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Exponential Distribution Calculator

Enter the rate λ or the mean of an exponential distribution and a value x, and get the density, the cumulative and survival probabilities, a range probability, the median and any percentile — with the working shown, a memorylessness check and a shaded curve. Free, no sign-up.

The parameter I know

Adds P(x ≤ X ≤ this value) to the results.

Shows that the wait still to come does not depend on s.

Finds the x with P(X ≤ x) = p, such as 0.9 for the 90th percentile.

Results

λ = 1/mean = 1/4 = 0.25

ProbabilityMeaningValue
P(X ≤ 6)at most 6 (also: less than 6)0.7769
P(X > 6)more than 6 (also: at least 6; the survival function)0.2231
f(6)Density at x: f(x) = λe^(−λx). A density, not a probability: it can exceed 1.0.055783

4

Mean (1/λ)

16

Variance (1/λ²)

4

Standard deviation (1/λ)

2.7726

Median (ln 2 / λ)

0.25

Hazard rate (λ)

Memorylessness

P(X > s + x | X > s) = P(X > 9) / P(X > 3) = 0.1054 / 0.4724 = 0.2231

P(X > x) = P(X > 6) = 0.2231. The two are equal: having waited 3 already changes nothing about the wait still to come.

Quantile

x = −ln(1 − p) / λ = −ln(1 − 0.9) / 0.25 = 9.2103. So P(X ≤ 9.2103) = 0.9.

Density curve

Exponential density with λ = 0.25. The shaded area under the curve is P(X ≤ x).

How to Use the Exponential Distribution Calculator

  1. 1. Say which parameter you know. Choose the rate λ (events per unit of time) or the mean 1/λ (units of time per event), then type it in. The calculator converts the other one and shows the conversion.
  2. 2. Enter x. The time, distance or other amount you are asking about. Add an upper end if you want the probability of a range.
  3. 3. Optional extras. Enter a time already waited, s, to see the memoryless property at work, or a probability p to find the x that cuts it off (p = 0.9 gives the 90th percentile).
  4. 4. Read the results. P(X ≤ x), P(X > x), the density f(x), the mean, variance, median and hazard rate, and a curve with your probability shaded.

What the Exponential Distribution Models

The exponential distribution describes the waiting time until the next event when events occur independently at a constant average rate: the gap between calls to a help line, the time until a radioactive atom decays, the distance between flaws along a cable. It is the continuous counterpart of the geometric distribution, and it is tied to the Poisson distribution: if the number of events in a period is Poisson with rate λ, the waits between events are exponential with the same λ.

Formulas for X with rate λ (mean 1/λ), for x ≥ 0
QuantityFormula
Densityf(x) = λe−λx
Cumulative probabilityP(X ≤ x) = 1 − e−λx
Survival functionP(X > x) = e−λx
Quantile for probability px = −ln(1 − p) / λ
Mean and standard deviation1/λ each
Variance1/λ²
Medianln 2 / λ ≈ 0.6931 / λ

Rate or mean? Check which one your source uses

Textbooks split on the parameter. Some write the rate λ; others write the mean (or scale) θ = β = 1/λ. Software splits the same way: R's dexp, pexp and qexp take the rate, and so does Excel's EXPON.DIST, while Python's scipy.stats.expon takes scale = 1/λ. Mixing them up is the commonest error with this distribution — a mean of 4 minutes is a rate of 0.25 per minute, not 4. Pick the matching option above and the calculator does the conversion.

Worked Example: Waiting Time Between Calls

Calls to a help line arrive on average every 4 minutes, so the mean is 4 and λ = 1/4 = 0.25 per minute. The chance that the next call takes at most 6 minutes is P(X ≤ 6) = 1 − e−1.5 = 0.7769, and the chance it takes longer is P(X > 6) = e−1.5 = 0.2231. The chance the wait falls between 2 and 6 minutes is e−0.5 − e−1.5 = 0.3834.

The median wait is ln 2 / 0.25 = 2.7726 minutes — shorter than the mean of 4, because the distribution is right-skewed. The 90th percentile is −ln(0.1) / 0.25 = 9.2103 minutes: nine calls in ten arrive within about 9.2 minutes of the last.

Memorylessness

Suppose 3 minutes have passed with no call. The chance of waiting at least 6 more is P(X > 9) / P(X > 3) = 0.1054 / 0.4724 = 0.2231 — exactly P(X > 6), the figure for a fresh start. The exponential is the only continuous distribution with this property, and it follows from the constant hazard rate: at every moment the chance of an event in the next instant is λ, however long you have waited.

When the exponential is the wrong model

Memorylessness is a strong assumption. A battery or a person ages, so a lifetime model with a rising hazard (a Weibull or gamma) fits better than an exponential; the exponential suits events that strike without wear, such as random arrivals.

Frequently Asked Questions

How do I find λ from the mean?
Take the reciprocal: λ = 1/mean. A mean wait of 4 minutes gives λ = 0.25 per minute, and a rate of 3 events per hour gives a mean of 1/3 hour, or 20 minutes. Keep the units of x consistent with the units of λ, or the probabilities will be wrong.
What does the memoryless property mean?
It means P(X > s + t | X > s) = P(X > t): the time you have already waited does not change the distribution of the time still to come. If a bus arrives at random with mean gap 10 minutes, after waiting 20 minutes your expected remaining wait is still 10 minutes.
How are the exponential and Poisson distributions related?
They describe the same process from two sides. The Poisson counts events in a fixed period; the exponential measures the time between events. If calls arrive at 3 per hour (Poisson, λ = 3), the gap between calls is exponential with mean 20 minutes, and the chance of waiting over 5 minutes is e−3 × 5/60 = 0.7788.
How do I calculate P(X > x) for an exponential distribution?
Use the survival function e−λx. With λ = 0.25 and x = 6 that is e−1.5 = 0.2231. There is no need to subtract from 1 — which is why the calculator computes the upper tail directly and keeps its precision far out in the tail.
Why is the median smaller than the mean?
The distribution is strongly right-skewed: many short waits and a few very long ones pull the mean up. The median is ln 2 / λ, about 69% of the mean 1/λ. Half of all waits are shorter than 0.69 of the average wait.
Is the exponential distribution a good model for lifetimes?
Only when the failure rate is constant, as for random shocks or electronic parts in their useful life. Wear-out, infant mortality and ageing all make the hazard rate change over time, and the exponential then misjudges both tails. Check the fit before relying on it.

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