Table 3.
Relative anion permeabilities of WT EAAT1 and R477H
pHTransporterErevPX/PCl
ClBrINO3PBr/PClPI/PClPNO3/PCl
  mV mV mV mV     
pH 5.5 EAAT1 51 ± 4 28 ± 3 −4 ± 3 −10 ± 3  2.5 ± 0.1 9.0 ± 0.5 11.1 ± 0.6 
 R477H 14 ± 2 0 ± 1 −29 ± 1 −25 ± 2  1.75 ± 0.07 5.8 ± 0.4 5.1 ± 0.5 
pH 8.5 EAAT1 50 ± 2 46 ± 2 17 ± 2 13 ± 2  1.19 ± 0.03 3.8 ± 0.2 4.4 ± 0.3 
 R477H −21 ± 3 −21 ± 3 −24 ± 3 −24 ± 2  ND ND ND 
pHTransporterErevPX/PCl
ClBrINO3PBr/PClPI/PClPNO3/PCl
  mV mV mV mV     
pH 5.5 EAAT1 51 ± 4 28 ± 3 −4 ± 3 −10 ± 3  2.5 ± 0.1 9.0 ± 0.5 11.1 ± 0.6 
 R477H 14 ± 2 0 ± 1 −29 ± 1 −25 ± 2  1.75 ± 0.07 5.8 ± 0.4 5.1 ± 0.5 
pH 8.5 EAAT1 50 ± 2 46 ± 2 17 ± 2 13 ± 2  1.19 ± 0.03 3.8 ± 0.2 4.4 ± 0.3 
 R477H −21 ± 3 −21 ± 3 −24 ± 3 −24 ± 2  ND ND ND 

Reversal potentials (Erev) of saturating l-glutamate–elicited currents were obtained in buffers containing 10 mM Cl, Br, I, and NO3 salts. Relative anion permeabilities were calculated from Erev measurements using the Goldman–Hodgkin–Katz equation (Eq. 3). ND indicates that no relative anion permeability could be measured as Cl is not permeant through R477H at pH 8.5. Data shown represent the mean ± SEM (n ≥ 4).

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