Waves I Formulas Flashcards
Sinusoidal Waves
y( x, t) = ym sin (kx - ωt)
note: ym is the amplitude
k is the angular wave number
kx - ωt is the phase
ω is the angular frequency
wavelength relationship to angular wave number (k)
k = 2π/λ
Relationship of period and frequency of the wave to ω
ω/2π = f = 1/T
wave speed (v) relation to k, f, T, ω, λ
v = ω/k = λ/T = λf
Equation of a travelling wave
y(x, t) = h (kx ± ωt)
Wave speed on stretch string
v = sqrt( tension/linear density)
note: density symbol = μ
Average power (sinusoidal wave on a stretched string)
Pavg = 1/2 μvω^2y^2
Interference of waves
y’(x, t) = [2ycos 1/2 Φ] sin (kx - ωt + 1/2 Φ)
note:
if Φ = 0 the waves are exactly in phase; interference is fully constructive
if Φ = πrad, waves are exactly out of phase; interference is fully destructive
Standing waves (string with fixed ends)
y’ (x, t) = [2y sin kx] cos ωt
Resonance frequency for a stretched string w/ fixed ends
f = v/λ = nv/2L
for n = 1,2,3
note: n = 1 [first harmonic], n = 2 [second harmonic]
Speed of sound wave
v = sqrt(B/ρ)
note: B = bulk modulus
Longitudinal displacement amplitude
s = sm cos (kx - ωt)
note: sm = displacement amplitude
equilibrium
k = 2π/λ ; ω = 2πf
pressure change caused by the wave
Δp = Δpm sin (kx - ωt)
pressure amplitude
Δpm = (vρω)sm
Interference two sound waves
Φ = (ΔL/λ) × 2π
what Φ does fully constructive interference occur?
Φ = m(2π)
note: for m = 0, 1, 2,….
and ΔL/λ = 0, 1, 2, …
what Φ does fully destructive interference occur?
Φ = (2m + 1)π
note: for m = 0, 1, 2,….
Φ is an odd multiple of π
and ΔL/λ = 0.5, 1.5, 2.5, …
Sound Intensity
I = P/A
P is the time rate of energy transfer (power) of the sound wave, A is the area
Relationship of Intensity to the displacement amplitude (sm)
I = 1/2 ρvω^2s^2
Intensity at a distance r from a point source that emits sound waves of power Ps
I = P/(4πr^2)
Sound level in decibels (β)
β = (10dB) log I/I0
Note: I0 = 10^(-12) W/m^2
Standing wave patterns (pipe open at both ends)
f = v/λ = nv/2L
n = 1, 2, 3…
Standing wave patter (pipe closed on one end and open at the other)
f = v/λ = nv/4L
n = 1, 3, 5…
General doppler effect
f’ = f × [( v ± vp ) / ( v ± vs )]
note:
vp is the speed of the detector relative to the medium
vs is that of the source
v is the speed of sound in the medium
The signs are chosen such that f’ tends to be greater for motion toward and less for motion away
Mach cone angle (shock wave)
sin θ = v/vs
*happens when the speed of a source relative to the medium exceeds the speed of sound in the medium
- doppler no longer applies