Derive, using the definitions of speed, frequency and wavelength, the wave equation
$$v = f \lambda$$
Consider a sinusoidal progressive wave travelling along the $x$‑axis. Let a particular crest be observed at position $x_1$ at time $t_1$ and the same crest be observed at position $x_2$ at a later time $t_2$.
Substituting $\lambda$ for the distance and $T$ for the time gives
$$v = \frac{\lambda}{T}.$$Frequency $f$ is the reciprocal of the period:
$$f = \frac{1}{T} \quad \Longrightarrow \quad T = \frac{1}{f}.$$Replacing $T$ in the speed expression:
$$v = \frac{\lambda}{1/f} = f\lambda.$$Thus the fundamental relationship for a progressive wave is
$$\boxed{v = f\lambda}$$| Quantity | Symbol | SI Unit | Typical A‑Level Example |
|---|---|---|---|
| Wave speed | $v$ | metre per second (m·s⁻¹) | Sound in air ≈ 340 m·s⁻¹ |
| Frequency | $f$ | hertz (Hz) | Middle C note ≈ 261 Hz |
| Wavelength | $\lambda$ | metre (m) | Visible light ≈ 5×10⁻⁷ m |
Find the wavelength of a sound wave travelling at $v = 340\ \text{m·s}^{-1}$ with a frequency of $f = 500\ \text{Hz}$.
Therefore the wavelength is $0.68\ \text{m}$.
The wave equation $v = f\lambda$ links three fundamental properties of a progressive wave. It follows directly from the definitions of speed (distance per time), frequency (cycles per time), and wavelength (distance per cycle). Mastery of this relationship enables analysis of a wide range of wave phenomena encountered in A‑Level physics.