Michelson's Interferometer — Question 2

Section 35-7 · Physics pages 5834–5835

Question 2 Evacuating a cell measures the gas refractivity A rigid gas cell of length ℓ= 0.100 m is placed in one Michelson arm and traversed twice. Removing the gas shifts the phase through 84 complete cycles at vacuum wavelength 632.8 nm. The windows, geometry, and the other arm remain unchanged; the final cell index is 1. M1 M2 detector input gas cell ℓ Schematic; labels, not drawing lengths, specify the data. (a) Infer the initial gas index. (b) Find the signed optical-path change on evacuation and the mirror motion needed in the cell arm to restore the initial optical path.
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Question 2 - Solution Evacuating a cell measures the gas refractivity M1 M2 detector input gas cell ℓ (a) Method and calculation Nλ0 = 2ℓ(n −1) =⇒n = 1 + 84(632.8 × 10−9) 0.200 = 1.000265776 . ∆Levacuation = −2ℓ(n −1) = −53.1552 µm . (b) Interpretation and further calculation ∆Levacuation + 2∆x = 0. ∆x = +26.5776 µm away from the beam splitter . Physical check The fixed windows cancel from the before-and-after difference, while the gas contribution doubles because of the return pass.

Question 2

Evacuating a cell measures the gas refractivity

A rigid gas cell of length ℓ=0.100m\ell=0.100\,\mathrm m is placed in one Michelson arm and traversed twice. Removing the gas shifts the phase through 84 complete cycles at vacuum wavelength 632.8nm632.8\,\mathrm{nm}. The windows, geometry, and the other arm remain unchanged; the final cell index is 1.

Diagram shown in the original SVG worksheet.

  1. Infer the initial gas index.

  2. Find the signed optical-path change on evacuation and the mirror motion needed in the cell arm to restore the initial optical path.

Question 2 - Solution

Evacuating a cell measures the gas refractivity

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Nλ0=2ℓ(n−1)⇒n=1+84(632.8×10−9)0.200=1.000265776.N\lambda_0=2\ell(n-1)\Longrightarrow\boxed{n=1+\frac{84(632.8\times10^{-9})}{0.200}=1.000265776}.Δℒevacuation=−2ℓ(n−1)=−53.1552μm.\boxed{\Delta\mathcal L_{\mathrm{evacuation}}=-2\ell(n-1)=-53.1552\,\mu\mathrm m}.

(b) Interpretation and further calculation

Δℒevacuation+2Δx=0.\Delta\mathcal L_{\mathrm{evacuation}}+2\Delta x=0.Δx=+26.5776μmaway from the beam splitter.\boxed{\Delta x=+26.5776\,\mu\mathrm m\ \text{away from the beam splitter}}.

Physical check

The fixed windows cancel from the before-and-after difference, while the gas contribution doubles because of the return pass.