The statistical evaluation of a sequence of measurements
Ask the tutor about The statistical evaluation of a sequence of measurementsOpen the graphing workbench
Checking for a normal distribution ends with a measurement series whose points hug the probability-paper line. So take the random variable to be normally distributed, with the normal distribution of mean and standard deviation . Neither nor is known. The empirical mean and empirical standard deviation and are only estimates from one series. How far from them can the true values lie?
Pay for an unknown σ with t
Proceed in two steps.
- Measure the quantity a total of times, giving .
- Choose a small number as the probability of being wrong, and look up in a table of Student's -distribution with degrees of freedom.
Then the unknown mean satisfies
and this statement is wrong with probability .
Compare this with the interval for a known , which uses . Here is unknown, so its estimate takes its place. The factor is larger than to pay for that extra uncertainty, and the whole half-width shrinks like .
Example 1. The heights in the empirical measurement series give , and . Choose . For the -table gives . Assuming height is normally distributed, with error probability ,
Drag and . The interval always stays centered on . Adding measurements narrows it twice over, because falls as grows and grows in the denominator.
The χ² interval is lopsided
With error probability , the standard deviation satisfies
The numbers and are read from a table of the -distribution with degrees of freedom.
Example 2. Take the same eight heights again. For , the -table gives and . Taking square roots gives
Drag . Both ends scale with it, but they do not sit evenly around it: is about above the left end and more than below the right end. The -values and are not mirror images of each other, so this interval is lopsided, unlike the one for .
Eight measurements leave a wide band
Both estimates are rough: the mean is pinned down only to a band about units wide, and only to a factor of four. Eight measurements are very few, so that width is expected. The interval for stays symmetric about ; the interval for does not.