An Angular Simple Harmonic Oscillator — Question 9

Section 15-4 · Physics pages 2308–2309

Question 9 A bias torque and a torque gradient leave different signatures A torsion balance of known inertia I and elastic constant κ experiences an additional torque τe = τ0 + cθ near its operating point. The total torque is τ0 −(κ −c)θ, with κ > c. θ τ A constant torque shifts the zero; the torque slope sets the oscillation frequency. (a) Find the equilibrium angle and small-oscillation frequency. (b) A test doubles the equilibrium angle while leaving the period unchanged. Under this linear model with fixed I and κ, which parameter changed? What additional measurement would a changed period provide?
Show solutionHide solution
Question 9 - Solution A bias torque and a torque gradient leave different signatures θ τ (a) Derivation and calculation I ¨θ = τ0 + cθ −κθ = τ0 −(κ −c)θ. θe = τ0 κ −c , Ω2 = κ −c I , κ > c. q = θ −θe ⇒I ¨q + (κ −c)q = 0. (b) Result and interpretation For fixed I, κ, an unchanged period implies unchanged c: T = 2π √ I/(κ −c), θ′ e = 2θe ⇒τ ′ 0 = 2τ0 . c = κ −4π2I T 2 , τ0 = 4π2I T 2 θe . Physical check The equilibrium measures the torque offset relative to stiffness; the period independently determines the torque slope.

Question 9

A bias torque and a torque gradient leave different signatures

A torsion balance of known inertia II and elastic constant κ\kappa experiences an additional torque τe=τ0+cθ\tau_e=\tau_0+c\theta near its operating point. The total torque is τ0−(κ−c)θ\tau_0-(\kappa-c)\theta, with κ>c\kappa>c.

Diagram shown in the original SVG worksheet.

  1. Find the equilibrium angle and small-oscillation frequency.

  2. A test doubles the equilibrium angle while leaving the period unchanged. Under this linear model with fixed II and κ\kappa, which parameter changed? What additional measurement would a changed period provide?

Question 9 - Solution

A bias torque and a torque gradient leave different signatures

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Iθ̈=τ0+cθ−κθ=τ0−(κ−c)θ.I\ddot\theta=\tau_0+c\theta-\kappa\theta=\tau_0-(\kappa-c)\theta.θe=τ0κ−c,Ω2=κ−cI,κ>c.\boxed{\theta_e=\frac{\tau_0}{\kappa-c}},\qquad\boxed{\Omega^2=\frac{\kappa-c}{I}},\quad\kappa>c.q=θ−θe⇒Iq̈+(κ−c)q=0.q=\theta-\theta_e\Rightarrow I\ddot q+(\kappa-c)q=0.

(b) Result and interpretation

For fixed I,κI,\kappa, an unchanged period implies unchanged cc:T=2πI/(κ−c),θe′=2θe⇒τ0′=2τ0.T=2\pi\sqrt{I/(\kappa-c)},\quad\theta_e^{\prime}=2\theta_e\Rightarrow\boxed{\tau_0^{\prime}=2\tau_0}.c=κ−4π2IT2,τ0=4π2IT2θe.\boxed{c=\kappa-\frac{4\pi^2I}{T^2}},\qquad\boxed{\tau_0=\frac{4\pi^2I}{T^2}\theta_e}.

Physical check

The equilibrium measures the torque offset relative to stiffness; the period independently determines the torque slope.