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Poisson Distribution Probability Calculator

Find the probability of observing exactly, at least, or at most a given number of rare, independent events in a fixed interval, from the average expected rate.

P(exactly 4)
19.5367%
P(at least 4)
56.653%
P(at most 4)
62.8837%
Standard deviation
2

How it works

The Poisson distribution models how many times a rare, independent event happens in a fixed interval, given only the average rate λ (lambda) — customer arrivals per hour, typos per page, or server errors per day. The exact probability of observing precisely k occurrences is P(X = k) = λᵏ × e^(−λ) ÷ k!, evaluated here in log space (k×ln(λ) − λ − ln(k!)) so it stays numerically accurate even for larger λ or k rather than overflowing k! or underflowing λᵏ directly.

"At most k" sums that exact-probability formula across every outcome from 0 to k. Because the Poisson distribution has no upper bound on how many events could occur, "at least k" is computed instead as 1 minus the probability of fewer than k occurrences — a finite sum — rather than summing an infinite tail. The mean and variance of a Poisson distribution are both exactly λ, so the standard deviation reported here is simply √λ.

FAQ

What makes an event a good fit for the Poisson model?

Three conditions: events happen independently of each other, the average rate λ stays constant over the interval you're measuring, and two events essentially can't occur at the exact same instant. Customer arrivals, typos, and radioactive decays all fit reasonably well; something with bursts or seasonal spikes (λ changing over time) doesn't.

How is this different from the Binomial Probability calculator?

Binomial probability needs a fixed number of trials n, each with the same success probability p (like 10 coin flips). Poisson instead models a count of events over a continuous interval with no fixed number of "trials" at all — just an average rate λ. In fact, the Poisson distribution is what the binomial distribution converges to as n grows very large and p grows very small while n×p stays fixed at λ.

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