Published by Patrick Mutisya · 14 days ago
Diffraction is the bending and spreading of a wave when it encounters an obstacle or an aperture whose dimensions are comparable to the wavelength of the wave. The phenomenon is a direct consequence of the wave nature of light, sound, water waves, etc.
The condition for the first minimum in a single‑slit diffraction pattern is
\$a \sin\theta = \lambda\$
where \$a\$ is the slit width, \$\\theta\$ the angle measured from the central axis, and \$\\lambda\$ the wavelength.
A monochromatic laser beam passes through a narrow slit and projects a pattern of a bright central maximum flanked by weaker side maxima on a screen.
Two parallel slits act as coherent sources. The resulting pattern shows alternating bright and dark fringes whose spacing depends on slit separation \$d\$ and wavelength \$\\lambda\$:
\$d \sin\theta = m\lambda \qquad (m = 0, \\pm1, \\pm2, …)\$
A grating contains many equally spaced slits. The condition for principal maxima is
\$N d \sin\theta = m\lambda\$
where \$N\$ is the number of illuminated slits. Gratings give very sharp, well‑separated spectral lines.
A ripple tank provides a visual demonstration of diffraction with water waves. A point source generates circular wavefronts that encounter a barrier with a gap of width \$a\$.
The relationship between the gap width \$a\$ and the wavelength \$\\lambda\$ determines the diffraction pattern. The table below summarises the observable behaviour.
| Ratio \$a/\\lambda\$ | Observed Diffraction | Typical Pattern |
|---|---|---|
| \$a/\\lambda \\gg 1\$ | Minimal bending; wavefronts remain essentially straight. | Sharp, well‑defined beam; small side fringes (if any). |
| \$a/\\lambda \\approx 1\$ | Significant bending; wavefronts spread noticeably. | Broad central maximum with visible side lobes. |
| \$a/\\lambda \\ll 1\$ | Strong bending; aperture behaves like a point source. | Nearly circular wavefronts; intensity falls off isotropically. |
Diffraction illustrates the wave nature of physical phenomena. By varying the size of an aperture relative to the wavelength, one can observe a continuum from straight‑line propagation to complete spreading. Experiments such as the single‑slit, double‑slit, diffraction grating, and ripple‑tank demonstrations provide clear, observable evidence of these effects, forming a cornerstone of the A‑Level Physics curriculum.