Diffraction by a Single Slit: Locating the Minima — Question 8

Section 36-2 · Physics pages 5886–5887

Question 8 Thermal widening moves a diffraction minimum toward the axis A slit width obeys a(T) = a0[1 + α∆T], with α = 2.0 × 10−5 K−1. A fixed-order minimum initially lies at θ = 30◦. The wavelength remains constant and the slit warms by 10 K. Use first-order changes. a P L a(T) Schematic; labels, not drawing lengths, specify the data. (a) Differentiate the minimum condition to find the angular shift. (b) If that minimum initially lies at y = 0.500 m on a fixed screen, find its transverse shift without making a small-angle approximation.
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Question 8 - Solution Thermal widening moves a diffraction minimum toward the axis a P L a(T) (a) Method and calculation a sin θ = mλ =⇒sin θ da + a cos θ dθ = 0. ∆θ ≃−α∆T tan θ = −1.15470 × 10−4 rad . (b) Interpretation and further calculation y = L tan θ =⇒∆y = L sec2 θ∆θ = −α∆T y sec2 θ. ∆y = −0.133333 mm . Physical check A wider opening narrows the pattern. Retaining the secant-squared factor matters when the observed angle is not small.

Question 8

Thermal widening moves a diffraction minimum toward the axis

A slit width obeys a(T)=a0[1+αΔT]a(T)=a_0[1+\alpha\Delta T], with α=2.0×10−5K−1\alpha=2.0\times10^{-5}\,\mathrm{K^{-1}}. A fixed-order minimum initially lies at θ=30∘\theta=30^\circ. The wavelength remains constant and the slit warms by 10K10\,\mathrm K. Use first-order changes.

Diagram shown in the original SVG worksheet.

  1. Differentiate the minimum condition to find the angular shift.

  2. If that minimum initially lies at y=0.500my=0.500\,\mathrm m on a fixed screen, find its transverse shift without making a small-angle approximation.

Question 8 - Solution

Thermal widening moves a diffraction minimum toward the axis

Diagram shown in the original SVG worksheet.

(a) Method and calculation

asin⁡θ=mλ⇒sin⁡θda+acos⁡θdθ=0.a\sin\theta=m\lambda\Longrightarrow\sin\theta\,da+a\cos\theta\,d\theta=0.Δθ≃−αΔTtan⁡θ=−1.15470×10−4rad.\boxed{\Delta\theta\simeq-\alpha\Delta T\tan\theta=-1.15470\times10^{-4}\,\mathrm{rad}}.

(b) Interpretation and further calculation

y=Ltan⁡θ⇒Δy=Lsec⁡2θΔθ=−αΔTysec⁡2θ.y=L\tan\theta\Longrightarrow\Delta y=L\sec^2\theta\Delta\theta=-\alpha\Delta T\,y\sec^2\theta.Δy=−0.133333mm.\boxed{\Delta y=-0.133333\,\mathrm{mm}}.

Physical check

A wider opening narrows the pattern. Retaining the secant-squared factor matters when the observed angle is not small.