Module 6: C24 - Particle Physics Flashcards

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1
Q

What did Rutherford carry out his Alpha-Scattering Experiment

A

A narrow beam of alpha particles, all of the same kinetic energy, from a radioactive source were targeted at a thin piece of gold foil which was only a few atomic layers thick. The alpha particles were scattered by the foil and detected on a zinc sulphide screen mounted in front of a microscope. Each alpha particle hitting this fluorescent screen produced a tiny speck of light. The microscope was moved around in order to count the number of alpha particles scattered through different values of the angle Θ per minute, for Θ from zero to almost 180°.

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2
Q

What Observations were made from Rutherford’s alpha-scattering experiment?

A
  • Most of the alpha particles passed straight through the thin gold foil with very little scattering. About 1 in every 2000 alpha particles were scattered.
  • Very few of the alpha particles (about 1 in every 10,000) were deflected through angles of more than 90°.
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3
Q

What does this conclusion from Rutherford’s alpha-scattering experiment:

Most of the alpha particles passed straight through the thin gold foil with very little scattering. About 1 in every 2000 alpha particles were scattered

A

This shows most of the atom is empty space, and most if the mass is concentrated in a small nucleus

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4
Q

What does this conclusion from Rutherford’s alpha-scattering experiment:

Very few of the alpha particles (about 1 in every 10,000) were deflected through angles of more than 90°.

A

This statement shows the nucleus has a positive charge because it repelled the few positive alpha particles.

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5
Q

Example Question:

Describe how the alpha-particle scattering experiments provide evidence for the existence, charge, and size of the nucleus.

A

In the alpha particle scattering experiment, most of the alpha particles passed straight through the gold foil with very little scattering. This highlights that most of the atom is made up of empty space. The fact that 1 in every 2000 alpha particles were scattered/deflected shows that there is very a very small mass concentrated within a particle, suggesting there is a nucleus/centre of mass in the atom. Additionally, 1 in every 1000 were deflected by angles of more than 90°, showing that the nucleus does have a positive charge, as it has repelled the positively charged alpha particles (two positives repel).

The size of the nucleus is about 10^-14 m

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6
Q

Exam Questions:

Rutherford used alpha particles of kinetic energy 1.2x10^-12 J in one of his experiments. Using the idea of conservation of energy, calculate the distance d of the closest approach between an alpha particle and the gold nucleus.

A

Energy = Qq/4πεοr
r = Qq/4πεοEnergy

1.2x10^-12 = (2x1.6x10^-19) x (79x1.6x10^-19) / (4πx8.85x10^-12 x r)

r = 3.029x10^-14m

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7
Q

Example Question:

Suggest why only a small number of alpha particles were scattered through large angles.

A

Only a small number were scattered, as the nucleus of an atom is very small compared to its size, making it less likely for head-on collisions to occur.

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8
Q

Example Question:

State the approximate radii of the atom and its nucleus

A

Nucleus: 10^-15 m

Radius: 10^-10m

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9
Q

Example Question:

Alpha particles of kinetic energy 8.8MeV are fired at lead atoms. The charge on the nucleus of lead is 82e. Calculate:

a) the minimum distance the alpha particles approach to the nucleus of lead
b) the maximum electrostatic force experienced by the alpha particle.

A

a)
8.8x10^6 x 1.6x10^-19 = Qq / 4πεοd
1.408x10^-12 = 82 x 2 x (1.6x10^-19)^2 / 4π x 8.85x10^-12 x d
d = 2.68x10^-14m
d = 2.7x10^-14m

b)
F = Qq / 4πεοr^2
F = 82 x 2 x (1.6x10^-19)^2 / 4π x 8.85x10^-12 x (2.68x10^-14)^2
F = 53N

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10
Q

Example Question:

A tiny droplet of oil diameter 1.0mm is placed on water. The oil spreads out as a circular disc of thickness approximately one atom thick. Estimate the radius of this oil disc.

A

Initial Volume = Final Volume

4/3π x (0.5x10^-3)^3 = 10^-10 x (π x r^2)
r = 1.29m
r = 1.3m

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11
Q

Nucleon Definition

A

The term nucleon is used to refer to
either a proton or neutron.

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12
Q

What is an Isotope?

A

Isotopes are nuclei of the same element that have the same number of protons but different numbers of neutrons.

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13
Q

What is an Atomic Mass Unit

A

The masses of atoms and nuclear particles are often expressed in atomic mass units (u).

One atomic mass unit (1u) is one-twelfth the mass of neutral carbon-12 atom.

The experimental value of 1u is about 1.661x10^-27 kg.

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14
Q

Equation for Radius of a Nucleus

A

R = ro ∛A

(A = nucleon number)
(Ro = 1.2 fm (10^-15m)

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15
Q

How do you derive the equation for density of a nucleus

A

ρ = m/v
ρ = m / (4/3πr^3)
ρ = m / (4/3π(ro∛A)^3)
ρ = m / (4/3π ro^3 A

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16
Q

Calculate the (a) the mass, (b) the radius, (c) the volume, (d) the density of a nickel nucleus containing 28 protons and 36 neutrons, and (e) the density of the atom. The mass of both protons and neutrons to 3sig.figs is 1.00u (1u = 1.66x10^-27 kg).

A

a)
28 + 36 = 64
64u = 64 x 1.66x10^-27 = 1.06x10^-25 kg.

b)
R = ro^3 ∛A
R = 1.2x10^-15 ∛64
R = 4.8x10^-15 m

c)
V = 4/3 πr^3
V = 4/3 x π x (4.8x10^-15)^3
V = 4.632x10^-43 m^3

d)
ρ = m/v
ρ = 1.06x10^-25 / 4/3π ro^3 A
ρ = 2.29x10^17 kgm^-3

e)
ρ = m/v
ρ = 1.06x10^-25 / 4π (10^-10)^3
ρ = 2.53x10^4 kgm^-3

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17
Q

Describe the nature and range of the three forces acting on the protons and neutrons in the nucleus

A

Gravitational - very small attractive force, will be stronger the closer two objects are.

Electrostatic force repelling the protons - very big relative to these forces, works when two charges are in close proximity

Strong Nuclear Force - very small range (<3fm). When too close they repel, otherwise this force is attractive and keeps the nucleus together

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18
Q

What keeps protons together in the Nucleus

A

The attractive gravitational force between the proton is far too small (about 10^-34) to keep them together, so there must be another, much stronger force acting on the protons. This force is the strong nuclear force.

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19
Q

What is the Strong Nuclear Force (what does it act on, what is its range?)

A

The strong nuclear force acts between all nucleons. It is a very short range force, effective over just a few fe to meters. Figure 3 shoes the variation of the strong nuclear force F between two nucleons with separation r. The force is attractive to about 3fm and repulsive below about 0.5fm.

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20
Q

When is the Strong Nuclear Force attractive and repulse

A

The force is attractive to about 3fm and repulsive below about 0.5fm.

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21
Q

What are Fundamental Particles?

A

Fundamental particles are a particle that have no internal structure and bend can’t be divided into smaller bits.

Protons and neutrons are not fundamental particles, because they are made up of quarks.

Quarks, electrons, and neutrinos are considered as fundamental particles.

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22
Q

What 3 things are considered a fundamental particles?

A

Quarks, electrons, and neutrinos are considered as fundamental particles.

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23
Q

What are the 4 Fundamental Forces

A

Magnetic Force
Gravitational Force
Strong Nuclear Force
Weak Nuclear Force

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24
Q

Strong Nuclear Force:

• Effect
• Relative Strength
• Range

A

Effect:
Experienced by nucleons

Relative Strength:
1

Range:
Only acts within 3fm

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25
Q

Electromagnetic Force:

• Effect
• Relative Strength
• Range

A

Effect:
Experienced by static and moving charged particles

Relative Strength:
10^-3

Range:
Infinite

26
Q

Weak Nuclear Force:

• Effect
• Relative Strength
• Range

A

Effect:
Responsible for beta decay

Relative Strength:
10^-6

Range:
10^-18

27
Q

Gravitational Force:

• Effect
• Relative Strength
• Range

A

Effect:
Experienced by all particles with mass

Relative Strength:
10^-40

Range:
Infinite

28
Q

How can you usually show something is an antiparticle

A

Most antiparticles are symbolised by a bar over the letter for the particle.

29
Q

What is Paul Dirac’s theory (what happens when a particle and antiparticle collide)

A

Paul Dirac’s theory predicted that every particle has a corresponding antiparticle, and that if the two meet, they completely destroy each other in a process called annihilation, where the masses of both particle and antiparticle are converted into a high-energy pair of photons.

30
Q

What is different/the same about the charge and mass of an antiparticle, compared to its opposite particle?

A

Every known particle has an opposite particle, its antiparticle pair.

An antiparticle has the same mass as its antiparticle pair, but has an opposite charge.

31
Q

What two families can subatomic particles be classified into?

A
  • Hadrons
  • Leptons
32
Q

What are Hadrons

A

Hadrons are particles and antiparticles that are affected by the Strong Nuclear Force. Examples include protons, neutrons, and mesons. Hadrons, if charged, also experience the electromagnetic force. Hadrons decay by the weak nuclear force.

33
Q

What are Leptons

A

Leptons are particles and antiparticles that are not affected by the string nuclear force. Examples include electrons, neutrinos, and muons. Leptons, if charged, also experience the electromagnetic force.

34
Q

State with a reason, whether or not protons and neutrons are fundamental particles.

A

Protons and neutrons are not fundamental particles, as they are made up of quarks

35
Q

State 2 fundamental particles that can be classified as leptons

A

Electrons, neutrinos

36
Q

The muon μ^- is a particle that is not affected by the strong nuclear force. It has a mass of 1.9x10^-28 kg. Calculate the mass of the antimuon μ^+ as a multiple of electron masses and state whether this antiparticle is a hadron or a lepton.

A

Mass of antimuon:
1.9x10^-28kg
or
209 electron masses

It would be a lepton, as it is not affected by the Strong Nuclear Force

37
Q

What are Baryons

A

Particles made up of 3 quarks, e.g. proton, neutron

38
Q

What are Mesons

A

Particles made up of a quark and an anti-quark

39
Q

Are Baryons and Mesons Quarks or Leptons?

A

Quarks

40
Q

What are the 6 known quarks

A
  • Up *
  • Top
  • Charm
  • Down *
  • Bottom
  • Strange *
41
Q

Up Quark:

  • Symbol
  • Charge
  • Baryon Number
  • Strangeness
  • Spin
A

Symbol:
u
Charge:
+2/3 e (antiquark -2/3 e)
Baryon Number:
+1/3
Strangeness:
0
Spin:
+1/2

42
Q

Down Quark:

  • Symbol
  • Charge
  • Baryon Number
  • Strangeness
  • Spin
A

Symbol:
d
Charge:
-1/3 e (antiquark +1/3 e)
Baryon Number:
+1/3
Strangeness:
0
Spin:
+1/2

43
Q

Top Quark:

  • Symbol
  • Charge
  • Baryon Number
  • Strangeness
  • Spin
A

Symbol:
t
Charge:
+2/3 e (antiquark -2/3 e)
Baryon Number:
+1/3
Strangeness:
0
Spin:
+1/2

44
Q

Bottom Quark:

  • Symbol
  • Charge
  • Baryon Number
  • Strangeness
  • Spin
A

Symbol:
b
Charge:
-1/3 e (antiquark +1/3e)
Baryon Number:
+1/3
Strangeness:
0
Spin:
+1/2

45
Q

Charm Quark:

  • Symbol
  • Charge
  • Baryon Number
  • Strangeness
  • Spin
A

Symbol:
c
Charge:
+2/3 e (antiquark -2/3 e)
Baryon Number:
+1/3
Strangeness:
0
Spin:
+1/2

46
Q

Strange Quark:

  • Symbol
  • Charge
  • Baryon Number
  • Strangeness
  • Spin
A

Symbol:
s
Charge:
-1/3 e (antiquark +1/3 e)
Baryon Number:
+1/3
Strangeness:
0
Spin:
+1/2

47
Q

What is the Baryon Number?

A

The number of baryons in a particle reaction is called the baryon number.
The total baryon number in a reaction never changes.

48
Q

Are mesons stable?

A

Mesons have a baryon number=0. All mesons are unstable.

49
Q

What is Strangeness?

A

Strangeness (S) is a quantum number assigned to particles. The term
strangeness was established before the discovery of quarks to explain
differing rates of reaction when strange particles were produced and
when they decayed.

50
Q

What is Spin?

A

Spin describes the angular momentum

51
Q

Quark Combination of Protons and Neutrons

A

Protons:
uud, charge 1e
(2/3 e + 2/3 e - 1/3 e = 1e)

Neutrons:
udd, charge 0
(2/3 e -1/3 e - 1/3 e = 0)

52
Q

Compare two things baryons and mesons have in common

A

They both contain quarks, and are both hadrons.

53
Q

What is the Neutrino, and what does it explain?

A

The existence of the neutrino was predicted to explain beta decay in terms of conservation laws. Each neutrino has its antiparticle, and in this course, we are only interested in the electron neutrino νₑ and the electron antineutrino v^-ₑ

54
Q

Symbol Equation for β- decay of a neutron

A

¹₀n —> ¹₁p + ⁰-₁e + v^- e (anti electron neutrino)

55
Q

Symbol Equation for β+ decay of a neutron

A

¹₁p —> ¹₀n + ⁰₁e + ve (electron neutrino)

56
Q

Symbol equation for quark transformation of d —> u

A

d —> u + ⁰-₁e + v^- e (anti electron neutrino)

57
Q

Symbol equation for quark transformation of u —> d

A

u —> d + ⁰₁e + ve (electron neutrino)

58
Q

Where/How was the Weak Nuclear Force?

A

In order for some reactions to occur it is necessary for one quark to transform into another. One such transformation is during beta decay where the weak interaction was first discovered.

59
Q

What does the Weak Nuclear Force act on and what is its range?

A

The weak interaction force acts between both leptons and quarks, whereas the strong force does NOT act between leptons such as electrons & neutrinos.

The weak interaction is short ranged, only 10^-18m and is only 1 millionth the size of the strong force.

60
Q

What things are conserved in Nuclear Reactions and what other things need to be conserved with Beta Decay?

A

We already are aware that mass/energy, charge and momentum are conserved in nuclear reactions.

When looking at beta decay we now must consider some other conservation laws including: conservation of spin, baryon number and proton number