Uniform Distribution Transformation

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SUMMARY

The discussion centers on finding the distribution of the random variable Y = X^2, where X is uniformly distributed on the interval [-1, 1]. The transformation is not monotonic, necessitating the use of a generalized theorem for transformations of random variables. The probability density function (PDF) for Y is derived as f_Y(y) = 1/(2√y) for y in [0, 1] and 0 otherwise. The expected value E[Y] is calculated as 1/3, while the variance can be computed using the law of the lazy statistician.

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Oxymoron
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Homework Statement


A random variable X is distributed uniformly on [-1,1]. Find the distribution of X^2, its mean and variance.

The Attempt at a Solution


Define a transformation of random variable as Y=X^2. Problem is that the transformation function is not monotonic on the range. If it was just on [0,1] or [-1,0] then it would be monotonic and I could find inverses and hence define the cumulative distribution function, then differentiate to find the distribution.

Is this a correct deduction? Or is there more to it?
 
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This is correct. So you can not apply the theorem directly because the square function is not increasing or decreasing on [-1,1].

There are two ways around this:
- Using a generalization of the theorem. Maybe you seen this:

Let X have pdf fX, let Y=g(X). Let S be the sample space. Suppose there is a partition of A0,...,Ak of S such that P(X\in A_0)=0 and that fX is continuous on each Ai. Further, suppose that there exists functions g1,...,gk on A1,..., Ak such that
  • g(x)=gi(x) for x in Ai.
  • gi(x) is monotone on Ai.
  • The range Y=gi(Ai) is the same for each i
  • gi-1 has a continuous derivative on Y

Then f_Y(y)=\sum_{i=1}^k{f_X(g_i^{-1}(y))\left|\frac{d}{dy}g_i^{-1}(y)\right|} for y in Y and 0 otherwise.

Apply this theorem with A_0=\emptyset,~A_1=[-1,0],~A_2=[0,1] and g(x)=x2.

- If you haven't seen this theorem, then a direct computation of the distribution of Y=X^2 is also possible:

F_Y(y)=P(Y\leq y)=P(X^2\leq y)=P(-\sqrt{y}<X\leq \sqrt{y})=F_X(\sqrt{y})-F_X(-\sqrt{y})

Now differentiate it to get the pdf.
 
Okay, so when I differentiate I get
f_Y(y) = \frac{\mbox{d}}{\mbox{d}y}F_Y(y) = \frac{\mbox{d}}{\mbox{d}y}F_X(\sqrt{y})\cdot\frac{1}{2\sqrt{y}}-\frac{\mbox{d}}{\mbox{d}y}F_X(-\sqrt{y})\cdot\frac{1}{-2\sqrt{y}}
=f_X(\sqrt{y})\cdot\frac{1}{2\sqrt{y}}-f_X(-\sqrt{y})\cdot\frac{1}{-2\sqrt{y}}
=\frac{1/2}{2\sqrt{y}}-\frac{1/2}{-2\sqrt{y}}
=\frac{1}{2\sqrt{y}}

and this is a PDF since

\int_{0}^{1}\frac{1}{2\sqrt{y}}\mbox{d}y = 1

I can change the limits of the integral because I have already imposed that this integral exists on the partition 0\leq y < 1.
 
Last edited:
I also tried using the theorem and got the same answer.

What about the expected value?

By definition:

E[Y] = \int_{-\infty}^{\infty}y\frac{1}{2\sqrt{y}}\mbox{d}y = \infty

But can I change the limits to 0 and 1 so that

E[Y] = \int_0^1y\frac{1}{2\sqrt{y}}\mbox{d}y = \frac{1}{3}

is this something I can do? Or is the mean (and hence the variance) actually infinity for Y?
 
Oxymoron said:
Okay, so when I differentiate I get
f_Y(y) = \frac{\mbox{d}}{\mbox{d}y}F_Y(y) = \frac{\mbox{d}}{\mbox{d}y}F_X(\sqrt{y})\cdot\frac{1}{2\sqrt{y}}-\frac{\mbox{d}}{\mbox{d}y}F_X(-\sqrt{y})\cdot\frac{1}{-2\sqrt{y}}
=f_X(\sqrt{y})\cdot\frac{1}{2\sqrt{y}}-f_X(-\sqrt{y})\cdot\frac{1}{-2\sqrt{y}}
=\frac{1/2}{2\sqrt{y}}-\frac{1/2}{-2\sqrt{y}}
=\frac{1}{2\sqrt{y}}

This is not entirely correct, you have said f_X(\sqrt{y})=1/2, but this is only true if y\leq 1. So for y>1, you would have f_Y(y)=0. So your density would actually be f_Y(y)=\frac{1}{2\sqrt{y}} if y\in [0,1] and 0 otherwise.<br /> <br /> This fixes your paradox with the calculation of the mean.
 
Yes it does. Thank you micromass, I should be able to go on and calculate the expected value and variance of this pdf.
 
Also note that you don't necessairily need to know the pdf to calculate the variance and the mean, since you have

E[X^2]=\int{x^2f_X(x)dx},~Var(X^2)=E[X^4]-E[X^2]^2=\int{x^4f_X(x)dx}-\left(\int{x^2f_X(x)}\right)^2

Here we have essentially used the more general formula

E[g(X)]=\int{g(x)f_X(x)dx}

which is often called "the law of the lazy statistician" :smile:
 

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