Nuclear Physics Flashcards

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1
Q

Definition of 1 u (atomic mass unit)

A

one atomic mass unit (1 u) is defined being equal to one-twelfth of the mass of a carbon-12 atom

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2
Q

Relationship equation between energy and mass

A

E=MC2

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3
Q

Define Mass Defect

A

Difference between total mass of the separate nucleons and the combined mass of the nucleus.

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4
Q

1 MeV is defined as

A

1 Mev is the energy gained by 1 electron accelerated by potential of 1 million volts

1 MeV = 1.6 x 10-13 J

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5
Q

Binding Energy

A

The Minimum energy needed to separate all nucleons in nucleus to infinity

Equal to mass defect

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6
Q

Fission

A

The splitting of a heavy nucleus into two lighter nuclei of approximately the same mass

increases binding energy per nucleon

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7
Q

Use of rods in Nuclear Fission

A

Chain reaction after heavy nuclei bombarded with nuetrons

Rods to control number of fission reactions by absorbing neutrons

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8
Q

Fussion

A

Process by which two light nuclei join together to form a heavier one

icreases Binding energy per nucleon

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9
Q

define λ

A

λ is the probability that an individual nucleus will decay per unit time

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10
Q

Define activity A

A

Activity of a radioactive sample is the rate at which nuclei decay or disintegrate

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11
Q

Differrence between λ and A

A

λ deals with individual nuclei

A with entire sample

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12
Q

A and undecayed nuclei Formula

A

A = λN

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13
Q

A and number of emissions formula

A

A = Number of emissions / time

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14
Q

Half life t½

A

mean time taken for the number of undecayed nuclei to be reduced to half its original value

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15
Q

exponential relationship equations for N, A, and R (count rate)

A

x=x0e-λt

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16
Q

Equation relating t½ and λ

A

λ = ln2 / t½

17
Q

Relevance of Binding energy per nucleon

A

the higher the binding energy per nucleon the more stable the nucleus

18
Q

Why Geiger - MÜller (GM) tube doesn’t give direct reading of Activity

A
  1. cannot detect all radiation emitted
    • detector directional, some radiation will move away from detector
  2. some radiation escapes past detectors or absorbed within sample itself
    • gamma rays not always detected
      • low/weak ionising power