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half-life decay const

Sparisoma Viridi
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Half-life and decay constant of radioactive material

As result of nuclear instability, radioactivity refers to the particles which are emitted from nuclei, where the most common types of radiation are called alpha, beta, and gamma radiation 1. There is also other point of view, that radioactivity is the act of emitting radiation spontaneously, where this is done by an atomic nucleus that is unstable for some reason and it wants to give up some energy in order to shift to a more stable configuration 2. There is an important term related to radioactivity known as half-life, which the interval of time required for the number of disintegrations per second of a radioactive material to decrease by one-half or, equivalently, is time interval required for one-half of the atomic nuclei of a radioactive sample to decay (change spontaneously into other nuclear species by emitting particles and energy) 3. Half-life is inversely proportional to decay constant with proportional constant 0.693 or ln 2 4.

At time tt with decay constant or decay rate λ\lambda, if number of nuclei is N(t)N(t) and number of expected decays per second is λN(t)\lambda N(t), then we have

dN(t)dt=λN(t)(1)\tag{1} \frac{dN(t)}{dt} = - \lambda N(t)

as the amount of number of parent nuclei decrease 5. The differential equation has following solution

N(t)=N0eλ(tt0),(2)\tag{2} N(t) = N_0 e^{-\lambda(t - t_0)},

where N0=N(t0)N_0 = N(t_0). For simplicity it is common to set t0=0t_0 = 0 and the time interval is measured from t=0t = 0.

At half-life or t=T12t = T_{\frac12} amount of nuclei is

N(T12)=12N0.(3)\tag{3} N(T_{\frac12}) = \tfrac12 N_0.

Using the half-life and Eqn (3), Eqn (2) will give

12N0=N0eλT12, \tfrac12 N_0 = N_0 e^{-\lambda T_\frac12},

which can be further simplified into

12=eλT12. \tfrac12 = e^{-\lambda T_\frac12}.

Rearrange the terms in previous equation and have

2=eλT12. 2 = e^{\lambda T_\frac12}.

Take natural logarithm of both sides and get

ln2=λT12. \ln 2 = \lambda T_\frac12.

Then following

T12=ln2λ T_\frac12 = \frac{\ln 2}{\lambda}

is the relation between half-life T12T_\frac12 and decay constant λ\lambda.


  1. Carl Rod Nave, “Radioactivity”, Hyperphysics, 2024, url http://hyperphysics.phy-astr.gsu.edu/hbase/Nuclear/radact.html [20241006]. ↩︎

  2. Shawn Denny, Mike Pizzuti, Chelene Neal, Kate Bessiere, “What Is Radioactivity?”, ACHRE Report, May 1997, url https://ehss.energy.gov/ohre/roadmap/achre/intro_9_2.html [20241006]. ↩︎

  3. The Editors of Encyclopaedia Britannica “half-life”, Encyclopedia Britannica, 19 Jan 2024, url https://www.britannica.com/science/half-life-radioactivity [20241006]. ↩︎

  4. Noor Al-Huda Talib Al-Aaraji, “Half-Lives: Physical, Biological, and Effective”, Al-Mustaqbal University College, Iraq, 31 Oct 2021, url https://www.uomus.edu.iq/img/lectures21/MUCLecture_2023_91020162.pdf [20241006]. ↩︎

  5. Alexander S Belyaev, “Radioactivity”, University of Southampton, United Kingdom, 23 Feb 2015, url https://www.personal.soton.ac.uk/ab1u06/teaching/phys3002/course/06_radioactivity.pdf ↩︎

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