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. Author manuscript; available in PMC: 2013 Dec 10.
Published in final edited form as: Neuron. 1989 Nov;3(5):573–581. doi: 10.1016/0896-6273(89)90267-5

Figure 7. Comparrson of the Voltage Ranges over Which IKx and Ih Gate and the Simulated Effect of IKx on the Photovoltage.

Figure 7

Recordings were made from cells bathed in Ringer solution containing 5 mM Cs+ and 0.1 mM Cd2+.

(A) Activation and τ curves for IKx and Ih as used in our computer reconstruction of the light response. The reversal potentials for IKx and Ih were –74 and –32 mV, respectively, and the rod's dark resting potential is marked by the vertical broken line. The data for salamander rod Ih come from Hestrin (1987).

(B, top) The photocurrent in response to a dim flash measured from published data for salamander rods (Baylor et al., 1984, their Figure 2A; response to 0.98 photons mm–2) with the points (closed circles) fitted by eye using the Independence equatron (I = (15.5(exp(–1.6t)))(1 – exp(–1.6t))3) from Baylor et al. (1974), in which I is the photocurrent (pA) and t is time (s). Zero on the vertical axis corresponds to an inward dark current of 40 pA. This current trajectory was applied to a computer model circuit with the following current components: gKxnKx(E – EKx) and gL(E – EL), in which E is membrane potential, EKx and EL are reversal potentials with values equal to –74 and –77 mV, respectively, gKx is the maximum conductance underlying IKx (1.04 ± 0.23 nS, mean ± SD, n = 12), and nKx is a value between 0 and 1 that represents the proportion of channels in the open state. A voltage-independent leak conductance, gL, of 0.35 nS and a membrane capacitance of 21 pF (Baylor et al., 1984) were assumed. (B, middle) Two calculated voltage responses to the photocurrent are shown: (a) the continuous line, when nKx was allowed to vary according to the differential equation: dnKx/dt = α(1 – nKx) – β(nKx) (α and β from Figure 3C); (b) the broken line, when the nKx term was held constant at the resting value of 0.719 (i.e., IKx with no voltage dependence). Zero on the vertical axis corresponds to a resting potential of –38.2 mV. The vertical arrows point to the peaks of the voltage responses. (B, bottom) Cating of the channels underlying IKx (described by nKx) during the photocurrent, correspondrng to the two voltage responses described above.