Confidence intervals

Confidence interval for one mean (unknown σ)

Estimate the population mean when the standard deviation is unknown, using Student's t distribution.

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Explanation

In practice, the population standard deviation \(\sigma\) is rarely known exactly. When it is estimated from the sample data itself using \(s\), extra uncertainty appears, which Student's t distribution with \(n-1\) degrees of freedom models correctly.

With large samples (n ≥ 30), Student's t converges to the standard normal and both intervals give very similar results. For small samples, t produces wider intervals, correctly reflecting the greater uncertainty.

Formula

Let \(C\) denote the confidence level and \(\alpha=1-C\) the total area outside the interval. For 95% confidence, \(C=0.95\), \(\alpha=0.05\) and \(\alpha/2=0.025\) in each tail.

\( \bar{x} \pm t_{\alpha/2,\, n-1} \cdot \dfrac{s}{\sqrt{n}} \)

  • \(\bar{x}\): observed sample mean.
  • \(t_{\alpha/2,\, n-1}\): critical value of Student's t with \(n-1\) degrees of freedom.
  • \(s\): sample standard deviation (with divisor \(n-1\)).
  • \(n\): sample size.

The margin of error is \(E = t_{\alpha/2,\, n-1} \cdot s/\sqrt{n}\) and the interval is \([\bar{x} - E,\; \bar{x} + E]\).

Worked example

The response time (in ms) of a web service is measured over 15 requests: \(\bar{x} = 245.3\) ms, \(s = 38.7\) ms. With 95% confidence (\(C=0.95\), \(\alpha=0.05\)) and \(df = 14\):

\( 245.3 \pm 2.145 \cdot \frac{38.7}{\sqrt{15}} \approx [223.9,\; 266.7] \text{ ms} \)

Assumptions of the t interval

  • The sample is random and independent.
  • The variable is normally distributed in the population (especially important for small samples). For large n, the central limit theorem justifies it even if the distribution isn't exactly normal.
  • \(\sigma\) is unknown and estimated with \(s\).

How to interpret the result

The interval \([L, U]\) is the range of values of the population mean \(\mu\) compatible with the observed data and the chosen confidence level. The frequentist meaning is the following: if you repeated the experiment many times — each time taking a sample of the same size and building the CI with the same procedure — approximately \(C \times 100\%\) of those intervals would contain the true value of \(\mu\). It is not a probability statement about the specific parameter, but about the long-run reliability of the method.

The width of the interval directly communicates the precision of the estimate. A narrow interval indicates greater precision: it is obtained with larger samples, lower variability in the data, or by accepting a somewhat lower confidence level. A wide interval is not an error in itself; it honestly reflects that with that sample there is a lot of uncertainty about \(\mu\). In the chart, the green region is the confidence zone under the t curve and the red tails each represent \(\alpha/2\) of the total area; the critical values \(\pm t_{\alpha/2,\,n-1}\) delimit those regions.

  • Connection with hypothesis testing: if a reference value \(\mu_0\) falls outside the interval, the data would reject \(H_0\!: \mu = \mu_0\) at significance level \(\alpha = 1 - C\) in the equivalent two-sided test. If \(\mu_0\) falls inside, there is no evidence to reject it.
  • Effect of sample size: doubling \(n\) reduces the margin of error by a factor of \(\sqrt{2} \approx 1.41\); to halve it you need to quadruple \(n\).
  • Effect of confidence level: increasing confidence from 95% to 99% widens the interval because the critical value \(t\) grows; demanding more certainty comes at the cost of less precision.

Frequently asked questions

  • Why use t instead of z? Because estimating \(\sigma\) with \(s\) introduces extra uncertainty; the t distribution has heavier tails to account for it.
  • When do t and z converge? For n ≥ 30 the difference is practically negligible in most applications.
  • Do I need the data to be normal? For small n it does matter. For large n, the CLT guarantees that \(\bar{x}\) is approximately normally distributed.

Reference: Confidence interval — Wikipedia