Nuclear Flashcards

(29 cards)

1
Q

Atomic Mass Unit

A

1/12 the mass of a carbon 12 atom

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2
Q

Mass Defect

A
  • The mass of the nucleus is less than the total mass of the individual particles it contains.
  • Strong force causes this as some of the mass is converted into energy to keep the nucleus together.
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3
Q

Thermal neutrons

A

In thermal equilibrium with moderator.

Low Ek

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4
Q

Control Rods

A

Absorbs neutrons to prevent further fission. The lower the rods are inserted the more neutrons are absorbed so less fissions occur.

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5
Q

Moderator

A

Responsible for slowing down neutrons released in fission so they become thermal neutrons and can induce further fission.

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6
Q

Fuel rods

A

Made of fissile material and each rod contains less than critical mass so reactions don’t become uncontrolled

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7
Q

Coolant

A

Carries away thermal energy produced by fission reactions

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8
Q

Critical mass

A

Minimum amount of fissile material needed to maintain a steady flow of fission reactions

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9
Q

What did the Rutherford Scattering experiment do?

A

Disproved the plum pudding model and provided evidence for the bohr model.

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10
Q

How did the Rutherford scattering experiment work?

A
  • Alpha particles fired at thin sheet of gold foil.
  • Most passed through with no deflection suggesting that the atom is mostly empty space.
  • Some were deflected by large angles suggesting most of the mass is concentrated in a small positive nucleus.
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11
Q

Alpha radiation

A

Helium nucleus
Strongly ionising
Slow moving
Stopped by a few cm of air or thin paper
positively charged
deflected in a magnetic field

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12
Q

Beta radiation

A

High energy electrons or positrons
Mildly ionising
Fast moving
Stopped by thin sheet of aluminium
Negatively or positively charged
Deflected in a magnetic field

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13
Q

Gamma radiation

A

High frequency em radiation
Weakly ionising
Travels at c
Stopped by a few cm of lead or a few m of concrete
No charge
Unaffected by a magnetic field

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14
Q

Alpha radiation application

A

Used in smoke detectors:

Alpha particles ionise the air between a source and detector allowing a current to flow
When smoke gets between them it absorbs the radiation
So the air cannot be ionised resulting in no current, which triggers an alarm

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15
Q

Beta radiation application

A

Used to measure the thickness of aluminium sheets:

An ideal count rate is determined
Material is placed between a beta source and detector
If not enough radiation reaches the detector then the sheet is too thick and the machine flattens it
Otherwise the sheet is too thin and the machine fattens it
Allows for effective quality control

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16
Q

Gamma radiation application

A

Used to sterilise medical equipment
Used to kill cancerous cells
Used as a medical tracer in diagnosis

17
Q

Background Radiation

A

Ionising radiation emitted from a variety of natural and artificial sources.

18
Q

Corrected count rate

A

The count rate with the measured count rate deducted

19
Q

Safety with radiation

A

Maximise distance with handling tools
Shielding, stand behind absorber such as lead

20
Q

Background radiation sources

A

Natural:
Cosmic rays
rocks
radon gas

Artificial:
medical
nuclear fallout

21
Q

Decay constant

A

The constant of proportionality, which links rate of decay to the number of undecayed nuclei It is the probability of a decay per unit time.

22
Q

Half Life

A

The time taken for half the original number of radioactive nuclei to decay or the time taken for the original activity to half.

23
Q

Radioactive dating

A

The use of radioactive isotopes with known half lives to date materials.

24
Q

Radioactive Decay

A

The spontaneous disintegration of the nucleus of an atom, which results in the emission of particles.

25
Random nature of radiation
It is impossible to predict when there will be a decay or which particular nucleus will decay.
26
Distance of closest approach upper bound
Particle and nucleus never touch so result is an upper bound of nuclear radius.
27
Nuclear radius equation
V = Q/(4 * Pi * E0 * r)
28
More accurate method of determining nuclear radius
High speed electrons fired at thin sheet of material, they diffract as they pass through, producing a diffraction pattern of concentric circles that can be used to calculate nuclear radius.
29