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J Gen Physiol
2016 Jul 01;1481:65-76. doi: 10.1085/jgp.201511559.
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Patch-clamp fluorometry-based channel counting to determine HCN channel conductance.
Liu C
,
Xie C
,
Grant K
,
Su Z
,
Gao W
,
Liu Q
,
Zhou L
.
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Counting ion channels on cell membranes is of fundamental importance for the study of channel biophysics. Channel counting has thus far been tackled by classical approaches, such as radioactive labeling of ion channels with blockers, gating current measurements, and nonstationary noise analysis. Here, we develop a counting method based on patch-clamp fluorometry (PCF), which enables simultaneous electrical and optical recordings, and apply it to EGFP-tagged, hyperpolarization-activated and cyclic nucleotide-regulated (HCN) channels. We use a well-characterized and homologous cyclic nucleotide-gated (CNG) channel to establish the relationship between macroscopic fluorescence intensity and the total number of channels. Subsequently, based on our estimate of the total number of HCN channels, we determine the single-channel conductance of HCN1 and HCN2 to be 0.46 and 1.71 pS, respectively. Such a small conductance would present a technical challenge for traditional electrophysiology. This PCF-based technique provides an alternative method for counting particles on cell membranes, which could be applied to biophysical studies of other membrane proteins.
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27353446
???displayArticle.pmcLink???PMC4924933 ???displayArticle.link???J Gen Physiol ???displayArticle.grants???[+]
Figure 1. Use ROONS-EGFP as a model to determine the relationship between macroscopic fluorescence intensity and the total number of channels on the membrane patch. (A, top) Two single-channel traces of ROONS-EGFP channel recorded at the potential of 80 mV. Transitions between opening and closing were recorded in the presence of 3.5 µM cGMP, a subsaturating concentration for ROONS-EGFP. (bottom left) Maximal channel opening recorded with 35 µM cGMP. The current level corresponding to the closed state is indicated by a gray line. (bottom right) The current trace of the same patch recorded in the absence of cGMP. The gray line represents the current level of the open state. (B) Histogram of the top recording trace from A. Averaged amplitude of single-channel currents was 4.29 ± 0.57 pA (n = 7). (C, left) Macroscopic current recorded under 35 µM cGMP and a voltage step from 0 to 40 mV. (right) The corresponding brightfield and fluorescence images. (D, left) Histogram of the pixel intensities of the whole fluorescence image collected using four different exposure durations. The Cascade 1K is a 16-bit camera so that the pixel intensity ranges from 0 to 65,535. (right) Total fluorescence intensity from the ROI surrounding the patch of membrane patch (green) and the background (blue), which was separately recorded after moving the recording pipette out of the view. (E) Cross-plots of fluorescence intensity versus current amplitude. Two x axes show the macroscopic current (bottom) and the corresponding number of channels (top). The amplitude of single-channel current, 4.29 pA, was used in the conversion. Linear fit statistics: Pearson correlation coefficient, 0.823. Green curves show the confidence bands (95%).
Figure 2. PCF recordings of the mHCN2-EGFP channel and cross-plots of fluorescence intensity versus current amplitude. (A, left) Macroscopic current recorded with 3 µM cAMP in the bath (red trace) and a voltage step from â40 to â140 mV. (right) The corresponding brightfield and fluorescence images. (B, left) Histogram of the pixel intensities of the whole image collected with four different exposure durations. Notice longer exposure durations, 100 and 200 ms, lead to saturated pixels. (right) Total fluorescence intensity from the membrane patch (green) and the background (blue). (C) Cross-plots of fluorescence intensity versus current amplitude. Linear fit statistics: Pearson correlation coefficient, 0.907. Green curves show the confidence bands (95%).
Figure 3. Cross-plots of fluorescence intensity versus current amplitude for mHCN1-EGFP and spHCN-EGFP channels. (A, left) Macroscopic current of the mHCN1-EGFP channel recorded with 3 µM cAMP in the bath. A voltage step from 0 to â120 mV was used for channel activation. Tail current was recorded at â40 mV. (B, left) Macroscopic current of spHCN-EGFP channel recorded with 30 µM cAMP in the bath. A voltage step from 0 to â120 mV was used for channel activation. Tail current was recorded at 40 mV. (A and B, right) The corresponding brightfield and fluorescence images. (C) Cross-plots of fluorescence intensity versus current amplitude for the mHCN1-EGFP channel. Linear fit statistics: Pearson correlation coefficient, 0.973. (D) Cross-plots of fluorescence intensity versus current amplitude for the spHCN-EGFP channel. Linear fit statistics: Pearson correlation coefficient, 0.859. Green curves show the confidence bands (95%).
Figure 4. NSNA of macroscopic mHCN2-EGFP currents. (A, top) Voltage protocol used for channel activation and deactivation. (bottom) 6 representative traces from 100 repeatedly collected traces. (B) Current variance over the complete time course of a single episode. (C) Current variance versus mean current amplitude. Red, parabola fit of the macroscopic current part. Green, parabola fit of the tail current part. (D) Normal residual after curve fit for macroscopic current (corresponding to the red trace in C). Results: single-channel current, â0.298 pA (â130 mV); single-channel conductance, 2.29 pS; total number of channels, 8,715; Po, 75.5%. Adjusted R2, 0.934. (E) Normal residual after curve fit for tail current (corresponding to the green trace in C). Results: single-channel current, â0.114 pA (â40 mV); single-channel conductance, 2.86 pS; total number of channels, 4,707; Po, 88.4%. Adjusted R2, 0.963.
Figure 5. Determining the relative ionic selectivity for the mHCN2-EGFP channel. Symmetrical solutions were used on both sides of the membrane. All recordings were collected in the presence of saturating concentration of cAMP (3 µM). (A) Current trace recorded with solutions containing 110 mM Na+ and 5 mM K+ as the charge carriers. (B) Current trace recorded with solutions containing 110 mM NH4+ and 5 mM K+. (C) Cross-plots of fluorescence intensity versus current amplitude. Symmetric solutions contain 110 mM Na+ only. The slope was 0.676 a.u./pA. As the control, the slope of the condition with 110 mM K+ and 2 mM Na+ was 0.0067 a.u./pA. Thus, PK+/PNa+ based on the ratio of two slopes was 101 (in the absence of K+). Linear fit statistics: Pearson correlation coefficient, 0.766. (D) Results of 110 mM Na+ and 5 mM K+. The slope was 0.023 a.u./pA. PK+/PNa+ was 3.4 (in the presence of 5 mM K+). Linear fit statistics: Pearson correlation coefficient, 0.845. (E) Results of 110 mM NH4+ only. The slope was 0.088 a.u./pA. PK+/PNH4+ was 13.1 (in the absence of K+). Linear fit statistics: Pearson correlation coefficient, 0.811. (F) Results of 110 mM NH4+ and 5 mM K+. The slope was 0.081 a.u./pA. PK+/PNH4+ was 12.1 (in the presence of 5 mM K+). Linear fit statistics: Pearson correlation coefficient, 0.832. Green curves show the confidence bands (95%).
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