Table 1.

Comparison of Boltzmann fit parameters from normalized conductance (G) or change in fluorescence (ΔF) for spHCNWT, spHCNR332C in 100K solution

ParameterspHCNWT (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 
ParameterspHCNWT (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).

a

Indicates significant difference between ALEXA and MTS-TAMRA fit parameters (t test, P < 0.05).

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