Michelson's Interferometer — Question 8

Section 35-7 · Physics pages 5846–5847

Question 8 Thermal expansion of one arm produces a measurable phase drift One Michelson mirror is mounted at the end of a support of length L = 0.150 m and linear expansion coefficient α = 23.0 × 10−6 K−1. The beam splitter end is fixed, the other arm is thermally stable, and light travels in vacuum at λ = 600 nm. The support warms uniformly by 0.0200 K. M1 M2 detector input support: L, α Schematic; labels, not drawing lengths, specify the data. (a) Calculate the mirror motion, phase drift, and number of fringe cycles. (b) Find the temperature increase required for one complete fringe cycle.
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Question 8 - Solution Thermal expansion of one arm produces a measurable phase drift M1 M2 detector input support: L, α (a) Method and calculation ∆x = αL∆T =⇒∆x = 69.0 nm . ∆N = 2∆x/λ = 0.230, ∆ϕ = 2π∆N = 0.460π rad . (b) Interpretation and further calculation 2αL∆T1 = λ. ∆T1 = λ/(2αL) = 0.0869565 K . Physical check The calculation isolates mechanical expansion. In an air-filled instrument, temperature-dependent refractive index could add another optical-path contribution.

Question 8

Thermal expansion of one arm produces a measurable phase drift

One Michelson mirror is mounted at the end of a support of length L=0.150mL=0.150\,\mathrm m and linear expansion coefficient α=23.0×10−6K−1\alpha=23.0\times10^{-6}\,\mathrm{K^{-1}}. The beam splitter end is fixed, the other arm is thermally stable, and light travels in vacuum at λ=600nm\lambda=600\,\mathrm{nm}. The support warms uniformly by 0.0200K0.0200\,\mathrm K.

Diagram shown in the original SVG worksheet.

  1. Calculate the mirror motion, phase drift, and number of fringe cycles.

  2. Find the temperature increase required for one complete fringe cycle.

Question 8 - Solution

Thermal expansion of one arm produces a measurable phase drift

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Δx=αLΔT⇒Δx=69.0nm.\Delta x=\alpha L\Delta T\Longrightarrow\boxed{\Delta x=69.0\,\mathrm{nm}}.ΔN=2Δx/λ=0.230,Δϕ=2πΔN=0.460πrad.\boxed{\Delta N=2\Delta x/\lambda=0.230,\quad\Delta\phi=2\pi\Delta N=0.460\pi\ \mathrm{rad}}.

(b) Interpretation and further calculation

2αLΔT1=λ.2\alpha L\Delta T_1=\lambda.ΔT1=λ/(2αL)=0.0869565K.\boxed{\Delta T_1=\lambda/(2\alpha L)=0.0869565\,\mathrm K}.

Physical check

The calculation isolates mechanical expansion. In an air-filled instrument, temperature-dependent refractive index could add another optical-path contribution.