Published by Patrick Mutisya · 14 days ago
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 \$x1\$ at time \$t1\$ and the same crest be observed at position \$x2\$ at a later time \$t2\$.
\$v = \frac{\text{distance travelled}}{\text{time taken}} = \frac{x2 - x1}{t2 - t1}.\$
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.