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PMID: 10866956
Zhang ZR, McDonough SI, McCarty NA
Interaction between permeation and gating in a putative pore domain mutant in the cystic fibrosis transmembrane conductance regulator.
Biophys J. 2000 Jul;79(1):298-313.,
[PubMed]
Sentences
No.
Mutations
Sentence
Comment
2
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:2:51
status:
NEW
view ABCC7 p.Ser1118Phe details
Here we report a serine-to-phenylalanine mutation (
S1118F
) in the 11th transmembrane domain that confers voltage-dependent, single-exponential current relaxations and moderate inward rectification of the macroscopic currents upon expression in Xenopus oocytes.
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3
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:3:21
status:
NEW
view ABCC7 p.Ser1118Phe details
At steady state, the
S1118F
-CFTR single-channel conductance rectifies, corresponding to the whole-cell rectification.
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5
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:5:0
status:
NEW
view ABCC7 p.Ser1118Phe details
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:5:117
status:
NEW
view ABCC7 p.Ser1118Phe details
S1118F
-CFTR currents are blocked in a voltage-dependent manner by diphenylamine-2-carboxylate (DPC); the affinity of
S1118F
-CFTR for DPC is similar to that of the wild-type channel, but blockade exhibits moderately reduced voltage dependence.
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22
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:22:51
status:
NEW
view ABCC7 p.Ser1118Phe details
Here we report a serine-to-phenylalanine mutation (
S1118F
) in TM11 that affects both permeation and gating.
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23
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:23:33
status:
NEW
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Most strikingly, the macroscopic
S1118F
-CFTR currents display voltage-dependent current relaxations; these relaxations are modulated by permeating anions.
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33
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:33:93
status:
NEW
view ABCC7 p.Ser1118Phe details
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:33:113
status:
NEW
view ABCC7 p.Ser1118Phe details
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 10866956:33:101
status:
NEW
view ABCC7 p.Ser1118Ala details
ABCC7 p.Phe1111Ser
X
ABCC7 p.Phe1111Ser 10866956:33:120
status:
NEW
view ABCC7 p.Phe1111Ser details
Preparation of oocytes and cRNA CFTR was subcloned into the pALTER vector (Promega), and the
S1118F
,
S1118A
, and
S1118F
/
F1111S
mutations were made using the Promega Altered Sites protocol (McDonough et al., 1994).
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80
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:80:62
status:
NEW
view ABCC7 p.Ser1118Phe details
Unexpectedly, the most obvious consequence of the mutation of
S1118F
-CFTR is the appearance of relaxations in current density upon stepping to a new membrane potential.
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85
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:85:9
status:
NEW
view ABCC7 p.Ser1118Phe details
However,
S1118F
-CFTR displays voltage-dependent current relaxations in response to protocols applying either depolarizing or hyperpolarizing prepotentials.
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87
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:87:162
status:
NEW
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These voltage-jump relaxations lead to a larger conductance for jumps to more negative potentials and to a smaller conductance for jumps in the FIGURE 1 Mutation
S1118F
-CFTR results in current relaxations.
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93
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:93:82
status:
NEW
view ABCC7 p.Ser1118Phe details
(B and C) Families of currents measured in oocytes expressing either wild-type or
S1118F
-CFTR channels, respectively.
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104
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:104:10
status:
NEW
view ABCC7 p.Ser1118Phe details
Note that
S1118F
-CFTR also displays tail currents (Figs. 1, 2, 6, and 7), which have not been described for WT or any mutant of CFTR studied thus far.
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116
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:116:78
status:
NEW
view ABCC7 p.Ser1118Phe details
In WT-CFTR, TM11 contains four phenylalanine residues (Fig. 1 A); mutation of
S1118F
adds a fifth.
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117
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:117:106
status:
NEW
view ABCC7 p.Ser1118Phe details
If this domain is ॷ-helical, as predicted from hydropathy analysis (Riordan et al., 1989), mutation
S1118F
would then place three phenylalanine residues in close mutual proximity (at positions 1107, 1111, and 1118) and on approximately the same face of the helix.
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118
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:118:75
status:
NEW
view ABCC7 p.Ser1118Phe details
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:118:154
status:
NEW
view ABCC7 p.Ser1118Phe details
ABCC7 p.Phe1111Ser
X
ABCC7 p.Phe1111Ser 10866956:118:161
status:
NEW
view ABCC7 p.Phe1111Ser details
To determine whether this imposed pattern was the source of relaxations in
S1118F
-CFTR, due to introduction of another bulky residue, the double mutation
S1118F
/
F1111S
was constructed.
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119
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:119:112
status:
NEW
view ABCC7 p.Ser1118Phe details
These channels displayed relaxations indistinguishable from those of the single FIGURE 2 Relaxations induced in
S1118F
-CFTR currents were fit to single-exponential decay functions.
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125
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 10866956:125:34
status:
NEW
view ABCC7 p.Ser1118Ala details
These relaxations are not seen in
S1118A
channels (not shown).
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126
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:126:7
status:
NEW
view ABCC7 p.Ser1118Phe details
mutant
S1118F
-CFTR (not shown).
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128
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 10866956:128:43
status:
NEW
view ABCC7 p.Ser1118Ala details
In addition, mutation of S1118 to alanine (
S1118A
-CFTR) did not cause relaxations.
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132
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:132:70
status:
NEW
view ABCC7 p.Ser1118Phe details
Gating behavior of single CFTR channels from oocytes expressing WT or
S1118F
-CFTR was studied in excised patch mode.
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139
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:139:122
status:
NEW
view ABCC7 p.Ser1118Phe details
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:139:173
status:
NEW
view ABCC7 p.Ser1118Phe details
Under these conditions, burst duration was 1392 afe; 77 ms for WT-CFTR (n afd; 441 bursts) and 102 afe; 8 ms for
S1118F
- FIGURE 3 The current-voltage relations for
S1118F
-CFTR channel shift during the voltage-jump relaxations.
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152
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:152:10
status:
NEW
view ABCC7 p.Ser1118Phe details
Note that
S1118F
-CFTR channels exhibit much briefer openings than does WT.
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153
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:153:51
status:
NEW
view ABCC7 p.Ser1118Phe details
Currents were not observed in phosphorylated WT or
S1118F
-CFTR channels bathed in solutions lacking ATP (not shown).
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155
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:155:33
status:
NEW
view ABCC7 p.Ser1118Phe details
Hence the mean burst duration in
S1118F
-CFTR is reduced to only 7% that of WT channels.
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166
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:166:18
status:
NEW
view ABCC7 p.Ser1118Phe details
We tested whether
S1118F
-CFTR exhibited alterations in the interaction with DPC, which would be consistent with a pore-lining position for this serine.
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167
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:167:35
status:
NEW
view ABCC7 p.Ser1118Phe details
Fig. 6 shows background-subtracted
S1118F
-CFTR currents for a representative cell before (Fig. 6 A) and several minutes after (Fig. 6 B) bath application of 200 òe;M DPC.
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171
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:171:29
status:
NEW
view ABCC7 p.Ser1118Phe details
At afa;100 mV, DPC blocks
S1118F
-CFTR and WT channels with roughly the same efficacy: the apparent KD (at afa;100 mV) was, respectively, 266 afe; 13 òe;M and 276 afe; 14 òe;M (mean afe; SE, n afd; 6 and 15; data for WT are from McDonough et al., 1994).
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174
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:174:30
status:
NEW
view ABCC7 p.Ser1118Phe details
The voltage dependence of the
S1118F
-CFTR block is significantly less steep than that of the wild type; the apparent binding distance is òa; afd; 0.27 afe; 0.01 (mean afe; SE, n afd; 6) for the mutant versus 0.41 afe; 0.03 for WT channels (McDonough et al., 1994).
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175
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:175:0
status:
NEW
view ABCC7 p.Ser1118Phe details
S1118F
-CFTR exhibits altered permeation characteristics S1118, according to our alignment, occupies a position in TM11 that is homologous to that of T338 in TM6.
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179
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:179:27
status:
NEW
view ABCC7 p.Ser1118Phe details
Because oocytes expressing
S1118F
-CFTR show voltage-jump relaxations, it was not appropriate to use the more common approach of applying voltage-ramp protocols to generate selectivity data.
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180
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:180:45
status:
NEW
view ABCC7 p.Ser1118Phe details
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 10866956:180:57
status:
NEW
view ABCC7 p.Ser1118Ala details
Instead, currents in oocytes expressing WT-,
S1118F
-, or
S1118A
-CFTR channels were elicited by stepping for 75 ms from the holding potential of afa;30 mV to a series of test potentials between afa;140 and af9;80 mV in af9;20 mV increments.
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182
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:182:199
status:
NEW
view ABCC7 p.Ser1118Phe details
If there are two open states that vary in the voltage dependence of microscopic kinetics, currents measured early in the relaxation and at later times likely represent different mixtures of FIGURE 5
S1118F
-CFTR channels show rectification of single-channel conductance.
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189
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:189:105
status:
NEW
view ABCC7 p.Ser1118Phe details
Hence currents at each potential were averaged over two time periods: either the first FIGURE 6 Mutation
S1118F
has mild effects on blockade by DPC.
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204
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:204:16
status:
NEW
view ABCC7 p.Ser1118Phe details
(B) Currents in
S1118F
-CFTR-expressing oocytes, showing pronounced relaxations at depolarizing test potentials.
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206
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 10866956:206:0
status:
NEW
view ABCC7 p.Ser1118Ala details
S1118A
-CFTR channels did not indicate time dependence with this protocol (not shown).
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207
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:207:36
status:
NEW
view ABCC7 p.Ser1118Phe details
Note the prominent tail currents in
S1118F
-CFTR but not in WT.
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220
ABCC7 p.Arg347Asp
X
ABCC7 p.Arg347Asp 10866956:220:147
status:
NEW
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This was initially attributed to interaction of this anion with R347 at the cytoplasmic end of TM6 in CFTR, based upon the loss of iodide block in
R347D
-CFTR.
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235
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:235:84
status:
NEW
view ABCC7 p.Ser1118Phe details
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 10866956:235:117
status:
NEW
view ABCC7 p.Ser1118Ala details
Data are shown for both instantaneous currents and steady-state currents for WT and
S1118F
-CFTR (Fig. 8, A and B) or
S1118A
-CFTR (Fig. 8, C and D).
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236
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:236:189
status:
NEW
view ABCC7 p.Ser1118Phe details
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 10866956:236:252
status:
NEW
view ABCC7 p.Ser1118Ala details
In Clafa; -containing solutions, before anion substitutions were made, there was a significant difference (p afd; 0.047) between instantaneous and steady-state reversal potentials in
S1118F
-CFTR (Table 2) compared to the WT (Table 1), but not in
S1118A
-CFTR.
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237
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:237:19
status:
NEW
view ABCC7 p.Ser1118Phe details
This suggests that
S1118F
-CFTR channels may be less Clafa; -selective than are WT channels.
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238
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:238:37
status:
NEW
view ABCC7 p.Ser1118Phe details
Comparing the selectivity pattern in
S1118F
-CFTR with that of WT, without respect to time dependence, showed significant changes for both relative permeabilities and relative conductances (compare Tables 1 and 2).
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239
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:239:143
status:
NEW
view ABCC7 p.Ser1118Phe details
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 10866956:239:132
status:
NEW
view ABCC7 p.Ser1118Ala details
The ability of the large anions (acetate, gluconate, glutamate, and isethionate) to gain access to the pore is altered by mutations
S1118A
and
S1118F
, as indicated by mild to significant changes in relative permeabilities for these anions compared to that in WT channels.
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242
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 10866956:242:0
status:
NEW
view ABCC7 p.Ser1118Ala details
S1118A
-CFTR exhibited reduced relative permeabilities for all of the large anions and for perchlorate.
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246
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:246:23
status:
NEW
view ABCC7 p.Ser1118Phe details
Accordingly, GX/GCl in
S1118F
-CFTR showed dramatic changes for seven of the nine test anions (Fig. 8 B).
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247
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:247:77
status:
NEW
view ABCC7 p.Ser1118Phe details
Relative conductances for the large anions were altered substantially in the
S1118F
-CFTR.
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249
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:249:0
status:
NEW
view ABCC7 p.Ser1118Phe details
S1118F
-CFTR also exhibited less block by iodide and thiocyanate, consistent with disruption of the high-affinity binding of these anions in the WT pore.
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250
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:250:74
status:
NEW
view ABCC7 p.Ser1118Phe details
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 10866956:250:54
status:
NEW
view ABCC7 p.Ser1118Ala details
Relative conductances were generally less affected in
S1118A
-CFTR than in
S1118F
-CFTR.
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251
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 10866956:251:22
status:
NEW
view ABCC7 p.Ser1118Ala details
In contrast, mutation
S1118A
had the greatest effects on PX/PCl relationships, particularly for the large polyatomic anions (Fig. 8, C and D).
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252
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:252:53
status:
NEW
view ABCC7 p.Ser1118Phe details
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 10866956:252:79
status:
NEW
view ABCC7 p.Ser1118Ala details
FIGURE 8 Selectivity data for WT CFTR as compared to
S1118F
-CFTR (A and B) and
S1118A
-CFTR (C and D).
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260
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:260:25
status:
NEW
view ABCC7 p.Ser1118Phe details
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 10866956:260:59
status:
NEW
view ABCC7 p.Ser1118Ala details
&#a7; p b0d; 0.01 for
S1118F
-CFTR or p afd; 0.02 for
S1118A
-CFTR.
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263
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:263:35
status:
NEW
view ABCC7 p.Ser1118Phe details
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 10866956:263:61
status:
NEW
view ABCC7 p.Ser1118Ala details
Nor does relative permeability for
S1118F
-CFTR (Fig. 8 A) or
S1118A
-CFTR (Fig. 8 C) show any time dependence.
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264
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:264:101
status:
NEW
view ABCC7 p.Ser1118Phe details
However, relative conductances for the largest anions studied (gluconate and glutamate) decreased in
S1118F
-CFTR during the 75-ms voltage jump (Fig. 8 B;&#a7; indicates p b0d; 0.01).
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265
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:265:25
status:
NEW
view ABCC7 p.Ser1118Phe details
Because these effects in
S1118F
-CFTR were only found for the largest anions tested, we propose that this result signifies a time-dependent change in the diameter of the narrowest part of the pore. We would expect this difference to be magnified in experiments in which Clafa; was replaced entirely with glutamate or gluconate (Khakh and Lester, 1999).
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267
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 10866956:267:124
status:
NEW
view ABCC7 p.Ser1118Ala details
As shown in Fig. 8 D, there was also a statistically significant time dependence of relative conductance to perchlorate for
S1118A
-CFTR (p afd; 0.02).
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269
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:269:122
status:
NEW
view ABCC7 p.Ser1118Phe details
Fig. 9 shows the current-voltage relations in the presence of chloride and glutamate for one representative experiment in
S1118F
-CFTR.
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274
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:274:141
status:
NEW
view ABCC7 p.Ser1118Phe details
Based upon the following observations, we reasoned that there may be a structural connection between the changes in permeation properties of
S1118F
-CFTR and the process underlying the voltage jump relaxations: 1) The change in permeation properties after a voltage jump (Figs. 1 and 9) is consistent with the steady-state kinetics of single channels (Fig. 5).
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278
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:278:98
status:
NEW
view ABCC7 p.Ser1118Phe details
To address this issue, we asked whether there is any interaction between permeation and gating in
S1118F
-CFTR channels studied under whole-cell conditions.
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280
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:280:121
status:
NEW
view ABCC7 p.Ser1118Phe details
Current-voltage relations in chloride and glutamate for instantaneous currents (--) and steady-state currents (- - -) in
S1118F
-CFTR were adjusted on the voltage axis so that their reversal potentials were set to zero.
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284
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:284:23
status:
NEW
view ABCC7 p.Ser1118Phe details
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:284:55
status:
NEW
view ABCC7 p.Ser1118Phe details
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 10866956:284:39
status:
NEW
view ABCC7 p.Ser1118Ala details
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 10866956:284:62
status:
NEW
view ABCC7 p.Ser1118Ala details
TABLE 2 Selectivity in
S1118F
-CFTR and
S1118A
-CFTR Ion
S1118F
S1118A
Erev (mV) PX/PCl GX/GCl Erev (mV) PX/PCl GX/GCl SCN afa;40.97 afe; 1.20* 1.84 afe; 0.08* 0.57 afe; 0.02* afa;56.44 afe; 0.93 2.59 afe; 0.09 0.20 afe; 0.01 NO3 afa;32.83 afe; 1.69 1.30 afe; 0.06 0.95 afe; 0.02 afa;37.35 afe; 0.87 1.21 afe; 0.04 0.88 afe; 0.01 Br afa;28.28 afe; 1.32 1.07 afe; 0.03 0.88 afe; 0.03* afa;34.53 afe; 0.85 1.12 afe; 0.02 0.77 afe; 0.01 Cl afa;26.14 afe; 1.59* 1.0 1.0 afa;30.63 afe; 0.64 1.0 1.0 I afa;8.46 afe; 1.14 0.52 afe; 0.03* 0.38 afe; 0.03* afa;10.35 afe; 1.26 0.39 afe; 0.01 0.27 afe; 0.05 Acetate 39.64 afe; 1.77* 0.05 afe; 0.01* 0.12 afe; 0.01* 23.24 afe; 1.83* 0.09 afe; 0.01* 0.50 afe; 0.01* Glutamate 23.93 afe; 3.61* 0.16 afe; 0.01* 0.23 afe; 0.01* 19.59 afe; 1.07* 0.09 afe; 0.01* 0.49 afe; 0.01* 0.32 afe; 0.01I * Isethionate 20.24 afe; 3.62* 0.14 afe; 0.03 0.25 afe; 0.02* 23.71 afe; 0.99* 0.09 afe; 0.01* 0.48 afe; 0.01 ClO4 afa;6.42 afe; 1.57* 0.42 afe; 0.02* 0.18 afe; 0.01 27.29 afe; 1.36* 0.06 afe; 0.01* 0.12 afe; 0.01* 0.14 afe; 0.01I * Gluconate 28.26 afe; 3.29* 0.12 afe; 0.02 0.20 afe; 0.01* 20.03 afe; 1.04* 0.10 afe; 0.01* 0.50 afe; 0.01* 0.27 afe; 0.01I * Ions are listed in the same order as in Table 1.
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288
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:288:6
status:
NEW
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WT or
S1118F
-CFTR channels were studied using the same voltage-clamp protocol as the one used for the data shown in Fig. 7.
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295
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:295:0
status:
NEW
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S1118F
-CFTR currents showed a relaxation as expected from previous experiments (Figs. 1, 2, and 7).
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298
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:298:114
status:
NEW
view ABCC7 p.Ser1118Phe details
Because SCNafa; blocks mutant channels as it does WT channels (Table 2), we would expect the time constant for
S1118F
-CFTR channels in the presence of SCNafa; to be reduced as it is for WT channels.
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299
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:299:32
status:
NEW
view ABCC7 p.Ser1118Phe details
In contrast, the relaxations in
S1118F
-CFTR were slowed by this less permeant anion such that the process underlying the relaxations was not complete even by the end of the 75-ms voltage jump.
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304
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:304:76
status:
NEW
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In summary, the lengthening of the gating process at positive potentials in
S1118F
-CFTR follows the relative conductance sequence.
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306
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:306:68
status:
NEW
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This implies a distinct connection between permeation and gating in
S1118F
-CFTR.
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314
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:314:49
status:
NEW
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(C) Time constants for the relaxations in WT and
S1118F
-CFTR channels were calculated by fitting the decay to an exponential function.
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315
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:315:43
status:
NEW
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Shown are the time constants () for
S1118F
-CFTR currents recorded in bath solution containing Clafa; , Brafa; , or SCNafa; .
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316
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:316:13
status:
NEW
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surements in
S1118F
-CFTR show modest current relaxations, on the order of 30%, during voltage jumps between afa;140 and af9;80 mV.
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321
ABCC7 p.Arg347Asp
X
ABCC7 p.Arg347Asp 10866956:321:135
status:
NEW
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Anomalous mole fraction effects (Tabcharani et al., 1993) and protocol-dependent block by iodide (Tabcharani et al., 1997) are lost in
R347D
-CFTR; this may be due to a severe disruption in secondary structure by the loss of a salt bridge between R347 and D924 (Cotten and Welsh, 1999).
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334
ABCC7 p.Thr1134Phe
X
ABCC7 p.Thr1134Phe 10866956:334:24
status:
NEW
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In particular, mutation
T1134F
in TM12 lowered single-channel conductance to b03;6 pS and increased DPC affinity without changing the voltage dependence of block (McDonough et al., 1994).
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335
ABCC7 p.Ser341Ala
X
ABCC7 p.Ser341Ala 10866956:335:9
status:
NEW
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Mutation
S341A
in TM6 reduced affinity for DPC fivefold, induced inward rectification, and decreased the single-channel conductance to b03;1 pS (McDonough et al., 1994).
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338
ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 10866956:338:9
status:
NEW
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Mutation
T338A
altered the voltage dependence of block by DPC without affecting affinity at afa;100 mV (McDonough et al., 1994).
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343
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:343:30
status:
NEW
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ABCC7 p.Thr338Ala
X
ABCC7 p.Thr338Ala 10866956:343:74
status:
NEW
view ABCC7 p.Thr338Ala details
With respect to block by DPC,
S1118F
-CFTR had an effect much like that of
T338A
-CFTR, wherein affinity at afa;100 mV was not changed significantly but the voltage dependence was reduced.
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344
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:344:92
status:
NEW
view ABCC7 p.Ser1118Phe details
The absolute difference in the apparent KD (at afa;100 mV) for DPC between wild type and
S1118F
-CFTR, taken by itself, is too small to conclude that residue S1118 lines the channel pore.
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345
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 10866956:345:11
status:
NEW
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Similarly,
S1118A
did not affect block by DPC (McDonough et al., 1994).
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346
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:346:30
status:
NEW
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ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 10866956:346:14
status:
NEW
view ABCC7 p.Ser1118Ala details
However, both
S1118A
-CFTR and
S1118F
-CFTR altered the selectivity behavior of the pore, suggesting that this position may contribute to the pore walls.
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347
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:347:72
status:
NEW
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Relative conductances for many of the substitute anions were altered in
S1118F
-CFTR.
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348
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 10866956:348:22
status:
NEW
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In contrast, mutation
S1118A
exhibited the greatest effects on relative permeabilities, especially for the large anions.
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353
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:353:13
status:
NEW
view ABCC7 p.Ser1118Phe details
Furthermore,
S1118F
-CFTR also exhibits a reduced single-channel conductance.
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365
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:365:0
status:
NEW
view ABCC7 p.Ser1118Phe details
S1118F
-CFTR single channels differ doubly from wild-type channels.
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366
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:366:7
status:
NEW
view ABCC7 p.Ser1118Phe details
First,
S1118F
-CFTR openings are much briefer than wild-type openings (burst duration is reduced by 93%).
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367
ABCC7 p.Arg117His
X
ABCC7 p.Arg117His 10866956:367:71
status:
NEW
view ABCC7 p.Arg117His details
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:367:21
status:
NEW
view ABCC7 p.Ser1118Phe details
The choppy bursts of
S1118F
-CFTR closely resemble the bursts of mutant
R117H
, a mutation that causes mild cystic fibrosis (Sheppard et al., 1993).
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368
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:368:42
status:
NEW
view ABCC7 p.Ser1118Phe details
Second, the single-channel conductance of
S1118F
-CFTR rectifies inwardly, in agreement with the steady-state rectification of macroscopic currents.
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369
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:369:65
status:
NEW
view ABCC7 p.Ser1118Phe details
The rectification of single-channel steady-state conductance for
S1118F
-CFTR arises primarily from decreased conductance at positive potentials, because the single-channel conductances for the WT and mutant are nearly equal at afa;100 mV but differ at af9;100 mV.
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371
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:371:5
status:
NEW
view ABCC7 p.Ser1118Phe details
That
S1118F
-CFTR has more defective conduction properties for positive current at depolarizing potentials (i.e., for inward flux of Clafa; ) suggests that the mutated residue affects the channel at a point nearer the extracellular than the cytoplasmic end of the channel.
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375
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:375:26
status:
NEW
view ABCC7 p.Ser1118Phe details
The shortened openings in
S1118F
-CFTR may reflect a destabilization of the global protein structure rather than a specific effect on the pore.
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377
ABCC7 p.Ser1118Ala
X
ABCC7 p.Ser1118Ala 10866956:377:166
status:
NEW
view ABCC7 p.Ser1118Ala details
Similarly, the current relaxations are not due to disruption of a putative interaction between S1118 and another amino acid, because no relaxations were observed for
S1118A
-CFTR.
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383
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:383:43
status:
NEW
view ABCC7 p.Ser1118Phe details
The single-channel recordings confirm that
S1118F
-CFTR openings are interrupted to a much greater extent than wild-type openings.
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389
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:389:157
status:
NEW
view ABCC7 p.Ser1118Phe details
Thus there is no reason to suspect that the relaxations are produced by voltage-dependent blocking events, and we tentatively favor the explanation that the
S1118F
-CFTR has altered gating kinetics.
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391
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:391:75
status:
NEW
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Although an additional state may have been added to the kinetic scheme for
S1118F
-CFTR, it is also possible that an existing state has been modified.
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392
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:392:162
status:
NEW
view ABCC7 p.Ser1118Phe details
For instance, it will be important to determine if the prominent voltage-dependent fast flicker in WT observed at hyperpolarizing potentials is modified by the
S1118F
mutation.
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393
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:393:20
status:
NEW
view ABCC7 p.Ser1118Phe details
Possible mechanisms
S1118F
-CFTR exhibits alterations in permeation properties, as might be expected given the location of this mutation, but also exhibits alterations in single-channel gating.
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397
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:397:54
status:
NEW
view ABCC7 p.Ser1118Phe details
It seems more likely that a unique process occurs for
S1118F
-CFTR.
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401
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:401:35
status:
NEW
view ABCC7 p.Ser1118Phe details
At the other end of the scale, the
S1118F
mutation might disrupt the stability of the protein global structure, leading to the observed effects on conduction.
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405
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:405:32
status:
NEW
view ABCC7 p.Ser1118Phe details
The relative conductance of the
S1118F
-CFTR channel to large anions decreases during the course of the relaxations, which may indicate that either the large anions are more capable of blocking the channels in the steady-state conformation, or that Clafa; permeation becomes blocked by an intrinsic portion of the protein in the steady-state conformation.
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418
ABCC7 p.Ser1118Phe
X
ABCC7 p.Ser1118Phe 10866956:418:4
status:
NEW
view ABCC7 p.Ser1118Phe details
The
S1118F
mutation may provide this reporter group in the form of the Phe side chain and/or slow the relaxations to a rate that is resolvable in macroscopic recordings.
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