Michelson's Interferometer — Question 7

Section 35-7 · Physics pages 5844–5845

Question 7 A plate insertion can be compensated by shortening one arm A plane-parallel plate of thickness t = 10.0 µm and index n = 1.50 is inserted normally into one initially balanced Michelson arm in air. It replaces air on both passes. Let the source wavelength be 600 nm and define positive mirror motion away from the beam splitter. M1 M2 detector input n, t Schematic; labels, not drawing lengths, specify the data. (a) Find the additional optical path and number of phase cycles caused by the insertion. (b) Find the signed mirror motion in that arm that restores exact optical-path equality, and explain why a single-color bright fringe is not sufficient to prove equality.
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Question 7 - Solution A plate insertion can be compensated by shortening one arm M1 M2 detector input n, t (a) Method and calculation ∆L = 2(n −1)t = 10.0 µm . ∆N = ∆L/λ = 50/3 = 16.6667 cycles . (b) Interpretation and further calculation 2∆x + 2(n −1)t = 0 =⇒∆x = −(n −1)t = −5.00 µm . δ = 2πm ⇐⇒∆L = mλ =⇒brightness alone allows integer-path ambiguity . Physical check Exact compensation means zero path difference, not merely an integer number of monochromatic wavelengths.

Question 7

A plate insertion can be compensated by shortening one arm

A plane-parallel plate of thickness t=10.0μmt=10.0\,\mu\mathrm m and index n=1.50n=1.50 is inserted normally into one initially balanced Michelson arm in air. It replaces air on both passes. Let the source wavelength be 600nm600\,\mathrm{nm} and define positive mirror motion away from the beam splitter.

Diagram shown in the original SVG worksheet.

  1. Find the additional optical path and number of phase cycles caused by the insertion.

  2. Find the signed mirror motion in that arm that restores exact optical-path equality, and explain why a single-color bright fringe is not sufficient to prove equality.

Question 7 - Solution

A plate insertion can be compensated by shortening one arm

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Δℒ=2(n−1)t=10.0μm.\Delta\mathcal L=2(n-1)t=\boxed{10.0\,\mu\mathrm m}.ΔN=Δℒ/λ=50/3=16.6667cycles.\boxed{\Delta N=\Delta\mathcal L/\lambda=50/3=16.6667\ \text{cycles}}.

(b) Interpretation and further calculation

2Δx+2(n−1)t=0⇒Δx=−(n−1)t=−5.00μm.2\Delta x+2(n-1)t=0\Longrightarrow\boxed{\Delta x=-(n-1)t=-5.00\,\mu\mathrm m}.δ=2πm⇔Δℒ=mλ⇒brightness alone allows integer-path ambiguity.\delta=2\pi m\Longleftrightarrow\Delta\mathcal L=m\lambda\Longrightarrow\boxed{\text{brightness alone allows integer-path ambiguity}}.

Physical check

Exact compensation means zero path difference, not merely an integer number of monochromatic wavelengths.