Post hoc power calculations for m independent experiments with Bonferroni correction k
Figure | Panel | Data structure | Type of test | Power |
---|---|---|---|---|
2 | C | Normality not assumed | Mann-Whitney | 55.9 |
D | Normality not assumed | Mann-Whitney | 53.2 | |
F | Normality not assumed | Mann-Whitney | 61.7 | |
G | Normality not assumed | Mann-Whitney | 10.7 | |
H | Normality not assumed | Mann-Whitney | 12.3 | |
I | Normality not assumed | Mann-Whitney | 2.6 | |
J | Normality not assumed | Mann-Whitney | 12.6 | |
3 | B | Normality not assumed | Mann-Whitney | 21.5 |
C | Normality not assumed | Mann-Whitney | 63.3 | |
D | Normality not assumed | Mann-Whitney | 36.4 | |
4 | B | Normality not assumed | Mann-Whitney | 100 |
D | Normality not assumed | Mann-Whitney | 100100 | |
7 | A | Normality not assumed | Mann-Whitney | 37.1 |
B | Normality not assumed | Mann-Whitney | 90 | |
J | Normality not assumed | Mann-Whitney | 100100 | |
K | Normality not assumed | Mann-Whitney | 99.9100 |
From Fisher's χ2 test for combined probabilities, we have that χ2 (df = 2m) ∼ –2ln(p1p2…pm), where pi is the p value for the ith independent experiment. The post hoc expected value of χ2 is just the df + the noncentrality parameter (λ). Thus, for three independent experiments, say λ is given by –2ln(p1p2p3) – 6. The power can then be obtained directly using G*Power 3 software with α = 0.05/k.