Optics, Waves, Lasers 2 Flashcards

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1
Q

displacement of wave - angular

A

y(x,t)=Acos{wt}

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2
Q

displacement of wave - linear

A

y(x,t)=Acos{2pift}

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3
Q

displacement of wave if wave travelling with speed v

A

y(x,t)=Acos{w(t-x/v)}

can be other way around since cos theta = cos -theta

can also change depending on what variables given (w=2pif, f=1/T)

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4
Q

wave number

A

k=2pi/lambda

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5
Q

phase of wave

A

{kx+/-wt}

radians

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6
Q

wave speed

A

v=dx/dt=w/k

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7
Q

expressions for transverse velocity and acceleration

A

differentiating equation for y (partial diff)

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8
Q

wave equation

A

consider d2y/dt2 / d2y/dx2 = v^2

rewrite as d2y/dx2=1/v^2 d2y/dt2

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9
Q

combining hookes law with acceleration in SHM

A

ax=Fx/m=-kx/m

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10
Q

energy in SHM

A

1/2mv^2+1/2kx^2=constant

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11
Q

maximum displacement in SHM

A

energy is entirely potential energy (no kinetic)

can rearrange this formula for v

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12
Q

total displacement

A

algebraic sum of displacements

*might need to use cos(a+/-b)=cosacosb-/+sinasinb

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13
Q

principle of superposition

A

when two or more waves overlap, the resultant displacement at any point and at any instant is found by adding the instantaneous displacements that would be produced at the point by the individual waves if each were present alone

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14
Q

standing wave

A

wave shape stays the same

zero points found when sin(kx)=0

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15
Q

coherent

A

two monochromatic sources of same frequency and constant phase relationship

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16
Q

constructive interference

A

if waves from two or more sources arrive in phases, then they reinforce each other

r2-r1=m lambda

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17
Q

destructive interference

A

meet exactly out of phase
“cancel out”

resulting amplitude is difference of individual As, ie if same = 0

r2-r1=(m+1/2)lambda

18
Q

most reliable way to ensure light from two sources remains in phase

A

use of slits

19
Q

slit experiment

A

light through one slit then either of two

shone onto screen

bright spots=constructive

20
Q

approximate geometry used in slit experiment

A

treat rays as paraleel so r2-r1=dsintheta

can do this because distance R to screen&raquo_space; distance d between slits

21
Q

expression to find centres of bright bands on the screen

A

let ym be distance from centre to centre of mth bright band

theta m be corresponding angle for band

ym=Rtanthetam

since R»d, thetam very small so tantheta=sintheta

so sinthetam=ym/R

so dsintheta=dym/R=m lambda

hence ym=Rmlambda/d

22
Q

assumption in interference in thin films

A

assume light comes in almost vertically

23
Q

monochromatic light shining on air wedge

A

would expect pattern of C and D interference

in reality, pattern is reversed, dark regions at integer multiple and bright at 1/2 integer multiples. Phase shift is a result of Maxwell’s equations, EM nature of light

24
Q

na>nb

A

slow in first
Ei and Er same sign, no phase shift between incident and reflected

25
Q

na=nb

A

no refletion

26
Q

na<nb

A

slow in 2nd

Ei and Er opposite signs

phase shift or reflected relative to incident is pi radians

27
Q

let thickness of film bet t, if neither or both reflected waves have phase shift then

A

2t=mlambda CON

2t=(m+1/2)lambda DEST

28
Q

let thickness of film bet t, if one of the reflected waves have phase shift then

A

2t=mlambda DEST

2t=(m+1/2)lambda CON

29
Q

newtons rings

A

convex surface in contact with plane glass surface, creating a thin air film

circular interference pattern

30
Q

to avoid glare, need

A

destructive interference

31
Q

Huygen’s principle

A

from shape of wave at some instant, can work out shape at later time

new wave found by building a surface that is tangential to secondary wavelets

drawing diagram and zooming in shows low of refelction

32
Q

refractive index

A

ration of speed of light in vacuum to material

33
Q

diffraction

A

bending of light around obstacles

34
Q

spontaneous emission

A

direction and phase of photons emitted are random

shining light to absorb photon. Excited atoms return to ground energy and emit photon

35
Q

stimulated emission

A

each incident photon encounters a previously excited atom. Each excited atom emits a second photon with same frequency, direction and phases as incident photon.

two photons in phase - coherent

36
Q

number of atoms in state i

A

ni=Aexp{-Ei/kbT

therefore less atoms exist in higher energy states - negative exponenet

37
Q

population inversion

A

number of atoms in excited state > lower energy state

rate of energy radiation by stimulated emission can exceed rate of absorption, system will act as a net source of radiation

38
Q

steps to create population inversion

A
  1. material pumped to excite atoms. (gas - electrodes used) High enough voltage, electric discharge occurs. Collision of atoms and electrons excite atoms
  2. spontaneously emit, states depopulated. Atoms pile up in E2 as long lifetime. E2 more populated than E1
  3. some E2 will transition to E1 and give off photons. Parallel mirrors send photons back and forth through gas, creating stimulated emission. Laser beam leaves as one mirror is partially trasnparent to desired wavelength
39
Q

holography

A

technique for recording and reproducing an image of an object through the use of interference effects

40
Q

how to make a hologram

A

illuminate object with monochromatic laser

place photographic film so that it is struck by scattering light and direct light

interference of the light forms interference pattern on film

to view: shine light through developed film creating virtual and real images