, and resistance R, the undamped resonance is ω₀ = 1/√(LC), f₀ = ω₀/(2π). In a series RLC, damping arises from R/(2L), giving ζ = (R/2)√(C/L) and Q = (1/R)√(L/C). In a parallel RLC, the roles invert: ζ = (1/2R)√(L/C) and Q = R√(C/L). The bandwidth is approximately Δf = f₀ / Q, a key spec for filters, amplifiers, and radio receivers.
Units and sanity checks: Use SI: m in kg, k in N/m, c in N·s/m, L in henries, C in farads, R in ohms. Increasing stiffness k or reducing mass m raises frequency. In circuits, increasing resistance R lowers Q for a series RLC but raises Q for a parallel RLC. These cross-checks help spot unit mistakes. In both domains, the resonance story is the same: energy storage, dissipation, and feedback combine to create rich dynamics that can be harnessed—or avoided.
The Tacoma Narrows Bridge collapse in 1940 wasn’t from high winds alone—it was wind energy locking onto the bridge’s torsional natural frequency, feeding the oscillation every cycle.
Super-tall buildings hide hundreds of tons of tuned mass dampers—giant pendulums or water tanks that are deliberately tuned to the tower’s sway frequency to cancel motion.
The tiny tuning-fork crystal inside a quartz watch resonates at 32,768 Hz with a Q in the tens of thousands, so it can count seconds by simply dividing a super-stable tone.
An RLC circuit tuned to a station is literally a frequency-selective “net.” Only currents near its natural frequency build up, letting your receiver ignore everything else on the dial.
Atomic force microscopes vibrate a cantilever at resonance and watch its frequency shift by a few Hz when it feels atomic forces—basically using resonance as a force magnifier.