waves Flashcards
transverse wave
elements move perpendicular to direction of propagation
longitudinal wave
elements move parallel to direction of propagation
y(x,t) for sinusoidal wave
y(x,t) = A sin[(2π/λ)(x - vt)]
velocity of wave
v = λf
wave number
k = 2π/λ
angular frequency
ω = 2π/T
wave max velocity
vmax = ωA
wave max acceleration
amax = ω2A
speed of waves on string
v = √(T/μ)
- T -> Tension*
- μ -> mass per unit length*
rate of energy transfer in sinusoidal wave
P = 1/2(μω2A2v)
general linear wave equation
∂2y/∂x2 = (1/v2)∂2y/∂t2
speed of sound in medium
v = √(B/ρ)
B -> bulk modulus of material
Pressure variation in sound wave
ΔP = ΔPmaxsin(kx-ωt)
max pressure in sound wave
ΔPmax= ρvωsmax
Intensity of wave (general)
I = P/A
intensity of sound wave
I = 1/2ρv(ωsmax)2= ΔP2max/2ρv
intensity of spherical wave
I = Pavg/4πr2
sound level in decibals
β = 10 log(I/I0)
I0 -> reference intensity
frequency of sound with observer moving towards source
f’ = f(v+vo)/v
- vo -> velocity of observer*
- speed of sound remains constant, wavelength and frequency change*
frequency of sound with observer moving away from source
f’ = f(v - vo)/v
doppler shift
f’ = f(v + v0)/(v - vs)
moving closer -> increases frequency
moving apart -> decreases frequency
mach angle
sinθ = v/vs
wave function of standing wave
y = (2Asin(kx))cos(ωt)
distance/definition between antinodes
antinodes are points of maximum displacement
distance is λ/2
distance between nodes
nodes are points of 0 displacement
distance between nodes is λ/2
distance between node and antinode
λ/4
frequency of standing wave in string
fn = n/(2L)√(T/ μ)
wavelength of standing wave in string
λn = 2L/n
node or antinode at open end of pipe?
antinode
node or antinode at closed end of pipe?
node
natural frequency of pipe open at bothe ends
fn = nv/2L
v -> speed of sound in air
natural frequency of pipes closed at one end, open at another
fn = nv/4L
beat frequency of 2 sound waves
fbeat = |f1 - f2|