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. 2002 Jul 15;542(Pt 2):515–527. doi: 10.1113/jphysiol.2002.017541

Figure 6.

Figure 6

Simulation of effect of osmolality on diffusion curves

Because electrode spacing, transport number and clearance vary slightly between experiments, the original curves cannot be easily compared so values of λ and α were derived from eqns (12) and (13). These values were then inserted in eqn (1) to generate the curves shown in this figure. Equation (2) was used with a bias current of 20 nA to give the baseline for the first 10 s, then a main current of 100 nA was applied in the interval 10–60 s. A constant clearance of k’ = 0.02 s−1 was used, the electrode spacing was 100 μm and the transport number was nt = 0.3. The shape of the concentration surface changes dramatically as osmolality increases as seen when every fourth concentration curve is projected on the [TMA+]-Time plane (cf. Figs 2 and 3).