What Observed Post Hoc Power Calculates
After a hypothesis test, it can seem helpful to calculate the study’s “observed power”: the probability that the test would reject the null if the true effect were equal to the effect estimated from the data. The calculation is possible, but it is usually a poor way to learn what the data say. In common settings, observed power is largely a restatement of the test statistic and p-value, not new evidence about the effect.
To make this precise, consider a one-sample test of a population mean. Suppose observations are independent and normally distributed with known standard deviation \(\sigma\), and the sample size \(n\) is fixed. We test \(H_0:\mu=0\) against \(H_a:\mu\ne 0\) using a two-sided z test at significance level \(\alpha\). Under this model, the standard error is \(SE=\sigma/\sqrt{n}\), and the test rejects when the absolute value of the standardized statistic exceeds the appropriate normal critical value.
Observed power is therefore conditional on a particular model, test, significance level, sample size, and assumed effect. It is not, in general, a probability or forecast for a future study. A future study’s rejection probability equals this calculation only if its relevant design and assumptions match and the true effect is assumed to equal the observed estimate.
Why It Largely Restates the Test Result
For the two-sided z test above, write the observed estimate as \(\hat{\theta}\), its standard error as \(SE\), and the observed test statistic as \(z_{\text{obs}}=\hat{\theta}/SE\). The null is zero, so the estimate is also the observed difference from the null value. Let \(\Phi\) denote the cumulative distribution function of a standard normal random variable, and let \(c=z_{1-\alpha/2}\) be the positive critical value. If the true effect were \(\hat{\theta}\), the test statistic would have a normal distribution with mean \(\hat{\theta}/SE\) and standard deviation 1. The observed power is consequently:
The two terms are the probabilities of crossing the positive and negative rejection boundaries under the plug-in effect. By contrast, the two-sided p-value is \(2\Phi(-|z_{\text{obs}}|)\). Both quantities are determined by the same absolute observed z statistic when the test and standard error are fixed.
The monotonic relationship can be checked directly. For a positive plug-in standardized effect \(d=|z_{\text{obs}}|\), power is \(g(d)=\Phi(d-c)+\Phi(-d-c)\). Its derivative is \(g'(d)=\phi(d-c)-\phi(d+c)\), where \(\phi\) is the standard normal density. Since \(d,c>0\) imply \(|d-c|<d+c\), and the standard normal density decreases as the absolute value of its argument increases, \(\phi(d-c)>\phi(d+c)\). Therefore \(g'(d)>0\): larger absolute z statistics produce larger observed power. The p-value moves in the opposite direction because \(2\Phi(-d)\) decreases as \(d\) increases.
This exact relationship applies to the stated z-test setup. Other tests or calculations may not yield this exact formula, especially if their standard errors or degrees of freedom are handled differently. The central concern remains: inserting the observed estimate as though it were the true effect uses the same data twice, first to obtain the estimate and then to calculate a power value from it.
Worked Example: A Nonsignificant Test and Its Observed Power
Suppose a hypothetical sample of \(n=25\) independent observations is drawn from a normal population with known \(\sigma=10\) units. The sample mean is \(\bar{x}=3\) units. Test \(H_0:\mu=0\) against \(H_a:\mu\ne0\) at \(\alpha=0.05\), and calculate observed power.
Check the model and test conditions. For this calculation, assume the observations are independent, normally distributed with the stated known standard deviation, and that \(n=25\) was fixed. The two-sided z test is then appropriate under the specified model. Its standard error and statistic are:
The two-sided p-value is \(2\Phi(-1.50)\approx0.1336\), so the test does not reject at the 0.05 level. For observed power, use the plug-in assumption that the true mean is the observed mean, 3 units. The critical value is approximately 1.96, and the plug-in standardized effect is \(3/2=1.50\):
The result is about 32.3% observed power. That number is a model-based rejection probability under the assumption that the true mean is 3 units, not an estimate of the probability that the null is false. The 95% confidence interval for the mean is \(3\pm1.96(2)\), or approximately \((-0.92,6.92)\) units. Its width makes clear that the estimate is imprecise; the interval displays a range of effects compatible with the data and model more directly than the post hoc power number does.
Use the Confidence Interval to Assess Uncertainty
A confidence interval reports estimated effects and their uncertainty in the units of the problem. In repeated samples under the model, a 95% confidence-interval procedure covers the fixed population parameter in 95% of samples. Once an interval has been calculated, it is not correct to say there is a 95% probability that the fixed parameter lies in that particular interval. Instead, examine the interval’s center, width, and range: which effect sizes are consistent with the data at the interval’s confidence level, and which would be substantively important?
For the known-\(\sigma\) one-sample mean model, the 95% interval is \(\bar{x}\pm1.96SE\). Other settings require the interval procedure appropriate to their model; the point here is to use an interval that matches the analysis, not to apply this formula universally. A confidence interval cannot remove uncertainty, but it expresses it in a way that makes the magnitude and precision of effects visible.
Worked Example: A Significant Result Can Still Have Modest Observed Power
In a second hypothetical study, suppose \(n=100\), the observations are independent and normally distributed, \(\sigma=10\) units is known, and \(\bar{x}=2\) units. Use the same two-sided z test at \(\alpha=0.05\). The fixed sample size, stated model, known standard deviation, and two-sided test meet the conditions for this calculation.
The standard error is \(10/\sqrt{100}=1\) unit, so \(z_{\text{obs}}=2/1=2.00\). The two-sided p-value is \(2\Phi(-2.00)\approx0.0455\), just below 0.05. The observed power, plugging in 2 units as the true mean, is:
The observed power is about 51.6%, even though the test is statistically significant. The 95% confidence interval is \(2\pm1.96(1)\), or \((0.04,3.96)\) units. The estimate is close to the threshold for statistical significance, and the interval indicates substantial uncertainty about the size of the mean. The observed power does not add a separate confirmation that the result is reliable; it is another transformation of the observed statistic.
Plan Power Around an Effect of Interest
Power is valuable when used before data collection to evaluate a proposed design. A researcher specifies a meaningful effect size in advance, along with a model, test, significance level, and planned sample size. The resulting power answers a design question: if the specified effect were true and the assumptions held, how often would this planned test reject the null in repeated studies?
This use differs from observed post hoc power in a crucial way. The target effect is chosen for scientific or practical reasons, rather than selected because it happened to be the estimate in the completed study. Planning across a range of plausible effects can also show how conclusions depend on the assumed effect size. Power is not a guarantee that a particular study will detect an effect, nor does it measure the probability that the effect is true.
Worked Example: Planning for a Meaningful Mean Difference
Suppose a hypothetical study is designed with \(n=25\) independent normal observations and known \(\sigma=10\) units. Before collecting data, investigators decide that a mean difference of 4 units would be scientifically meaningful. They plan a two-sided z test at \(\alpha=0.05\). Assume the model and fixed sample size stated above hold. What is the planned power at a true mean difference of 4 units?
Here \(SE=10/\sqrt{25}=2\) units. Under the specified true effect, the standardized mean of the test statistic is \(4/2=2.00\). With critical value 1.96, the planned rejection probability is:
Thus, this design has about 51.6% power to detect a 4-unit mean difference with the specified two-sided test under the model. This is a prospective statement about repeated studies if the true effect is 4 units and the design assumptions hold. It also signals that this design would not detect that target effect in every study; investigators could consider whether the planned sample size is adequate for their purpose.
Now suppose the completed study instead produced \(\bar{x}=1.2\) units. The observed-power calculation would substitute 1.2, giving a standardized plug-in effect of \(1.2/2=0.60\):
The two-sided p-value for this observed result is \(2\Phi(-0.60)\approx0.5485\). The 95% confidence interval is \(1.2\pm1.96(2)\), or approximately \((-2.72,5.12)\) units. The post hoc power of about 9.21% follows from plugging the observed estimate into the same test calculation; the planned power of about 51.6% addressed the prespecified 4-unit effect. These are answers to different questions, and the first should not replace examination of the interval or of the design assumptions.
Common Pitfall and Practical Guidance
Wrong reasoning: “The observed power is low, so the study shows there is probably no effect,” or “the observed power is high, so a future study is likely to be significant.” Neither conclusion follows. Observed power assumes the observed estimate is the true effect; it does not assign probabilities to possible true effects. It is not, in general, an unconditional forecast for a future study. Only when the future test’s relevant design and assumptions match, and its true effect is assumed to equal the observed estimate, does its rejection probability equal the plug-in observed power.
Correction: Report the estimate and a suitable confidence interval to communicate effect size and uncertainty. Interpret the test result using the p-value and prespecified decision rule, without treating either as a measure of the probability that the null is true. If the question is whether a design can reliably detect an effect that matters, calculate power prospectively for that specified effect and design. The earlier material on why a nonsignificant result does not prove no effect addresses that related interpretive issue; a low observed-power value does not resolve it.
In practice, observed power may be requested by software or included in a report, but its presence does not make it informative beyond the test result in the fixed-standard-error z setting developed here. The more useful questions are: What effect did the study estimate? How precise is that estimate? What range of effects is consistent with the data? And, for a future study, what power would its design have for a scientifically meaningful target effect?
Check Your Understanding
Answer each question using the definitions and model assumptions in this tutorial.
- In your own words, define observed post hoc power and identify the assumption about the true effect that it uses.
- For the two-sided z test described here, explain why observed power and the p-value are not independent summaries of the data.
- A researcher reports low observed power after obtaining a nonsignificant result. Why does that calculation not show that the null hypothesis is probably true?
- What information about an estimated mean effect can a confidence interval communicate that a single observed-power value does not?
- Before a study begins, a team calculates power for a prespecified effect it considers meaningful. How does that design-based question differ from calculating power after substituting the observed effect?