Diffraction Gratings — Question 2

Section 36-7 · Physics pages 5974–5975

Question 2 Groove density determines the set of propagating diffraction orders A transmission grating has 600 lines per millimeter and is illuminated normally at λ = 500 nm. Treat the slits as narrow and require |θ| < 90◦. d N illuminated slits Schematic; labels, not drawing lengths, specify the data. (a) Find the first and third positive principal-order angles. (b) List all allowed principal orders and explain why the fourth is absent.
Show solutionHide solution
Question 2 - Solution Groove density determines the set of propagating diffraction orders d N illuminated slits (a) Method and calculation d = (600 mm−1)−1 = 1.66667 µm; sin θm = mλ/d = 0.300m. θ1 = 17.4576◦, θ3 = 64.1581◦. (b) Interpretation and further calculation |0.300m| < 1 =⇒m = −3, −2, −1, 0, 1, 2, 3 . m = 4 : sin θ4 = 1.20 > 1 =⇒no propagating fourth order . Physical check The existence of an order follows from the grating equation; its brightness also depends on slit width and groove structure.

Question 2

Groove density determines the set of propagating diffraction orders

A transmission grating has 600 lines per millimeter and is illuminated normally at λ=500nm\lambda=500\,\mathrm{nm}. Treat the slits as narrow and require |θ|<90∘|\theta|<90^\circ.

Diagram shown in the original SVG worksheet.

  1. Find the first and third positive principal-order angles.

  2. List all allowed principal orders and explain why the fourth is absent.

Question 2 - Solution

Groove density determines the set of propagating diffraction orders

Diagram shown in the original SVG worksheet.

(a) Method and calculation

d=(600mm−1)−1=1.66667μm;sin⁡θm=mλ/d=0.300m.d=(600\,\mathrm{mm^{-1}})^{-1}=1.66667\,\mu\mathrm m;\quad\sin\theta_m=m\lambda/d=0.300m.θ1=17.4576∘,θ3=64.1581∘.\boxed{\theta_1=17.4576^\circ,\quad\theta_3=64.1581^\circ}.

(b) Interpretation and further calculation

|0.300m|<1⇒m=−3,−2,−1,0,1,2,3.|0.300m|<1\Longrightarrow\boxed{m=-3,-2,-1,0,1,2,3}.m=4:sin⁡θ4=1.20>1⇒no propagating fourth order.m=4:\ \sin\theta_4=1.20>1\Longrightarrow\boxed{\text{no propagating fourth order}}.

Physical check

The existence of an order follows from the grating equation; its brightness also depends on slit width and groove structure.