The Poisson counts how many events arrive. This page times them. The wait for the next event is exponential, the wait for the r-th event is gamma, and both fall out of the Poisson formula you already have. Along the way you meet the most testable fact about the exponential, that it has no memory. 4 past-paper questions at the end.
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Imagine events arriving at random, at an average of λ per hour. Two different questions can be asked of the same process. How many events in the next hour? That is the Poisson of the previous page. How long until the next one? That is the exponential. And how long until the third? That is the gamma.
The two questions are tied together by one observation: you wait longer than t hours exactly when the count over those t hours is zero. Every formula below comes from that sentence, or from adding independent waits.
Suppose events arrive at random at an average rate of λ per hour (buses at a stop, calls to a helpline). From the previous page, the number of events in t hours is Poisson with mean λt, so P(Nt = k) = e−λt(λt)k ÷ k!.
Let T be the time until the first event. The wait lasts longer than t hours exactly when no event has happened in the first t hours. So
With λ = 0.5 per hour, the chance of waiting more than 2 hours is e−1 = 0.3679.
The chance of the event arriving by time t is what is left over, and the density is its slope:
The density is highest at t = 0 and falls steadily: short waits are the most likely, and very long ones are rare but possible.
For a non-negative variable, the mean is the area under its survival curve, and E[T²] is the area under 2t times it. Both integrals are easy here:
So Var(T) = 2 ÷ λ² − 1 ÷ λ² = 1 ÷ λ². The standard deviation equals the mean. The median m solves e−λm = ½, so m = ln 2 ÷ λ ≈ 0.69 ÷ λ, which is less than the mean 1 ÷ λ: a few long waits pull the mean up (DSE 2021).
Suppose you have already waited s hours. The chance of waiting at least t more is a ratio of survival chances:
The wait so far cancels out. Drag s in the lab and the two curves stay on top of each other. JAM 2024: for a mean of 50, λ = 1/50, and P(X > 70 | X > 60) = P(X > 10) = e−10/50 = e−1/5.
For n observed waits x1, …, xn the likelihood is λne−λΣx. Its log is n ln λ − λΣx, with derivative n ÷ λ − Σx. Setting it to zero gives the maximum-likelihood estimate
The sample 1.75, 2.25, 2.50, 2.75, 3.25 has mean 2.5, so λ̂ = 0.4 = 2/5 (JAM 2023).
P(T > s + t | T > s) = P(T > t). It holds for the exponential, and for no other continuous waiting-time distribution.
After each event, the process starts afresh (the exponential has no memory), so the gaps between events are independent exponentials with the same rate. The time of the r-th event is their sum, Tr = T1 + … + Tr. Independence lets means and variances add:
The r-th event has not happened by time t exactly when fewer than r events have happened. So P(Tr > t) is a sum of Poisson probabilities:
For r = 2 and λ = 1 at t = 2 this is e−2(1 + 2) = 0.406.
The density is minus the slope of the survival function. Each term has slope
When you add the terms for k = 0, …, r − 1, each positive piece cancels the negative piece of the term before it. Only the last negative piece survives, so
For r = 2, f(t) = λ²te−λt, which you can confirm by differentiating e−λt(1 + λt) directly.
The only piece that needs a whole number is (r − 1)!. Replace it with the gamma function, Γ(α) = ∫ xα−1e−x dx. Integrating by parts gives Γ(α + 1) = αΓ(α), and Γ(1) = 1, so Γ(n) = (n − 1)! for whole n. The gamma density with shape α and rate λ is
With α = 1 it is the exponential. For α ≥ 1 it peaks at (α − 1) ÷ λ. The lab shows the family, and, for whole shapes, simulated sums of exponentials landing on the curve.
JNU 2018 gives F(x) = 1 − e−x − xe−x = 1 − e−x(1 + x). That is exactly the survival function above with r = 2 and λ = 1. So the variable is gamma with shape 2 and rate 1: mean 2 ÷ 1 = 2, mode (2 − 1) ÷ 1 = 1. The density is te−t, and 0.3679 at its peak t = 1.
| Question | Distribution | Mean | Variance |
|---|---|---|---|
| How many events in time t? | Poisson, mean λt | λt | λt |
| How long until the first event? | Exponential, rate λ | 1 ÷ λ | 1 ÷ λ² |
| How long until the r-th event? | Gamma, shape r, rate λ | r ÷ λ | r ÷ λ² |
Two warnings in that table. The Poisson and the exponential look as if they share the symbol λ, but λ is a rate in the exponential (events per hour, so the mean wait is its reciprocal) and a mean count in the Poisson. And the Poisson’s mean equals its variance, while the exponential’s mean equals its standard deviation. Back on the previous page, the Poisson derivation is the source of everything here, and the continuous distributions lesson applies the exponential to the exam questions.
Give answers to four decimal places where they are not whole numbers.
Classification traps, multi-step numericals and statement questions, up to the hardest JNU, JAM and GATE items.
The Delhi School entrance asks this topic harder than any other exam. These questions are kept apart from the ordinary sets.
These are questions from the TestStop bank. A free account answers 10 a day, each with its worked solution; All-Access opens every set with no daily limit.
The exponential distribution describes the waiting time until the first event of a process in which events arrive at random at a constant rate λ. Its density is λe^(−λt) for t ≥ 0, the chance of waiting longer than t is e^(−λt), the mean is 1/λ and the variance is 1/λ².
A waiting time is memoryless if the time already waited does not change the distribution of the time still to wait: P(T > s + t | T > s) = P(T > t). The exponential has this property because e^(−λ(s+t)) divided by e^(−λs) is e^(−λt). It is the only continuous distribution on the positive axis with the property.
The median m solves e^(−λm) = 1/2, so m = ln 2 / λ, about 0.69/λ. The mean is 1/λ. The distribution has a long right tail of rare, very long waits, which pull the mean above the median.
They describe the same process from two sides. In a Poisson process with rate λ, the number of events in a time t is Poisson with mean λt, and the waiting time to the first event is exponential with rate λ. The Poisson counts, and the exponential times.
The gamma distribution with whole shape r and rate λ is the waiting time for the r-th event of a Poisson process, the sum of r independent exponential waits. Its density is λ^r t^(r−1) e^(−λt) / (r − 1)!, its mean is r/λ and its variance is r/λ². With a non-integer shape, the factorial is replaced by the gamma function.
A chi-square distribution with k degrees of freedom is a gamma distribution with shape k/2 and rate 1/2. The chi-square is built from squared normal variables, and the derivations library covers it separately.