Diffraction by a Single Slit: Locating the Minima — Question 10

Section 36-2 · Physics pages 5890–5891

Question 10 Minimum-position sensitivity grows sharply near grazing angles For fixed slit width a, screen distance L, and nonzero order m, the wavelength is inferred from λ = (a/m)y/ √ L2 + y2. Assume a and L are exact and the measured y has small standard uncertainty σy. a P L Schematic; labels, not drawing lengths, specify the data. (a) Derive the relative wavelength uncertainty caused by σy. (b) Compare the sensitivity to relative y error at y ≪L and at y = L, then derive the inverse sensitivity d ln y/d ln λ.
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Question 10 - Solution Minimum-position sensitivity grows sharply near grazing angles a P L (a) Method and calculation ln λ = ln(a/m) + ln y −1 2 ln(L2 + y2). σλ λ = L2 L2 + y2 σy |y| = cos2 θ σy |y| . (b) Interpretation and further calculation y ≪L : factor 1 ; y = L : factor 1/2 . d ln y d ln λ = sec2 θ →∞ as |θ| →90◦. Physical check Near grazing, a small wavelength change moves a minimum a large distance, but the required screen size also grows without bound.

Question 10

Minimum-position sensitivity grows sharply near grazing angles

For fixed slit width a, screen distance L, and nonzero order m, the wavelength is inferred from λ=(a/m)y/L2+y2\lambda=(a/m)y/\sqrt{L^2+y^2}. Assume a and L are exact and the measured y has small standard uncertainty σy\sigma_y.

Diagram shown in the original SVG worksheet.

  1. Derive the relative wavelength uncertainty caused by σy\sigma_y.

  2. Compare the sensitivity to relative y error at y≪Ly\ll L and at y=Ly=L, then derive the inverse sensitivity dln⁡y/dln⁡λd\ln y/d\ln\lambda.

Question 10 - Solution

Minimum-position sensitivity grows sharply near grazing angles

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ln⁡λ=ln⁡(a/m)+ln⁡y−12ln⁡(L2+y2).\ln\lambda=\ln(a/m)+\ln y-\tfrac12\ln(L^2+y^2).σλλ=L2L2+y2σy|y|=cos⁡2θσy|y|.\boxed{\frac{\sigma_\lambda}{\lambda}=\frac{L^2}{L^2+y^2}\frac{\sigma_y}{|y|}=\cos^2\theta\frac{\sigma_y}{|y|}}.

(b) Interpretation and further calculation

y≪L:factor 1;y=L:factor 1/2.y\ll L:\ \boxed{\text{factor }1};\qquad y=L:\ \boxed{\text{factor }1/2}.dln⁡ydln⁡λ=sec⁡2θ→∞as|θ|→90∘.\boxed{\frac{d\ln y}{d\ln\lambda}=\sec^2\theta\to\infty\quad\text{as}\ |\theta|\to90^\circ}.

Physical check

Near grazing, a small wavelength change moves a minimum a large distance, but the required screen size also grows without bound.