Waves and Acoustics Flashcards
The general equation for a harmonic oscillator (Sec. 1) is:
m d2ψ/dt2 = −sψ − b dψ/dt + F0 cos ωf t.
where m is the mass of the oscillator, s is a stiffness (and gives the restoring force), b is a resistance or damping and the driving force F0 oscillates at frequency ωf.
Solution of the general equation:
Acos(wt+phi)
A simple harmonic oscillator will respond at a frequency:
ω = ω0 = sqrt(s/m)
A driven harmonic oscillator will respond at:
the driving frequency ωf in the steady state
The impedance is defined as
the amplitude of the driving force divided by the complex amplitude of the oscillator velocity
Two (or more) oscillations can be
added to give a resulting oscillation
With the same frequency, the resultant can be found using
a phasor diagram or complex exponential arithmetic
• With different frequencies, the phenomenon of ____ is found. What is the equation?
ψ(t) = A cos ω1t + A cos ω2t = 2A cos ωt cos ∆ωt.
where ω = (ω1 + ω2)/2 and ∆ω = (ω1 − ω2)/2
Normal modes (Sec. 1.5) are
collective, harmonic motions of coupled oscillators
By considering combinations of the oscillators (for two, the sum and difference motions) we find
simple harmonic solutions
The wave equation (Sec. 2) is
where c is the speed of points of constant phase, or phase velocity.

Speed of a wave on a stretched string
c = sqrt(T / mu) with T the tension and µ the mass per unit length
The most general solution for the wave equation is
ψ(x, t) = f(x − ct) + g(x + ct)
When there is periodic motion, we write _____________ with k = ___ and λ (________) and ω =_____ is the angular frequency, f is the ____ and T ______ (or the time interval between two peaks or troughs)
- ψ(x, t) = f(kx − ωt) + g(kx + ωt)
- 2π/λ
- the wavelength (or distance between two peaks or two troughs)
- 2πf = 2π/T
- frequency
- time period
What is the solution for ψ(x, t), for a general periodic wave?
Aei(kx−ωt+φ)
There is energy associated with a wave: for a stretched string, the potential energy is
1/2 T A2k2sin2 (kx − ωt)
There is energy associated with a wave: for a stretched string, the kinetic energy is
1/2 µA2ω2sin2(kx − ωt)
One of the two solutions ψ =____ or ψ = ____ is called a ______ (Sec. 2.4), with the direction of travel given by ______.
- ψ = f(x − ct)
- ψ = g(x + ct)
- travelling wave
- the sign between x and t
• The impedance of a stretched string,
Z0 = √ T µ
To create a wave, a ______ must be applied
driving force FD = Z0(∂ψ/∂t)
To terminate a wave, a _____ must be applied
damping force or load FL = Z0(∂ψ/∂t)
At a boundary between different ______ we can get _______and ________, with R = ______ the reflection coefficient and T = 1 + R the transmission coefficient.
- impedances
- reflection
- transmission
- (Z1−Z2)/(Z1+Z2)
• Standing waves (Sec. 3.4) arise when
a wave is confined to a finite area with free or fixed boundary conditions
For a stretched string of length L with fixed ends, we have ψ(x, t) = ______, with kn =____ for n = 1, 2, 3, . . .
2A sinωt sin knx, with kn = nπ/L
Every point on the string moves in phase; the points with zero displacement are ____and the points with maximum displacement are ______
- nodes
- antinodes
Longitudinal wave displacement:
displacement ψ in the direction of the wave travel
• On an elastic rod, the wave motion consists of
compression and expansion of the rod
On a elastic rod, the same wave equation is obeyed, but
with different speeds.
For elastic waves on a rod with ________ A, ______ρ and ________ Y , c = ___ and Z0 = ___
- cross-sectional area
- density
- Young’s modulus
- √Y/ρ
- A √ρY
In a fluid with _____ B and _____ρ, c = ____
- bulk modulus
- density
- sgrt(B/ρ)
For an intensity (_____) of i1, the sound level in dB is defined as β = _____, with I0 = _____
- (power/area)
- 10 log10(I1/I0)
- I0 = 10−12W/m2
If a sound level β2 is n dB greater than β1, then I2 = ______
- (10n/10 )i1
A moving source and a moving observer will both lead to a change in the frequency observed. Moving observer: f0 =______ for a wave moving with velocity v and an observer moving with velocity vO
(1 + vO/v)f
• A moving source and a moving observer will both lead to a change in the frequency observed.
Moving source: ______ for a source moving with velocity vS
f 0 = fv/(v − vS)
- A moving source and a moving observer will both lead to a change in the frequency observed.
- Both moving: _______
f 0 = f(v + vO)/(v − vS)
Wave packets can be represented as a
sum of harmonic waves
• The carrier wave (the wave with the _________________) moves at the phase velocity, vp = ___
- the average frequency in beats
- ω/k
The envelope (_____________) moves at the group velocity vg = _____
- slow variation at the difference frequency in beats
- dω/dk
We can also write vg = _______
vp + kdvp/dk
The relationship between _______ω and ________k is called the _________
- angular velocity
- wavenumber
- dispersion relation
For a non-dispersive wave, ω =___
ck