Wave Optics and Diffraction Part 1 Flashcards

1
Q

What is the general exponential function for a stationary wave and what is its trig function equal to?

A

exp(-ikx) = coskx + isinkx

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2
Q

What is the wavenumber, k, equal to?

A

k = 2π/λ = ω/c

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3
Q

How do we know if a wave is right or left travelling?

A
  • Rearrange exponent by taking out k
  • Phase of wave Ф = k(x-ct) = const
  • Rearrange to find x = const + ct, so is moving is +ve x-direction
  • Left travelling wave has opposite sign
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4
Q

What is the function for a right-travelling wave?

A

u(x,t) = A*exp(-i(kx-ωt))

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5
Q

How do we check that a wave function is a solution to the wave equation? What can we use this for?

A

Plug it into the wave equation. Can use this to find equations for variables (wave equation can only hold if these relationships are true)

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6
Q

How do we write a wave function in more than one dimension?

A

u(r,t) = G*exp(-i(kr-ωt))

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7
Q

What can we do to understand the wavenumber k?

A
  • Imagine surface of constant phase, Ф = kr-ωt = const + 2nπ
  • Wave is family of planes separated by λ = 2π/|k|
  • Sub in k = k(hat) * |k| and rearrange for k(hat)*r
  • Find that k(hat)*r = d, the distance from origin to closest point on plane
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8
Q

What is another way of writing the k vector?

A

k(hat) * |k|

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9
Q

What do both the terms mean in the equation for k(hat)*r?

A

The first part is d0, the distance to surface of plane at t=0, the second part is the distance after time t, moving away are speed c

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10
Q

What do we get from taking a fourier transform of a right-moving 1D wave?

A
  • u(k,ω) tells us how much of each wavenumber and frequency we have in real life space signal
  • u(k’,ω’) = 𝛿(k’+k)*𝛿(ω’+ω)
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11
Q

What are 3 real world phenomena with wave-like properties?

A
  • Acoustics
  • Optics
  • Quantum Mechanics
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12
Q

In interference, when is it destructive or constructive?

A

Destructive if 2 waves have phase difference (n+1/2)λ, constructive if nλ.

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13
Q

What is Huygens principle of secondary sources?

A

Consider slits to have point sources inside them, and the interference is the superposition to the waves coming from all of these sources.

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14
Q

What are two equations for the intensity (power per unit area) of a point source and how can these be used?

A
  • I = 4πr^2 = const = u^2

- Can use this to show that u ∝ 1/r

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15
Q

How can we start to find a solution to the 3d wave equation of the form u(r,t) = v(r,t)/r?

A

Use wave equation but instead of d^2u/dx^2, have ∇^2 u in 1d

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16
Q

What is ∇^2 u equal to?

A

= 2/r * du/dr + d^2u/dr^2

17
Q

What do we find ∇^2 is equal to after subbing in u(r,t)?

A

1/r * d^2v/dr^2

18
Q

What is the finding after subbing in ∇^2 to the wave equation?

A

Takes same form as normal wave equation.

19
Q

What is the solution to the new wave equation in 3D?

A

v(r,t) = Aexp(ik(r/ct))+Bexp(ik(r+ct)), and u(r,t = v(r,t)/r

20
Q

What do we do to the B term in the solution to the 3D wave equation and why?

A

Set it equal to zero as we only want to look at waves travelling away from aperture not towards.

21
Q

Which two coordinate systems do we need to consider?

A

One on the aperture screen (y1,y2,y2) and one of the detector screen (x1,x2,x3)

22
Q

What are the position vectors y and x for the two screens and why?

A

y = (y1, y2, 0) since the origin lies in centre of aperture so the “z” part is zero

x = (x1, x2, D), since the detector screen is a distance D from the origin

23
Q

What is the equation for the amplitude of light at x and t from y, and what is r equal to?

A

1/r * exp(ik(r-ct))

r = x-y = |x-y|

24
Q

How do we add together all the separate sources amplitudes?

A

Do a sum over i and keep the x values the same but A and y have i values (change for each source)

25
Q

What is a good way of starting the sum to find the phase difference?

A
  • Only have 2 point sources at y1 and y2, y1 = y and y2 = 0
  • l1 = |x-y|
  • l2 = |x-0| = |x|