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two conditions for sources to be coherent
waves must have a constant phase difference
waves must have same frequency
superposition and interference
when waves meet, they pass through each other / overlap
at this point, they combine before they move apart - superpose
the total dispacement at a point is equal to the sum of the individual displacements at that point
for coherent waves: interference can occur - cancellation (destructive) when crest meets trough (out of phase) and reinforcement (constructive) when crest meets crest (in phase) - occur in fixed positions
two progressive waves of same speed, frequency and wavelength can superpose to produce a wave with maximum displacement
diffraction
waves spread out after passing through a gap or around an obstacle - the narrower the gap or the longer the wavelength relative to gap, the more the waves spread out
diffraction pattern most noticeable when the gap width is approximately equal to the wavelength
less diffraction / spreading out of waves means that energy is concentrated in smaller area - amplitude increases of central max of interference pattern and side fringes get closer together
refractive index
n=vc
refractive index of air is approx. 1
low to high refractie index - bends towards the normal as it slows down
Snell’s law
n1 sin theta = n2 sin theta
n1sinθ1=n2sinθ2
total internal reflection
theta c = n2/n1
occurs when ray is incident at greater than the critical angle
occurs from a higher to lower refractive index boundary
fibre optics
used in communications to carry light signals and in medical endoscopes to see inside the body
communication optical fibre allows pulses to light to enter from an transmitter and reach a receiver at the other end - must be highly transparent - minimise absorption which would otherwise reduce the energy and so the amplitude of signal the further it travels
core: propagates / guides wave by TIR with low absorption
refractive index of core greater than that of cladding
cladding; protects core from damage, prevents cross talk between touching fibres, provides clean boundary for TIR
Dispersion problems
both cause pulse broadening
Material: different wavelengths have different speeds due to different refractive indices in the core - monochromatic light will reduce this dispersion
from highest to lowest refractive index in any material: violet - red. The light with the lower refractive index will have a greater speed and shorter transit time. ( and higher critical angle)
modal: spreading of pulse / parts of a pulse take different times to travel through the fibre due to entering at diffreent angles - different paths have different lengths so effective time along fibre differs - use narrow core to reduce this dispersion - smaller range of possible paths
reduce dispersion to increase transmission rate
fibre optic core bending
angle of incidence on core cladding boundary can decrease and become less than the critical angle (which does not change)
some light will leave core and be refracted into cladding (partial reflection)
bending may cause cracks in core / cladding
amount of internally reflected light changes as a result
path difference
coherent waves that travel different distances will have a path difference - can cause phase difference
in phase (phase diff 0) if the path difference is an integer multiple of the wavelength mλ
antiphase (phase diff π rad) if path difference is an integer multiple of half the wavelength (m+21λ)
phase difference
in phase - phase difference is 0 rad
out of phase any other phase difference that is not in phase
antiphase refers to a phase difference of π rad
single slit diffraction
a central fringe that is much more intense and twice as large as lower intensity, narrower fringes on either side
maxima on either side decrease in intensity with distance from centre and are all the same width
width of central fringe W=2λD/a
where a is slit width
increasing wavelength also increases fringe spacing of subsequent maxima
range of wavelengths - central maximum unchanged - other maxima gradually getting broader / more spread out for greater order maxima
young’s double slit
light passes through a single narrow slit first which acts as a single source diffracting light to both slits - the path lengths between the single slit and the double slit are constant / fixed / the same
this light then passes through two closely spaced double slits which act as cohernt sources of waves
alternate dark and bright fringes can be seen on a screen which are caused by the interference of light from the two slits
equally spaced
width of central diffraction fringe W=2λD/a
fringe spacing w=λD/s
white light interference pattern - intense central white fringe as all wavelengths arrive here - fringes either side each showing range of colours / spectrum - red furthest on outside of fringe and violet closest on inside of fringe to centre - difference wavelengths mean that the two fringe patterns do not overlap exactly
bright and dark fringes
light from both slits undergoes diffraction
waves meet and superpose at a point
at a maxima, they path difference is a whole number of wavelenths so are arriving in phase - reinforce constructively - peaks meet peaks and troughs meet troughs - total amplitude increases
moving away from the maxima point introduces a path difference that is not a whole number of wavelengths - destructive reinforcement - partial cancellation and amplitude decreases
At a minima, waves arrive completely out of phase
moving away, waves move back in phase
diffraction grating
many closely spaced parallel slits
monochromatic light incident normally - light transmitted in certain directions only as light passing through each slit is diffracted - interferes constructively in certain directions and destructively in other directions
central maximum is 0th order
dsinθ=nλ
the maximum possible angle of an order is 90 - total number of maxima given by 2n+
higher order are less well defined / dimmer - harder to observe than lower orders
diffraction grating uses
to analyse chemical compositionn of a sample
to determine wavelength of a light source
to provide a monochromatic source / select a particular colour of laser light
uncertainty - diffraction grating
measure across all visible maxima / choose a higher order maxima
this increases the distance measured, reducing the percentage uncertainty in sin theta
needed to calculate wavelength so percentage uncertainty in wavelength decreases
or
increase screen to grating distance
this increases the fringe spacing
decreases percentage uncertainty in both
needed to calculate wavelength so percentage uncertainty in wavelength decreases
a value that involves fewer readings has a lower percentage uncertainty
there may be difficulty in locating exact position of centre of each spot / lining up ruler
to ensure a light ray doesn’t devatiate
same material / same refractive index
no gaps
effect of refractive index of a material varying by a few percent across it
variation may be too small to deviate the ray significantly within the material
or
may cause a summative effect when multiple reflections at boundary occur, changing direction of ray
transmitter and receiver arranged in a line with metal plate parallel to both
reading at receiver depends on the superposition of waves travelling directly to R and other waves that reach it after reflecting off the metal sheet
as the metal sheet is moved away, the reading at the receiver continuously fluctuates from decreasing to a minimum and increasing to a maximum
does not reach 0 as waves reflected at metal plate loose some energy through absorption - intensity decreases - amplitude decreases - combining waves do not have the same amplitude - not complete cancellation even when 180 degrees out of phase
or if it is not a point source / receiver so imperfect calcellation