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Mean and variance, and link to Poisson processesAQA A-Level Further Maths: Revision notes

Section 1

Mean, variance and standard deviation

For XX with an exponential distribution with parameter λ\lambda: E(X)=1λ,Var(X)=1λ2,σ=1λ.\mathrm{E}(X)=\frac{1}{\lambda},\qquad \mathrm{Var}(X)=\frac{1}{\lambda^2},\qquad \sigma=\frac{1}{\lambda}. The mean and standard deviation are equal. Example: λ=0.05\lambda=0.05 per day gives mean 2020 days, variance 400400 and standard deviation 2020 days. A higher rate λ\lambda means shorter gaps on average.

Key termsmeanstandard deviation
Common mistake

Giving 1λ\frac{1}{\lambda} as the variance. The variance is 1λ2\frac{1}{\lambda^2}; 1λ\frac{1}{\lambda} is the mean and the standard deviation.

Section 2

Proof of the mean

E(X)=∫0∞xλe−λx dx.\mathrm{E}(X)=\int_0^\infty x\lambda e^{-\lambda x}\,dx. Integrate by parts with u=xu=x and dvdx=λe−λx\frac{dv}{dx}=\lambda e^{-\lambda x}, so v=−e−λxv=-e^{-\lambda x}: [−xe−λx]0∞+∫0∞e−λx dx=0+[−1λe−λx]0∞=1λ.\left[-xe^{-\lambda x}\right]_0^\infty+\int_0^\infty e^{-\lambda x}\,dx=0+\left[-\frac{1}{\lambda}e^{-\lambda x}\right]_0^\infty=\frac{1}{\lambda}. The boundary term is 00 because xe−λx→0xe^{-\lambda x}\to0 as x→∞x\to\infty.

Key termsintegration by parts
Exam tip

State that the boundary term is zero because e−λxe^{-\lambda x} decays faster than xx grows. The mark depends on saying so.

Section 3

Proof of the variance

First, by parts again: E(X2)=∫0∞x2λe−λx dx=[−x2e−λx]0∞+∫0∞2xe−λx dx=2λ∫0∞xλe−λx dx=2λ×1λ=2λ2.\mathrm{E}(X^2)=\int_0^\infty x^2\lambda e^{-\lambda x}\,dx=\left[-x^2e^{-\lambda x}\right]_0^\infty+\int_0^\infty2xe^{-\lambda x}\,dx=\frac{2}{\lambda}\int_0^\infty x\lambda e^{-\lambda x}\,dx=\frac{2}{\lambda}\times\frac{1}{\lambda}=\frac{2}{\lambda^2}. Then Var(X)=E(X2)−[E(X)]2=2λ2−1λ2=1λ2.\mathrm{Var}(X)=\mathrm{E}(X^2)-[\mathrm{E}(X)]^2=\frac{2}{\lambda^2}-\frac{1}{\lambda^2}=\frac{1}{\lambda^2}. The remaining integral is 2λE(X)\frac{2}{\lambda}\mathrm{E}(X), which reuses the previous result.

Section 5

Linking the two distributions

A gap longer than tt is the same event as no events in a time tt. Both have probability e−λte^{-\lambda t}: P(X>t)=P(Poisson with mean λt equals 0)=e−λt\mathrm{P}(X>t)=\mathrm{P}(\text{Poisson with mean }\lambda t\text{ equals }0)=e^{-\lambda t}. Example: λ=0.8\lambda=0.8 faults per km, so P(gap>2 km)=P(no faults in 2 km)=e−1.6=0.202\mathrm{P}(\text{gap}>2\text{ km})=\mathrm{P}(\text{no faults in 2 km})=e^{-1.6}=0.202. If the rate varies, for instance faults are more common near joints, neither model applies.

Exam tip

Use the Poisson count for 'how many events in a period', and the exponential for 'how long until the next event'.

That's the notes covered.

Carry on to the next subtopic.

Exam questions on Mean and variance, and link to Poisson processes

  1. The lifetime, XX days, of a type of battery is modelled by an exponential distribution with parameter λ=0.05\lambda=0.05.
    Find the probability that a battery lasts longer than its mean lifetime.2 marks
  2. Particles strike a detector at random, independently of each other, at a constant average rate of 12 per hour, so the number of strikes follows a Poisson process. Let TT minutes be the time between two successive strikes.
    Find the standard deviation of TT in minutes.2 marks
  3. The continuous random variable XX has an exponential distribution with parameter λ>0\lambda>0, so that f(x)=λe−λxf(x)=\lambda e^{-\lambda x} for x≥0x\ge0. You may use the fact that xe−λx→0xe^{-\lambda x}\to0 and x2e−λx→0x^2e^{-\lambda x}\to0 as x→∞x\to\infty.
    Prove that E(X)=1λ\mathrm{E}(X)=\frac{1}{\lambda}.3 marks
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Written by the Exaim team, led by Shaun Daswani (Head of Upper Secondary, Improve ME Institute; MSc Financial Mathematics, Imperial College London; BSc, UCL) and Jason Daswani (operational lead, Improve ME Institute; LSE).