Half Life and Activity

Definition of Half-Life:

The half-life of a radioactive substance is the time required for half of the radioactive atoms in a sample to decay into a different element or isotope.

For any given radioactive isotope, the half-life is a constant value that does not change with the amount of substance present or environmental conditions.

Equation(s):

N = No e-λt

With:

(N) = Undecayed atoms remaining

(No) = Original amount of undecayed atoms

(λ) = Decay constant

(t) = Duration decay is measured (s)

N = No / 2x

(x) = number of Half Lives passed

Definition of Activity:

Activity refers to the rate at which a radioactive substance undergoes decay.

It is measured in decays per second, commonly expressed in units such as becquerels (Bq), where 1 Bq is equal to one decay per second.

Activity is directly proportional to the number of radioactive atoms present in a sample; as the number of undecayed atoms decreases over time, the activity of the substance also diminishes.

Equation(s):

A = Ao e-λt

With:

(A) = number of decays detected per second

(Ao) = Original amount of undecayed atoms

(λ) = Decay constant

(t) = Duration decay is measured (s)

A = Ao / 2x

(x) = number of Half Lives passed

Equations Linking Activity and Half Life

A = λN

A = ΔN / Δt

ΔN / Δt = - λN

Exponential Decay Graphs

Derivation of λ = ln2 / T½

1. The Law of Radioactive Decay

The number of undecayed nuclei, N, at any time t is given by:

N (t) = N0 e−λt

2. Definition of Half-Life

The half-life (T½ ) is the time required for half of the radioactive nuclei to decay:

N (T½) = N0 / 2​​

3. Substituting Half-Life

Using the decay law:

N0 / 2 = N0 e−λT½

Cancel N0 (assuming N0 ≠ 0):

1 / 2 = e−λT½

4. Solve for λT½

Take the natural logarithm (ln) on both sides:

ln⁡(1 / 2)= −λ T½

Simplify ln⁡ (1 / 2) using logarithmic properties ( ln⁡ ( a / b ) = ln⁡ ( a ) − ln⁡ ( b ) ):

ln⁡ (1 / 2) = ln⁡ (1) − ln ⁡(2) = 0 −ln ⁡(2) = − ln ⁡(2)

So:

− ln⁡ (2) = − λT½

Cancel the negatives:

λT½ = ln⁡ (2)

Finally, solve for λ:

λ = ln ⁡(2) / T½