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PMID: 19381710
Fatehi M, Linsdell P
Novel residues lining the CFTR chloride channel pore identified by functional modification of introduced cysteines.
J Membr Biol. 2009 Apr;228(3):151-64. Epub 2009 Apr 19.,
[PubMed]
Sentences
No.
Mutations
Sentence
Comment
66
ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 19381710:66:14
status:
NEW
view ABCC7 p.Ser1118Cys details
An example is
S1118C
(Fig. 2c, d).
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71
ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 19381710:71:212
status:
NEW
view ABCC7 p.Ser1118Cys details
ABCC7 p.Val1129Cys
X
ABCC7 p.Val1129Cys 19381710:71:244
status:
NEW
view ABCC7 p.Val1129Cys details
ABCC7 p.Thr1121Cys
X
ABCC7 p.Thr1121Cys 19381710:71:220
status:
NEW
view ABCC7 p.Thr1121Cys details
ABCC7 p.Gly1127Cys
X
ABCC7 p.Gly1127Cys 19381710:71:236
status:
NEW
view ABCC7 p.Gly1127Cys details
ABCC7 p.Ile1132Cys
X
ABCC7 p.Ile1132Cys 19381710:71:263
status:
NEW
view ABCC7 p.Ile1132Cys details
ABCC7 p.Thr1122Cys
X
ABCC7 p.Thr1122Cys 19381710:71:228
status:
NEW
view ABCC7 p.Thr1122Cys details
ABCC7 p.Ile1131Cys
X
ABCC7 p.Ile1131Cys 19381710:71:252
status:
NEW
view ABCC7 p.Ile1131Cys details
As described previously for modification of cysteines introduced into TM6 (Fatehi and Linsdell 2008) and the extracellular loop between TMs 1 and 2 (Zhou et al. 2008), MTSET and MTSES altered the IREL-V shape in
S1118C
,
T1121C
,
T1122C
,
G1127C
,
V1129C
,
I1131C
and
I1132C
.
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72
ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 19381710:72:142
status:
NEW
view ABCC7 p.Ser1118Cys details
ABCC7 p.Val1129Cys
X
ABCC7 p.Val1129Cys 19381710:72:233
status:
NEW
view ABCC7 p.Val1129Cys details
ABCC7 p.Thr1121Cys
X
ABCC7 p.Thr1121Cys 19381710:72:150
status:
NEW
view ABCC7 p.Thr1121Cys details
ABCC7 p.Gly1127Cys
X
ABCC7 p.Gly1127Cys 19381710:72:166
status:
NEW
view ABCC7 p.Gly1127Cys details
ABCC7 p.Thr1122Cys
X
ABCC7 p.Thr1122Cys 19381710:72:158
status:
NEW
view ABCC7 p.Thr1122Cys details
ABCC7 p.Ala1136Cys
X
ABCC7 p.Ala1136Cys 19381710:72:177
status:
NEW
view ABCC7 p.Ala1136Cys details
Of 21 cysteine mutants studied, only six significantly altered I-V relationship shape in the absence of external MTS reagents (Fig. 3a), with
S1118C
,
T1121C
,
T1122C
,
G1127C
and
A1136C
all causing significant inward rectification and
V1129C
showing outward rectification.
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75
ABCC7 p.Ile1131Cys
X
ABCC7 p.Ile1131Cys 19381710:75:121
status:
NEW
view ABCC7 p.Ile1131Cys details
As described above (Fig. 2), six mutants had I-V relationships that were sensitive to both MTSET and MTSES and only one (
I1131C
) was altered by MTSET but not MTSES.
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76
ABCC7 p.Ala1136Cys
X
ABCC7 p.Ala1136Cys 19381710:76:99
status:
NEW
view ABCC7 p.Ala1136Cys details
There was strong overlap between changes in control I-V shape and sensitivity to MTS reagents-only
A1136C
showed an I-V relationship that was significantly different in shape from wild-type in the absence of MTS reagents (Fig. 3a) but insensitive to charged MTS reagents (Fig. 3b).
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82
ABCC7 p.Ile1132Cys
X
ABCC7 p.Ile1132Cys 19381710:82:24
status:
NEW
view ABCC7 p.Ile1132Cys details
ABCC7 p.Ile1131Cys
X
ABCC7 p.Ile1131Cys 19381710:82:13
status:
NEW
view ABCC7 p.Ile1131Cys details
In contrast,
I1131C
and
I1132C
did not significantly affect the form of either the i-V relationship (Fig. 4b) or the I-V relationship (Fig. 3a).
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83
ABCC7 p.Val1129Cys
X
ABCC7 p.Val1129Cys 19381710:83:16
status:
NEW
view ABCC7 p.Val1129Cys details
Only one mutant-
V1129C
-significantly affected the magnitude of unitary currents at hyperpolarized voltages (Figs. 4, 5a), giving a decrease in unitary current amplitude of *12% at -80 mV (Fig. 5a).
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84
ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 19381710:84:73
status:
NEW
view ABCC7 p.Ser1118Cys details
ABCC7 p.Val1129Cys
X
ABCC7 p.Val1129Cys 19381710:84:138
status:
NEW
view ABCC7 p.Val1129Cys details
ABCC7 p.Thr1121Cys
X
ABCC7 p.Thr1121Cys 19381710:84:81
status:
NEW
view ABCC7 p.Thr1121Cys details
ABCC7 p.Gly1127Cys
X
ABCC7 p.Gly1127Cys 19381710:84:100
status:
NEW
view ABCC7 p.Gly1127Cys details
ABCC7 p.Thr1122Cys
X
ABCC7 p.Thr1122Cys 19381710:84:89
status:
NEW
view ABCC7 p.Thr1122Cys details
Unitary currents at depolarized voltages were significantly decreased in
S1118C
,
T1121C
,
T1122C
and
G1127C
and significantly increased in
V1129C
(Fig. 5b).
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85
ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 19381710:85:107
status:
NEW
view ABCC7 p.Ser1118Cys details
ABCC7 p.Val1129Cys
X
ABCC7 p.Val1129Cys 19381710:85:182
status:
NEW
view ABCC7 p.Val1129Cys details
ABCC7 p.Thr1121Cys
X
ABCC7 p.Thr1121Cys 19381710:85:115
status:
NEW
view ABCC7 p.Thr1121Cys details
ABCC7 p.Gly1127Cys
X
ABCC7 p.Gly1127Cys 19381710:85:134
status:
NEW
view ABCC7 p.Gly1127Cys details
ABCC7 p.Thr1122Cys
X
ABCC7 p.Thr1122Cys 19381710:85:123
status:
NEW
view ABCC7 p.Thr1122Cys details
This resulted in changes in the shape of the i-V relationship, causing inward rectification in the case of
S1118C
,
T1121C
,
T1122C
and
G1127C
and outward rectification in the case of
V1129C
(Figs. 4b, 5c).
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86
ABCC7 p.Ile1132Cys
X
ABCC7 p.Ile1132Cys 19381710:86:52
status:
NEW
view ABCC7 p.Ile1132Cys details
ABCC7 p.Ile1131Cys
X
ABCC7 p.Ile1131Cys 19381710:86:42
status:
NEW
view ABCC7 p.Ile1131Cys details
No changes in i-V shape were observed for
I1131C
or
I1132C
.
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91
ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 19381710:91:64
status:
NEW
view ABCC7 p.Ser1118Cys details
ABCC7 p.Val1129Cys
X
ABCC7 p.Val1129Cys 19381710:91:96
status:
NEW
view ABCC7 p.Val1129Cys details
ABCC7 p.Thr1121Cys
X
ABCC7 p.Thr1121Cys 19381710:91:72
status:
NEW
view ABCC7 p.Thr1121Cys details
ABCC7 p.Gly1127Cys
X
ABCC7 p.Gly1127Cys 19381710:91:88
status:
NEW
view ABCC7 p.Gly1127Cys details
ABCC7 p.Ile1132Cys
X
ABCC7 p.Ile1132Cys 19381710:91:115
status:
NEW
view ABCC7 p.Ile1132Cys details
ABCC7 p.Thr1122Cys
X
ABCC7 p.Thr1122Cys 19381710:91:80
status:
NEW
view ABCC7 p.Thr1122Cys details
ABCC7 p.Ile1131Cys
X
ABCC7 p.Ile1131Cys 19381710:91:104
status:
NEW
view ABCC7 p.Ile1131Cys details
Indeed, changes in unitary current amplitude were observed in
S1118C
,
T1121C
,
T1122C
,
G1127C
,
V1129C
,
I1131C
and
I1132C
, but not wild-type, when MTS reagents were included in the pipette solution (Fig. 6).
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98
ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 19381710:98:65
status:
NEW
view ABCC7 p.Ser1118Cys details
c, d Example I-V relationships and mean rectification ratios for
S1118C
under the same conditions.
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114
ABCC7 p.Ile1131Cys
X
ABCC7 p.Ile1131Cys 19381710:114:156
status:
NEW
view ABCC7 p.Ile1131Cys details
Note that the rectification ratio in six cysteine mutants is significantly affected by both MTSET and MTSES (indicated by asterisks), whereas in a seventh (
I1131C
) it is significantly altered by MTSET but not by MTSES voltages as an indicator, Fig. 8 shows that MTS reagents had charge-dependent effects on i-V relationship shape that broadly mirrored those observed in the macroscopic I-V relationships (see Fig. 3c).
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118
ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 19381710:118:16
status:
NEW
view ABCC7 p.Ser1118Cys details
ABCC7 p.Thr1121Cys
X
ABCC7 p.Thr1121Cys 19381710:118:24
status:
NEW
view ABCC7 p.Thr1121Cys details
ABCC7 p.Gly1127Cys
X
ABCC7 p.Gly1127Cys 19381710:118:40
status:
NEW
view ABCC7 p.Gly1127Cys details
ABCC7 p.Thr1122Cys
X
ABCC7 p.Thr1122Cys 19381710:118:32
status:
NEW
view ABCC7 p.Thr1122Cys details
Four mutations (
S1118C
,
T1121C
,
T1122C
,
G1127C
) led to significant decreases in unitary current amplitude (Fig. 5b), which were relatively strongly affected by MTS modification-in each case conductance was further decreased by reaction with MTSES and increased to near wild-type levels by MTSET (Fig. 9a).
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119
ABCC7 p.Val1129Cys
X
ABCC7 p.Val1129Cys 19381710:119:40
status:
NEW
view ABCC7 p.Val1129Cys details
ABCC7 p.Ile1132Cys
X
ABCC7 p.Ile1132Cys 19381710:119:56
status:
NEW
view ABCC7 p.Ile1132Cys details
ABCC7 p.Ile1131Cys
X
ABCC7 p.Ile1131Cys 19381710:119:48
status:
NEW
view ABCC7 p.Ile1131Cys details
In contrast, the other three mutations (
V1129C
,
I1131C
,
I1132C
) led to no change or even a slight increase in unitary current amplitude (Fig. 5b) and more minor effects of MTS modification, resulting in no change or a small decrease in amplitude with MTSES and increases in amplitude to levels above wild-type with MTSET (Fig. 9b).
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124
ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 19381710:124:122
status:
NEW
view ABCC7 p.Ser1118Cys details
ABCC7 p.Val1129Cys
X
ABCC7 p.Val1129Cys 19381710:124:170
status:
NEW
view ABCC7 p.Val1129Cys details
ABCC7 p.Thr1121Cys
X
ABCC7 p.Thr1121Cys 19381710:124:159
status:
NEW
view ABCC7 p.Thr1121Cys details
ABCC7 p.Ile1132Cys
X
ABCC7 p.Ile1132Cys 19381710:124:69
status:
NEW
view ABCC7 p.Ile1132Cys details
ABCC7 p.Ile1131Cys
X
ABCC7 p.Ile1131Cys 19381710:124:207
status:
NEW
view ABCC7 p.Ile1131Cys details
Under these conditions, SCN- block was significantly strengthened in
I1132C
(at hyperpolarized and depolarized voltages),
S1118C
(at hyperpolarized voltages),
T1121C
and
V1129C
(at depolarized voltages) and
I1131C
(at very depolarized voltages only) Fig. 4 Single-channel currents carried by cysteine mutant forms of CFTR.
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125
ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 19381710:125:56
status:
NEW
view ABCC7 p.Ser1118Cys details
ABCC7 p.Val1129Cys
X
ABCC7 p.Val1129Cys 19381710:125:83
status:
NEW
view ABCC7 p.Val1129Cys details
ABCC7 p.Thr1121Cys
X
ABCC7 p.Thr1121Cys 19381710:125:64
status:
NEW
view ABCC7 p.Thr1121Cys details
ABCC7 p.Thr1122Cys
X
ABCC7 p.Thr1122Cys 19381710:125:72
status:
NEW
view ABCC7 p.Thr1122Cys details
a Example single-channel currents carried by wild-type,
S1118C
,
T1121C
,
T1122C
and
V1129C
, at membrane potentials of ?60 (top) and -60 (bottom) mV.
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130
ABCC7 p.Gly1127Cys
X
ABCC7 p.Gly1127Cys 19381710:130:56
status:
NEW
view ABCC7 p.Gly1127Cys details
ABCC7 p.Thr1122Cys
X
ABCC7 p.Thr1122Cys 19381710:130:46
status:
NEW
view ABCC7 p.Thr1122Cys details
Block was not significantly altered in either
T1122C
or
G1127C
(data not shown).
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133
ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 19381710:133:73
status:
NEW
view ABCC7 p.Ser1118Cys details
ABCC7 p.Val1129Cys
X
ABCC7 p.Val1129Cys 19381710:133:148
status:
NEW
view ABCC7 p.Val1129Cys details
ABCC7 p.Thr1121Cys
X
ABCC7 p.Thr1121Cys 19381710:133:140
status:
NEW
view ABCC7 p.Thr1121Cys details
ABCC7 p.Gly1127Cys
X
ABCC7 p.Gly1127Cys 19381710:133:116
status:
NEW
view ABCC7 p.Gly1127Cys details
ABCC7 p.Ile1132Cys
X
ABCC7 p.Ile1132Cys 19381710:133:167
status:
NEW
view ABCC7 p.Ile1132Cys details
ABCC7 p.Thr1122Cys
X
ABCC7 p.Thr1122Cys 19381710:133:105
status:
NEW
view ABCC7 p.Thr1122Cys details
ABCC7 p.Ile1131Cys
X
ABCC7 p.Ile1131Cys 19381710:133:156
status:
NEW
view ABCC7 p.Ile1131Cys details
Under these conditions, SCN- permeability was significantly increased in
S1118C
and (to a lesser extent)
T1122C
and
G1127C
and unaltered in
T1121C
,
V1129C
,
I1131C
and
I1132C
(Fig. 11).
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158
ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 19381710:158:76
status:
NEW
view ABCC7 p.Ser1118Cys details
ABCC7 p.Val1129Cys
X
ABCC7 p.Val1129Cys 19381710:158:108
status:
NEW
view ABCC7 p.Val1129Cys details
ABCC7 p.Thr1121Cys
X
ABCC7 p.Thr1121Cys 19381710:158:84
status:
NEW
view ABCC7 p.Thr1121Cys details
ABCC7 p.Gly1127Cys
X
ABCC7 p.Gly1127Cys 19381710:158:100
status:
NEW
view ABCC7 p.Gly1127Cys details
ABCC7 p.Thr1122Cys
X
ABCC7 p.Thr1122Cys 19381710:158:92
status:
NEW
view ABCC7 p.Thr1122Cys details
Of the seven mutants that were functionally modified by MTS reagents, five (
S1118C
,
T1121C
,
T1122C
,
G1127C
,
V1129C
) also showed significantly altered unitary current amplitude in the absence of MTS modification (Figs. 4, 5).
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161
ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 19381710:161:2
status:
NEW
view ABCC7 p.Ser1118Cys details
ABCC7 p.Val1129Cys
X
ABCC7 p.Val1129Cys 19381710:161:52
status:
NEW
view ABCC7 p.Val1129Cys details
ABCC7 p.Thr1121Cys
X
ABCC7 p.Thr1121Cys 19381710:161:14
status:
NEW
view ABCC7 p.Thr1121Cys details
ABCC7 p.Gly1127Cys
X
ABCC7 p.Gly1127Cys 19381710:161:38
status:
NEW
view ABCC7 p.Gly1127Cys details
ABCC7 p.Ile1132Cys
X
ABCC7 p.Ile1132Cys 19381710:161:76
status:
NEW
view ABCC7 p.Ile1132Cys details
ABCC7 p.Thr1122Cys
X
ABCC7 p.Thr1122Cys 19381710:161:26
status:
NEW
view ABCC7 p.Thr1122Cys details
ABCC7 p.Ile1131Cys
X
ABCC7 p.Ile1131Cys 19381710:161:64
status:
NEW
view ABCC7 p.Ile1131Cys details
a
S1118C
(d),
T1121C
(j),
T1122C
(),
G1127C
(h); b
V1129C
(m),
I1131C
(r),
I1132C
(.).
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168
ABCC7 p.Ala1136Cys
X
ABCC7 p.Ala1136Cys 19381710:168:66
status:
NEW
view ABCC7 p.Ala1136Cys details
Only one mutant that was apparently not affected by MTS reagents (
A1136C
) had a small effect on the shape of the I-V relationship (Fig. 3a).
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177
ABCC7 p.Leu333Cys
X
ABCC7 p.Leu333Cys 19381710:177:80
status:
NEW
view ABCC7 p.Leu333Cys details
ABCC7 p.Ile331Cys
X
ABCC7 p.Ile331Cys 19381710:177:73
status:
NEW
view ABCC7 p.Ile331Cys details
Effects of external MTS reagents on the gating of CFTR cysteine mutants (
I331C
,
L333C
) have been described (Beck et al. 2008) but would presumably not be noticed using our experimental approach.
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183
ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 19381710:183:49
status:
NEW
view ABCC7 p.Ser1118Cys details
ABCC7 p.Val1129Cys
X
ABCC7 p.Val1129Cys 19381710:183:157
status:
NEW
view ABCC7 p.Val1129Cys details
ABCC7 p.Thr1121Cys
X
ABCC7 p.Thr1121Cys 19381710:183:57
status:
NEW
view ABCC7 p.Thr1121Cys details
ABCC7 p.Gly1127Cys
X
ABCC7 p.Gly1127Cys 19381710:183:73
status:
NEW
view ABCC7 p.Gly1127Cys details
ABCC7 p.Thr1122Cys
X
ABCC7 p.Thr1122Cys 19381710:183:65
status:
NEW
view ABCC7 p.Thr1122Cys details
We speculate that one group of reactive mutants (
S1118C
,
T1121C
,
T1122C
,
G1127C
) is located relatively deep in the pore from the outside and that the other (
V1129C
, Fig. 11 Thiocyanate permeability of mutants.
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185
ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 19381710:185:93
status:
NEW
view ABCC7 p.Ser1118Cys details
In these examples, the current reversal potential is ?36.4 mV for wild-type and ?47.8 mV for
S1118C
(shown by arrows), suggesting an increased PSCN/PCl in this mutant.
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187
ABCC7 p.Ile1132Cys
X
ABCC7 p.Ile1132Cys 19381710:187:60
status:
NEW
view ABCC7 p.Ile1132Cys details
ABCC7 p.Ile1131Cys
X
ABCC7 p.Ile1131Cys 19381710:187:52
status:
NEW
view ABCC7 p.Ile1131Cys details
* Significant difference from wild-type (P \ 0.05)
I1131C
,
I1132C
) represents mutations at the outermost mouth of the pore.
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188
ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 19381710:188:63
status:
NEW
view ABCC7 p.Ser1118Cys details
ABCC7 p.Thr1121Cys
X
ABCC7 p.Thr1121Cys 19381710:188:71
status:
NEW
view ABCC7 p.Thr1121Cys details
ABCC7 p.Gly1127Cys
X
ABCC7 p.Gly1127Cys 19381710:188:87
status:
NEW
view ABCC7 p.Gly1127Cys details
ABCC7 p.Thr1122Cys
X
ABCC7 p.Thr1122Cys 19381710:188:79
status:
NEW
view ABCC7 p.Thr1122Cys details
In this scenario, charge-neutral mutations deeper in the pore (
S1118C
,
T1121C
,
T1122C
,
G1127C
) (Fig. 9a) disrupt Cl- movement in the pore in a nonelectrostatic fashion, leading to reduced unitary currents at depolarized voltages, as described previously for TM6 mutations (McDonough et al. 1994; Linsdell et al. 1998; Linsdell 2001a).
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191
ABCC7 p.Val1129Cys
X
ABCC7 p.Val1129Cys 19381710:191:230
status:
NEW
view ABCC7 p.Val1129Cys details
ABCC7 p.Ile1132Cys
X
ABCC7 p.Ile1132Cys 19381710:191:246
status:
NEW
view ABCC7 p.Ile1132Cys details
ABCC7 p.Ile1131Cys
X
ABCC7 p.Ile1131Cys 19381710:191:238
status:
NEW
view ABCC7 p.Ile1131Cys details
Chloride conductance was further reduced by MTSES modification at these sites, indicating the detrimental effect of depositing a negative charge within the permeation pathway. Cysteine substitution at the outer mouth of the pore (
V1129C
,
I1131C
,
I1132C
) (Fig. 9b) had somewhat different effects.
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200
ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 19381710:200:10
status:
NEW
view ABCC7 p.Ser1118Cys details
ABCC7 p.Gly1127Cys
X
ABCC7 p.Gly1127Cys 19381710:200:29
status:
NEW
view ABCC7 p.Gly1127Cys details
ABCC7 p.Thr1122Cys
X
ABCC7 p.Thr1122Cys 19381710:200:18
status:
NEW
view ABCC7 p.Thr1122Cys details
Mutations
S1118C
,
T1122C
and
G1127C
also altered the anion selectivity of CFTR, significantly increasing SCN- per- meability (Fig. 11), which is consistent with changes in pore structure and function.
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201
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 19381710:201:75
status:
NEW
view ABCC7 p.Ser1118Phe details
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 19381710:201:99
status:
NEW
view ABCC7 p.Ser1118Ala details
Previously, SCN- permeabil- ity was shown to be significantly decreased in
S1118F
but unaltered in
S1118A
(Zhang et al. 2000).
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214
ABCC7 p.Ser1118Cys
X
ABCC7 p.Ser1118Cys 19381710:214:147
status:
NEW
view ABCC7 p.Ser1118Cys details
It should be stressed that, in some cases, the cysteine mutations we used in the present study represent rather conservative mutations (especially
S1118C
, which effectively changes one oxygen atom to sulfur).
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