Past exam of the mathematics course of the University of Cambridge 2014 ia Paper 3 12A a Created 2026-09-24 Updated 2026-09-24
Past exam of the mathematics course of the University of Cambridge 2014 ia Paper 3 11A iv Created 2026-09-24 Updated 2026-09-24
Past exam of the mathematics course of the University of Cambridge 2014 ia Paper 3 11A iii Created 2026-09-24 Updated 2026-09-24
Past exam of the mathematics course of the University of Cambridge 2014 ia Paper 3 11A ii Created 2026-09-24 Updated 2026-09-24
Past exam of the mathematics course of the University of Cambridge 2014 ia Paper 3 11A i Created 2026-09-24 Updated 2026-09-24
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Past exam of the mathematics course of the University of Cambridge 2014 ia Paper 3 10A b Created 2026-09-24 Updated 2026-09-24
Past exam of the mathematics course of the University of Cambridge 2014 ia Paper 3 10A a Created 2026-09-24 Updated 2026-09-24
Past exam of the mathematics course of the University of Cambridge 2014 ia Paper 2 9F Solution Created 2026-09-24 Updated 2026-10-06
A probability space consists of a sample space , a sigma-algebra of events, and a probability measure satisfying:
- for every .
- .
- For pairwise disjoint events, .
For arbitrary events, Boole's inequality is . To prove it, replace each by . The are disjoint, have the same union, and satisfy . Countable additivity and monotonicity give . Finite unions are included by taking subsequent events empty.
Let be the th heads event. For every , the event of infinitely many heads lies inside . By the union bound, its probability is at most , which tends to zero. Thus the probability of infinitely many heads is . This is the First Borel-Cantelli lemma, and requires no independence of the coin tosses.
For the dice experiment there are ordered outcomes giving a sum of and giving , out of . Each trial therefore has , and irrelevant-outcome probability . By independence between trials, summing over the number of initial irrelevant outcomes givesThe geometric series also shows that one of the two relevant sums eventually appears almost surely. Equivalently, first-step analysis gives .
Past exam of the mathematics course of the University of Cambridge 2014 ia Paper 2 8B iv Created 2026-09-24 Updated 2026-09-24
Past exam of the mathematics course of the University of Cambridge 2014 ia Paper 2 8B iii Created 2026-09-24 Updated 2026-09-24
Past exam of the mathematics course of the University of Cambridge 2014 ia Paper 2 8B ii Created 2026-09-24 Updated 2026-09-24
Past exam of the mathematics course of the University of Cambridge 2014 ia Paper 2 8B i Created 2026-09-24 Updated 2026-09-24
Past exam of the mathematics course of the University of Cambridge 2014 ia Paper 2 7B b Created 2026-09-24 Updated 2026-09-24
Past exam of the mathematics course of the University of Cambridge 2014 ia Paper 2 7B a Created 2026-09-24 Updated 2026-09-24
Past exam of the mathematics course of the University of Cambridge 2014 ia Paper 2 6B iii Created 2026-09-24 Updated 2026-09-24
Past exam of the mathematics course of the University of Cambridge 2014 ia Paper 2 6B ii Created 2026-09-24 Updated 2026-09-24
Past exam of the mathematics course of the University of Cambridge 2014 ia Paper 2 6B i Created 2026-09-24 Updated 2026-09-24
Past exam of the mathematics course of the University of Cambridge 2014 ia Paper 2 5B Solution Created 2026-09-24 Updated 2026-10-06
For and on an interval where , the logarithmic derivative substitution givesThe quadratic terms cancel. Multiplying by gives the linearization of a Riccati equation:Multiplying by a nonzero constant leaves unchanged. If , that substitution is undefined, but the original equation is already a first-order linear ordinary differential equation, solvable by an integrating factor.
For the particular equation, and the linear equation is . Use the PDF's logarithmic coordinate and write . The chain rule gives and , leaving . Thus , as also follows from the Euler-Cauchy equation. Recovering the Riccati equation solution yieldsThe initial value imposes ; choose . ThereforeThe denominator vanishes only at , and its numerator is then nonzero. This is a simple pole: . The maximal interval containing is ; the same expression on is a separate solution branch. These are poles of a Riccati solution from zeros of its linearizing solution.
Past exam of the mathematics course of the University of Cambridge 2014 ia Paper 2 4F Solution Created 2026-09-24 Updated 2026-10-06
Write the countable supports as and the marginal masses as . Independence gives joint mass . Assuming finite expected values, absolute integrability is justified by Tonelli theorem:Consequently Fubini's theorem permits factorization of the signed sum, proving the expectation of a product of independent random variables:
The second claim holds as a general assertion with the additional hypothesis that the positive variables are integer-valued. For a nonnegative integer-valued , the pointwise identity and Tonelli theorem give the tail-sum formulaIf each is integer-valued, their product is too. Apply this identity to each factor and to the product, then use independence:Under the literal broader meaning of a discrete random variable, the second claim is false. Two independent constants are positive and discrete, but the left side is and the right side is . More generally the integer-indexed tail sum of a positive real-valued variable is , not . This is the integer-valued hypothesis in the tail-sum formula.
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