Simple Harmonic Motion and Uniform Circular Motion — Question 7

Section 15-6 · Physics pages 2344–2345

Question 7 A quarter-period sample supplies the missing quadrature A harmonic oscillator of known period T is sampled at t and t + T/4. The readings are p = .030 m and q = −.040 m. Let ω = 2π/T. x y p −q Quarter-period sampling obtains the two quadratures of a harmonic state. (a) Find its amplitude and velocity at the first sample without fitting a full sinusoid. (b) Derive the corresponding amplitude formula for samples separated by phase ∆instead. Why does the reconstruction fail at an integer half-period separation?
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Question 7 - Solution A quarter-period sample supplies the missing quadrature x y p −q (a) Derivation and calculation p = A cos ψ, q = A cos(ψ + π/2) = −A sin ψ. A = √ p2 + q2 = √ .0302 + .0402 = .0500 m . v(t) = −Aω sin ψ = ωq = −.0400ω m/s . (b) Result and interpretation For a general sample phase separation ∆, q = p cos ∆−A sin ψ sin ∆. A sin ψ = p cos ∆−q sin ∆ ⇒A2 = p2 + (p cos ∆−q sin ∆ )2 . ∆= nπ ⇒q = (−1)np. At these separations the second sample supplies no independent quadrature; small | sin ∆| amplifies errors. Physical check At ∆= π/2, the general result reduces exactly to A2 = p2 + q2.

Question 7

A quarter-period sample supplies the missing quadrature

A harmonic oscillator of known period TT is sampled at tt and t+T/4t+T/4. The readings are p=.030mp=.030\,\mathrm{m} and q=−.040mq=-.040\,\mathrm{m}. Let ω=2π/T\omega=2\pi/T.

Diagram shown in the original SVG worksheet.

  1. Find its amplitude and velocity at the first sample without fitting a full sinusoid.

  2. Derive the corresponding amplitude formula for samples separated by phase Δ\Delta instead. Why does the reconstruction fail at an integer half-period separation?

Question 7 - Solution

A quarter-period sample supplies the missing quadrature

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

p=Acos⁡ψ,q=Acos⁡(ψ+π/2)=−Asin⁡ψ.p=A\cos\psi,\quad q=A\cos(\psi+\pi/2)=-A\sin\psi.A=p2+q2=.0302+.0402=.0500m.\boxed{A=\sqrt{p^2+q^2}=\sqrt{.030^2+.040^2}=.0500\,\mathrm m}.v(t)=−Aωsin⁡ψ=ωq=−.0400ωm/s.\boxed{v(t)=-A\omega\sin\psi=\omega q=-.0400\omega\,\mathrm{m/s}}.

(b) Result and interpretation

For a general sample phase separation Δ\Delta,q=pcos⁡Δ−Asin⁡ψsin⁡Δ.q=p\cos\Delta-A\sin\psi\sin\Delta.Asin⁡ψ=pcos⁡Δ−qsin⁡Δ⇒A2=p2+(pcos⁡Δ−qsin⁡Δ)2.A\sin\psi=\frac{p\cos\Delta-q}{\sin\Delta}\Rightarrow\boxed{A^2=p^2+\left(\frac{p\cos\Delta-q}{\sin\Delta}\right)^2}.Δ=nπ⇒q=(−1)np.\Delta=n\pi\Rightarrow q=(-1)^np.At these separations the second sample supplies no independent quadrature; small |sin⁡Δ||\sin\Delta| amplifies errors.

Physical check

At Δ=π/2\Delta=\pi/2, the general result reduces exactly to A2=p2+q2A^2=p^2+q^2.