Standing Wave
Trap a wave between two fixed ends and it stops traveling — freezing into a pattern of motionless nodes and violently swinging antinodes.
Standing Wave
A standing wave is what a traveling wave becomes when it is confined. Tie a string down at both ends, send a wave along it, and the reflections from the two ends superpose with the incoming wave. For most frequencies the result is a mess, but at special resonant frequencies the pattern locks into place: certain points, the nodes, never move at all, while points halfway between them, the antinodes, swing with maximum amplitude. The wave no longer travels — it stands.
Mathematically it is two identical traveling waves going opposite directions, summed via the Superposition Principle:
Notice that x and t have separated. The spatial shape \sin(kx) is frozen; only its overall height breathes in and out as \cos(\omega t). Every point oscillates in lockstep — that is precisely a normal mode, the same object you met for Coupled Oscillators, now with infinitely many beads.
The harmonic ladder
Fixed ends force the string to hold a node at each end, so only whole numbers of half-wavelengths fit: L=n\lambda/2. That quantizes the allowed frequencies into a ladder:
The lowest, f_1, is the fundamental; the rest are its Harmonics — exactly the integer-multiple frequencies that a Fourier Series uses to build any periodic shape. This is why a plucked string sounds like a definite musical pitch: it can only ring at f_1,2f_1,3f_1,\dots
Resonance and instruments
You can only excite a standing wave by driving the string near one of its f_n — drive off-resonance and the reflections fight the input. This is Resonance in spatial form: the boundary conditions pick out the natural frequencies, and energy pours in only when you match one. Strings, organ pipes, drumheads, and the cavity of a laser all work this way; the shape of the boundary chooses which Harmonics are allowed to ring.