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Torsional pendulum, modulus of rigidity

Short answer

Bar pendulum swings about horizontal axis under gravity; torsional pendulum twists about vertical wire with elastic torque. Motion is angular SHM: d²θ/dt² + (C/I)θ = 0. With C = πηr⁴/(2l) and T = 2π√(I/C), modulus of rigidity η = 8πl I/(r⁴ T²).

Differentiate between bar (compound) pendulum and torsional pendulum. Using a torsional pendulum, derive a relation for the modulus of rigidity of the metallic wire. (Show that the motion of a torsional pendulum is angular SHM.)

Difference between bar pendulum and torsional pendulum

Bar (compound) pendulumTorsional pendulum
Rigid body swings about a horizontal axisBody twists about a vertical wire
Restoring torque is due to gravity: −mgl sinθRestoring torque is due to elasticity of wire: −Cθ
T = 2π√((k² + l²)/gl)T = 2π√(I/C)
Depends on gIndependent of g
Small angles needed (sinθ ≈ θ)Twist must stay within elastic limit
Used to find gUsed to find η and moment of inertia I

Angular SHM of a torsional pendulum

A disc of moment of inertia I is hung from a wire of length l and radius r. Twist the disc by angle θ.

  1. Wire exerts restoring torque proportional to the twist: τ = −Cθ, where C = torsional constant (torque per unit twist).
  2. Newton's law for rotation: I d²θ/dt² = −Cθ.
  3. d²θ/dt² + (C/I) θ = 0, which is of the form of SHM, d²θ/dt² + ω²θ = 0, with ω = √(C/I).
  4. So the motion is angular SHM with period T = 2π√(I/C).

Modulus of rigidity

  1. Consider a thin cylindrical shell of radius x, thickness dx, length l. Twisting by θ shears its surface through angle φ = xθ/l.
  2. Shear stress = ηφ, force on the shell's cross-section = ηφ · 2πx dx, torque = force × x:
dτ = η (xθ/l)(2πx dx) x = (2πηθ/l) x³ dx
τ = (2πηθ/l) ∫₀ʳ x³ dx = πηr⁴ θ / 2l
  1. Compare with τ = Cθ: C = πηr⁴/2l.
  2. Substitute in T = 2π√(I/C): T² = 4π²I/C = 8π l I /(η r⁴).
η = 8π l I / (r⁴ T²)

Measure l, r, T and know I (e.g. I = ½MR² for a disc) to get η of the wire.

✓ Answer checked by Claude Opus 5.5 (high effort)

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