← Back to article

Equation 1 · Radioactive Clocks: How Nuclear Physics Gave Evolution Its Time

What does this equation mean?

N(t)=N0 e−λt,t1/2=ln⁡2λ,N(t) = N_0\, e^{-\lambda t}, \qquad t_{1/2} = \frac{\ln 2}{\lambda},

Read the formula alongside the article passage below. Each part has a deeper page with its role in the equation, the supporting passage and nearby citations.

Start withln 2
Divide byλ
This relates toN(t)
How to read the two sides of this formula. Follow the article passage for the meaning of each quantity.

This equation states an equality: the expressions on both sides have the same value under the article’s assumptions. Read the equation part by part below; each part has a contextual explanation and a link to its mathematical background.

Read it piece by piece

NN

Symbol N

N is part of the quantity the equation computes from the expression on the right.

Understand this part →

tt

Symbol t

t is an argument of the function-like quantity on the left; its role is set by that function’s stated inputs.

Understand this part →

N0N_0

Symbol N_0

the initial population.

Understand this part →

e−λte^{-\lambda t}

Symbol e^-λ t

e−e^-λ t is one of the signed contributions combined to compute the quantity on the left.

Understand this part →

t1/2t_{1/2}

Symbol t_1/2

the half-life derived from it.

Understand this part →

λ\lambda

Symbol λ

the decay constant characteristic of the isotope.

Understand this part →

=

=

The expressions on both sides represent the same quantity under the stated assumptions.

Understand this part →

See an illustrated explanation →
fraction

fraction

Divide the expression above the line by the one below it.

Understand this part →

See an illustrated explanation →
subscript

subscript

The lower label selects a particular version, component, or indexed member of the quantity. For example, x₀ and xₜ can be values at different positions.

Understand this part →

superscript

superscript

A raised number can be a power. When it is a label or bound, it selects a case or the upper limit of a sum; the formula’s structure distinguishes these uses.

Understand this part →

See an illustrated explanation →
ln⁡2\ln 2

Numerator: ln 2

The complete quantity above the fraction bar.

Understand this part →

See an illustrated explanation →

How to interpret it

With a fixed numerator, increasing a nonzero denominator reduces the fraction. Read it with the definitions, units, and assumptions supplied by the article.

What the article says around this equation

The property that makes radioactive decay useful as a clock is not that it happens on a convenient timescale — some isotopes decay in fractions of a second, others over timescales longer than the universe’s age — but that it happens with no memory. An atom of uranium-238 that has existed, undecayed, for four billion years is exactly as likely to decay in the next second as one formed a microsecond ago. There is no wear, no fatigue, no accumulated probability of failure the way there is in a mechanical clock’s escapement or a living organism’s senescence. This absence of memory is what makes decay first-order: the number of decays in a short interval is proportional only to the number of…
Read the full surrounding passage
The property that makes radioactive decay useful as a clock is not that it happens on a convenient timescale — some isotopes decay in fractions of a second, others over timescales longer than the universe’s age — but that it happens with no memory. An atom of uranium-238 that has existed, undecayed, for four billion years is exactly as likely to decay in the next second as one formed a microsecond ago. There is no wear, no fatigue, no accumulated probability of failure the way there is in a mechanical clock’s escapement or a living organism’s senescence. This absence of memory is what makes decay first-order: the number of decays in a short interval is proportional only to the number of atoms present, not to their age, giving the population as a whole an exponential decline, N(t)=N0 e−λt,t1/2=ln⁡2λN(t) = N_0\, e^{-\lambda t}, \qquad t_{1/2} = \frac{\ln 2}{\lambda}. where N0N_0 is the initial population, λ\lambda is the decay constant characteristic of the isotope, and t1/2t_{1/2} is the half-life derived from it. This is the one place in the article where the evolutionary-population analogy is exact rather than suggestive: a sample of N0N_0 identical atoms behaves, statistically, exactly as a population geneticist’s model of a large population with a fixed per-individual probability of an event per unit time behaves. Individual atoms are unpredictable; the population’s decline is not.

Read the equation in its article →

Sources cited in the article section

These citations give research context. Read each source to check which claims it supports.

Return to Radioactive Clocks: How Nuclear Physics Gave Evolution Its Time

See this formula across 1 published context →

Browse the mathematical compendium →