Diffraction — Question 9

Section 35-2 · Physics pages 5748–5749

Question 9 A lens makes angular diffraction accessible on a nearby plane A thin converging lens is placed immediately after a slit. Parallel rays leaving the slit at small angle θ meet at y = fθ in the rear focal plane. The slit has a = 0.25 mm, wavelength 625 nm, and the lens has f = 0.40 m. Assume a sufficiently large lens aperture. f Schematic; labels, not drawing lengths, specify the data. (a) Find the focal-plane position of the first slit minimum. (b) If the detector pixels are 10 µm wide, calculate the number of pixels across the central maximum and how it changes for a lens with twice f.
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Question 9 - Solution A lens makes angular diffraction accessible on a nearby plane f (a) Method and calculation aθ1 ≃λ =⇒y1 = fλ/a. y1 = 1.00 mm, W = 2y1 = 2.00 mm . (b) Interpretation and further calculation N = W/p = 2.00 mm/(0.010 mm) = 200 . f →2f =⇒W →4.00 mm, N →400 . Physical check The lens maps direction into position; a physical screen at one focal length can display the angular spectrum without a very long free-space propagation distance.

Question 9

A lens makes angular diffraction accessible on a nearby plane

A thin converging lens is placed immediately after a slit. Parallel rays leaving the slit at small angle θ\theta meet at y=fθy=f\theta in the rear focal plane. The slit has a=0.25mma=0.25\,\mathrm{mm}, wavelength 625nm625\,\mathrm{nm}, and the lens has f=0.40mf=0.40\,\mathrm m. Assume a sufficiently large lens aperture.

Diagram shown in the original SVG worksheet.

  1. Find the focal-plane position of the first slit minimum.

  2. If the detector pixels are 10μm10\,\mu\mathrm m wide, calculate the number of pixels across the central maximum and how it changes for a lens with twice f.

Question 9 - Solution

A lens makes angular diffraction accessible on a nearby plane

Diagram shown in the original SVG worksheet.

(a) Method and calculation

aθ1≃λ⇒y1=fλ/a.a\theta_1\simeq\lambda\Longrightarrow y_1=f\lambda/a.y1=1.00mm,W=2y1=2.00mm.\boxed{y_1=1.00\,\mathrm{mm},\quad W=2y_1=2.00\,\mathrm{mm}}.

(b) Interpretation and further calculation

N=W/p=2.00mm/(0.010mm)=200.\boxed{N=W/p=2.00\,\mathrm{mm}/(0.010\,\mathrm{mm})=200}.f→2f⇒W→4.00mm,N→400.f\to2f\Longrightarrow\boxed{W\to4.00\,\mathrm{mm},\quad N\to400}.

Physical check

The lens maps direction into position; a physical screen at one focal length can display the angular spectrum without a very long free-space propagation distance.