Comparison of Boltzmann fit parameters from normalized conductance (G) or change in fluorescence (ΔF) for spHCNWT, spHCNR332C in 100K solution
| . | Parameter . | spHCNWT (5) . | spHCNR332C . | |||
|---|---|---|---|---|---|---|
| Unlabeled (3) . | ALEXA-488 (5) . | MTS-TAMRA (8) . | ||||
| G | V0.5G (mV) | −56.1 ± 2.4 | −126.9 ± 2.4 | −114.6 ± 2.4a | −88.7 ± 3.9a | |
| zG | 1.30 ± 0.12 | 1.17 ± 0.13 | 1.24 ± 0.09a | 0.94 ± 0.09a | ||
| ∆F | ∆Ftotal | ALEXA-488 (14) | MTS-TAMRA (7) | |||
| V0.5F (mV) | −71.9 ± 1.7a | −59.0 ± 6.0a | ||||
| zF | 1.05 ± 0.06a | 0.66 ± 0.07a | ||||
| ∆Ffast | ||||||
| V0.5F (mV) | −96.4 ± 2.0 | −93.5 ± 12.2 | ||||
| zF | 0.77 ± 0.04 | 0.97 ± 0.29 | ||||
| ∆Fslow | ||||||
| V0.5F (mV) | −53.3 ± 2.10a | −38.0 ± 2.10a | ||||
| zF | 1.51 ± 0.16 | 1.19 ± 0.01 | ||||
| . | Parameter . | spHCNWT (5) . | spHCNR332C . | |||
|---|---|---|---|---|---|---|
| Unlabeled (3) . | ALEXA-488 (5) . | MTS-TAMRA (8) . | ||||
| G | V0.5G (mV) | −56.1 ± 2.4 | −126.9 ± 2.4 | −114.6 ± 2.4a | −88.7 ± 3.9a | |
| zG | 1.30 ± 0.12 | 1.17 ± 0.13 | 1.24 ± 0.09a | 0.94 ± 0.09a | ||
| ∆F | ∆Ftotal | ALEXA-488 (14) | MTS-TAMRA (7) | |||
| V0.5F (mV) | −71.9 ± 1.7a | −59.0 ± 6.0a | ||||
| zF | 1.05 ± 0.06a | 0.66 ± 0.07a | ||||
| ∆Ffast | ||||||
| V0.5F (mV) | −96.4 ± 2.0 | −93.5 ± 12.2 | ||||
| zF | 0.77 ± 0.04 | 0.97 ± 0.29 | ||||
| ∆Fslow | ||||||
| V0.5F (mV) | −53.3 ± 2.10a | −38.0 ± 2.10a | ||||
| zF | 1.51 ± 0.16 | 1.19 ± 0.01 | ||||
Values are shown as mean ± SE as reported by fit to normalized pooled data using the Boltzmann equation (Eq. 1). Number of cells analyzed given in parentheses. ∆Ftotalmeasured at end of 1-s test pulse at each potential for both labels. ∆Ffast,slow refer to components obtained by fitting a single exponential plus offset to ALEX-488 data or double exponential to MTS-TAMRA data (see text).
Indicates significant difference between ALEXA and MTS-TAMRA fit parameters (t test, P < 0.05).