ABCMdb

ABCC7 p.Gly314Gln

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Publications

PMID: 9922376 [PubMed] Dawson DC et al: "CFTR: mechanism of anion conduction."

No. Sentence Comment

425 Iodide permeation ing must be interpreted with caution for a number of reasons. First, it has been demonstrated (101) that the In any survey of the permeation of monatomic and polyatomic anions through CFTR, iodide stands out asCFTR mutations (e.g., G314Q or G314E) result in CFTR channels that exhibit markedly reduced anion binding, exhibiting some unique, or perhaps exaggerated, properties. Login to comment
597 Transmembrane segment 2 and TM6 sequences formed anion-selective channels in bilayers,the site of two patient mutations, and found that SCN block of CFTR was abolished in G314E and G314Q CFTR, whereas peptides based on TM1, TM3, TM4, and TM5 did not. Login to comment

PMID: 9512029 [PubMed] Mansoura MK et al: "Cystic fibrosis transmembrane conductance regulator (CFTR) anion binding as a probe of the pore."

No. Sentence Comment

62 Expression levels Wild-type and 11 mutant CFTR constructs were used in this study: G91A, G91E, G91R, G314A, G314D, G314E, G314Q, K335R, K335A, K335D, and K335E. Login to comment
116 It was of particular interest that the introduction of a glutamine (G314Q) also produced increased conductance ratios for the highly permeant anions and I, whereas the aspartic-acid-substituted construct (G314D) was not different from wtCFTR. Login to comment
136 In the case of the G314E and G314Q mutants, however, the SCN effect appeared to be moderately voltage dependent (Fig. 2 TABLE 2 Summary of permeability and conductance ratios from anion substitution experiments n SCN NO3 Br HCOO I A. Login to comment
137 Permeability Ratios Wild type 4-9 3.42 Ϯ 0.28 1.42 Ϯ 0.04 1.22 Ϯ 0.02 0.39 Ϯ 0.01 0.44 Ϯ 0.03 G91A 3-6 3.24 Ϯ 0.26 1.53 Ϯ 0.04 1.27 Ϯ 0.02 0.37 Ϯ 0.04 0.40 Ϯ 0.04 G91E 3-7 3.50 Ϯ 0.54 1.59 Ϯ 0.04 1.27 Ϯ 0.01 0.35 Ϯ 0.01 0.51 Ϯ 0.04 G91R 3-4 5.26 ؎ 0.46* 1.60 Ϯ 0.03 1.40 ؎ 0.01* 0.32 Ϯ 0.04 0.64 ؎ 0.04* G314A 3-4 2.87 Ϯ 0.17 1.45 Ϯ 0.03 1.19 Ϯ 0.02 0.31 Ϯ 0.03 0.33 Ϯ 0.03 G314D 4 3.42 Ϯ 0.34 1.44 Ϯ 0.05 1.25 Ϯ 0.04 0.33 Ϯ 0.03 0.51 Ϯ 0.05 G314E 3-4 3.72 Ϯ 0.56 1.65 ؎ 0.09* 1.35 ؎ 0.03* 0.49 Ϯ 0.04 0.53 Ϯ 0.04 G314Q 3-4 3.89 Ϯ 0.37 1.62 Ϯ 0.11 1.27 Ϯ 0.04 0.36 Ϯ 0.03 0.62 Ϯ 0.05 K335R 3-5 3.44 Ϯ 0.29 1.35 Ϯ 0.04 1.22 Ϯ 0.03 0.40 Ϯ 0.05 0.41 Ϯ 0.07 K335A 5-6 5.34 ؎ 0.58* 1.48 Ϯ 0.06 1.28 Ϯ 0.04 0.37 Ϯ 0.03 0.60 Ϯ 0.06 K335D 4-6 3.02 Ϯ 0.19 1.50 Ϯ 0.03 1.10 ؎ 0.02* 0.54 ؎ 0.04* 0.65 ؎ 0.06* K335E 5-8 3.64 Ϯ 0.21 1.48 Ϯ 0.06 1.29 Ϯ 0.03 0.46 Ϯ 0.04 1.10 ؎ 0.04* B. Conductance Ratios Wild type 4-9 0.14 Ϯ 0.02 0.75 Ϯ 0.02 0.64 Ϯ 0.02 0.52 Ϯ 0.03 0.18 Ϯ 0.03 G91A 3-6 0.14 Ϯ 0.01 0.77 Ϯ 0.02 0.61 Ϯ 0.02 0.47 Ϯ 0.02 0.19 Ϯ 0.02 G91E 3-7 0.15 Ϯ 0.03 0.73 Ϯ 0.02 0.60 Ϯ 0.01 0.50 Ϯ 0.04 0.30 Ϯ 0.02 G91R 3-4 0.14 Ϯ 0.00 0.84 Ϯ 0.01 0.63 Ϯ 0.01 0.32 ؎ 0.01* 0.14 Ϯ 0.01 G314A 3-4 0.30 Ϯ 0.09 0.89 ؎ 0.01* 0.66 Ϯ 0.01 0.48 Ϯ 0.09 0.24 Ϯ 0.01 G314D 4 0.28 Ϯ 0.05 0.82 Ϯ 0.01 0.70 Ϯ 0.02 0.49 Ϯ 0.06 0.27 Ϯ 0.03 G314E 3-4 0.62 ؎ 0.07* 1.18 ؎ 0.04* 0.84 ؎ 0.05* 0.42 Ϯ 0.05 0.29 Ϯ 0.09 G314Q 3-4 0.63 ؎ 0.02* 1.01 ؎ 0.04* 0.82 ؎ 0.03* 0.50 Ϯ 0.02 0.42 ؎ 0.02* K335R 3-5 0.14 Ϯ 0.01 0.76 Ϯ 0.03 0.61 Ϯ 0.02 0.59 Ϯ 0.06 0.16 Ϯ 0.03 K335A 6 0.20 Ϯ 0.03 0.77 Ϯ 0.02 0.61 Ϯ 0.02 0.45 Ϯ 0.03 0.21 Ϯ 0.02 K335D 4-6 0.65 ؎ 0.04* 1.25 ؎ 0.02* 0.89 ؎ 0.02* 0.61 Ϯ 0.06 0.58 ؎ 0.06* K335E 5-8 0.50 ؎ 0.06* 1.19 ؎ 0.03* 0.89 ؎ 0.02* 0.53 Ϯ 0.03 0.48 ؎ 0.03* (A) The apparent permeability ratios (PS/PCl) for each substitute anion were calculated from the shift in reversal potential using the Goldman-Hodgkin-Katz relation (noted in Materials and Methods). Login to comment
147 The data in Table 3 show that for wtCFTR and G314Q and G314E, two of the most severely affected constructs, PSCN/PCl calculated from the shift in Vr was independent of the fractional abundance of [SCN]o. Login to comment
169 TABLE 4 Quantitative analyses of the macroscopic I-V shape changes Mutant ⌬ Net charge n RR g(ϩ30)/g(-30) RR/RRWT Wild type 5 1.220 Ϯ 0.06 1.00 G91A 0 4 1.293 Ϯ 0.06 1.06 G91E -1 5 1.512 ؎ 0.10* 1.24 G91R 1 4 8.041 ؎ 0.87* 6.59 G314A 0 4 1.201 Ϯ 0.09 0.98 G314D -1 4 1.362 Ϯ 0.08 1.12 G314E -1 7 1.405 Ϯ 0.08 1.15 G314Q 0 5 1.376 Ϯ 0.10 1.13 K335R 0 4 1.209 Ϯ 0.06 0.99 K335A -1 4 1.295 Ϯ 0.07 1.06 K335D -2 5 0.762 ؎ 0.02* 0.62 K335E -2 4 0.919 ؎ 0.02* 0.75 The slope conductance was measured at ϩ30 mV and -30 mV with respect to the reversal potential. Login to comment
171 TABLE 3 The permeability ratio (PSCN/PCl) is independent of the mole fraction of [SCN]0 for wtCFTR and the G314 variants [SCN]/{[SCN]ϩ[Cl]} n PSCN/PCl 0.02 0.05 0.10 0.20 0.50 0.90 Wild type 12 3.82 Ϯ 0.50 4.43 Ϯ 0.57 4.58 Ϯ 0.48 4.69 Ϯ 0.43 4.66 Ϯ 0.38 4.44 Ϯ 0.35 G314A 9 4.32 Ϯ 0.73 3.78 Ϯ 0.53 3.81 Ϯ 0.47 3.79 Ϯ 0.34 3.82 Ϯ 0.29 3.72 Ϯ 0.25 G314D 3 2.99 Ϯ 0.26 2.56 Ϯ 1.05 2.82 Ϯ 1.07 2.68 Ϯ 0.97 2.87 Ϯ 0.65 2.89 Ϯ 0.43 G314E 6 4.48 Ϯ 1.05 4.01 Ϯ 0.69 4.17 Ϯ 0.62 4.15 Ϯ 0.59 3.96 Ϯ 0.41 3.82 Ϯ 0.40 G314Q 3 5.39 Ϯ 0.57 4.49 Ϯ 0.58 4.69 Ϯ 1.26 4.05 Ϯ 1.26 3.86 Ϯ 1.47 3.68 Ϯ 1.51 The permeability ratios were calculated from the shift in reversal potential using the Goldman-Hodgkin-Katz equation. Login to comment
173 TABLE 5 Concentration-dependent activation of wtCFTR, G91, G314, and K335 variants by IBMX in the presence of 10 ␮M forskolin Mutant n K1/2(IBMX) (mM) Wild type 15 0.35 Ϯ 0.04 G91A 5 0.42 Ϯ 0.06 G91E 8 0.51 ؎ 0.06* G91R 5 0.49 Ϯ 0.09 G314A 10 1.21 ؎ 0.11* G314D 3 1.35 ؎ 0.16* G314E 8 6.39 ؎ 1.35* G314Q 4 14.26 ؎ 6.64* K335R 4 0.46 Ϯ 0.04 K335A 2 0.35 Ϯ 0.15 K335D 7 0.87 ؎ 0.13* K335E 3 0.95 ؎ 0.07* The steady-state slope conductance was measured at -60 mV as increasing concentrations of IBMX (0.02-5.0 mM) were added to the perfusate in the continued presence of 10 mM forskolin. Login to comment
175 Note that this fitting procedure allows us to estimate K1/2 values for even the most insensitive constructs, G314E and G314Q, despite the fact that these values were greater than the highest concentration of IBMX used in this study. Login to comment
178 The K1/2 seen with either G314E or G314Q was comparable to that seen with nucleotide-binding mutations such as G551D that are associated with severe CF (Wilkinson et al., 1996). Login to comment
195 The pattern of the effect of anion substitution was identical for Br, NO3, and SCN, and the conductance ratio for all three ions was increased in G314E and G314Q CFTR channels. Login to comment
198 The results presented here are consistent with the notion that the binding of anions within the CFTR pore is a sensitive indicator of changes in pore structure whereas permeability ratios appear to be rather insensitive to similar TABLE 6 Qualitative summary of the functional consequences of mutations at G91, G314, and K335 Property G91 (TM1) K335 (TM6) G314 (TM5) G91A G91E G91R K335R K335A K335D K335E G314A G314D G314E G314Q I-V shape - - ϩϩϩ - - ϩϩ ϩ - - - - Psub/PCl - - - - - - ϩϩ - - - - gsub/gCl - - - - - ϩϩϩ ϩϩϩ ϩϩ - ϩϩϩ ϩϩϩ SCN- binding - - - - - ϩϩϩ ϩϩϩ ϩϩ - ϩϩϩϩ ϩϩϩϩ Activation - - - - - ϩϩ ϩϩ ϩϩϩ ϩϩϩ ϩϩϩϩ ϩϩϩϩ Results are expressed as follows: -, function of the CFTR construct with the indicated substitution was indistinguishable from wild type; ϩ to ϩϩϩϩ, semiquantitative indication of the magnitude of the change in the function compared with wild type. Login to comment
233 The increased conductance ratios seen in G314E, G314Q, and to a lesser extent, G314A channels are compatible with the hypothesis that substitution for G314 distorted an anion binding site such that the affinities for Br, NO3, and SCN were all reduced relative to Cl. Login to comment
237 Furthermore, the dramatic reduction in SCN binding seen in G314Q CFTR demonstrates that the presence of arginines, such as R347, is not sufficient to induce tight anion binding in the pore. Login to comment
117 It was of particular interest that the introduction of a glutamine (G314Q) also produced increased conductance ratios for the highly permeant anions and I, whereas the aspartic-acid-substituted construct (G314D) was not different from wtCFTR. Login to comment
138 Permeability Ratios Wild type 4-9 3.42 afe; 0.28 1.42 afe; 0.04 1.22 afe; 0.02 0.39 afe; 0.01 0.44 afe; 0.03 G91A 3-6 3.24 afe; 0.26 1.53 afe; 0.04 1.27 afe; 0.02 0.37 afe; 0.04 0.40 afe; 0.04 G91E 3-7 3.50 afe; 0.54 1.59 afe; 0.04 1.27 afe; 0.01 0.35 afe; 0.01 0.51 afe; 0.04 G91R 3-4 5.26 d1e; 0.46* 1.60 afe; 0.03 1.40 d1e; 0.01* 0.32 afe; 0.04 0.64 d1e; 0.04* G314A 3-4 2.87 afe; 0.17 1.45 afe; 0.03 1.19 afe; 0.02 0.31 afe; 0.03 0.33 afe; 0.03 G314D 4 3.42 afe; 0.34 1.44 afe; 0.05 1.25 afe; 0.04 0.33 afe; 0.03 0.51 afe; 0.05 G314E 3-4 3.72 afe; 0.56 1.65 d1e; 0.09* 1.35 d1e; 0.03* 0.49 afe; 0.04 0.53 afe; 0.04 G314Q 3-4 3.89 afe; 0.37 1.62 afe; 0.11 1.27 afe; 0.04 0.36 afe; 0.03 0.62 afe; 0.05 K335R 3-5 3.44 afe; 0.29 1.35 afe; 0.04 1.22 afe; 0.03 0.40 afe; 0.05 0.41 afe; 0.07 K335A 5-6 5.34 d1e; 0.58* 1.48 afe; 0.06 1.28 afe; 0.04 0.37 afe; 0.03 0.60 afe; 0.06 K335D 4-6 3.02 afe; 0.19 1.50 afe; 0.03 1.10 d1e; 0.02* 0.54 d1e; 0.04* 0.65 d1e; 0.06* K335E 5-8 3.64 afe; 0.21 1.48 afe; 0.06 1.29 afe; 0.03 0.46 afe; 0.04 1.10 d1e; 0.04* B. Conductance Ratios Wild type 4-9 0.14 afe; 0.02 0.75 afe; 0.02 0.64 afe; 0.02 0.52 afe; 0.03 0.18 afe; 0.03 G91A 3-6 0.14 afe; 0.01 0.77 afe; 0.02 0.61 afe; 0.02 0.47 afe; 0.02 0.19 afe; 0.02 G91E 3-7 0.15 afe; 0.03 0.73 afe; 0.02 0.60 afe; 0.01 0.50 afe; 0.04 0.30 afe; 0.02 G91R 3-4 0.14 afe; 0.00 0.84 afe; 0.01 0.63 afe; 0.01 0.32 d1e; 0.01* 0.14 afe; 0.01 G314A 3-4 0.30 afe; 0.09 0.89 d1e; 0.01* 0.66 afe; 0.01 0.48 afe; 0.09 0.24 afe; 0.01 G314D 4 0.28 afe; 0.05 0.82 afe; 0.01 0.70 afe; 0.02 0.49 afe; 0.06 0.27 afe; 0.03 G314E 3-4 0.62 d1e; 0.07* 1.18 d1e; 0.04* 0.84 d1e; 0.05* 0.42 afe; 0.05 0.29 afe; 0.09 G314Q 3-4 0.63 d1e; 0.02* 1.01 d1e; 0.04* 0.82 d1e; 0.03* 0.50 afe; 0.02 0.42 d1e; 0.02* K335R 3-5 0.14 afe; 0.01 0.76 afe; 0.03 0.61 afe; 0.02 0.59 afe; 0.06 0.16 afe; 0.03 K335A 6 0.20 afe; 0.03 0.77 afe; 0.02 0.61 afe; 0.02 0.45 afe; 0.03 0.21 afe; 0.02 K335D 4-6 0.65 d1e; 0.04* 1.25 d1e; 0.02* 0.89 d1e; 0.02* 0.61 afe; 0.06 0.58 d1e; 0.06* K335E 5-8 0.50 d1e; 0.06* 1.19 d1e; 0.03* 0.89 d1e; 0.02* 0.53 afe; 0.03 0.48 d1e; 0.03* (A) The apparent permeability ratios (PS/PCl) for each substitute anion were calculated from the shift in reversal potential using the Goldman-Hodgkin-Katz relation (noted in Materials and Methods). Login to comment
148 The data in Table 3 show that for wtCFTR and G314Q and G314E, two of the most severely affected constructs, PSCN/PCl calculated from the shift in Vr was independent of the fractional abundance of [SCN]o. Login to comment