Waves Flashcards

1
Q

What do waves do?

A

Transport momentum and energy without transporting matter

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2
Q

Transverse Wave

Definition

A

Disturbance is perpendicular to the direction of propagation

E.g. Waves on a string, EM waves

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3
Q

Longitudinal Wave

Definition

A

Disturbance is parallel to the direction of propagation

E.g. Sound, primary seismic

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4
Q

What does the speed of a transverse wave on a string depend on?

A

String tension
Mass per unit length

  • the greater the tension, the faster the Wave
  • Wave velocity is greater in a lighter string
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5
Q

Travelling Wave

Definition

A

A wave pulse that has constant shape but moves with speed v

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6
Q

Wave on a String

Wave Function

A
  • string lies on the X axis at equilibrium

- the function y(x,t) defines the shape of the string at a given instant

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7
Q

General form of the wave function for a travelling wave on a string

A

y(x,t) = g(x-vt)

For a wave moving to the right with speed v

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8
Q

The Wave Equations

A

d²y/dx² = μ/T d²y/dt²

v² = μ/T

T = tension
v = velocity
μ = mass per unit length
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9
Q

Solutions to the Wave Equation

Stationary Wave

A

g(x) = Asin(2π/λ * x)

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10
Q

Solutions to the Wave Equation

Harmonic Wave Moving to the Right

A

g(x) = Asin(2π/λ(x-vt))

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11
Q

Harmonic Wave

A

A sinusoidal wave

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12
Q

Solution to the Wave Equation

Harmonic Wave

A

y = Asin(kx-ωt)
This assumes y=0 at x=0 and t=0

For more general initial conditions:
y = Asin(kx-ωt+d)

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13
Q

Kinetic Energy of a Wave Travelling Along a String

A

KE = 1/2 μΔxω²A²cos²(kx-ωt)

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14
Q

Elastic Potential Energy of a Wave Travelling Along a String

A

For a wave to move along a string, the wave has to stretch

EPE = 1/2 μΔxω²A²cos²(kx-ωt)

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15
Q

Energy of a Wave Travelling Along a String

A

KE and PE of the string segment are equal

E = μΔxω²A²cos²(kx-ωt)

But this energy is constantly varying with t and x so we average the energy over 1 Period

Eav = 1/2 μΔxω²A²

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16
Q

Power

Definition

A

Energy transmitted per unit time

17
Q

Power of a Wave on a String

Equations

A

Pav = 1/2 μω²A²v

Pmax = 2Pav

18
Q

Maximum Segment Velocity in the y Direction

A

Vmax = ωA

19
Q

Wave Impedance

Definition

A

Velocity response to a driving force

Large impedance means a small velocity response

20
Q

What does wave impedance depend on?

A

String tension and mass

21
Q

Wave Impedance

Equation

A

Z = F/v

22
Q

Reflection Coefficient

A

r = (Z1 -Z2) / (Z1 + Z2)

23
Q

Transmission Coefficient

A

t = 2Z1 / (Z1 + Z2)

24
Q

When does complete transmission occur?

A

Only if impedances are matched

25
Q

Transmission and Reflection

Fixed endpoint

A

Z2 = infinity
r = -1
t = 0
Reflected Wave has reverse direction and opposite sign (negative amplitude)

26
Q

Transmission and Reflection

Freely movable end point (e.g. End of string)

A

Z2 = 0
r = 1
Reflected Wave is the right way up

27
Q

Power Reflection and Transmission

A

Pr/ Pi = r² = (Z1-Z2 / Z1+Z2)²

28
Q

Principle of Superposition

A
  • obeyed by linear waves
  • if two or more waves are moving through a medium, the resultant wave function at any point is the sum of the wave functions of the individual waves
29
Q

Reflection of Harmonic Waves

A
  • if a harmonic wave travels on a string fixed at the end, it is reflected, incident and reflected waves superimpose
  • 2 sinusoidal waves with same amplitude, frequency and wavelength but travelling in opposite directions

y = 2A0 sin(kx) cos(wt)

Every part of the string vibrates in SHM with the same f and phase unlike a travelling harmonic wave where amplitude is constant but phase is different