Waves and Optics ༄ Flashcards

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1
Q

Explain how light from the diffraction grating forms a maximum on the screen

A

(1) Light from slits overlap
(2) Arrive at screen in phase
(3) undergo superposition

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2
Q

Explain what is meant by modal dispersion in an optical fibre

A

(1) Pulse broadening occurs
(2) Because light rays enter the fibre at different angles
(3) Takes a different amount of time to travel along the fibre

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3
Q

Explain, with reference to refractive index, why the pulse of red light has a shorter transit
time than the pulse of blue light

A

(1) The refractive index of core for blue light is greater than the refractive index for
red
(2) The speed of the blue light is less than the speed of the red light and travel the
same distance

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4
Q

State why emergent ray does not change direction as it leaves an object

A

(1) Angle of incidence is 0

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5
Q

Progressive wave

A

Transfers energy without transferring material and is made up of particles of a medium oscillating

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6
Q

Amplitude

A

Wave maximum displacement from equilibrium position

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7
Q

Frequency

A

Number of complete oscillations passing through a point per second

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8
Q

Wavelength

A

Length of one whole oscillation

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9
Q

Speed

A

Distance travelled by the wave per unit time

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10
Q

Phase

A

Position of a certain point on a wave cycle

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11
Q

Phase difference

A

How much a particle/wave lags behind another

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12
Q

Period

A

Time taken for one full oscillation

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13
Q

Points in phase

A

Two points on a wave are in phase if they are both at the same point of the wave cycle, they will
have the same displacement and velocity and their phase difference will be a multiple of 360°
(2π radians), they do not need the same amplitude, only the same frequency and wavelength.

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14
Q

Points out of phase

A

Two points are completely out of phase when they’re an odd integer of half cycles apart e.g. 5
half cycles apart where one half cycle is 180°

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15
Q

Speed equation

A

c = fλ

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16
Q

Frequency equation

A

f = 1/T

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17
Q

Transverse waves

A

Oscillations at perpendicular to direction of energy transfer
All electromagnetic waves are transverse at travel at 3x10^8 ms in a vacuum
Can be demonstrated by shaking a slinky vertically

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18
Q

Longitudinal waves

A

Oscillations are parallel to direction of energy transfer
Made up of compressions and rarefactions
Shown by sound waves or shaking a slinky horizontally

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19
Q

Polarising waves

A

Can only travel in one plane
Only transverse waves can be polarised
Provides evidence for the nature of transverse waves as polarised waves must travel perpendicular to direction of energy transfer

20
Q

Superposition

A

Where the displacements of two waves are combined as they pass each other,
the resultant displacement is the vector sum of each wave’s displacement

21
Q

Two types of superposition

A

● Constructive interference occurs when 2 waves have displacement in the same
direction
● Destructive interference occurs when one wave has positive displacement and the other has negative displacement, if the waves have equal but opposite displacements, total destructive interference occurs

22
Q

Stationary wave

A

A stationary wave is formed from the superposition of 2 progressive waves, travelling in opposite directions in the same plane, with the same frequency, wavelength and amplitude
No energy is transferred by a stationary wave

23
Q

Nodes

A

● Where the waves meet in phase, constructive interference occurs so antinodes are
formed, which are regions of maximum amplitude
● Where the waves meet completely out of phase, destructive interference occurs and nodes are formed, which are regions of no displacement

24
Q

First harmonic

A

The lowest frequency at which a stationary wave forms is the first harmonic, which forms a stationary wave with two nodes and a single antinode. The distance between adjacent nodes (or antinodes) is half a wavelength (for any harmonic

25
Q

Frequency of harmonic equation

A

f = 1/2L root T/mu

26
Q

Example of stationary waves

A

● Stationary microwaves can be formed by reflecting a microwave beam at a metal plate, to find the nodes and antinodes use a microwave probe
● Stationary sound waves can be formed by placing a speaker at one end of a closed glass tube, lay powder across the bottom of the tube, it will be shaken at the antinodes and settle at the nodes. The distance between each node is half a wavelength, and the frequency of the signal generator to the speaker is known so by c=fλ the speed of sound in air can be found

27
Q

Path difference

A

The difference in the distance travelled by two waves

28
Q

Coherent light source

A

Has the same frequency and wavelength and a fixed phase difference

29
Q

Laser nature

A

Lasers are an example of light which is coherent and monochromatic, meaning they emit a single (or small range of) wavelength(s) of light. Lasers are usually used as sources of light in diffraction experiments as they form clear interference patterns

30
Q

Young’s double slit experiment

A

Demonstrates interference of light from two-sources. In this experiment you can use two coherent sources of light or you could use one coherent source and a double slit in order to form an interference pattern. If you do not have a coherent source of light for example a light bulb, you could place a single slit before the double slit to make the light have a fixed path difference, and a filter to make the light monochromatic. Below is a brief procedure to describe Young’s double slit experiment:
● Shine a coherent light source through 2 slits about the same size as the wavelength of the laser light so the light diffracts
● Each slit acts as a coherent point source making a pattern of light and dark fringes. Light fringes are formed where the light meets in phase and interferes constructively, this occurs
where the path difference between waves is a whole number of wavelengths
Dark fringes are formed where the light meets completely out of phase and
interferes destructively, this occurs where the path difference is a whole number and a half wavelengths ((n+½)λ).

31
Q

Young’s double slit equation

A

w = λD/s

32
Q

White light instead of mono

A

Using white light instead of monochromatic laser light gives wider maxima and a less intense diffraction pattern with a central white fringe with alternating bright fringes which are spectra, violet is closest to the central maximum and red furthest

33
Q

Diffraction

A

The spreading out of waves when they pass through or around a gap

34
Q

Diffraction sizes

A

The greatest diffraction occurs when the gap is the same size as the wavelength. When the gap is smaller than the wavelength most waves are reflected, whereas when it is larger there is less noticeable diffraction. When a wave meets an obstacle you get diffraction round the edges, the wider the obstacle compared to the wavelength, the less diffraction

35
Q

Monochromatic light on a screen

A

Can be diffracted through a single slit onto a screen, which forms an
interference pattern of light and dark fringes. The pattern has a bright central fringe, which is double the width of all other fringes, with alternating dark and bright fringes on either side, the bright fringes are caused by constructive interference where the waves meet in phase and the dark fringes are caused by destructive interference where waves arrive completely out of phase

36
Q

How to vary slit width

A

● Increasing the slit width decreases the amount of diffraction so the central maximum becomes narrower and its intensity increases.
● Increasing the light wavelength increases the amount diffraction as the slit is closer in size to the light’s wavelength, therefore the central maximum becomes wider and its intensity decreases

37
Q

Diffraction grating

A

A diffraction grating is a slide containing many equally spaced slits very close together. When monochromatic light is passed through a diffraction grating the interference pattern is much sharper and brighter than it would be after being passed through a double slit like in Young’s double slit, this is because there are many more rays of light reinforcing the pattern. This means measurements of slit widths are much more accurate as they are easier to take

38
Q

Order lines

A

The ray of light passing through the centre of a diffraction grating is called the zero order line, lines either side of the zero order are the first order lines, then the lines outside the two first order lines are the second order lines

39
Q

Diffraction equation

A

d sinθ = nλ
(Where d is the distance between the slits, θ is the angle to the normal made by the maximum, n is the order and λ is the wavelength. As λ increases (by for example changing the laser light from blue to red), the distance between the orders will increase because θ is larger due to the increase in diffraction as the slit spacing is closer in size to the wavelength, this means the pattern will spread out.
The maximum value of sin θ is 1, therefore any values of n, which give sin θ as greater than 1 are impossible)

40
Q

Refractive index (n)

A

A property of a material which measures how much it slows down light passing through it. This is calculated by dividing the speed of light in a vacuum (c) by the speed of light in that substance (cs)
n = c/cs

41
Q

Refraction

A

Occurs when a wave enters a different medium, causing it to change direction, either
towards or away from the normal depending on the material’s refractive index

42
Q

Snell’s law

A

n1sinθ1=n2sinθ2

43
Q

Total internal reflection

A

can occur when the angle of incidence is greater than the
critical angle and the incident refractive index (n1) is greater than the refractive index of the material at the boundary (n2)

44
Q

TIR use

A

A useful application of total internal reflection are optical fibres; these are flexible, thin tubes of plastic or glass which carry information in the form of light signals. They have an optically dense
core surrounded by cladding with a lower optical density allowing TIR to occur, this cladding also protects the core from damage and prevents signal degradation through light escaping the core, which can cause information to be lost

45
Q

Signal degradation causes

A

● Absorption - where part of the signal’s energy is absorbed by the fibre, reducing the amplitude of the signal, which could lead to a loss of information
● Dispersion - this causes pulse broadening, which is where the received signal is broader than the original transmitted signal. Broadened signals can overlap causing loss of information

46
Q

Types of dispersion

A

➔ Modal - caused by light rays entering the fibre at different angles, therefore they take different paths along the fibre, (for example some may travel down the middle
of the fibre, while others are reflected repeatedly,) this leads to the rays taking a different amount of time to travel along the fibre, causing pulse broadening.
➢ This can be reduced by making the core very narrow, therefore making the possible difference in path lengths smaller.
➔ Material - caused by using light consisting of different wavelengths, meaning light rays will travel at different speeds along the fibre, which leads to pulse broadening
➢ This can be prevented by using monochromatic light