waves and the particle nature of light Flashcards

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1
Q

wave velocity

A

v=λf

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2
Q

longitudinal waves

A

oscillations are parallel to the direction of energy transfer, made up of compressions and rarefactions. sound is the best example

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3
Q

rarefaction stage of longitudinal wave

A

pressure is decreased, neighbouring particles move away from each other

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4
Q

compression stage of transverse wave

A

pressure is increased, neighbouring particles move towards a point

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5
Q

interference

A

occurs during superposition

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6
Q

constructive interference

A

occurs when two waves are in phase and so their displacements are added

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7
Q

destructive interference

A

occurs when two waves are completely out of phase and so displacements are subtracted

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8
Q

phase difference

A

two waves are in phase if they are both at the same point in the wave cycle, so they have the same frequency, wavelength and their phase difference is an integer of 360°. the waves do not need the same amplitude

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9
Q

path difference equation

A

∆x=∆ φx λ/2π

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10
Q

stationary waves

A

formed by the superposition of two waves, travelling in opposite directions in the same plane, with the same frequency, wavelength and amplitude. no energy is transferred in a stationary wave

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11
Q

stationary wave in phase

A

constructive interference, where an antinode forms at a point of maximum displacement

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12
Q

stationary wave out if phase

A

destructive interference, a side forms at a point of minimum displacements

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13
Q

speed of transverse wave on string equation

A

v=rootT/μ

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14
Q

refractive index

A

a property of a material which measures how much it slows down loath passing through it, n=c/v. higher refractive index means the material is more optically dense

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15
Q

refraction

A

when a wave enters a different medium, causing it tot change direction, either towards or away from the normal depending on the materials refractive index. as the light moves across the boundary, its speed changes which causes its direction to change.
n1sinθ1=n2sinθ2

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16
Q

n2>n1, which way does light bend

A

towards the normal

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17
Q

critical angle

A

as the angle of incidence is increased, the angle of refraction also increases until it gets closer to 90°. when the angle of refraction is exactly 90° and the light is refracted along the boundary, the angle of incidence has reached the critical angle (C)

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18
Q

critical angle equation

A

if n2 is air: sinC=1/n
if otherwise: sinC=n2/n1

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19
Q

total internal reflection

A

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

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20
Q

converging lenses

A

cause parallel rays to move closer

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21
Q

diverging lens

A

cause parallel rays to move apart

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22
Q

3 features of lenses

A

-principle focus:
converging-where light rays focus
diverging- where rays appear to come from
-focal length: distance from lens to principle focus
-power: measure of lens’ ability to bend light. in a converging lens it is positive. diverging it is negative

23
Q

power of a lens

A

the reciprocal of the focal length
P=1/f

24
Q

power of several thin lessons in combination

A

acts as a single lens with a power equal to the sum of the powers of the individual lenses
P=P1+P2+P3

25
Q

real vs virtual image

A

real image can be projected onto a screen, a virtual image cannot

26
Q

magnification

A

the ratio of the size of the image it creates with respect to the size of the object
image height/object height

27
Q

plane polarisation

A

allowing oscillation of waves in one plane. a polarised wave only oscillates in one plane. only transverse waves can be polarised.

28
Q

why does light diffract less through a door than sound

A

the wavelength of light is so much smaller, and the greatest amount of diffraction occurs when the gap is the same size as the wavelength

29
Q

diffraction grating

A

a slide containing many equally spaced slits very close together. when light is passed through, it forms an interference pattern composed of light and dark fringes

30
Q

diffraction grating equation

A

nλ=dsinθ
d= distance between slits

31
Q

what is the pattern produced when blue and red light pass through a diffraction grating

A

lines seen where constructive interference occurs. red wavelength longer than blue so diffracted greater and so blue lines on the inside and red lines on the outside of the light fringes.

32
Q

electron diffraction

A

using an electron gun to accelerate electrons through a vacuum towards a crystal lattice, they interact with the small gaps between atoms and form an interference pattern on a fluorescent screen behind the crystal. the pattern looks like concentric rings

33
Q

deBroglie hypothesis

A

λ=h/p
this shows all particles have a wave nature

33
Q

what does electron diffraction show

A

if electrons had particle nature, the pattern would be a singular point. this is nit the case as the electrons are diffracted which proves evidence of their wave nature

34
Q

wave behaviour at an interface

A

transmitted- pass into next material
reflected- bounce off surface

35
Q

pulse echo technique using ultra sound to form an image

A

1) short pulse of ultra sound waves are transmitted into the target
2) pulse travels until it reaches a boundary between two mediums where some of the pulse is reflected back. the amount of reflection depends on the difference in densities. the greater the difference the greater the reflection
3) reflected waves are deflected as they leave
4) the intensities of the reflected waves are used to determine the structure and the time taken is used to determine the position

36
Q

issues with pulse echo technique

A

-if the duration is too long, they will likely overlap, meaning the amount of information you obtain will decrease
-the larger the wavelength, the less fine details can be resolved, meaning less information

37
Q

wave model of light

A

EM radiation can be described as a transverse wave

37
Q

the work function

A

minimum energy required for electrons to be emitted from the surface of a metal

38
Q

photon model of light

A

EM waves travel in discrete packets called photons, which have energy directly proportional to their frequency (E=hf)

39
Q

photoelectric effect as evidence of the particle nature of EM radiation

A

-wave theory suggests any frequency of light should be able to cause photoelectric emission
-photoelectric effect is immediate
-increasing the intensity does nit increase the speed of emission, but increases the amount of electrons emitted
-electrons released with a range of kinetic energies

39
Q

photoelectric effects

A

photoelectrons are emitted from the surface of a metal after light above a certain frequency (threshold frequency) is shine on it.
photoelectrons are emitted because electrons near the surface of the metal absorb a photon and gain enough energy to leave the surface

40
Q

why must light be a particle, not a wave?

A

-all photon energy is transferred to the electron, one photon interacts with one electron
-energy transfer ins immediate
-intensity is equal to the number of photons released per second, an increase would increase the number of interactions with electrons per second
-all electrons receive the same amount of energy, but those deeper electrons loose energy through collisions and so have less kinetic energy

41
Q

evidence that electrons in atoms can only transition between discrete wavelengths

A

inside a fluorescent tube, electrons are accelerated, causing gas atoms to become excited and then de-excite, releasing a photon. by passing the light through a diffraction grating or prism, you get a line spectrum. Each line in the spectrum represents a different wavelength of light emitted. spectrum contains discrete values of wavelength , the photon energies correspond to these wavelengths.

41
Q

the difference in energy levels

A

it is equal to a specific photon energy emitted or absorbed, therefore the energy of emitted photon:
∆E=E1-E2
hf=E1-E2
f=(E1-E2)/h

41
Q

atomic line spectra

A

electrons in atoms exist in discrete energy levels, if an electron gains enough energy it can move up in energy level, however t will quickly return to its original level and release the energy it gained in the form of a photon of light

42
Q

superposition definition

A

when two waves meet, their resultant displacement is the sum of their individual displacements

43
Q

visible light wavelengths

A

400-750nm

44
Q

intensity relation to amplitude

A

I is proportional to A^2, and so if intensity is doubled, the amplitude is multiplied by four

45
Q

phase difference calculation

A

∆d/λ= ∆t/T then multiply by 2π or 360

46
Q

how to calculate how many order will be visible

A

using dsinx=nλ, make x=90 and then you should find a value for n e.g 4.7 and so 4 is the maximum order found and 9 is how many light fringes will be seen

47
Q

order in relation to wavelength

A

as d is proportional to nλ, λ and n are inversely proportional and so a smaller wavelength means more visible orders

48
Q

number of slits

A

you will be told how many slits per mm which should be converted into metres and then find the reciprocal to fid the distance between slits which =d