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Waves: Revision
Definiton
Representing Waves
Types of waves
Definition: A propagating disturbance that transport energy through a medium.
Propagation – way the wave travels/moves
Medium – matter that a wave moves through
Oscillate – to move back and forth between two points
Waves transfer energy from without moving matter
Waves are oscillating particles
Representing Waves
Wave fronts – a line that represents the crest of the wave (birds eye view of wave)
Distance between them is the wavelength
Rays – a line that shows directions of the wave travels (perpendicular to wavefronts)
Angles of rays are measured relative to the normal
Types
transverse - direction of particle oscillation is perpendicular to propagation
longitudinal - direction of particle oscillation is parallel to propagation
mechanical - changing in kinetic and gravitational energy
EM - change in electric and magnetic energy
Early Classical Models of Light: Huygens vs. Newton
Newton vs Huygens: Reflection
Through observations, light was known to reflect of smooth surfaces following the Law of Reflection: The angle of incidence = the angle of reflection
Newton vs Huygens: Refraction
The bending of waves as they travel from one medium into another
Angle of incidence = 0°, Angle of refraction = 0° (no refraction, but speed will change)
Frequency stays the same for the incident and refracted waves → v and λ change
Dispersion – when colours refract by different amounts, and spread out into a rainbow
Refraction is described by Snell’s Law:
Wave moves to denser medium = it slows down (wavelength decreases + frequency stays constant) = bends towards normal
Wave moves to less dense medium = speeds up (wavelength increases + frequency stays constant) = bends away from normal
Relative speed of light in air and water
In 1850, Leon Foucault performed an experiment that determining whether light travelled faster in air or water.
Method |
Since, it takes time for light to travel from mirror R, to mirror M, back to mirror R, we can compare the point the beam lands on the screen when putting a different medium between mirror R and M |
Result |
This shows that light travels slower through water, as the mirror R had more time to rotate to a steeper position, and thus have a greater angle of incidence from mirror M |
Impact on the model of light | This proved that Newton’s model was incorrect, as he believed light travelled faster in a denser medium, when it in fact, does not. |
Diffraction of light
the bending of waves around obstacles and through gaps
Speed, frequency or wavelength don’t change when a sound wave is diffracted
Diffraction effect is greatest when the width of the gap is about the same size as the wavelength of the wave
Occurs when a wave: passes an edge, passes through a narrow gap, goes past an object
Explaining diffraction with huygens’ principle
The wavelets away from the barrier interface interfere and cancel out in all directions other than the forwards direction producing a straight propagating wavefront
Wavelets hitting the barrier are blocked and produce no waves
Wavelets near edges that are free to propagate (since there are no other wavelets to interfere with) produce curved wavefronts
Newton’s theory could not explain diffraction
Interference
the superposition of two or more waves
Depending on the relative phase of the superimposed waves, two different types of interference can occur:
Constructive interference – amplitudes of each wave produce a higher amplitude
Destructive interference – amplitudes of each wave produce a lower amplitude
Single vs double slit vs diffraction grating
Single | Double | Grating |
When light passes through a slit, it diffracts → The closer the aperture is to the wavelength of light, the more obvious diffraction is The slit acts as a new point source of light This point source consists of many self-propagating wavelets which interfere to make a wavefront The most outside wavelets (ones closest to the edge of the gap) cannot interfere with other wavelets since they are blocked, so they spread around to form a curved wavefront The interference of these wavelets makes the diffraction pattern | Thomas Young: Devised in 1801 to demonstrate that light is a wave → light undergoes diffraction and interference (wave phenomena)
Diffraction of white light
| We pretend it’s like many double slit experiments next to each other |
d = the distance of the gap/aperture (m) m = the ‘order’ of minima (dark fringes) | d= distance between double slit m = order of maxima | d = the distance between two adjacent slits = total distance ÷ number of lines m = the ‘order’ of maxima |
Max Number of maxima
For a particular wavelength of light and distance (d) between slits, the number of orders (m) of bright spots (maxima) is finite
A maximum cannot form more than 90 degrees from the midline between the two slits.
Thus, the angle at which the furthest maximum is formed must be smaller than 90°
Substitute an angle of 90° into the diffraction equation, the greatest order of maxima is given by: m=d/λ
The greatest order is the largest integer lower than the calculated value
Polarisation
the orientation of a wave’s oscillations (its plane of oscillation)
Proved that light was a transverse wave
Huygen assumed it was longitudinal, and longitudinal waves cannot be polarised since they are one dimensional (plane of propagation is the same as oscillation), and thus their plane cannot be changed since there is only one
Polarisers – devises that only allows one polarisation of light to be transmitted
Only allows the component of that wave that is travelling in the same plane as the polariser to pass through
Linearly polarised – when the oscillation is restricted to one plane
If polariser is in the same plane as wave oscillations = all of it passes through → intensity remains the same
If the polariser is perpendicular to the plane of wave oscillations = none of it passes through → intensity is zero
If unpolarised light passes through a polariser = half of it is passed through → it is 50% of the original intensity
generally EM waves are polarised according the their electric field’s plane