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A rigid body (disc/rod) suspended by a thin wire. Small twist → restoring torque by wire → angular SHM.
τ = −C θ (C: torsion constant), I d²θ/dt² + C θ = 0, period T = 2π√(I/C).
Standing wave formed by superposition of two opposite travelling waves of same f, A.
Perceived sensation is proportional to log of stimulus intensity:
S = k log(I/I₀) (I₀: threshold).
Apparent frequency changes due to relative motion of source/observer.
f' = f \frac{v \pm v_o}{v \mp v_s} (signs: approach ↑, recede ↓); v is speed of sound.
Ferromagnets (Ni/Fe/Co) change length in a magnetic field. A rod in a coil with high-frequency AC experiences rapid elongation/contraction → emits ultrasonic waves.
Resonance when drive f matches rod’s natural longitudinal mode.
Two bonded metals with different thermal expansion. Heating bends strip toward lower-expansion metal.
Used in thermostats, circuit breakers, dial thermometers.
Rate of heat flow per unit area for unit temperature gradient (normal to area).
Q̇ = −k A (dT/dx); SI unit: W m⁻¹ K⁻¹.
White has high reflectance & low absorptance → less solar heat gain → cooler building & reduced AC load.
Fe–Ni alloy (~64% Fe, ~36% Ni) with very low CTE near room temperature → minimal expansion; used in precision instruments, clock pendulums, gauge blocks.
Temperature difference between junctions of two dissimilar conductors produces an EMF → continuous current in closed circuit. Basis of thermocouples.
Seebeck coefficient: S = ΔV/ΔT.
Given: A = 90×10⁻⁴ m², d = 1.2×10⁻³ m, ΔT = 20 K, k = 0.04 W m⁻¹ K⁻¹, Δt = 1 s.
Fourier: Q = kA(ΔT/d)Δt = 0.04×0.009×(20/1.2×10⁻³)×1 = 6 J.
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