Physics- Topic 23 ( Nuclear Physics)

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17 Terms

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Energy and Mass Equivalence

E = mc2 where E= energy, m= mass and c = speed of light

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Representing simple nuclear reactions

AZX where A: nucleon number/mass number, Z= atomic number/ proton number and X= chemical symbol of the element

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Mass defect

The difference between an atom’s mass and the sum of the masses of its protons and neutrons

∆m = Zmp + (A-Z) mn - mtotal

where:

  • Z = proton number

  • A = nucleon number

  • Mp= mass of a proton

  • Mn = mass of a neutron

  • Mtotal = measured mass of a nucleus

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Binding energy

The energy required to break a nucleus into it’s constituent protons and neutrons

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Energy released in nuclear reaction

E = c2m

The formation of a nucleus from a system of isolated protons and neutrons is therefore an exothermic reaction

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Binding energy per nucleon

The binding energy of a nucleus divided by the number of nucleons in their nucleus

A higher binding energy per nucleon indicates a higher stability

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Graph of number of nucleons vs the binding energy per nucleon

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  • At high values of nucleon number

    • The general binding energy per nucleon is high & gradually decreases with nucleon number

    • This means the heaviest elements are volatile and undergo fission

  • At low values of nucleon number

    • The nuclei tend to have a lower binding energy per nucleon, hence they are generally less stable

    • This means thatthe lightest elements have weaker electrostatic forces and most likely undergo fusion

NOTE: Oxygen, Carbon, and Helium do not fit the trend

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Nuclear fusion

Fusion is the fusing together of two small nuclei to produce a large nuclei nucleus

For two nuclei to fuse, both nuclei must have high kinetic energy

  • This is because protons repel each other

Eg: Deutrium + tritium → Helium + energy

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Nuclear fission

Fission is the splitting of large atomic nuclei into smaller nuclei

  • Fission must be induced by firing neutrons at a nucleus

  • When the nucleus is struck by a neutron, it splits into 2 or more daughter nuclei and ejects neutrons which can react with another nuclei causing a cascade effect

    • This reaction needs to be controlled otherwise it can cause a nuclear bomb effect

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Significance of binding energy per nucleon

  • At Lower values of A

    • Attractive nuclear forces between nucleons outweigh repulsive electrostatic forces between protondprotons

    • In the right conditions, nuclei undergo fusion

      • In fusion, the mass of nucleus that is created is slightly less than the total mass of the original nuclei

      • The mass defect is equal to the binding energy released since the nucleus formed is more stable

  • At higher values of A

    • Repulsive electrostatic forces begin to dominate, and these forces tend to break apart the nucleus rather than hold together

    • In the right conditions, nuclei will undergo fission

      • In fission, an unstable nucleus is converted to a more stable nuclei with a smaller total mass

      • Mass defect = binding energy

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Radioactive decay

Is spontaneous disintegration of a nucleus to form a more stable nucleus, resulting in the emission of an alpha, beta or gamma particle

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Evidence for the random nature of radioactive decay

This can be observed with the count rate of a Geiger-Muller(GM) tube

When a GM tube is placed near a radioactive source, the counts are found to be irregular and can’t be perdicted

Each count represents a decay of an unstable nucleus

These fluctuations in count rate on the GM tube provide evidence for the randomness of radioactive decay

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Characteristics of radioactive decay

  • Spontaneous: A process which can not be influenced by environmental factors

  • Random: A process in which the exact time of decay of a nucleus can not be predicted

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Decay constant

Is the probability that an individual nucleus will decay per unit time

Average number of nuclei which are expected to decay per unit time

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Activity

Is the rate at which radioactive decay occurs

A = ΔN/ Δt = -λN

Where:

  • A = activity

  • λ = decay constant

  • ΔN = number of undecayed nuclei

  • Δt = time interval

  • N = number of nuclei remaining in a sample

The minus sign shows that the number of undecayed nuclei decreases over time

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Half-life

Is the time taken for the initial number of nuclei to reduce by half

This means when a time equal to half-life has passed, the activity of the sample will also have decreased by half.

A ∝ N

λ = 0.693 / t1/2

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Exponential nature of radioactive decay

In radioactive decay, the number of nuclei falls very rapidly without ever reaching zero

  • Such a model is known as exponential decay

The steeper the graph is, the larger the decay constant

General Equation

X = X0e-λt where X can be activity, number of undecayed nuclei or received count rate