Cochran's theorem
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In statistics, Cochran's theorem is used in the analysis of variance.
Suppose U1, ..., Un are independent standard normally distributed random variables, and an identity of the form
- [\sum_^n U_i^2=Q_1+\cdots + Q_k]
- [r_1+\cdots +r_k=n]
Cochran's theorem is the converse of Fisher's theorem.
Example
If X1, ..., Xn are independent normally distributed random variables with mean μ and standard deviation σ then
- [U_i=(X_i-\mu)/\sigma]
It is possible to write
- [\sum U_i^2=\sum\left(\frac}\right)^2+ n\left(\frac-\mu}\right)^2]
- [\sum(X_i-\mu)^2=\sum(X_i-\overline+\overline-\mu)^2]
- [\sum(X_i-\overline)^2+\sum(\overline-\mu)^2+2\sum(X_i-\overline)(\overline-\mu).]
- [\sum(\overline-X_i),]
Combining the above results (and dividing by σ2), we have:
- [\sum\left(\frac\right)^2=\sum\left(\frac}\right)^2+n\left(\frac-\mu}\right)^2=Q_1+Q_2.]
Cochran's theorem then states that Q1 and Q2 are independent, with Chi-squared distribution with n − 1 and 1 degree of freedom respectively.
This shows that the sample mean and sample variance are independent; also
- [(\overline-\mu)^2\sim \frac\chi^2_1.]
- [\widehat^2=\frac\sum\left(X_i-\overline\right)^2. ]
- [\widehat^2\sim\frac\chi^2_]
Both these distributions are proportional to the true but unknown variance σ2; thus their ratio is independent of σ2 and because they are independent we have
- [\frac-\mu\right)^2}\sum\left(X_i-\overline\right)^2}\simF_]
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