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Continuous Random Variables Arthur White∗ 7th December 2016 A random variable X is said to be continuous if its behaviour is described by a continuous probability density function (PDF), f . In particular, Z P(X ∈ A) = f (x)dx. A Note that from this definition, it necessarily follows that P(X = x) = 0, for all x. For a continuous random variable, it does not make meaningful sense to consider the probability of observing an exact value to infinite precision. R∞ For f (x) to be a valid PDF, it is required that f (x) ≥ 0 for all x, and that −∞ f (x)dx = 1. Rx We are often interested in P(X ≤ x) = −∞ f (t)dt = F (x). We call F the cumulative density d F (x). function (CDF). Note that it then immediately follows that f (x) = dx Expectation and Variance R∞ For continuous distributions, the expected value of X is given as: E[X] = −∞ xf (x)dx. This is more or less the same as the definition as for a discrete random variable that we saw before, except that the summation had been replaced by an integral. As before, Var[X] = E[(X − µ)2 ] = E[X 2 ] − E[X]2 . Uniform Distribution We say that a random variable X ∼ U(a, b) follows a uniform distribution on the interval [a, b] if 1 a≤x≤b b−a f (x) = 0 otherwise. It is straightforward to show that Z ∞ Z f (x)dx = −∞ ∗ a b 1 dx = 1, b−a Based extensively on material previously taught by Eamonn Mullins. 1 and Z x F (x) = a 1 x−a dt = . b−a b−a It can also be shown that E[X] = and Var[X] = b+a , 2 (b − a)2 . 12 This is left as an exercise. Example Suppose that X ∼ U(0, 10). What is P(X ≤ 3)? What is P(3 ≤ X ≤ 8)? Using the CDF F (x), we see that P(X ≤ 3) = F (3) = 3/10. Similarly, P(3 ≤ X ≤ 8) = P(X ≤ 8) − P(≤ 3) = F (8) − F (3) = 8/10 − 3/10 = 1/2. Monte Carlo integration Unlike the normal distribution, it is unusual for a uniform distribution to be chosen to model the behaviour of real life applications. Nonetheless, it has several useful properties that mean it is regularly used to perform calculations. In particular, it is often used to perform Monte Carlo (named after the casino in Monaco) simulations. In what follows we will assume that we can generate y1 , . . . , yn ∼ U(0, 1). Integral estimation Suppose that we wish to estimate an integral Z 1 g(x)dx, I= 0 but that g(x) has a complicated form, making the integral intractable to compute exactly. Let Y ∼ U(0, 1). Then f (y) = 1, for all y ∈ [0, 1], and it follows that Z 1 Z 1 E[g(Y )] = g(y)f (y)dy = g(y)dy = I. 0 0 If we then generate y1 , . . . , yn ∼ U(0, 1), then the Law of Large Numbers tells us that, for sufficiently large n, n X g(yi )/n ≈ I. ḡ = i=1 2