y = A sin(kx - omega t + phi)
y equals A sine of the quantity k x minus omega t plus phi, describing a harmonic wave travelling in the positive x direction.
Describes a harmonic wave travelling in the +x direction.
- A
- amplitude (m)
- y
- displacement (m)
- x
- position (m)
- k
- angular wave number (rad/m)
- omega
- angular frequency (rad/s)
- phi
- initial phase (rad)
Use when — Modelling a sinusoidal progressive wave.
Common trap — Reading particle velocity as wave speed.
k = 2 pi / lambda ; omega = 2 pi f
k equals two pi over lambda, and omega equals two pi times f.
Connects the spatial and temporal angular rates of the wave to wavelength and frequency.
- lambda
- wavelength (m)
- f
- frequency (Hz)
Use when — Any harmonic wave.
Common trap — Mixing cycles with radians.
v = omega / k = f lambda
v equals omega over k, which equals f times lambda.
Gives the phase speed of the wave.
- v
- phase speed (m/s)
Use when — A nondispersive relation for the stated wave.
Common trap — Assuming frequency changes wave speed in a fixed ideal medium.
v = sqrt(T / mu)
v equals the square root of T over mu.
Gives the speed of small transverse waves on an ideal stretched string.
- T
- tension (N)
- mu
- linear mass density (kg/m)
Use when — Small transverse waves on a uniform taut string.
Common trap — Using total mass instead of linear density.
f_n = (n / 2L) sqrt(T / mu)
f sub n equals n over two L, times the square root of T over mu.
Gives the normal-mode frequencies of a string fixed at both ends.
- f_n
- nth mode frequency (Hz)
- L
- string length (m)
- n
- mode number, n = 1, 2, ...
Use when — A string fixed at both ends.
Common trap — Using closed-pipe mode rules on a string problem.
f_n = n v / (2L)
f sub n equals n v over two L.
Gives the ideal normal-mode frequencies of a pipe open at both ends.
- f_n
- nth mode frequency (Hz)
- v
- speed of sound in the gas (m/s)
- L
- pipe length (m)
Use when — Both ends open, end correction neglected.
Common trap — Treating pressure and displacement nodes as identical.
f_n = (2n - 1) v / (4L)
f sub n equals the quantity two n minus one, times v, over four L.
Gives the ideal normal-mode frequencies of a pipe closed at one end.
- n
- mode number, n = 1, 2, ...
Use when — One end closed, end correction neglected.
Common trap — Including even harmonics in the ideal one-closed-end model.
f_b = |f_1 - f_2|
f sub b equals the absolute value of f one minus f two.
Gives the beat frequency produced by two nearby coherent frequencies.
- f_b
- beat frequency (Hz)
Use when — Nearby coherent audible frequencies.
Common trap — Confusing the beat rate with the average pitch.
f' = f (v ± v_o) / (v ∓ v_s)
f prime equals f times the quantity v plus or minus v sub o, over the quantity v minus or plus v sub s.
Gives the classical Doppler-shifted frequency heard for sound, an Advanced-scope relation.
- f'
- observed frequency (Hz)
- v
- speed of sound in the medium (m/s)
- v_o
- observer speed relative to the medium (m/s)
- v_s
- source speed relative to the medium (m/s)
Use when — Straight-line source and observer motion in a medium, JEE Advanced scope.
Common trap — Choosing signs from memory instead of from an approach-or-recession sketch.