11. Fission, Decay, Waste Flashcards

1
Q

Briefly describe the two types fission

A

Spontaneous - Happens without external energy

Induced - Initiated by addition of energy

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2
Q

What does SEMF predict about the splitting of nuclie in fission, and what is observed?

A

SEMF predicts equal size splitting

However asmmetry is observed due to shell structure

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3
Q

From SEMF, what nucleus size can spontaneous fission occur

A

Typically A > 100

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4
Q

What typically happens to daughter nuclei after spontaneous fission?

A

They are still neutron rich so undergo several beta decays until they reach a stable nuclide

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5
Q

At which point does spontaneous fission have a larger probability, to where it competes with alpha decay?

A

When you have very heavy nuclei, A > 270

- Z^2 / A = 49 for an ellipsoid

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6
Q

What type of problem is spontaneous fission, and describe it

A

A potential barrier problem like alpha decay

  • Daughter nuclei needs to get through the barrier
  • About 5-6MeV below the top potential (Activation energy)
  • Spontaneous fission occurs when this disappears with a large probability
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7
Q

What is the probability of a daughter nucleus tunnelling through the potential barrier and why?

A

Very small because we are dealing with very large objects

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8
Q

How can we induce fission in terms of the activation energy?

A

Add energy to the nucleus typically by absorption of neutrons as they don’t feel the EM force

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9
Q

Describe the energies involved in induced fission between even N and odd N nuclei

A

Odd - Adds the energy of the neutron as well as the pairing energy (often > activation energy)
Even - Capturing neutron movees to a less energetically favourable state by a change in pairing energy

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10
Q

Describe and explain the differences in crosssections for U235 and U238

A

U235 is odd N so very low energy (thermal) neutrons can induce fission
U238 needs neutrons with 1.2MeV

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11
Q

State the multiplication factor

A

k = (no. neutrons produced in n+1 stage) / (no. neutrons produced in n state)

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12
Q

Describe what happens to the product nuclei after U235 Fission

A
  • Most of the released energy is carried away by fragments
  • 2.5 neutrons created which have a reasonable high energy
  • Some fragments give off further neutrons with a mean delay time of 13s
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13
Q

What are the k values of interest (multiplication factor)

A

k = 1: Critical, constant chain reaction rate
k < 1: Subscritical, rate goes down
k > 1: Supercritical, rate goes up

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14
Q

What is the equation for the mean free path of a neutron between two collisions

A

L = 1/(ρ_nucleus * mean σ_total)

  • Density of nucleus and mean total cross section
  • Mean cross section if U235 and 238 present
  • Typically 3cm
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15
Q

Describe the critical mass for U235

A

1 in 6 neutrons cause fission, so will travel Lsqrt(6) = 7cm and then induce fission
- Critical mass corresponds to a radius of 7cm on fission starts

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16
Q

What is the equation for the power output of a reactor?

A

W_f = J N σ_fission
J - Neutron flux
N - Number of nuclei that can undergo fission
W - Fission rate

17
Q

What is the energy released by a single fission?

A

200MeV for U235

18
Q

Why do we slow the neutrons down, and how are they slowed?

A

For U235, the cross section is much higher at low neutron energies
- Slow down with a moderator to increase fission efficiency

19
Q

What are actinides?

A

Radioactive elements with an atomic number between 89 and 103

  • Mainly Uranium itself with other elements
  • Have very long lifetimes (000s of years)
20
Q

What are the two forms of nuclear waste, and state their lifetimes

A

Actinides (> 000s of years) and fission products (decades)

21
Q

What is the general cycle of nuclear waste after it is removed from a reactor?

A
  • Stored near reactor for cooling as it has a very high activity even without fission
  • Once activity decreases, longer term storage
22
Q

What are the three forms of long term storage for nuclear waste?

A
  1. Deep underground

2. Transmutation + induced fission in accelerator systems

23
Q

What must happen QMically for fusion to occur

A

The two nuclei have to overcome the Coulomb potential barrier in order to get close enough to fuse