Young's Interference Experiment — Question 3

Section 35-3 · Physics pages 5756–5757

Question 3 Oblique illumination shifts the zero-order direction A plane wave reaches two narrow slits at incidence angle α from the normal. Define the phase difference at outgoing angle θ by δ = (2πd/λ)(sin θ −sin α). Let d = 20 µm, λ = 500 nm, and sin α = 0.10. P(y) d L α Schematic; labels, not drawing lengths, specify the data. (a) Find the zero-order outgoing direction and the two adjacent bright directions. (b) Determine the bright-fringe order that lies on the normal to the slit plane.
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Question 3 - Solution Oblique illumination shifts the zero-order direction P(y) d L α (a) Method and calculation δ = 2πm =⇒sin θm = 0.10 + 0.025m . θ0 = 5.7392◦, θ−1 = 4.3012◦, θ+1 = 7.1808◦. (b) Interpretation and further calculation θ = 0 : m = −d sin α λ = −20(0.10) 0.50 . m = −4 . Physical check The central phase-matched direction follows the incident wave, while the laboratory screen center can carry a nonzero interference order.

Question 3

Oblique illumination shifts the zero-order direction

A plane wave reaches two narrow slits at incidence angle α\alpha from the normal. Define the phase difference at outgoing angle θ\theta by δ=(2πd/λ)(sin⁡θ−sin⁡α)\delta=(2\pi d/\lambda)(\sin\theta-\sin\alpha). Let d=20μmd=20\,\mu\mathrm m, λ=500nm\lambda=500\,\mathrm{nm}, and sin⁡α=0.10\sin\alpha=0.10.

Diagram shown in the original SVG worksheet.

  1. Find the zero-order outgoing direction and the two adjacent bright directions.

  2. Determine the bright-fringe order that lies on the normal to the slit plane.

Question 3 - Solution

Oblique illumination shifts the zero-order direction

Diagram shown in the original SVG worksheet.

(a) Method and calculation

δ=2πm⇒sin⁡θm=0.10+0.025m.\delta=2\pi m\Longrightarrow\boxed{\sin\theta_m=0.10+0.025m}.θ0=5.7392∘,θ−1=4.3012∘,θ+1=7.1808∘.\boxed{\theta_0=5.7392^\circ,\quad\theta_{-1}=4.3012^\circ,\quad\theta_{+1}=7.1808^\circ}.

(b) Interpretation and further calculation

θ=0:m=−dsin⁡αλ=−20(0.10)0.50.\theta=0:\quad m=-\frac{d\sin\alpha}{\lambda}=-\frac{20(0.10)}{0.50}.m=−4.\boxed{m=-4}.

Physical check

The central phase-matched direction follows the incident wave, while the laboratory screen center can carry a nonzero interference order.