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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.
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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].
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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].
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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].
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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).
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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).
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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).
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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].
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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 - .
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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].
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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).
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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.
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111
ABCC7 p.Glu1371Gln
X
ABCC7 p.Glu1371Gln 23955087:111:96
status:
NEW
view ABCC7 p.Glu1371Gln details
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.
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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).
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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).
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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).
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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).
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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].
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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
.
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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.
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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].
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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.
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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.
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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.
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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.
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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).
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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].
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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.
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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].
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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.
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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.
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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.
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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.
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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).
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160
ABCC7 p.Thr1115Ala
X
ABCC7 p.Thr1115Ala 23955087:160:34
status:
NEW
view ABCC7 p.Thr1115Ala details
Conductance was also unaltered in
T1115A
.
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161
ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 23955087:161:171
status:
NEW
view ABCC7 p.Ser1118Cys details
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].
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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].
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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).
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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].
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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.
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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].
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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).
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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.
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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].
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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).
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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).
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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
view ABCC7 p.Ser1118Gln details
ABCC7 p.Thr1115Ala
X
ABCC7 p.Thr1115Ala 23955087:183:58
status:
NEW
view ABCC7 p.Thr1115Ala details
Acetate permeability was slightly increased in
S1118A
and
T1115A
, but not significantly changed in
S1118Q
or
S1118V
(Fig. 8b).
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184
ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:184:52
status:
NEW
view ABCC7 p.Thr338Ala details
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.
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187
ABCC7 p.Arg334Cys
X
ABCC7 p.Arg334Cys 23955087:187:274
status:
NEW
view ABCC7 p.Arg334Cys details
ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 23955087:187:244
status:
NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 23955087:187:254
status:
NEW
view ABCC7 p.Ser1118Cys details
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].
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199
ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 23955087:199:93
status:
NEW
view ABCC7 p.Thr338Cys details
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).
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200
ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 23955087:200:62
status:
NEW
view ABCC7 p.Thr338Cys details
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).
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206
ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:206:219
status:
NEW
view ABCC7 p.Thr338Ala details
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
.
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207
ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:207:258
status:
NEW
view ABCC7 p.Thr338Ala details
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
.
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208
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 23955087:208:8
status:
NEW
view ABCC7 p.Ser1118Ala details
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).
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209
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 23955087:209:94
status:
NEW
view ABCC7 p.Ser1118Phe details
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].
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211
ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:211:58
status:
NEW
view ABCC7 p.Thr338Ala details
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).
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213
ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:213:124
status:
NEW
view ABCC7 p.Thr338Ala details
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).
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214
ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:214:70
status:
NEW
view ABCC7 p.Thr338Ala details
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).
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215
ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:215:242
status:
NEW
view ABCC7 p.Thr338Ala details
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.
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216
ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:216:192
status:
NEW
view ABCC7 p.Thr338Ala details
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.
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217
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 23955087:217:103
status:
NEW
view ABCC7 p.Ser1118Ala details
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.
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218
ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 23955087:218:14
status:
NEW
view ABCC7 p.Thr338Ala details
Nevertheless,
T338A
(which results in a similarly small reduction in side chain volume) is associated with much greater changes in pore properties.
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219
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 23955087:219:337
status:
NEW
view ABCC7 p.Ser1118Ala details
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).
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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.
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