Diffraction by a Single Slit: Locating the Minima — Question 7

Section 36-2 · Physics pages 5884–5885

Question 7 A wire diameter can be inferred from its complementary slit minima Use scalar complementarity: away from the direct beam, a thin opaque wire and a slit of the same width produce identical diffraction intensities. At wavelength 650 nm, a wire gives third-order minima at y = ±39.0 mm on a screen L = 2.00 m away. wire a Schematic; labels, not drawing lengths, specify the data. (a) Infer the wire diameter using exact screen geometry. (b) Find the percentage error made by replacing sine of the diffraction angle with y/L.
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Question 7 - Solution A wire diameter can be inferred from its complementary slit minima wire a (a) Method and calculation sin θ3 = y √ L2 + y2 , a = 3λ √ L2 + y2 y . a = 100.019 µm . (b) Interpretation and further calculation aparax = 3λL/y = 100.000 µm. a −aparax a = 1 − L √ L2 + y2 = 0.0190071% . Physical check The complementary-pattern argument applies offaxis; the unobstructed forward field must still be treated separately.

Question 7

A wire diameter can be inferred from its complementary slit minima

Use scalar complementarity: away from the direct beam, a thin opaque wire and a slit of the same width produce identical diffraction intensities. At wavelength 650nm650\,\mathrm{nm}, a wire gives third-order minima at y=±39.0mmy=\pm39.0\,\mathrm{mm} on a screen L=2.00mL=2.00\,\mathrm m away.

Diagram shown in the original SVG worksheet.

  1. Infer the wire diameter using exact screen geometry.

  2. Find the percentage error made by replacing sine of the diffraction angle with y/L.

Question 7 - Solution

A wire diameter can be inferred from its complementary slit minima

Diagram shown in the original SVG worksheet.

(a) Method and calculation

sin⁡θ3=yL2+y2,a=3λL2+y2y.\sin\theta_3=\frac{y}{\sqrt{L^2+y^2}},\quad\boxed{a=\frac{3\lambda\sqrt{L^2+y^2}}y}.a=100.019μm.\boxed{a=100.019\,\mu\mathrm m}.

(b) Interpretation and further calculation

aparax=3λL/y=100.000μm.a_{\mathrm{parax}}=3\lambda L/y=100.000\,\mu\mathrm m.a−aparaxa=1−LL2+y2=0.0190071%.\boxed{\frac{a-a_{\mathrm{parax}}}a=1-\frac L{\sqrt{L^2+y^2}}=0.0190071\%}.

Physical check

The complementary-pattern argument applies off axis; the unobstructed forward field must still be treated separately.