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Physics HL · Chapter 14: Wave Phenomena

14.5 Multiple Slits and Diffraction Gratings (AHL)

Scale from two slits to many slits, then use grating equations, order limits, and resolution logic for practical spectroscopy questions.

Estimated time: 28 minutes

From Two Slits to Many Slits

As slit count increases, principal maxima become narrower and more intense while side lobes weaken. Physically, more coherent emitters impose a stricter phase-matching requirement for strong constructive interference, so bright peaks occupy smaller angular ranges.

This is why gratings are powerful for wavelength analysis. A two-slit pattern is useful for demonstrating wave nature, but a many-slit grating creates sharp angular peaks that separate nearby wavelengths more clearly.

Grating Equation and Order Structure

dsinθ=nλ,n=0,±1,±2,d\sin\theta = n\lambda, \qquad n=0,\pm1,\pm2,\ldots

d is slit spacing (inverse line density), n is order number, and valid orders require |sin(theta)| <= 1.

If line density is L lines per meter, then d = 1/L. Larger line density means smaller d and typically larger diffraction angles for a given order. This increases angular dispersion, which helps spectral separation but can also cause order overlap when bandwidth is broad.

Resolution and Order Overlap

R=λΔλ=nNR = \frac{\lambda}{\Delta\lambda} = nN

For a grating with N illuminated slits, higher order and more illuminated lines increase resolving power.

Increasing order n improves resolution, but usable order is capped by the condition |n lambda / d| <= 1. In white-light applications, different wavelength-order combinations can land at similar angles, producing overlap. Practical instrument design balances dispersion, intensity, and overlap risk.

Note

When solving grating problems, convert line density to slit spacing first. Many wrong answers come from skipping d = 1/L.

Simulation: Multi-Slit and Grating Peak Sharpening

Move from double-slit to grating mode and increase slit count to watch principal maxima narrow while envelope and order limits remain active.

Wave Phenomena Studio

Current mode: Diffraction and Interference

sourceslit planescreen
intensity profilepeak-normalized: I / I0

Pattern mode

10-slit grating

Single-slit first minimum

5.16 cm

Fringe spacing

0.58 cm

Maximum visible order

|m| <= 275

Increase slit count to sharpen principal maxima (grating behavior) and decrease slit width to broaden the diffraction envelope. The intensity profile combines diffraction envelope physics with multi-slit interference spacing.

Test Yourself

A grating has 600 lines/mm and is illuminated by 600 nm light. Enter the second-order angle in degrees.

Hint: Use d = 1/(600000 m^-1), then d sin(theta) = 2 lambda.