To determine the relative contribution of magnitude asymmetries compared to temporal asymmetries in generating directional selectivity in the PSPs, we manipulated the conductance waveforms and tested them in model cells. (a) A schematic depicting how the magnitudes of the original conductance waveforms (top) were ‘swapped’ (bottom). One swapped conductance had the preferred timing (latency and shape) and the null magnitude (area under the curve, bottom left). The other had the null timing and the preferred magnitude (bottom right). (b, c) We swapped magnitudes of both inhibitory and excitatory conductances, and the resulting swapped conductances were injected into the same model cell as the control conductances. The swapped conductances with the preferred magnitudes (c, right) evoked a larger PSP compared to those with the null magnitudes, showing that magnitude asymmetries were more important than timing in generating PSP directionality. (PSPs in black, Excitation in red, inhibition in blue.) (d) We compared directionality in the swapped PSPs (swap-DSIs) to the directionality in the control PSPs (PSP-DSI). Swap-DSI > 0 indicates that timing was more important than magnitude; swap-DSI < 0 indicates that magnitude was more important than timing; swap-DSI = 0 indicates equal importance of both timing and magnitude. Points on the unity lines would indicate that directionality was determined by only timing (top diagonal) or only magnitude (bottom diagonal). Example cell shown in red.