Chapter 5 - Transverse Wave Motion Flashcards
Name the three distinct wave velocities associated with transverse waves.
- The particle velocity: Which is the simple harmonic velocity of the oscillator about is equilibrium position. (∂y/∂t)
- The wave or phase velocity: The Velocity with which planes of equal phase, crests or throughs, progress through the medium. (∂x/∂t)
- The group velocity: A number of waves of different frequencies, wavelengths and velocities may be superimposed to form a group.
Give the wave equation.
∂2y = 1 ∂2y
∂x2 c2 ∂t2
Where
c = T/p, (Tension on string/linear density)
What is the solution of the wave equation?
y = a sin(ωt – ϕ) = a sin (2π/λ) (ct – x)
Where:
- ω = 2πc/λ
- ϕ = 2πx/λ (The phase lag between the oscillator at x = 0 and x)
- λ is defined as the wavelength (Distance between x when the phase difference in 2π rad).
- Note that c can also be written as c = vλ.(The product of frequency and wavelength)
Give 4 equivalent expressions for y = f(ct-x) (Could be sine of cosine)
y = a sin (2π/λ) (ct-x)
y = a sin (2π) (vt – x/λ)
y = a sin ω(t – x/c)
y = a sin (ωt – kx)
y = aei(ωt – kx)
Where k = 2π/λ = ω/c which is called the wave number.
What is the wave number?
The wave number is:
k = 2π/λ = ω/c
Define the impedance of a string.
Z = transverse force = F
transverse velocity v
OR
Z = T/c = pc (Since T = pc2)
What would happen when a wave travelling along a string with impedance Z1 travel across a section with impedance Z2?
Part of the wave will continue in the region of impedance Z2 and part would be relected into the region Z1.
- What is the reflection coefficient amplitude
- Give the equation of the reflection coefficient amplitude
- What is the transmission coefficient amplitude
- Give the equation od the transmission coefficient amplitude
- The reflection coefficient amplitude is the ratio of the reflected wave amplitude to the incident wave amplitude.
- B1/A1 = (Z1-Z2)/(Z1 + Z2)
- The transmission coefficient amplitude is the ration of the transmitted wave amplitude to the incident wave amplitude.
- A2/A1 = (2Z1)/((Z1 + Z2)
- Explain what would happen when the end of the string is fixed.
- Explain what would happen when the end of the string is loose.
- If the end of the string is fixed, then Z2 = ∞, so that B1/A1 = -1, thus the wave is completely reflected but has a phase change of π.
- If the end of the string is loose, then Z2 = 0, so that B1/A1 = 1 and A2/A1 = 2, which explains the ‘flick’ of the loose end. (double the amplitude).
- What is the reflected intensity coefficient.
- Give the equation of the reflected intensity coefficient.
- What is the transmitted intensity coefficient.
- Give the equation of the transmitted intensity coefficient.
- The reflected intensity coefficient is the ratio of the reflected wave energy to the incident wave energy.
- Reflected energy = Z1B12 = (B1/A1)2 = [(Z1 – Z2)/(Z1 + Z2)]2
Incident energy Z1A12
- The transmitted intensity coefficient is the ration of the transmitted wave energy to the incident wave energy.
- Transmitted energy = Z2A22 = (2Z1Z2)/(Z1 + Z2)2
Incident energy Z1A12
Describe how you would math two impedances of Z1 and Z3 for a wave of wavelength λ.
The impedances are mathed when a object with impedance:
Z2 = sqrt(Z1Z3)
with a length of
l = λ\4
is inserted between Z1 and Z3.
This is true for waves in all media.
How is the normal mode frequencies or modes of vibration defined on a string of length l?
At which points will the string remain at rest?
sin (ωnx/c) = sin (nπx/l)
The string will remain at rest where:
sin (ωnx/c) = sin (nπx/l) = 0
or
nπx/l = rπ ( r = 0,1,2,3,…,n)
- When will a standing wave ratio be applicable.
- Give the equation for the standing wave ration.
- How can the reflection coefficient be calculated from the minumum and maximum amplitudes.
- If energy is lost between the incident and reflected waves, then the amplitudes will not completely cancel resulting in a standing wave. (no nodes).
- Standing wave ratio = (A1 + B1)/(A1 - B1) = (1 +r)(1-r), where r is the reflection coefficient (B1/A1).
- r = B1/A1 = (SWR - 1)/(SWR + 1)
- Give the equation of the observed frequency when the source is moving and the observer stationary.
- Give the equation of the observed frequency when the observer is moving and the source stationary.
- Give the combination if both observer and source are moving.
- v’ = vc/(c-s)
- v’’ = v(c-o)/c
- v’’’ = v(c-o)/(c-s)