Past exam of the mathematics course of the University of Cambridge 2009 iii Paper 37 3 Solution Created 2026-10-03 Updated 2026-10-14
In the classical risk model, let be the Poisson process of claim arrivals, independent of the independent claim sizes. The reserve starts at and earns premiums continuously at rate , soHere is the ultimate ruin probability and is the survival probability. The relative safety loading is .
To derive the survival integro-differential equation, condition on the first claim time , which has the exponential distribution of rate . Immediately before that claim the available capital is . A claim leaves survival probability , since the future claim process restarts with the same independent law; a larger claim causes ruin immediately. The first-claim decomposition for survival probability is thereforePut and . Changing variables to yieldsThis representation justifies differentiation. The function is continuous: extend by zero to negative arguments, then use continuity of translations of the integrable density in to control its convolution with the bounded function . Differentiating the lower endpoint of the displayed integral gives . Since ,This deduction uses the first-arrival law rather than taking the desired differential equation as an assumption.
For , the claim law is an Erlang distribution of shape two and rate two. Its mean is . With , we have . Changing the convolution variable to givesHence the first requested specialization isLet . Differentiation under the finite integral gives and . Differentiating the preceding equation and using then givesThus the second identity isDifferentiate once more:The preceding second-derivative equation gives . Substitution cancels the undifferentiated terms and provesThis is the Erlang claim-size differential equation for survival probability with and .
Its characteristic polynomial factors as . The limit therefore makes the general bounded solutionThe supplied zero-capital survival probability is , so . We also need the initial derivative carried by the original integral equation: implies , giving . Solving gives and . Therefore the survival and ruin probabilities areThe extra initial derivative is essential: and the limit at infinity alone would leave one free parameter in the third-order equation. The result has and tends to zero. It is positive and decreasing, since for . These signs agree with its interpretation as an ultimate ruin probability.