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PMID: 9511930
Akabas MH, Cheung M, Guinamard R
Probing the structural and functional domains of the CFTR chloride channel.
J Bioenerg Biomembr. 1997 Oct;29(5):453-63.,
[PubMed]
Sentences
No.
Mutations
Sentence
Comment
81
ABCC7 p.Lys335Cys
X
ABCC7 p.Lys335Cys 9511930:81:34
status:
NEW
view ABCC7 p.Lys335Cys details
The effect of modification of the
K335C
mutant by the MTS reagents on CFTR current would be indirect.
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87
ABCC7 p.Gln353Cys
X
ABCC7 p.Gln353Cys 9511930:87:92
status:
NEW
view ABCC7 p.Gln353Cys details
DIAMETER OF THE CHANNEL LUMEN MTSET+ can penetrate from the extracellular end to react with
Q353C
(Cheung and Akabas, 1996).
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89
ABCC7 p.Gln353Cys
X
ABCC7 p.Gln353Cys 9511930:89:78
status:
NEW
view ABCC7 p.Gln353Cys details
Therefore, the channel diameter from the extracellular end to the position of
Q353C
, flanking the cytoplasmic end of the M6 segment, must be at a minimum 6 A.
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115
ABCC7 p.Leu333Cys
X
ABCC7 p.Leu333Cys 9511930:115:55
status:
NEW
view ABCC7 p.Leu333Cys details
ABCC7 p.Leu333Cys
X
ABCC7 p.Leu333Cys 9511930:115:234
status:
NEW
view ABCC7 p.Leu333Cys details
The ratio of the reaction rates of MTSES- /MTSET+ with
L333C
, the most extracellular residue tested, is also 0.08, suggesting that there is no charge selectivity for the movement of the MTS reagents from the extracellular solution to
L333C
.
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116
ABCC7 p.Leu333Cys
X
ABCC7 p.Leu333Cys 9511930:116:195
status:
NEW
view ABCC7 p.Leu333Cys details
Thus, in order to normalize for the difference in the intrinsic reaction rates of the two MTS reagents we divide the ratio of the rates at a given residue by the ratio of the reaction rates with
L333C
.
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122
ABCC7 p.Gln353Cys
X
ABCC7 p.Gln353Cys 9511930:122:78
status:
NEW
view ABCC7 p.Gln353Cys details
ABCC7 p.Thr351Cys
X
ABCC7 p.Thr351Cys 9511930:122:68
status:
NEW
view ABCC7 p.Thr351Cys details
The major site of charge selectivity appears to be in the region of
T351C
and
Q353C
where the anion- to-cation selectivity rises to between 15 and 25 (Fig. 3B) (Cheung and Akabas, 1997).
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127
ABCC7 p.Gln353Cys
X
ABCC7 p.Gln353Cys 9511930:127:35
status:
NEW
view ABCC7 p.Gln353Cys details
ABCC7 p.Thr351Cys
X
ABCC7 p.Thr351Cys 9511930:127:25
status:
NEW
view ABCC7 p.Thr351Cys details
Arg352, which is between
T351C
and
Q353C
, appears to be a majordeterminantof the anion selectivity in this region.
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128
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 9511930:128:11
status:
NEW
view ABCC7 p.Arg352Cys details
Thus, when
cysteine is substituted for Arg352
the charge selectivity drops to the same low level that is observed in the more extracellular portion of the channel (Fig. 3B).
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129
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 9511930:129:117
status:
NEW
view ABCC7 p.Arg352Cys details
If other residues in this region were the main determinants of anion selectivity, then, the anion selectivity of the
R352C
mutant should have been similar to that of the adjacent residues.
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130
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 9511930:130:60
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Gln353Cys
X
ABCC7 p.Gln353Cys 9511930:130:133
status:
NEW
view ABCC7 p.Gln353Cys details
ABCC7 p.Thr351Cys
X
ABCC7 p.Thr351Cys 9511930:130:124
status:
NEW
view ABCC7 p.Thr351Cys details
Moreover, based on our measurements of electrical distance,
R352C
is closer to the extracellular end of the channel than is
T351C
or
Q353C
(Fig. 3A).
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131
ABCC7 p.Gln353Cys
X
ABCC7 p.Gln353Cys 9511930:131:184
status:
NEW
view ABCC7 p.Gln353Cys details
ABCC7 p.Thr351Cys
X
ABCC7 p.Thr351Cys 9511930:131:175
status:
NEW
view ABCC7 p.Thr351Cys details
Thus, ions passing from the extracellular end of the channel would first encounter Arg352, which we infer forms part of the charge-selectivity filter, before they could reach
T351C
or
Q353C
, thereby accounting for the greater anion selectivity observed at these residues.
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140
ABCC7 p.Lys335Glu
X
ABCC7 p.Lys335Glu 9511930:140:23
status:
NEW
view ABCC7 p.Lys335Glu details
ABCC7 p.Lys95Asp
X
ABCC7 p.Lys95Asp 9511930:140:14
status:
NEW
view ABCC7 p.Lys95Asp details
The mutations
K95D
and
K335E
altered the halide permeability sequence, leading to the suggestion that these residues might be involved in anion binding (Anderson et al., 1991b).
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141
ABCC7 p.Lys335Glu
X
ABCC7 p.Lys335Glu 9511930:141:13
status:
NEW
view ABCC7 p.Lys335Glu details
The mutation
K335E
, however,did not alter the SCN- - induced anomalous mole fraction effects (Tabcharani et al., 1993), and our data imply that Lys335 is on the opposite side of the helix from the channel-liningface (Fig. 2B) (Cheung and Akabas, 1996), making it unlikely that this residue is part of an anion binding site.
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142
ABCC7 p.Lys335Glu
X
ABCC7 p.Lys335Glu 9511930:142:16
status:
NEW
view ABCC7 p.Lys335Glu details
More likely,the
K335E
mutationinduces aconfor- mational change in residues that form ananion-binding site, possibly at quite a distance from this residue.
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143
ABCC7 p.Pro99Leu
X
ABCC7 p.Pro99Leu 9511930:143:100
status:
NEW
view ABCC7 p.Pro99Leu details
A similar mechanism is likely involved in the alteration of the halide permeability sequence by the
P99L
mutation (Sheppard et al., 1996) because Pro99 is also not a channel-lining residue (Akabas et al., 1994b).
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148
ABCC7 p.Leu333Cys
X
ABCC7 p.Leu333Cys 9511930:148:65
status:
NEW
view ABCC7 p.Leu333Cys details
ABCC7 p.Ser341Cys
X
ABCC7 p.Ser341Cys 9511930:148:74
status:
NEW
view ABCC7 p.Ser341Cys details
The lack of significant electrical distance to the residues from
L333C
to
S341C
(Fig. 3A) implies that the MTS reagents do not pass through the electrical field to reach these residues.
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155
ABCC7 p.Thr351Cys
X
ABCC7 p.Thr351Cys 9511930:155:61
status:
NEW
view ABCC7 p.Thr351Cys details
ABCC7 p.Ser341Cys
X
ABCC7 p.Ser341Cys 9511930:155:52
status:
NEW
view ABCC7 p.Ser341Cys details
The electrical distance increases dramatically from
S341C
to
T351C
(Fig. 3A), suggesting that most of the electrical potential falls in this region of the channel.
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159
ABCC7 p.Gln353Cys
X
ABCC7 p.Gln353Cys 9511930:159:64
status:
NEW
view ABCC7 p.Gln353Cys details
ABCC7 p.Thr351Cys
X
ABCC7 p.Thr351Cys 9511930:159:54
status:
NEW
view ABCC7 p.Thr351Cys details
The largest electrical distances that we measured, to
T351C
and
Q353C
, was only 0.6.
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