Cyclic AMP Diffusion Coefficient in Frog Olfactory Cilia

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Cyclic AMP Diffusion Coefficient in Frog Olfactory Cilia Chunhe Chen, Tadashi Nakamura, Yiannis Koutalos  Biophysical Journal  Volume 76, Issue 5, Pages 2861-2867 (May 1999) DOI: 10.1016/S0006-3495(99)77440-0 Copyright © 1999 The Biophysical Society Terms and Conditions

Figure 1 Currents elicited by different concentrations of cAMP from an excised olfactory cilium. L=38μm; V=−40mV. Biophysical Journal 1999 76, 2861-2867DOI: (10.1016/S0006-3495(99)77440-0) Copyright © 1999 The Biophysical Society Terms and Conditions

Figure 2 Dependence of steady-state currents on cAMP concentration. (A) Steady-state currents plotted as a function of the cAMP concentration for the experiment of Fig. 1. The currents have been normalized with respect to the current at 20μM cAMP. The smooth curve is the Hill equation (Eq. 4) with K1/2=2.8μM and n=1.8. (B) Averaged results from six cilia. Error bars indicate standard errors. The smooth curve is a least-squares fit according to the Hill equation, giving K1/2=3.3μM and n=1.8. Biophysical Journal 1999 76, 2861-2867DOI: (10.1016/S0006-3495(99)77440-0) Copyright © 1999 The Biophysical Society Terms and Conditions

Figure 3 Determinations of the scaling factor α from currents activated by low concentrations of cAMP. (A) Scaled fits of the template J(T) (thick lines) to the current record (thin line) for the 0.5μM cAMP step in Fig. 1. The scaling factor α was 0.25s−1 and 0.30s−1 for the rising and the falling phase, respectively. (B) Template fits for the 1μM cAMP step in Fig. 1. α=0.25s−1 for both the rising and falling phases. (C) Template fits for the 2μM cAMP step in Fig. 1. α=0.30s−1 for the rising phase and 0.25s−1 for the falling phase. Biophysical Journal 1999 76, 2861-2867DOI: (10.1016/S0006-3495(99)77440-0) Copyright © 1999 The Biophysical Society Terms and Conditions

Figure 4 Determinations of the scaling factor α from currents activated by high concentrations of cAMP. (A) The solid line is a scaled fit of the template J(T) to the early rising phase of the current elicited by the 5μM cAMP step in Fig. 1. The scaling factor α was 0.30s−1. The dashed line is an exponential fit to the falling phase, giving a scaling factor of 0.23s−1. (B) Analysis of the current elicited by 10μM cAMP in Fig. 1. The scaling factors for the rising and the falling phase were 0.25s−1 and 0.24s−1, respectively. (C) Analysis of the current elicited by 20μM cAMP in Fig. 1. The scaling factors for the rising and the falling phase were 0.20s−1 and 0.23s−1, respectively. Biophysical Journal 1999 76, 2861-2867DOI: (10.1016/S0006-3495(99)77440-0) Copyright © 1999 The Biophysical Society Terms and Conditions

Figure 5 Dependence of the amplitude and kinetics of the cAMP-activated current on membrane voltage. (A) Currents elicited by 20μM cAMP at different voltages. Leak currents have been subtracted. From left to right, membrane voltage was held at −60, −40, −20, +20, +40, and +60mV. (B) Normalized currents from (A) plotted on a logarithmic scale. The time scale is the same as in (A). The dashed lines are exponential fits to the falling phases. The decay rates were (from left to right) 1.30, 1.04, 1.10, 0.95, 1.11, and 1.14s−1. Same cilium as in Fig. 1. Biophysical Journal 1999 76, 2861-2867DOI: (10.1016/S0006-3495(99)77440-0) Copyright © 1999 The Biophysical Society Terms and Conditions

Figure 6 The cAMP diffusion coefficient is independent of membrane voltage. The diffusion coefficient, as calculated from the decay rates of the currents in Fig. 5, is plotted as a function of the membrane voltage. The horizontal line is a least-squares fit to the points and corresponds to a diffusion coefficient of 4 · 10−6cm2s−1. Biophysical Journal 1999 76, 2861-2867DOI: (10.1016/S0006-3495(99)77440-0) Copyright © 1999 The Biophysical Society Terms and Conditions

Figure 7 Effect of the phosphodiesterase activity on the kinetics of the cAMP-activated current. The scaling factors for the current elicited by 5μM cAMP in the presence of 0.5mM IBMX were 0.07 and 0.10s−1 for the rising and the falling phase, respectively. For the current elicited by 200μM cAMP in the absence of IBMX, the scaling factors were 0.008 and 1.12s−1 for the rising and the falling phase, respectively. Different cilium from the one shown in Fig. 1. L=46μm. Biophysical Journal 1999 76, 2861-2867DOI: (10.1016/S0006-3495(99)77440-0) Copyright © 1999 The Biophysical Society Terms and Conditions

Figure 8 Collected results for the scaling factor α measured from different cilia and plotted as a function of the inverse square of the length of the cilium, 1/L2. Each point represents averaged measurements from one cilium. Error bars represent standard errors. The straight line is a least-squares fit to the data points constrained to pass through the origin. The slope of the line is D=2.7±0.2 · 10−6cm2s−1. Biophysical Journal 1999 76, 2861-2867DOI: (10.1016/S0006-3495(99)77440-0) Copyright © 1999 The Biophysical Society Terms and Conditions