Gratings: Dispersion and Resolving Power — Question 6

Section 36-8 · Physics pages 6002–6003

Question 6 A finite entrance-slit image can dominate the spectral line width A centered camera has focal length f = 0.500 m. Its grating uses d = 1.00 µm, m=1, λ = 500 nm, and N=10000 illuminated slits. The entrance slit is imaged to width w = 50.0 µm at the detector. For this engineering estimate, combine slit and diffraction wavelength widths in quadrature. w λ detector slit image Schematic; labels, not drawing lengths, specify the data. (a) Calculate the slit-equivalent and ideal diffraction wavelength widths. (b) Find the combined width and effective resolving power under the stated model.
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Question 6 - Solution A finite entrance-slit image can dominate the spectral line width w λ detector slit image (a) Method and calculation θ = 30◦, D = 1/(d cos θ); ∆λs = w/(fD). ∆λs = 0.0866025 nm, ∆λd = λ/(mN) = 0.0500 nm . (b) Interpretation and further calculation ∆λeff= √ ∆λ2s + ∆λ2 d = 0.1000 nm . Reff= 500/0.1000 = 5000 . Physical check The quadrature rule is an explicitly supplied approximation; exact line shapes require convolution of the slit image with the diffraction response.

Question 6

A finite entrance-slit image can dominate the spectral line width

A centered camera has focal length f=0.500mf=0.500\,\mathrm m. Its grating uses d=1.00μmd=1.00\,\mu\mathrm m, m=1, λ=500nm\lambda=500\,\mathrm{nm}, and N=10000 illuminated slits. The entrance slit is imaged to width w=50.0μmw=50.0\,\mu\mathrm m at the detector. For this engineering estimate, combine slit and diffraction wavelength widths in quadrature.

Diagram shown in the original SVG worksheet.

  1. Calculate the slit-equivalent and ideal diffraction wavelength widths.

  2. Find the combined width and effective resolving power under the stated model.

Question 6 - Solution

A finite entrance-slit image can dominate the spectral line width

Diagram shown in the original SVG worksheet.

(a) Method and calculation

θ=30∘,𝒟=1/(dcos⁡θ);Δλs=w/(f𝒟).\theta=30^\circ,\quad\mathcal D=1/(d\cos\theta);\quad\Delta\lambda_s=w/(f\mathcal D).Δλs=0.0866025nm,Δλd=λ/(mN)=0.0500nm.\boxed{\Delta\lambda_s=0.0866025\,\mathrm{nm},\quad\Delta\lambda_d=\lambda/(mN)=0.0500\,\mathrm{nm}}.

(b) Interpretation and further calculation

Δλeff=Δλs2+Δλd2=0.1000nm.\boxed{\Delta\lambda_{\mathrm{eff}}=\sqrt{\Delta\lambda_s^2+\Delta\lambda_d^2}=0.1000\,\mathrm{nm}}.ℛeff=500/0.1000=5000.\boxed{\mathcal R_{\mathrm{eff}}=500/0.1000=5000}.

Physical check

The quadrature rule is an explicitly supplied approximation; exact line shapes require convolution of the slit image with the diffraction response.