We also measured the amount and duration of the phase shifts and the voltage deflections caused by IPSPs and I-pulses, averaged all individual plots of membrane potential vs. time of every cell (temporally aligned at the beginning of the IPSP/I-pulse), and equally extrapolated a linear fit to the 300 ms before the IPSP/I-pulse.
This conclusion is backed up by Figure 3, which shows a plot of the membrane permeability k (m) against the dimensionless slip parameter, calculated using the retentate flowrate equation given in (15) (using the Q l,out, Qe,out and values at time =3 min).
(E ) dV/dt is plotted as function of membrane voltage for the APs in panel (D ) (dKO, red; WT, black).
The activation energy was calculated from plot of the maximum membrane exit flux (Jamax) versus (1/T) at 300 rpm(Equation 3), as presented in Figure 4. Figure 4 Arrhenius plots for transport of mercury II) in liquid membrane.
A comprehensive view over all 17 RBCs is given in a plot of iBP versus membrane potential (Figure 3D, circles), which clearly shows the two ranges.
In agreement with this idea, a phase-plane plot of dV/dt vs membrane voltage showed that APs induced by PP stimulation in CA2 PNs consistently exhibited an initial rapid dV/dt signal at potentials sub-threshold to the main spike.
Fig. 6 Box plot representing mean values of membrane thicknesses for the investigated groups Fig. 7 Box and Whisker plot representing median and range values of membrane thicknesses with different morphologies.
(B ) Fractional inhibition is plotted as a function of membrane voltage.
At the right of each panel, histogram plotting the peak amplitude of membrane depolarizations induced by Bk.
At the right of each panel, histogram plotting the peak amplitude of membrane depolarizations induced by Bk before (black) and after (red) the superfusion of the medium.
