Michelson's Interferometer — Question 3

Section 35-7 · Physics pages 5836–5837

Question 3 A fringe rate measures mirror speed but not its sign A Michelson mirror moves at constant speed v in vacuum. The source wavelength is 600 nm, and a stationary detector records 1200 full intensity cycles per second. Other phases are constant. M1 M2 detector input v Schematic; labels, not drawing lengths, specify the data. (a) Derive the relation between fringe frequency and mirror velocity and infer its speed. (b) Calculate the displacement magnitude during a 0.25 s observation and explain why one intensity channel cannot determine the direction of motion.
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Question 3 - Solution A fringe rate measures mirror speed but not its sign M1 M2 detector input v (a) Method and calculation ϕ(t) = ϕ0 + 4πvt λ , ffringe = | ˙ϕ| 2π = 2|v| λ . |v| = ffringeλ/2 = 0.360 mm/s . (b) Interpretation and further calculation |∆x| = |v|T = 90.0 µm, N = fT = 300 . cos(ϕ0 + ωt) = cos(−ϕ0 −ωt) =⇒direction needs additional phase information . Physical check A fringe counter measures the magnitude of phase winding; a second quadrature channel can establish its sign.

Question 3

A fringe rate measures mirror speed but not its sign

A Michelson mirror moves at constant speed v in vacuum. The source wavelength is 600nm600\,\mathrm{nm}, and a stationary detector records 1200 full intensity cycles per second. Other phases are constant.

Diagram shown in the original SVG worksheet.

  1. Derive the relation between fringe frequency and mirror velocity and infer its speed.

  2. Calculate the displacement magnitude during a 0.25s0.25\,\mathrm s observation and explain why one intensity channel cannot determine the direction of motion.

Question 3 - Solution

A fringe rate measures mirror speed but not its sign

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ϕ(t)=ϕ0+4πvtλ,ffringe=|ϕ̇|2π=2|v|λ.\phi(t)=\phi_0+\frac{4\pi vt}{\lambda},\quad f_{\mathrm{fringe}}=\frac{|\dot\phi|}{2\pi}=\frac{2|v|}{\lambda}.|v|=ffringeλ/2=0.360mm/s.\boxed{|v|=f_{\mathrm{fringe}}\lambda/2=0.360\,\mathrm{mm/s}}.

(b) Interpretation and further calculation

|Δx|=|v|T=90.0μm,N=fT=300.\boxed{|\Delta x|=|v|T=90.0\,\mu\mathrm m,\quad N=fT=300}.cos⁡(ϕ0+ωt)=cos⁡(−ϕ0−ωt)⇒direction needs additional phase information.\cos(\phi_0+\omega t)=\cos(-\phi_0-\omega t)\Longrightarrow\boxed{\text{direction needs additional phase information}}.

Physical check

A fringe counter measures the magnitude of phase winding; a second quadrature channel can establish its sign.