Gratings: Dispersion and Resolving Power — Question 8

Section 36-8 · Physics pages 6006–6007

Question 8 Adjacent-order coincidences give unequal exact wavelength gaps A spectral line at λ = 600 nm is measured in order m=10. At the same angle, order 11 admits a shorter wavelength and order 9 a longer wavelength. Assume these orders are supported by the instrument. d N illuminated slits orders 9, 10, 11 Schematic; labels, not drawing lengths, specify the data. (a) Calculate both coincident wavelengths. (b) Calculate the blue and red gaps from 600 nm and compare with the large-order estimate λ/m.
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Question 8 - Solution Adjacent-order coincidences give unequal exact wavelength gaps d N illuminated slits orders 9, 10, 11 (a) Method and calculation 10λ = 11λb =⇒λb = 6000/11 = 545.455 nm . 10λ = 9λr =⇒λr = 6000/9 = 666.667 nm . (b) Interpretation and further calculation λ −λb = λ/(m + 1) = 54.5455 nm, λr −λ = λ/(m −1) = 66.6667 nm . λ/m = 60.0 nm is only the large-m approximation. Physical check The exact neighboring-order coincidences are not symmetrically placed in wavelength about the chosen line.

Question 8

Adjacent-order coincidences give unequal exact wavelength gaps

A spectral line at λ=600nm\lambda=600\,\mathrm{nm} is measured in order m=10. At the same angle, order 11 admits a shorter wavelength and order 9 a longer wavelength. Assume these orders are supported by the instrument.

Diagram shown in the original SVG worksheet.

  1. Calculate both coincident wavelengths.

  2. Calculate the blue and red gaps from 600 nm and compare with the large-order estimate λ/m\lambda/m.

Question 8 - Solution

Adjacent-order coincidences give unequal exact wavelength gaps

Diagram shown in the original SVG worksheet.

(a) Method and calculation

10λ=11λb⇒λb=6000/11=545.455nm.10\lambda=11\lambda_b\Longrightarrow\boxed{\lambda_b=6000/11=545.455\,\mathrm{nm}}.10λ=9λr⇒λr=6000/9=666.667nm.10\lambda=9\lambda_r\Longrightarrow\boxed{\lambda_r=6000/9=666.667\,\mathrm{nm}}.

(b) Interpretation and further calculation

λ−λb=λ/(m+1)=54.5455nm,λr−λ=λ/(m−1)=66.6667nm.\boxed{\lambda-\lambda_b=\lambda/(m+1)=54.5455\,\mathrm{nm},\quad\lambda_r-\lambda=\lambda/(m-1)=66.6667\,\mathrm{nm}}.λ/m=60.0nmis only the large-m approximation.\boxed{\lambda/m=60.0\,\mathrm{nm}}\quad\text{is only the large-m approximation}.

Physical check

The exact neighboring-order coincidences are not symmetrically placed in wavelength about the chosen line.