--- title: "Comparison with G*Power" output: rmarkdown::html_vignette vignette: > %\VignetteIndexEntry{Comparison with G*Power} %\VignetteEngine{knitr::rmarkdown} %\VignetteEncoding{UTF-8} --- ```{r, include = FALSE} knitr::opts_chunk$set( collapse = TRUE, comment = "#>", warning = FALSE ) ``` ```{r setup, message=FALSE} library(anovapowersim) ``` The balanced simulation and calculation-only functions accept `gpower = TRUE` when results should follow G\*Power's noncentrality convention. For within-subject designs, this corresponds to selecting G\*Power's **as in Cohen (1988)** option. ## A typical 2 x 2 design In a 2 x 2 mixed design, the default and G\*Power conventions usually give very similar results. Here they differ by one participant per group: ```{r two-by-two} default_2x2 <- power_n_calc( between = c(group = 2), within = c(time = 2), term = "group:time", target_pes = 0.08, power = 0.90 ) gpower_2x2 <- power_n_calc( between = c(group = 2), within = c(time = 2), term = "group:time", target_pes = 0.08, power = 0.90, gpower = TRUE ) c(default = default_2x2$n_needed, gpower = gpower_2x2$n_needed) ``` Set `gpower = TRUE` in `power_n()`, `power_curve()`, `power_achieved()`, or `power_sensitivity()` in the same way when running simulations. ## More than three within-subject levels The conventions can diverge more noticeably for smaller samples and for terms with more degrees of freedom, such as within-subject factors with more than three levels. With four within-subject levels, the same inputs produce: ```{r four-levels} default_4 <- power_n_calc( between = c(group = 2), within = c(time = 4), term = "group:time", target_pes = 0.08, power = 0.90 ) gpower_4 <- power_n_calc( between = c(group = 2), within = c(time = 4), term = "group:time", target_pes = 0.08, power = 0.90, gpower = TRUE ) c(default = default_4$n_needed, gpower = gpower_4$n_needed) ``` In this case, use the package default, `gpower = FALSE`, so `target_pes` continues to match the partial eta squared you supplied. Use `gpower = TRUE` only when reproducing G\*Power's **as in Cohen (1988)** result is specifically required.