Class 12 Physics Radioactivity and nuclear reaction Notes

Chapter 24 – Radioactivity and Nuclear Reaction | Nepal eNotes
PHYSICS • CHAPTER 24

Radioactivity and Nuclear Reaction

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Radioactivity

The process of emission of α, β, γ radiations when an unstable nucleus becomes stable is called radioactivity or radioactive disintegration.

Properties of α-Particles

  1. They are helium nuclei.
  2. They are positively charged.
  3. They are deflected in electric and magnetic field.
  4. They have less penetrating power.
  5. They can ionise the gas through which they pass.
α-particle = 42He

Properties of β-Particles

  1. They are fast moving electrons.
  2. They are negatively charged.
  3. They are deflected in electric and magnetic field.
  4. The penetrating power is more than α-particles.
  5. They have less ionising power than α-particles.
β-particle = 0−1e

Properties of γ-Rays

  1. They are electromagnetic waves.
  2. They are chargeless.
  3. They are not deflected in electric and magnetic field.
  4. They have high penetrating power.
  5. The ionising power is less than α and β-particles.

Laws of Radioactivity

  1. The radioactivity process is not affected by external factors like pressure, temperature, humidity etc.
  2. Either α-particle is emitted or β-particle is emitted but not both simultaneously.

When α-Particle is Emitted

When α-particle is emitted, atomic number decreases by 2 and mass number decreases by 4.

AZX  →  A−4Z−2X + 42He

Example

23892U  →  23490Th + 42He + Q

When β-Particle is Emitted

When β-particle is emitted, atomic number increases by 1 and mass number remains unchanged / same.

AZX  →  AZ+1X + 0−1e + Q

Example

146C  →  147N + 0−1e

Radioactive Decay Law

The rate of decay of a radioactive sample at time is directly proportional to number of atoms present at that time.

If a sample contains N atoms at time t, then:

dN/dt ∝ N
dN/dt = −λN    …(1)

where λ is decay constant.

NOTE: The rate of decay per unit number of atom is decay constant.

Let N0 be the initial number of atoms at time t = 0.

dN/N = −λdt
Integrating both sides,
∫N₀N dN/N = ∫0t −λdt
[ln N]N₀N = −λ[t]0t
ln N − ln N0 = −λ(t − 0)
ln(N/N0) = −λt
N/N0 = e−λt
N = N0e−λt
NOTE
N = N0e−λt
A = A0e−λt
m = m0e−λt

Decay Curve

N t N₀

Fig: Decay curve

Half Life (T1/2)

The time taken to decay half the number of atoms is called half-life.

Relation Between Half-Life and Decay Constant

Since:

N = N0e−λt

If t = T1/2 and N = N0/2, then:

N0/2 = N0e−λT₁/₂
1/2 = e−λT₁/₂
ln(1/2) = −λT1/2
−0.693 = −λT1/2
λ = 0.693 / T1/2
T1/2 = 0.693 / λ

Mean-Life

The ratio of total life of atoms to the total number of atoms is called mean-life.

Mean life = (sum of lives of all atoms) / (number of atoms)

Also,

Tav or Tm = 1/λ

Remaining Number of Atoms after nth Half-Life

Remaining atoms after nth half-life:

N = (1/2)nN0

Remaining activity after nth half-life:

A = (1/2)nA0

Units of Radioactivity

1) Becquerel

1 Bq = 1 dis/sec

2) Rutherford

1 Rd = 106 dis/sec

3) Curie (Ci)

1 Ci = 3.7 × 1010 dis/sec
The supplied 6-page PDF ends with units of radioactivity. Although the file title includes “Nuclear Reaction,” no separate nuclear-reaction section is present in these scanned pages.

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