PMID: 23955087

Wang W, El Hiani Y, Rubaiy HN, Linsdell P
Relative contribution of different transmembrane segments to the CFTR chloride channel pore.
Pflugers Arch. 2014 Mar;466(3):477-90. doi: 10.1007/s00424-013-1317-x. Epub 2013 Aug 20., [PubMed]
Sentences
No. Mutations Sentence Comment
4 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 23955087:4:246
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 23955087:4:44
status: NEW
view ABCC7 p.Ser1118Cys details
ABCC7 p.Thr1115Cys
X
ABCC7 p.Thr1115Cys 23955087:4:33
status: NEW
view ABCC7 p.Thr1115Cys details
Two accessible residues in TM11 (T1115C and S1118C) were found to be more readily modified from the extracellular solution in closed channels, but more readily modified from the intracellular solution in open channels, as previously reported for T338C in TM6. Login to comment
31 ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:31:28
status: NEW
view ABCC7 p.Thr338Ala details
Overall, the effects of the T338A mutation have been interpreted as reflecting an increase in functional diameter of the narrowest part of the pore [26] and a reduced barrier to the movement of permeant ions inside the pore [11]. Login to comment
38 ABCC7 p.Val510Ala
X
ABCC7 p.Val510Ala 23955087:38:250
status: NEW
view ABCC7 p.Val510Ala details
In this study, we have used two different human CFTR variants as backgrounds for further mutagenesis: wild type CFTR and "cys-less" CFTR in which all cysteines have been removed by mutagenesis [30] and that also includes a mutation in the first NBD (V510A) to increase protein expression in the cell membrane [20]. Login to comment
46 ABCC7 p.Glu1371Gln
X
ABCC7 p.Glu1371Gln 23955087:46:69
status: NEW
view ABCC7 p.Glu1371Gln details
In some cases, cysteine mutants were combined with the NBD2 mutation E1371Q, which we have used previously to abolish ATP-dependent channel gating and so isolate effects of cysteine reactive substances on open CFTR channels [41-43]. Login to comment
70 ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:70:26
status: NEW
view ABCC7 p.Thr338Ala details
ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:70:169
status: NEW
view ABCC7 p.Thr338Ala details
Because the properties of T338A-CFTR channels have been investigated in detail previously, simplified protocols were used to facilitate comparison of the effects of the T338A mutation with those of other mutations (Figs. 5, 6, 7, and 8). Login to comment
77 ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 23955087:77:93
status: NEW
view ABCC7 p.Ser1118Cys details
ABCC7 p.Thr1115Cys
X
ABCC7 p.Thr1115Cys 23955087:77:82
status: NEW
view ABCC7 p.Thr1115Cys details
ABCC7 p.Ile1112Cys
X
ABCC7 p.Ile1112Cys 23955087:77:115
status: NEW
view ABCC7 p.Ile1112Cys details
Note that while MTSES caused rapid inhibition of macroscopic current amplitude in T1115C and S1118C, inhibition of I1112C current was much slower (note different time scale for this mutant). Login to comment
78 ABCC7 p.Thr1121Cys
X
ABCC7 p.Thr1121Cys 23955087:78:21
status: NEW
view ABCC7 p.Thr1121Cys details
MTSES did not affect T1121C currents; however, these were inhibited by CFTRinh-172 (5 bc;M; hatched bar). Login to comment
82 ABCC7 p.Ile1119Cys
X
ABCC7 p.Ile1119Cys 23955087:82:23
status: NEW
view ABCC7 p.Ile1119Cys details
ABCC7 p.Leu1120Cys
X
ABCC7 p.Leu1120Cys 23955087:82:34
status: NEW
view ABCC7 p.Leu1120Cys details
Note that TM11 mutants I1119C and L1120C were not tested since they have previously been shown to be unaffected by extracellular MTS reagents and were therefore described as being non-pore lining [10]. Login to comment
83 ABCC7 p.Glu873Cys
X
ABCC7 p.Glu873Cys 23955087:83:11
status: NEW
view ABCC7 p.Glu873Cys details
TM7 mutant E873C expression did not yield functional CFTR channel currents in BHK cell patches approximated from: Kd &#bc; Au CN &#f0; &#de;2 -  . Login to comment
87 ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:87:0
status: NEW
view ABCC7 p.Thr338Ala details
ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:87:180
status: NEW
view ABCC7 p.Thr338Ala details
T338A, as well as other substitutions at this position, cause complex changes in the relative permeability of different anions in CFTR [26]; however, the major changes observed in T338A can be summarized as (a) an increase in the relative permeability of lyotropic anions such as SCN- , NO3 - , Br- , I- , and ClO4 - , and (b) an increase in the relative permeability of extracellular organic (kosmotropic) monvalent anions including formate, acetate, propanoate, and pyruvate [26]. Login to comment
104 ABCC7 p.Ile1112Cys
X
ABCC7 p.Ile1112Cys 23955087:104:81
status: NEW
view ABCC7 p.Ile1112Cys details
Black bars represent a significant difference from cys-less (P<0.05); gray bars (I1112C only) no significant difference. Mean of data from three to six patches Results Accessibility of cysteine side chains introduced into TMs 5, 7, and 11 We hypothesized that the central portion of the CFTR pore might be lined by TMs 1, 5, 6, 7, 11, and 12 (Fig. 1). Login to comment
107 ABCC7 p.Glu1371Gln
X
ABCC7 p.Glu1371Gln 23955087:107:126
status: NEW
view ABCC7 p.Glu1371Gln details
Figure 2a shows the effect of internal MTSES on currents carried by some TM11 mutant channels in inside- Fig. 4 Effect of the E1371Q mutation on modification by internal and external MTSES. Login to comment
111 ABCC7 p.Glu1371Gln
X
ABCC7 p.Glu1371Gln 23955087:111:96
status: NEW
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ABCC7 p.Glu1371Gln
X
ABCC7 p.Glu1371Gln 23955087:111:114
status: NEW
view ABCC7 p.Glu1371Gln details
ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 23955087:111:107
status: NEW
view ABCC7 p.Ser1118Cys details
ABCC7 p.Thr1115Cys
X
ABCC7 p.Thr1115Cys 23955087:111:88
status: NEW
view ABCC7 p.Thr1115Cys details
b Example whole cell currents recorded continuously at +30 mV for constitutively active T1115C/ E1371Q and S1118C/E1371Q channels. Login to comment
112 ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 23955087:112:46
status: NEW
view ABCC7 p.Ser1118Cys details
ABCC7 p.Thr1115Cys
X
ABCC7 p.Thr1115Cys 23955087:112:35
status: NEW
view ABCC7 p.Thr1115Cys details
In contrast to currents carried by T1115C and S1118C channels (see Fig. 3), these whole cell currents were not significantly affected by addition of 200 bc;M MTSES to the extracellular solution (black bars), even though these currents were positively identified as being carried by CFTR by sensitivity to GlyH-101 (50 bc;M, hatched bars). Login to comment
115 ABCC7 p.Glu1371Gln
X
ABCC7 p.Glu1371Gln 23955087:115:111
status: NEW
view ABCC7 p.Glu1371Gln details
In both c and d, black bars represent the named mutants in a cys-less background, and white bars in a cys-less/E1371Q background, and asterisks indicate a significant difference between these two backgrounds (P<0.05). Login to comment
117 ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 23955087:117:154
status: NEW
view ABCC7 p.Ser1118Cys details
ABCC7 p.Thr1121Cys
X
ABCC7 p.Thr1121Cys 23955087:117:173
status: NEW
view ABCC7 p.Thr1121Cys details
ABCC7 p.Thr1115Cys
X
ABCC7 p.Thr1115Cys 23955087:117:143
status: NEW
view ABCC7 p.Thr1115Cys details
ABCC7 p.Ile1112Cys
X
ABCC7 p.Ile1112Cys 23955087:117:135
status: NEW
view ABCC7 p.Ile1112Cys details
ABCC7 p.Phe1116Cys
X
ABCC7 p.Phe1116Cys 23955087:117:239
status: NEW
view ABCC7 p.Phe1116Cys details
ABCC7 p.Ala1113Cys
X
ABCC7 p.Ala1113Cys 23955087:117:223
status: NEW
view ABCC7 p.Ala1113Cys details
ABCC7 p.Phe1110Cys
X
ABCC7 p.Phe1110Cys 23955087:117:207
status: NEW
view ABCC7 p.Phe1110Cys details
ABCC7 p.Phe1111Cys
X
ABCC7 p.Phe1111Cys 23955087:117:215
status: NEW
view ABCC7 p.Phe1111Cys details
ABCC7 p.Val1114Cys
X
ABCC7 p.Val1114Cys 23955087:117:231
status: NEW
view ABCC7 p.Val1114Cys details
ABCC7 p.Ile1117Cys
X
ABCC7 p.Ile1117Cys 23955087:117:250
status: NEW
view ABCC7 p.Ile1117Cys details
ABCC7 p.Ile1109Cys
X
ABCC7 p.Ile1109Cys 23955087:117:199
status: NEW
view ABCC7 p.Ile1109Cys details
Application of MTSES (200 bc;M) following channel activation with PKA and ATP caused a decrease in macroscopic current amplitude in I1112C, T1115C and S1118C, but not in T1121C (Fig. 2a, b) or in I1109C, F1110C, F1111C, A1113C, V1114C, F1116C, or I1117C (Fig. 2c). Login to comment
120 ABCC7 p.Glu873Cys
X
ABCC7 p.Glu873Cys 23955087:120:74
status: NEW
view ABCC7 p.Glu873Cys details
We did not observe any CFTR current in inside-out patches associated with E873C (TM7). Login to comment
122 ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 23955087:122:29
status: NEW
view ABCC7 p.Ser1118Cys details
ABCC7 p.Thr1121Cys
X
ABCC7 p.Thr1121Cys 23955087:122:37
status: NEW
view ABCC7 p.Thr1121Cys details
ABCC7 p.Thr1122Cys
X
ABCC7 p.Thr1122Cys 23955087:122:49
status: NEW
view ABCC7 p.Thr1122Cys details
ABCC7 p.Ile1119Cys
X
ABCC7 p.Ile1119Cys 23955087:122:80
status: NEW
view ABCC7 p.Ile1119Cys details
ABCC7 p.Leu1120Cys
X
ABCC7 p.Leu1120Cys 23955087:122:91
status: NEW
view ABCC7 p.Leu1120Cys details
ABCC7 p.Phe1116Cys
X
ABCC7 p.Phe1116Cys 23955087:122:64
status: NEW
view ABCC7 p.Phe1116Cys details
ABCC7 p.Ile1117Cys
X
ABCC7 p.Ile1117Cys 23955087:122:72
status: NEW
view ABCC7 p.Ile1117Cys details
Previously it was shown that S1118C, T1121C, and T1122C-but not F1116C, I1117C, I1119C, or L1120C-are accessible to externally applied MTS reagents [10]. Login to comment
123 ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 23955087:123:188
status: NEW
view ABCC7 p.Ser1118Cys details
ABCC7 p.Thr1121Cys
X
ABCC7 p.Thr1121Cys 23955087:123:200
status: NEW
view ABCC7 p.Thr1121Cys details
ABCC7 p.Thr1115Cys
X
ABCC7 p.Thr1115Cys 23955087:123:180
status: NEW
view ABCC7 p.Thr1115Cys details
ABCC7 p.Ile1112Cys
X
ABCC7 p.Ile1112Cys 23955087:123:219
status: NEW
view ABCC7 p.Ile1112Cys details
Figure 3 confirms that application of external MTSES (200 bc;M) following channel activation with cAMP-stimulatory cocktail caused a decrease in whole cell current amplitude in T1115C, S1118C, and T1121C, but not in I1112C. Login to comment
124 ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 23955087:124:52
status: NEW
view ABCC7 p.Ser1118Cys details
Together, these results (Figs. 2b, 3b) suggest that S1118C represents the outermost extent of internal MTSES penetration into the pore, and T1115 the innermost extent of external MTSES penetration. Login to comment
127 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 23955087:127:206
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 23955087:127:44
status: NEW
view ABCC7 p.Ser1118Cys details
ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 23955087:127:86
status: NEW
view ABCC7 p.Ser1118Cys details
ABCC7 p.Thr1115Cys
X
ABCC7 p.Thr1115Cys 23955087:127:33
status: NEW
view ABCC7 p.Thr1115Cys details
ABCC7 p.Thr1115Cys
X
ABCC7 p.Thr1115Cys 23955087:127:75
status: NEW
view ABCC7 p.Thr1115Cys details
State-dependent accessibility of T1115C and S1118C in TM11 Modification of T1115C and S1118C by both internal and external MTSES is reminiscent of the accessibility pattern observed for TM6 cysteine mutant T338C [42]. Login to comment
128 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 23955087:128:119
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 23955087:128:129
status: NEW
view ABCC7 p.Ser1118Cys details
This similarity is perhaps not surprising since a disulfide bond can be formed between the two cysteine side chains of T338C and S1118C in open channels [43], indicating close physical proximity of these pore-exposed side chains. Login to comment
129 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 23955087:129:44
status: NEW
view ABCC7 p.Thr338Cys details
Previously we suggested that the ability of T338C to be modified by MTSES from both sides of the membrane was due to this residue Fig. 5 Single channel currents carried by TM11 mutant channels. Login to comment
136 ABCC7 p.Glu1371Gln
X
ABCC7 p.Glu1371Gln 23955087:136:62
status: NEW
view ABCC7 p.Glu1371Gln details
This suggestion was based in large part on the effects of the E1371Q mutation, which results in constitutively open CFTR channels, on side-dependent modification. Login to comment
137 ABCC7 p.Glu1371Gln
X
ABCC7 p.Glu1371Gln 23955087:137:28
status: NEW
view ABCC7 p.Glu1371Gln details
ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 23955087:137:114
status: NEW
view ABCC7 p.Ser1118Cys details
ABCC7 p.Thr1115Cys
X
ABCC7 p.Thr1115Cys 23955087:137:103
status: NEW
view ABCC7 p.Thr1115Cys details
As shown in Fig. 4a, c, the E1371Q mutation significantly accelerated the rate of modification of both T1115C and S1118C by intracellular MTSES, suggesting that these cysteines are more readily modified from the inside in open channels. Login to comment
138 ABCC7 p.Glu1371Gln
X
ABCC7 p.Glu1371Gln 23955087:138:40
status: NEW
view ABCC7 p.Glu1371Gln details
In contrast, these channels bearing the E1371Q mutation were almost completely insensitive to external MTSES (Fig. 4b), suggesting that these cysteines are much more difficult to modify from the outside in open channels (Fig. 4d). Login to comment
141 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 23955087:141:83
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 23955087:141:45
status: NEW
view ABCC7 p.Ser1118Cys details
This suggestion is consistent with data that S1118C can form a disulfide bond with T338C in open channels [43]. Login to comment
150 ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:150:128
status: NEW
view ABCC7 p.Thr338Ala details
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 23955087:150:134
status: NEW
view ABCC7 p.Ser1118Ala details
In addition, possible additive effects of reducing the side chain volumes of these two nearby residues was investigated using a T338A/S1118A double mutant. Login to comment
152 ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 23955087:152:33
status: NEW
view ABCC7 p.Ser1118Cys details
Previously it was shown that the S1118C mutation reduced single channel conductance at depolarized membrane potentials [10]. Login to comment
153 ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 23955087:153:13
status: NEW
view ABCC7 p.Ser1118Ala details
ABCC7 p.Ser1118Val
X
ABCC7 p.Ser1118Val 23955087:153:67
status: NEW
view ABCC7 p.Ser1118Val details
ABCC7 p.Ser1118Gln
X
ABCC7 p.Ser1118Gln 23955087:153:56
status: NEW
view ABCC7 p.Ser1118Gln details
In contrast, S1118A had no effect on conductance, while S1118Q and S1118V were associated with Fig. 7 Thiocyanate permeability of mutants. Login to comment
155 ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:155:108
status: NEW
view ABCC7 p.Thr338Ala details
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 23955087:155:114
status: NEW
view ABCC7 p.Ser1118Ala details
The depolarizing (rightward) shift in the current reversal potential indicates an increased PSCN/PCl in the T338A/S1118A double mutant. Login to comment
156 ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:156:314
status: NEW
view ABCC7 p.Thr338Ala details
b Mean PSCN/PCl values calculated from reversal potential measurements under these conditions as described in the "Materials and methods" section. Mean of data from three to six patches. Asterisks indicate a significant difference from wild type (P<0.01), while hashtag indicates a significant difference from the T338A mutant (P<0.0002) Fig. 8 Acetate permeability of mutants. Login to comment
158 ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:158:111
status: NEW
view ABCC7 p.Thr338Ala details
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 23955087:158:117
status: NEW
view ABCC7 p.Ser1118Ala details
The hypolarizing (leftward) shift in the current reversal potential indicates an increased Pacetate/PCl in the T338A/S1118A double mutant. Login to comment
159 ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:159:310
status: NEW
view ABCC7 p.Thr338Ala details
b Mean Pacetate/PCl values calculated from reversal potential measurements under these conditions as described in the "Materials and methods" section. Mean of data from three to five patches. Asterisks indicate a significant difference from wild type, while hashtag indicates a significant difference from the T338A mutant (P<0.01) very small (<5 %) reductions in conductance (Fig. 5). Login to comment
160 ABCC7 p.Thr1115Ala
X
ABCC7 p.Thr1115Ala 23955087:160:34
status: NEW
view ABCC7 p.Thr1115Ala details
Conductance was also unaltered in T1115A. Login to comment
161 ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 23955087:161:171
status: NEW
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In each case, the single channel I-V relationship remained linear (e.g., Fig. 5b), in contrast to the strongly inwardly rectified I-V relationship previously observed for S1118C [10]. Login to comment
162 ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:162:96
status: NEW
view ABCC7 p.Thr338Ala details
These very minor effects on conductance are in contrast with the large (>25 %) increase seen in T338A (Fig. 5), as reported previously [26]. Login to comment
163 ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:163:18
status: NEW
view ABCC7 p.Thr338Ala details
ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:163:118
status: NEW
view ABCC7 p.Thr338Ala details
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 23955087:163:24
status: NEW
view ABCC7 p.Ser1118Ala details
The double mutant T338A/S1118A had a similarly elevated conductance that was not significantly different from that of T338A alone (P>0.75; Fig. 5). Login to comment
164 ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:164:49
status: NEW
view ABCC7 p.Thr338Ala details
Altered movement of permeant ions in the pore of T338A-CFTR is also reflected by changes in the voltage-dependent block of Cl-currents by low concentrations of permeant Au(CN)2 - ions [11, 14, 15]. Login to comment
165 ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:165:105
status: NEW
view ABCC7 p.Thr338Ala details
As shown in Fig. 6, channel block by intracellular Au(CN)2 - ions is altered in two distinct ways by the T338A mutation: (a) block is significantly weakened and (b) the I-V relationship in the presence of Au(CN)2 - shows an unusual "N"-shape (Fig. 6a), resulting in a "U"- shaped fractional current-voltage relationship (Fig. 6c) that indicates strongest block close to 0 mV membrane potential that is weakened at both more hyperpolarized and more depolarized voltages. Login to comment
166 ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:166:186
status: NEW
view ABCC7 p.Thr338Ala details
This unusual shape is thought to reflect increased unblock by blocker permeation at hyperpolarized voltages, which may reflect a reduced barrier to Au(CN)2 - movement inside the pore in T338A [11]. Login to comment
167 ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 23955087:167:68
status: NEW
view ABCC7 p.Ser1118Ala details
ABCC7 p.Thr1115Ala
X
ABCC7 p.Thr1115Ala 23955087:167:88
status: NEW
view ABCC7 p.Thr1115Ala details
ABCC7 p.Ser1118Thr
X
ABCC7 p.Ser1118Thr 23955087:167:76
status: NEW
view ABCC7 p.Ser1118Thr details
Block by intracellular Au(CN)2 - was also significantly weakened in S1118A, S1118T, and T1115A compared to wild type, especially at hyperpolarized membrane potentials (Fig. 6); however, no apparent "U"-shape to the fractional current-voltage relationship was observed (Fig. 6b). Login to comment
168 ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:168:28
status: NEW
view ABCC7 p.Thr338Ala details
ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:168:84
status: NEW
view ABCC7 p.Thr338Ala details
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 23955087:168:34
status: NEW
view ABCC7 p.Ser1118Ala details
Interestingly, block of the T338A/S1118A double mutant was slightly weaker than for T338A alone (Fig. 6c, d), suggesting that these two mutations might have additive effects on Au(CN)2 - binding in the pore. Login to comment
169 ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 23955087:169:218
status: NEW
view ABCC7 p.Ser1118Cys details
As observed at the single channel level (Fig. 5), the macroscopic I-V relationships for all mutants remained linear (e.g., Fig. 6a), in contrast to the strongly inwardly rectifying relationship previously observed for S1118C [10]. Login to comment
180 ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:180:372
status: NEW
view ABCC7 p.Thr338Ala details
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 23955087:180:294
status: NEW
view ABCC7 p.Ser1118Ala details
ABCC7 p.Thr1115Ala
X
ABCC7 p.Thr1115Ala 23955087:180:305
status: NEW
view ABCC7 p.Thr1115Ala details
As proposed previously for TM6 residue T338 [42], the channel is shown as being in an "outward facing" configuration when closed (with T1115 and S1118 accessible from the outside), and switching to an "inward facing" configuration on opening (with T1115 and S1118 accessible from the inside) S1118A and T1115A, although this increase was much less than that observed in T338A (Fig. 7b). Login to comment
181 ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:181:62
status: NEW
view ABCC7 p.Thr338Ala details
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 23955087:181:68
status: NEW
view ABCC7 p.Ser1118Ala details
Interestingly, SCN- permeability was further increased in the T338A/S1118A double mutant (Fig. 7). Login to comment
183 ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 23955087:183:47
status: NEW
view ABCC7 p.Ser1118Ala details
ABCC7 p.Ser1118Val
X
ABCC7 p.Ser1118Val 23955087:183:109
status: NEW
view ABCC7 p.Ser1118Val details
ABCC7 p.Ser1118Gln
X
ABCC7 p.Ser1118Gln 23955087:183:99
status: NEW
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ABCC7 p.Thr1115Ala
X
ABCC7 p.Thr1115Ala 23955087:183:58
status: NEW
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Acetate permeability was slightly increased in S1118A and T1115A, but not significantly changed in S1118Q or S1118V (Fig. 8b). Login to comment
184 ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:184:52
status: NEW
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ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:184:93
status: NEW
view ABCC7 p.Thr338Ala details
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 23955087:184:99
status: NEW
view ABCC7 p.Ser1118Ala details
Again, the increase in acetate permeability seen in T338A was significantly augmented in the T338A/S1118A mutation (Fig. 8), suggesting an additive effect of these two mutations on organic anion permeability. Login to comment
187 ABCC7 p.Arg334Cys
X
ABCC7 p.Arg334Cys 23955087:187:274
status: NEW
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ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 23955087:187:244
status: NEW
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ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 23955087:187:254
status: NEW
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ABCC7 p.Thr1122Cys
X
ABCC7 p.Thr1122Cys 23955087:187:284
status: NEW
view ABCC7 p.Thr1122Cys details
The proposed relative alignment of TMs 6 and 11 presented in Fig. 9a is consistent not only with the pattern of MTSES accessibility from different sides of the membrane, but also with previous data showing that disulfide bonds can form between T338C and S1118C, and between R334C and T1122C, in open channels [43]. Login to comment
199 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 23955087:199:93
status: NEW
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ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 23955087:199:130
status: NEW
view ABCC7 p.Ser1118Cys details
ABCC7 p.Thr1115Cys
X
ABCC7 p.Thr1115Cys 23955087:199:119
status: NEW
view ABCC7 p.Thr1115Cys details
Furthermore, using the same approach used previously to study side-dependent modification of T338C [42], we found that T1115C and S1118C were more readily modified from the extracellular solution in closed channels, but more readily modified from the intracellular solution in open channels (Fig. 4). Login to comment
200 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 23955087:200:62
status: NEW
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This pattern, which is common to that previously observed for T338C [42], is consistent with these residues showing alternating access to the extracellular and intracellular sides of the membrane during channel opening and closing (Fig. 9c). Login to comment
206 ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:206:219
status: NEW
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However, mutagenesis of S1118 to residues with smaller (alanine) or larger (glutamine, valine) residues had surprisingly small effects on channel functional properties, in particular compared to those of mutagenesis of T338A. Login to comment
207 ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:207:258
status: NEW
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ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 23955087:207:19
status: NEW
view ABCC7 p.Ser1118Ala details
ABCC7 p.Thr1115Ala
X
ABCC7 p.Thr1115Ala 23955087:207:306
status: NEW
view ABCC7 p.Thr1115Ala details
The effects of the S1118A mutation on permeant anion (Au(CN)2 - ) binding (Fig. 6), permeability of the lyotropic SCN- anion (Fig. 7), and permeability of the organic acetate anion (Fig. 8) were qualitatively similar to, but generally smaller than, those of T338A, and in fact similar effects were seen in T1115A. Login to comment
208 ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 23955087:208:8
status: NEW
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ABCC7 p.Ser1118Val
X
ABCC7 p.Ser1118Val 23955087:208:145
status: NEW
view ABCC7 p.Ser1118Val details
ABCC7 p.Ser1118Gln
X
ABCC7 p.Ser1118Gln 23955087:208:134
status: NEW
view ABCC7 p.Ser1118Gln details
ABCC7 p.Thr1115Ala
X
ABCC7 p.Thr1115Ala 23955087:208:19
status: NEW
view ABCC7 p.Thr1115Ala details
Neither S1118A nor T1115A significantly altered single channel conductance, although introduction of larger amino acid side chains in S1118Q and S1118V led to very small decreases in conductance (Fig. 5). Login to comment
209 ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 23955087:209:94
status: NEW
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Previously, it was shown that substitution of S1118 with a much larger phenylalanine residue (S1118F) caused a larger (~35 %) decrease in single channel conductance [46]. Login to comment
211 ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:211:58
status: NEW
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ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 23955087:211:34
status: NEW
view ABCC7 p.Ser1118Ala details
ABCC7 p.Ser1118Val
X
ABCC7 p.Ser1118Val 23955087:211:313
status: NEW
view ABCC7 p.Ser1118Val details
ABCC7 p.Ser1118Gln
X
ABCC7 p.Ser1118Gln 23955087:211:305
status: NEW
view ABCC7 p.Ser1118Gln details
ABCC7 p.Thr1115Ala
X
ABCC7 p.Thr1115Ala 23955087:211:45
status: NEW
view ABCC7 p.Thr1115Ala details
Reduction of side chain volume in S1118A and T1115A, like T338A, led to an increase in the relative permeability of the small organic anion acetate, consistent with an increase in the apparent diameter of the narrowest region of the pore [25, 26]; however, introduction of side chains with larger volume (S1118Q, S1118V) did not lead to a decrease in acetate permeability (Fig. 8). Login to comment
213 ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:213:124
status: NEW
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Simultaneous mutagenesis of T338 and S1118 to small alanine residues also had only small additional effects compared to the T338A mutation alone (Figs. 5, 6, 7, and 8). Login to comment
214 ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:214:70
status: NEW
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ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 23955087:214:76
status: NEW
view ABCC7 p.Ser1118Ala details
Most striking here were a significantly increased permeability of the T338A/S1118A double mutant both to SCN- (Fig. 7) and to acetate (Fig. 8). Login to comment
215 ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:215:242
status: NEW
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ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 23955087:215:252
status: NEW
view ABCC7 p.Ser1118Ala details
Permeability of small lyotropic anions like SCN- might be influenced by interactions throughout the pore [18, 38] or might be determined predominantly at a localized "selectivity filter" [18, 24] and so the apparently additive effects of the T338A and S1118A mutations is difficult to interpret in terms of the relative roles or locations of these two residues. Login to comment
216 ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:216:192
status: NEW
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ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 23955087:216:198
status: NEW
view ABCC7 p.Ser1118Ala details
Permeability of large anions such as acetate is thought to be determined predominantly by steric factors at the narrowest part of the pore [25], and so the increase in acetate permeability in T338A/S1118A compared to either mutation alone might be considered evidence that these two mutations impact the dimensions of a common, narrow region of the pore. Login to comment
217 ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 23955087:217:103
status: NEW
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ABCC7 p.Thr1115Ala
X
ABCC7 p.Thr1115Ala 23955087:217:115
status: NEW
view ABCC7 p.Thr1115Ala details
One possible reason contributing to the minor functional effects observed in these experiments is that S1118A (and T1115A) might be considered relatively conservative mutations leading to only small changes in amino acid side chain volume. Login to comment
218 ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:218:14
status: NEW
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Nevertheless, T338A (which results in a similarly small reduction in side chain volume) is associated with much greater changes in pore properties. Login to comment
219 ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 23955087:219:337
status: NEW
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ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 23955087:219:16
status: NEW
view ABCC7 p.Ser1118Cys details
ABCC7 p.Ser1118Gln
X
ABCC7 p.Ser1118Gln 23955087:219:345
status: NEW
view ABCC7 p.Ser1118Gln details
Previously, the S1118C mutation was shown to decrease conductance at positive voltages, leading to inward rectification of both the single channel and macroscopic current-voltage relationships [10], and although this would be considered a very conservative mutation (one oxygen atom replaced by sulfur) this effect was not reproduced in S1118A, S1118Q or S1118 (Fig. 5). Login to comment
220 ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 23955087:220:30
status: NEW
view ABCC7 p.Ser1118Cys details
Given that the effects of the S1118C mutation on single channel conductance and rectification were exacerbated by modification by external MTSES, and mostly reversed by modification with positively charged MTSET [10], these effects might reflect partial negative charge of the introduced cysteine side chain rather than a change in side chain volume. Login to comment