The diffraction grating

Section: Superposition  |  Syllabus: Cambridge AS Level Physics (9702)

What is a Diffraction Grating?

A diffraction grating consists of a large number of equally spaced parallel slits (or lines). When light passes through, it produces sharp, bright maxima at specific angles.

Diffraction Grating A plate with many parallel, equally spaced slits (typically hundreds to thousands per millimetre) used to produce interference patterns and measure wavelengths with high precision. Grating Spacing:

If grating has N lines per mm: d = (1/N) mm = (1/N × 10^3) m

Example: 500 lines/mm → d = (1/500 × 10^3) m = 2.0 × 10^-6 m

Difference Between Young's Slits and Diffraction Gratings

FIG 8.20: Comparison of Double-Slit and Grating Patterns

Show side-by-side: (a) Double-slit pattern with broad, overlapping fringes of similar intensity, gradual intensity variation. (b) Diffraction grating pattern with sharp, narrow, intense maxima separated by wide dark regions. Label: central maximum (n=0), first order (n=1), second order (n=2). Show intensity vs angle graphs below each.

Feature Young's Double Slit Diffraction Grating
Number of slits 2 Many (hundreds to thousands)
Bright maxima Broad, gradually varying Sharp, narrow, intense
Dark regions Gradual transition Wide and dark
Measurement precision Lower Higher (sharp maxima easier to locate)

Why More Slits Give Sharper Maxima

With two slits: gradual transition between constructive and destructive interference → broad fringes.

With many slits:

Counter-Intuitive Result

More slits does NOT mean more bright maxima. It means sharper maxima, wider dark regions, and fewer visible spots (secondary maxima suppressed). Students sometimes think incorrectly that more slits = more light = more maxima.

The Diffraction Grating Equation

FIG 8.21: Diffraction Grating Geometry

Show: parallel light rays incident on grating (multiple slits with spacing d). Rays diffracted at angle θ to the normal. Show path difference between rays from adjacent slits = d sin θ. Mark the central maximum (n = 0, θ = 0), first order (n = 1), second order (n = 2) on both sides. Show how angle increases with order number.

The Diffraction Grating Equation:

d sinθ = nλ

where:

Order Numbers

Maximum Observable Order:

Since sinθ ≤ 1: n_max = floor((d/λ))

If calculation gives sinθ > 1, that order does not exist.

Using a Diffraction Grating to Determine Wavelength

Diffraction gratings provide a highly accurate method for measuring the wavelength of light.

Procedure (Conceptual)

  1. Direct monochromatic light (e.g., from a laser or discharge lamp) at the grating
  2. Observe the diffraction pattern-a series of bright spots at specific angles
  3. Measure the angle θ to a particular order maximum (e.g., first order)
  4. Use the grating equation dsinθ = nλ to calculate λ

Why Gratings are More Accurate than Young's Slits

Spectrometer Not Required

For the Cambridge AS Level syllabus, knowledge of the structure and use of the spectrometer is not required. The focus is on understanding the principles of the diffraction grating.

Worked Examples

Worked Example 1: Finding Wavelength

Question: A diffraction grating has 600 lines per mm. Monochromatic light produces a first-order maximum at an angle of 20.5° to the normal. Calculate the wavelength of the light.

Solution

First, find the grating spacing:

d = (1/600) mm = (1/600 × 10^3) m = 1.67 × 10^-6 m

Using dsinθ = nλ with n = 1:

λ = (dsinθ/n) = 1.67 × 10^-6 × sin(20.5°)1

λ = 1.67 × 10^-6 × 0.350 = 5.85 × 10^-7 m

λ = 585 nm (yellow light)

Worked Example 2: Finding the Angle

Question: Light of wavelength 650 nm passes through a diffraction grating with spacing 2.0 μm. At what angle does the second-order maximum appear?

Solution

Given: λ = 650 × 10^-9 m, d = 2.0 × 10^-6 m, n = 2

Using dsinθ = nλ:

sinθ = (nλ/d) = 2 × 650 × 10^-92.0 × 10^-6

sinθ = 1.3 × 10^-62.0 × 10^-6 = 0.65

θ = sin^-1(0.65) = 40.5°

Worked Example 3: Maximum Possible Order

Question: A diffraction grating has 400 lines per mm. What is the maximum order that can be observed for light of wavelength 700 nm?

Solution

Grating spacing: d = (1/400 × 10^3) m = 2.5 × 10^-6 m

For the maximum to be visible, sinθ ≤ 1

From dsinθ = nλ: n ≤ (d/λ)

n ≤ 2.5 × 10^-6700 × 10^-9 = 2.5 × 10^-67.0 × 10^-7 = 3.57

Maximum order n_max = 3 (taking the integer part)

Orders 0, 1, 2, and 3 can be observed (on each side of centre).

Worked Example 4: Grating with Lines per mm

Question: A grating has 750 lines per mm. Calculate the angle at which the first-order maximum for light of wavelength 450 nm appears.

Solution

Grating spacing: d = (1/750 × 10^3) m = 1.33 × 10^-6 m

Using sinθ = (nλ/d):

sinθ = 1 × 450 × 10^-91.33 × 10^-6 = 0.338

θ = sin^-1(0.338) = 19.7°

Common Exam Mistakes

Avoid These Errors
  1. Confusing lines per mm with grating spacing: If there are N lines per mm, then d = (1/N) mm. Remember to convert to metres.
  2. Forgetting that sinθ ≤ 1: If your calculation gives sinθ > 1, that order does not exist.
  3. Using degrees vs radians: Ensure your calculator is in the correct mode. The grating equation works with either, but be consistent.
  4. Misidentifying the order: n = 0 is the central maximum (straight through); n = 1 is the first-order maximum on either side.
  5. Thinking more slits = more maxima: More slits give sharper, brighter maxima and wider dark regions-not more maxima.
  6. Unit errors: Wavelength is often given in nm (10^-9 m) and grating spacing derived from lines/mm. Convert carefully.

Concept Check Questions

Interactive revision notes, videos and practice questions load below.

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