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. 2002 Jul 15;542(Pt 2):477–492. doi: 10.1113/jphysiol.2001.013197

Figure 7.

Figure 7

VmS2s with non-parallel time courses at high field intensities

A, a cell (length:143 μm)that was successively stimulated with S2 stimuli of 38.3 and 56.2 V cm−1. B, upper and lower sets of traces, show the VmS2 responses for the two S2 stimuli,which change from a parallel behaviour (at 38.3 V cm−1) to non-parallel behaviour (at 56.2 V cm−1). Moreover,following the pulse a depression in the plateau potential was observed for the S2 of 56.2 V cm−1, indicated by the arrow in B, lower set of traces. For comparison with other cells the V^mS2s are indicated in parentheses. C, the S2 response measured at 1 ms (VmS2(n, 1.0)) and 9 ms (VmS2(n, 9.0)). The VmS2(n, 9.0) decreased in slope, and shifted in the depolarizing direction from VmS2(n, 1.0). D, the slope reduction Δ (∇VmS2), which is equivalent to the internal field Ei, rises exponentially during S2 (τ = 2.7 ms). E, the slope reduction at the end of S2, Δ(∇VmS2(n, 10)), increases monotonically with V^mS2 (r = 0.66, P < 0.05, n = 17).The dashed lines indicate that Ei is 3.2 V cm−1 for a V^mS2 of 300 mV.