| Medium | Speed formula | Typical variables |
|---|---|---|
| Water surface (shallow depth < λ) | v = √(g d) | g = 9.8 m s⁻², d = water depth |
| String (tension T, linear density μ) | v = √(T/μ) | Not required for the tank but part of the syllabus |
| General relationship (all media) | v = f λ | f = frequency, λ = wavelength |
| Term | Symbol | Definition / Units |
|---|---|---|
| Wave speed | v | distance travelled by a crest per unit time (m s⁻¹) |
| Frequency | f | number of crests passing a point per second (Hz) |
| Wavelength | λ | distance between successive crests (m) |
| Amplitude | A | maximum vertical displacement of the water surface (m) |
| Incident wave | – | wave approaching a boundary |
| Reflected wave | – | wave that returns from a boundary |
| Refracted wave | – | wave that changes direction on entering a new medium |
| Diffracted wave | – | wave that spreads after passing an opening or around an edge |
| Normal | – | imaginary line perpendicular to a surface at the point of incidence |
| Angle of incidence | θi | angle between incident ray and the normal |
| Angle of reflection | θr | angle between reflected ray and the normal |
| Angle of refraction | θt | angle between refracted ray and the normal |
Measured λ = 2.0 cm, f = 5 Hz.
Law of reflection: θi = θr (measured with respect to the normal).
\$\frac{\sin\theta{1}}{\sin\theta{2}}=\frac{v{1}}{v{2}}=\frac{\lambda{1}}{\lambda{2}}=\frac{\sqrt{d{1}}}{\sqrt{d{2}}}\$
Measured angles: θ₁ = 35° (shallow) and θ₂ = 55° (deep).
| Slit width a | Pattern observed |
|---|---|
| a ≫ λ | Little spreading; wavefronts remain essentially planar (geometrical‑optics limit). |
| a ≈ λ | Pronounced spreading; semi‑circular wavefronts emerge from the slit – classic diffraction. |
| a < λ | Slit behaves like a point source; concentric circles of low intensity appear. |
Every point on the slit acts as a secondary source of circular wavelets. The new wavefront is the envelope of these wavelets, producing the observed spreading.
For a single slit, intensity varies with angle θ as
\$\$I(\theta)\;\propto\;\left(\frac{\sin\beta}{\beta}\right)^{2},\qquad
\beta=\frac{\pi a\sin\theta}{\lambda}\$\$
The first minimum occurs when β = π → a sin θ = λ.
λ = 1.2 cm, a = 1.2 cm → first minimum at sin θ = λ/a = 1 → θ ≈ 90°. In practice a broad central maximum and weak side lobes are seen, illustrating limited resolution for a narrow aperture.
Every point on the illuminated part of the edge acts as a secondary source. The superposition of the resulting wavelets produces the curved fronts and the partial shadow.
The width of the first bright Fresnel zone behind an edge is roughly
\$w \;\approx\; \sqrt{\lambda D}\$
where D is the distance from the edge to the observation screen.
λ = 1.0 cm, D = 4 cm → w ≈ √(1.0 × 4) ≈ 2 cm, matching the observed width of the first bright fringe.
| Phenomenon | Experimental condition | Key observation | Principle / Equation |
|---|---|---|---|
| Reflection | Vertical plane glass plate | θi = θr | Law of reflection |
| Refraction (depth step) | Two water depths d₁ ≠ d₂ | Wave bends toward normal in slower (shallower) region, away in faster (deeper) region | Snell’s law for water waves
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