Particle Physics - A Level Physics Edexcel

0.0(0)
Studied by 0 people
call kaiCall Kai
learnLearn
examPractice Test
spaced repetitionSpaced Repetition
heart puzzleMatch
flashcardsFlashcards
GameKnowt Play
Card Sorting

1/119

encourage image

There's no tags or description

Looks like no tags are added yet.

Last updated 4:56 PM on 5/31/26
Name
Mastery
Learn
Test
Matching
Spaced
Call with Kai

No analytics yet

Send a link to your students to track their progress

120 Terms

1
New cards

What is the order of the scientists in the history of the atom?

1) Thomson 2) Rutherford 3) Bohr 4) Chadwick

2
New cards

What did Thomson discover about particles?

He used cathode rays to theorise the plum pudding. (sphere of positive charge with electrons in it)

<p>He used cathode rays to theorise the plum pudding. (sphere of positive charge with electrons in it)</p>
3
New cards

Cathode ray experiment

A high p.d. between two plates, where the cathode rays (ray of light) are attracted to the positive plate, and deflected away from the negative plate, detected on a fluorescent screen.

Discovering the electron.

<p>A high p.d. between two plates, where the cathode rays (ray of light) are attracted to the positive plate, and deflected away from the negative plate, detected on a fluorescent screen.</p><p>Discovering the electron.</p>
4
New cards

Rutherford experiments

The Geiger Marsden experiment (or gold foil experiment) is where alpha particles are fired at a thin sheet of gold foil, and detected on a fluorescent screen

<p>The Geiger Marsden experiment (or gold foil experiment) is where alpha particles are fired at a thin sheet of gold foil, and detected on a fluorescent screen</p>
5
New cards

Gold foil experiment findings (Geiger Marsden)

Nuclear Model

Most particles passed straight through (atom mostly empty space)

Some deflected back at small angles (nucleus is positively charged)

Very few deflected right back

(nucleus is in the centre and most of the mass of an atom)

<p>Nuclear Model</p><p>Most particles passed straight through (atom mostly empty space)</p><p>Some deflected back at small angles (nucleus is positively charged)</p><p>Very few deflected right back</p><p>(nucleus is in the centre and most of the mass of an atom)</p>
6
New cards

What did Bohr discover about particles?

Planetary Model

Electrons in orbitals, electrons have discrete energy levels, evidenced by emission line spectra

<p>Planetary Model</p><p>Electrons in orbitals, electrons have discrete energy levels, evidenced by emission line spectra</p>
7
New cards

Chadwicks experiments

Alpha particles fired at Beryllium, a highly penetrating uncharged radiation is emitted which knocked out hugh energy protons from paraffiin wax.

8
New cards

Chadwicks Findings

Atomic Model

to knock out protons, the alpha radiation must contain a similar size (mass) but neutral particle

The neutron is discovered.

9
New cards

point of closest approach

R0, the closest a particle can get to the nucleus before being deflected

Combine Kinetic energy and Electric potential energy (work done by field) equations.

1/2mv^2 = qV

V is (electric potential)

1/2mv^2 = kqQ/r

then solve for r, which is R0

10
New cards

What must occur for the alpha particle to be deflected

The radius of nucleus must be smaller than r0

11
New cards

When work is done on the alpha particle to deflect it,what is gained

Electric potential energy

12
New cards

Work done by electric field of gold nucleus =

Electric potential energy stored + Original kinettic energy of the particle

13
New cards

What does ε0 represent?

permittivity of free space

14
New cards

Electric potential definition

Work done per unit of positive charge to make it from a point r metres away from Q

15
New cards

Work done equation in terms of charge and velocity

Work done = Q x V

16
New cards

4 important equations for work done on particles

V=E/Q

K=1/4(pi)ε0

V=kQ/r

V inversely proportional to r

17
New cards

Work one on particle significant equation involving charges and ε0

W=Q(gold)Q(alpha particle)/4(pi)ε0r0

18
New cards

thermionic emission

the release of electrons from a heated filament

(Energy absorbed by electrons from heat, so electrons escape valence band and enter conducting band)

19
New cards

How does a vacuum allow for electrons to behave

No collisions with oxygen molecules, meaning they can leave their trajectory untouched

20
New cards

How does an electron gun work

small metal filament is heated by a current in a vacuum, providing electrons with kinetic energy, which will cause some to escape from the surface of the metal, which are then attracted to an anode, causing a narrow beam of electrons to accelerate towards a small gap in the anode, creating a beam of electrons

21
New cards

How do calculate electron volt in an electron gun

Vq= 1/2 mv ^2

Vq=p^2/2m

22
New cards

How are electrons accelerated in an electron gun

The electric field working in the opposite direction

23
New cards

Fields travel in what direction

Positive to Negative

24
New cards

Electrons travel in what direction

Negative to positive

25
New cards

Va (voltage and electron charge) represent what

Electronvolt

26
New cards

What direction is the force of the magnetic field in relation to the current

Perpendicular

27
New cards

Conventional current

Current that flows in opposition to electrons

28
New cards

What is the difference between F=BQV and F=BqV

Q= Big/multiple particles

q= 1 small particle

29
New cards

When the electron is fired into the magnetic field, what force does the magnetic field act on the electron

a Centripetal force

30
New cards

equation for r of the fired particle into the magnetic field

r= P/BQ

31
New cards

Electron gun diagram

A coil used for thermionic emission-cathode-anode-magnetic field

<p>A coil used for thermionic emission-cathode-anode-magnetic field</p>
32
New cards

How to calculate m of the electron fired from the electron gun

m=V^2B^2q/2V

33
New cards

Describe the structure of a cyclotron

2 horizontal 'Dees' facing each other with a gap in the middle. 2 electromagnets, one above one below, both north-facing up. An alternating PD connected to the Dees.

34
New cards

How does a cyclotron work

A proton suspended in the gap between 2 Dees will be accelerated by the electric current to the negative D. The magnetic field will act perpendicular to the proton and cause a centripetal force, spiraling the proton back to the gap. At this point the alternating PD is switched and the polarities swapped, the particle is now accelerated to the other D, increasing in velocity and therefore radius of spiral. This repeats until the particle is fired out of the cyclotron.

<p>A proton suspended in the gap between 2 Dees will be accelerated by the electric current to the negative D. The magnetic field will act perpendicular to the proton and cause a centripetal force, spiraling the proton back to the gap. At this point the alternating PD is switched and the polarities swapped, the particle is now accelerated to the other D, increasing in velocity and therefore radius of spiral. This repeats until the particle is fired out of the cyclotron.</p>
35
New cards

What is the difference in terms of a particle between a magnetic and electric field

Magnetic field changes particle direction

Electric current accelerates particle

36
New cards

Frequency of supply (Cyclotron) =

Frequency of rotations

37
New cards

Equation to calculate Kinetic energy of the proton in a cyclotron

Final Ek= 2xVqxNorbits

38
New cards

Equation to calculate frequency of a cyclotron

f= Bq/m2(pi)

39
New cards

What must an alternating voltage have to function properly in a cyclotron

An equal frequency to orbits around cyclotron

40
New cards

Synchrotron

Lowers the frequency of the supply in sync with the orbital frequency of particles, therefore accelerating them to a greater velocity

Donut shaped rather than disc shaped

<p>Lowers the frequency of the supply in sync with the orbital frequency of particles, therefore accelerating them to a greater velocity</p><p>Donut shaped rather than disc shaped</p>
41
New cards

Why do we sometimes need a Synchrotron

When a particle approaches the speed of light, it's mass changes. Due to the frequency equation needing mass, this would be disrupted however with a synchro-cyclotron we can alter frequency too

42
New cards

Linear accelerators (Linacs)

Electrons travelling in a vacuum, entering tubes of increasing length and accelerating in the gaps between tubes, done by a high freq alternating p.d.

<p>Electrons travelling in a vacuum, entering tubes of increasing length and accelerating in the gaps between tubes, done by a high freq alternating p.d.</p>
43
New cards

How is a particle accelerated to the next drift tube in a linear acclerator

The alternating PD will swap the next tube either positive or negative depending on the previous one to attract the electron

Adjacent tubes are connected to opposite terminals

44
New cards

Why does length of drift tubes increase in the linear accelerator

Because time spent in the tube must be a constant so length increases with velocity

45
New cards

What does the length of the LINAC limit?

The max speed

46
New cards

What is the advantage of the LINAC?

It can accelerate greater masses than cylotrons and synchrotrons as these require particles to be bent by a magnetic field so are limited by the strength of the magnetic field

47
New cards

What is the advantage of the cyclotron over the LINAC?

It has a spiral path so the particles travel a greater distance so go to greater speeds than the LINAC

48
New cards

Electron Scattering (to find properties of proton)

Electrons fired at proton from LINAC, proton is very small, so the wavelength of electron must also be very small. The way to achive this is by LINAC speeding up the electron to a really high energy as λ = h/p.

At relativistic speeds, E = mc^2, E = mcc = pc,

as a result λ = hc/E so wavelength is inversely proportional to KE.

49
New cards

Structure of the large Hadron Collider and Synchrotron

Accelerating cavities spin particles until they are ejected

<p>Accelerating cavities spin particles until they are ejected</p>
50
New cards

3 types of particle detectors

Cloud chambers, Bubble chambers, Multi wire chamber

51
New cards

Why do only charged particles leave tracks in particle detectors?

When a charged particle passes through a substance it causes ionisation and electrons are knocked out of atoms so the particle leaves a trail of ions as it goes

52
New cards

What does radius of path of a track represent in a particle detector

Momentum

53
New cards

What does direction of a path represent in a particle detector

Charge

Opposite charges have different directions

54
New cards

How would you tell if a particle is more ionising in a particle detector

A thicker/shorter path

55
New cards

Cloud chamber

In super saturated air (with ethanol), charged particles ionise the air and vapour form droplets along the line of ionisation. By shining a light on this a photograph can be taken.

<p>In super saturated air (with ethanol), charged particles ionise the air and vapour form droplets along the line of ionisation. By shining a light on this a photograph can be taken.</p>
56
New cards

Bubble chamber

Liquid nitrogen boils along the path of ionisation, forming bubbles which can be photographed under light

<p>Liquid nitrogen boils along the path of ionisation, forming bubbles which can be photographed under light</p>
57
New cards

Multi wire chamber/Drift chamber/Spark chamber

A number of wires carrying alternating voltages are contained within a chamber filled with inert gas. The particle ionises the gas and the ions move to the oppositely charged wire, creating a spark. This creates pulses of current in the wires, which can be measured and used to calculate the 3D trajectory from the timing of the charged particles.

58
New cards

If the ionising path suddenly jumps forward what could we assume

potential collision with neutral particles

59
New cards

How to calculate radius of curvature of a path created by an ionising particle in a particle detector

r=p/BQ

60
New cards

Where does the positive curve if the magnetic field shows .

Field leaves page so positive curves down (clockwise)

Then use left hand rule

61
New cards

Where does positive curve if field shows X

Field going into page so positive curves up (anticlockwise)

62
New cards

Why do you see spirals on particle detector diagrams?

Interactions with the detector decrease the kinetic energy of the particle so the radius decreases as the particle loses kinetic energy

63
New cards

What is Einstein's theory of special relativity?

1) The laws of physics are the same for all non-accelerating observers 2) The speed of light within a vacuum is the same no matter the speed at which an observer travels

64
New cards

Why does lifespan of a particle increasing with relativistic effects

When a particle has such a high speed, time passes slower for it (it has an higher observed lifespan)

65
New cards

What happens to an object as it gains energy during relativistic effects

It gains mass because energy holds mass

66
New cards

Relationship between energy and mass

Energy can be converted to mass and vice versa

67
New cards

Why would the change in m be so small

Because c^2 is so large and change in energy is divided by c^2

68
New cards

Change in energy equation (relativity)

(delta)E=c^2(delta)m

69
New cards

how to convert from Kg to MeV/c^2

use E = mc^2

M = E/c^2

so to convert from kg to MeV/c^2, convert energy to MeV, then multiply by speed of light

70
New cards

How to calculate energy changes

Total Energy before = Total energy after

Account for rest masses (energy req to have a mass with 0 speed)

and account for KE.

71
New cards

Loss of Ke in a collision=

Total mass x c^2

72
New cards

Particle collisions do not conserve mass entirely but what is conserved entirely

Mass+Energy. If mass is lost there will be greater energy and vice versa.

73
New cards

Why does a particle in a cyclotron experience a centripetal force

Due to Fleming's left hand rule, motion switches direction

74
New cards

Equation to find the kinetic energy of the particle in a cyclotron

Final Ek= Vq x Norbits

(Final Ek= Protonvolt x Number of orbits)

75
New cards

Equation to find the frequency of rotations in a cyclotron

F= Bq/m2(pi)

(Frequency= magnetic flux density x charge of particle/ mass x 2pi)

76
New cards

How does a Synchrotron work

A synchro-cyclotron lowers the frequency of the supply in sync with the orbital frequency of particles, therefore it can accelerate particles to a greater velocity.

77
New cards

Why would a Synchrotron be necessary instead of a normal cyclotron

When the particle approaches speed of light, it's mass will increase, therefore the frequency of orbits will be out from the frequency of supply and accelerator will not work

78
New cards

What are fermions

Matter particles e.g. quarks and leptons

79
New cards

What are the bosons (force carriers)?

Gluon (Strong nuclear force between quarks)

Photon (Electromagnetic force)

Z boson and W boson (Weak nuclear force, responsible for radioactive decay)

Higgs Boson (Interacts with particle to give them mass)

80
New cards

What do bosons do?

Think of them as force transferring particles

81
New cards

Particle spins:

Fermions : Non integer

Bosons: Integer

non int spins mean they occupy space, int spins dont, therefore you can theoretically have infinite bosons in one space.

(Technically mesons are also bosons as they have 0 spin)

82
New cards

3 types of sub-atomic particles

Hadrons, Leptons, Quarks

83
New cards

2 fundamental particles

Quarks and Leptons

84
New cards

6 types of quarks in increasing energy levels

up, charm, top

down, strange, bottom

(the quarks exist in pairs of generations of similar energy levels, e.g. up and down have the same energy)

85
New cards

What is antimatter?

It consists of particles that are just like those of ordinary matter except with opposite properties, such as opposite charge.

86
New cards

What happens when a particle and antiparticle pair collide?

They annihilate. This means that their mass is converted to energy (in the form of a photon), The opposite can happen - energy can be converted to a particle-antiparticle pair. This is called pair production.

(Pair production tends to happen near a nucleus, and the singular photon needs to have enough energy to produce all the mass)

87
New cards

Charge of up, charm and top quarks

+2/3

88
New cards

Charge of anti up, anti charm and anti top quarks

-2/3

89
New cards

Charge of down, strange and bottom quarks

-1/3

90
New cards

Charge of anti down, anti strange and anti bottom quarks

+1/3

91
New cards

What is a proton made up of

2 up quarks and 1 down quark

92
New cards

Types of Leptons

Electron, Electron neutrino, Muon, Muon neutrino, Tau, Tau neutrino

93
New cards

Charge of electron, muon and tau leptons

-1

94
New cards

Charge of anti electron, anti muon, and anti tau leptons

+1

95
New cards

Charge of electron neutrino, muon neutrino, and tau neutrino

0

96
New cards

Charge of anti electron neutrino, anti muon neutrino and anti tau neutrino

0

97
New cards

Types of leptons in order of increasing mass

Electron, Muon, Tau

Electron neutrino, Muon neutrino, Tau neutrino,

(Neutrinos are very light almost massless)

98
New cards

2 types of Hadron

Meson, Baryon

99
New cards

What Hadron has greater mass

baryon is heavier than a meson

100
New cards

Meson

Made up of any one quark and any one antiquark