Published by Patrick Mutisya · 14 days ago
Explain the principle of superposition and use it to derive the properties of stationary (standing) waves in strings and air columns.
Consider two sinusoidal travelling waves of equal amplitude \$A\$, angular frequency \$\omega\$ and wave‑number \$k\$, moving in opposite directions along the \$x\$‑axis:
\$y_1(x,t)=A\sin(kx-\omega t)\$
\$y_2(x,t)=A\sin(kx+\omega t)\$
Applying the superposition principle, the resultant displacement is
\$y(x,t)=y1+y2=2A\sin(kx)\cos(\omega t)\$
or, using the identity \$\sin\alpha\cos\beta = \tfrac12[\sin(\alpha+\beta)+\sin(\alpha-\beta)]\$, the same result can be written as
\$y(x,t)=2A\cos(kx)\sin(\omega t)\$
Both forms describe a standing wave: the spatial part (\$\sin(kx)\$ or \$\cos(kx)\$) determines the positions of nodes and antinodes, while the temporal part (\$\cos(\omega t)\$ or \$\sin(\omega t)\$) describes the oscillation of each point.
From \$y(x,t)=2A\sin(kx)\cos(\omega t)\$:
Since \$k=2\pi/\lambda\$, the distance between adjacent nodes (or antinodes) is \$\lambda/2\$.
| System | Boundary Conditions | Allowed Wavelengths | Fundamental Frequency \$f_1\$ |
|---|---|---|---|
| String | Both ends fixed | \$\lambda_n = \dfrac{2L}{n}\;(n=1,2,3,\dots)\$ | \$f_1 = \dfrac{v}{2L}\$ |
| Open–Closed Pipe (organ pipe) | One end open, one end closed | \$\lambda_n = \dfrac{4L}{2n-1}\;(n=1,2,3,\dots)\$ | \$f_1 = \dfrac{v}{4L}\$ |
| Open–Open Pipe (organ pipe) | Both ends open | \$\lambda_n = \dfrac{2L}{n}\;(n=1,2,3,\dots)\$ | \$f_1 = \dfrac{v}{2L}\$ |
\$f1 = \frac{v}{\lambda1}= \frac{1}{2L}\sqrt{\frac{T}{\mu}}.\$
Problem: A string 1.20 m long is fixed at both ends and under a tension of 80 N. Its linear mass density is \$2.0\times10^{-3}\,\text{kg m}^{-1}\$. Find the frequencies of the first three harmonics.
Solution:
\$v = \sqrt{\frac{T}{\mu}} = \sqrt{\frac{80}{2.0\times10^{-3}}}= \sqrt{4.0\times10^{4}} = 200\ \text{m s}^{-1}.\$
\$f_1 = \frac{v}{2L}= \frac{200}{2\times1.20}= \frac{200}{2.40}=83.3\ \text{Hz}.\$
\$\$f2 = 2f1 = 166.7\ \text{Hz},\qquad
f3 = 3f1 = 250.0\ \text{Hz}.\$\$
The principle of superposition allows us to combine two identical travelling waves moving in opposite directions to form a stationary wave. The resulting pattern is characterised by nodes and antinodes, with a spatial separation of \$\lambda/2\$. Boundary conditions dictate the permissible wavelengths and thus the discrete set of resonant frequencies (harmonics). Mastery of these concepts enables analysis of musical instruments, resonant cavities, and many A‑Level exam questions.