PMID: 22923500

Norimatsu Y, Ivetac A, Alexander C, O'Donnell N, Frye L, Sansom MS, Dawson DC
Locating a Plausible Binding Site for an Open Channel Blocker, GlyH-101, in the Pore of the Cystic Fibrosis Transmembrane Conductance Regulator.
Mol Pharmacol. 2012 Aug 24., [PubMed]
Sentences
No. Mutations Sentence Comment
7 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:7:112
status: NEW
view ABCC7 p.Phe342Ala details
A molecular mechanics-generalized Born/surface area analysis of GlyH-101 binding predicted that substitution of Phe342 with alanine would substantially increase blocker affinity, primarily because of decreased intramolecular strain within the blocker-protein complex. Login to comment
51 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:51:17
status: NEW
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The structure of F342A CFTR was generated by replacing F342 of wt CFTR from the predicted complex with alanine in Maestro (version 9.1, Schrödinger LLC). Login to comment
52 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:52:44
status: NEW
view ABCC7 p.Phe342Ala details
GlyH-101 was docked to the structure of the F342A CFTR using the IFD protocol and the structure of the resulting complex was used for MM-GB/SA analysis (see Binding Free Energy Calculation for more details). Login to comment
73 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:73:21
status: NEW
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The structure of the F342A CFTR was generated with Maestro 9.1 by replacing Phe342 of the wt CFTR in the predicted complex with alanine. Login to comment
74 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:74:44
status: NEW
view ABCC7 p.Phe342Ala details
GlyH-101 was docked to the structure of the F342A CFTR by using the IFD protocol, and the structure of the resulting complex was used for MM-GB/SA analysis (see Calculation of Binding Free Energy for more details). Login to comment
108 ABCC7 p.Phe337Cys
X
ABCC7 p.Phe337Cys 22923500:108:64
status: NEW
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In this example, externally-applied [Au(CN)2]- was reacted with F337C CFTR. Login to comment
115 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:115:89
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Phe337Cys
X
ABCC7 p.Phe337Cys 22923500:115:79
status: NEW
view ABCC7 p.Phe337Cys details
Figure 3C and 3D contain the time courses for the reactions of [Au(CN)2]- with F337C and T338C CFTR pre-and post-activation. Login to comment
116 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:116:15
status: NEW
view ABCC7 p.Thr338Cys details
In the case of T338C CFTR, different concentrations of [Au(CN)2]- were used to construct the time course (50 µM for the pre-activation rate; 5 µM for the post-activation rate), in order to compensate for the slower reaction rate in the pre-activation condition. Login to comment
125 ABCC7 p.Arg334Cys
X
ABCC7 p.Arg334Cys 22923500:125:80
status: NEW
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Figure 4 shows the time courses for the reactions of [Au(CN)2]- and MTSET+ with R334C CFTR channels. Login to comment
127 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:127:22
status: NEW
view ABCC7 p.Thr338Cys details
When either Phe337 or Thr338 was replaced with cysteine, the EC50 for GlyH-101 blockade at 0 mV was only modestly increased (Table 1).1 Increasing the bulk of either cysteine side chain through alkylation with iodoacetamide further increased the EC50(0) b03;6-fold for position 338 but only 1.3-fold for position 337. Login to comment
130 ABCC7 p.Arg334Cys
X
ABCC7 p.Arg334Cys 22923500:130:33
status: NEW
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ABCC7 p.Lys95Cys
X
ABCC7 p.Lys95Cys 22923500:130:10
status: NEW
view ABCC7 p.Lys95Cys details
Beck et al., (2008) also studied R334C CFTR channels expressed in Xenopus oocytes using a protocol similar to that employed here, but failed to detect increased reactivity toward externally-applied MTSEA+ in the activated state. Login to comment
138 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:138:157
status: NEW
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Figure 5A contains a representative time course showing the cumulative effect of 30 s and 1 min applications of 5 µM [Au(CN)2]- to an oocyte expressing T338C CFTR. Login to comment
140 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:140:97
status: NEW
view ABCC7 p.Thr338Cys details
Inspection of the response to the first, 30s exposure reveals that the extent of modification of T338C conductance by [Au(CN)2]- was markedly reduced when the reagent was applied in the presence of the blocker. Login to comment
141 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:141:60
status: NEW
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ABCC7 p.Phe337Cys
X
ABCC7 p.Phe337Cys 22923500:141:45
status: NEW
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Figure 5C and 5D summarize the inhibition of F337C CFTR and T338C CFTR by [Au(CN)2]- in the presence and in the absence of GlyH-101. Login to comment
144 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:144:100
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Phe337Cys
X
ABCC7 p.Phe337Cys 22923500:144:90
status: NEW
view ABCC7 p.Phe337Cys details
In Figure 5E and 5F the measured second order rate constants for covalent modification of F337C and T338C CFTR are plotted versus GlyH-101 concentration. Login to comment
148 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:148:83
status: NEW
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As a test for the role of charge-charge interactions we compared the protection of T338C CFTR against reaction with MTSET+ and MTSES- . Login to comment
149 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:149:45
status: NEW
view ABCC7 p.Thr338Cys details
The results summarized in Figure 6 show that T338C is protected by GlyH-101 from negatively-charged MTSES- but not from positively-charged MTSET+ , indicating that the charge on the blocker is a major determinant of the protection effect at this position. Login to comment
151 ABCC7 p.Phe337Cys
X
ABCC7 p.Phe337Cys 22923500:151:74
status: NEW
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ABCC7 p.Ile1131Cys
X
ABCC7 p.Ile1131Cys 22923500:151:32
status: NEW
view ABCC7 p.Ile1131Cys details
We also studied the reaction of I1131C CFTR with MTSES- . Login to comment
154 ABCC7 p.Ile1131Cys
X
ABCC7 p.Ile1131Cys 22923500:154:25
status: NEW
view ABCC7 p.Ile1131Cys details
ABCC7 p.Ile1131Cys
X
ABCC7 p.Ile1131Cys 22923500:154:106
status: NEW
view ABCC7 p.Ile1131Cys details
In fact, no occlusion of I1131C was observed with 10 µM GlyH-101, despite more than 80% block of the I1131C CFTR current. Login to comment
155 ABCC7 p.Ile1131Cys
X
ABCC7 p.Ile1131Cys 22923500:155:40
status: NEW
view ABCC7 p.Ile1131Cys details
The rate of reaction between MTSES- and I1131C CFTR was actually somewhat greater in the presence of GlyH-101 (Figure 7A). Login to comment
156 ABCC7 p.Ile1131Cys
X
ABCC7 p.Ile1131Cys 22923500:156:44
status: NEW
view ABCC7 p.Ile1131Cys details
The reaction rates of charged reagents with I1131C CFTR would be influenced by relative positions of nearby charges, which may change slightly in the event of binding of GlyH-101. Login to comment
158 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:158:102
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:158:444
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:158:481
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Lys95Cys
X
ABCC7 p.Lys95Cys 22923500:158:312
status: NEW
view ABCC7 p.Lys95Cys details
ABCC7 p.Phe337Cys
X
ABCC7 p.Phe337Cys 22923500:158:92
status: NEW
view ABCC7 p.Phe337Cys details
ABCC7 p.Phe337Cys
X
ABCC7 p.Phe337Cys 22923500:158:348
status: NEW
view ABCC7 p.Phe337Cys details
ABCC7 p.Phe337Cys
X
ABCC7 p.Phe337Cys 22923500:158:385
status: NEW
view ABCC7 p.Phe337Cys details
Figure 3, C and D, contains the time courses for the reactions of [Au(CN)2]afa; with the F337C and T338C CFTRs before TABLE 1 EC50 at 0 mV (mean afe; S.E.M.) for GlyH-101 for wt and mutant CFTRs, with and without modification with iodoacetamide CFTR EC50 at 0 mV òe;M wt 1.1 afe; 0.11 (n afd; 4) K95C 1.4 afe; 0.35 (n afd; 4) F337C 1.8 afe; 0.06 (n afd; 3) F337C af9; iodoacetamide 2.4 afe; 0.29 (n afd; 3) T338C 3.7 afe; 0.27 (n afd; 3) T338C af9; iodoacetamide 24 afe; 2.6 (n afd; 3) Fig. 3. Login to comment
159 ABCC7 p.Phe337Cys
X
ABCC7 p.Phe337Cys 22923500:159:34
status: NEW
view ABCC7 p.Phe337Cys details
ABCC7 p.Ile1131Cys
X
ABCC7 p.Ile1131Cys 22923500:159:93
status: NEW
view ABCC7 p.Ile1131Cys details
The presence of negative charges near I1131 is consistent with the observed slow reaction of I1131C CFTR with MTSES- (20 M-1 sec-1 ; Figure 7) which is more than 100-fold less than that seen for a Cys at 338 (3.3 x 103 M-1 sec-1 ; Figure 6). Login to comment
160 ABCC7 p.Phe337Cys
X
ABCC7 p.Phe337Cys 22923500:160:147
status: NEW
view ABCC7 p.Phe337Cys details
ABCC7 p.Phe337Cys
X
ABCC7 p.Phe337Cys 22923500:160:270
status: NEW
view ABCC7 p.Phe337Cys details
ABCC7 p.Ile1131Cys
X
ABCC7 p.Ile1131Cys 22923500:160:79
status: NEW
view ABCC7 p.Ile1131Cys details
As reported previously (Norimatsu et al., 2012) the macroscopic conductance of I1131C CFTR was increased by depositing the negatively charged sulfonic acid group via reaction with MTSES- . Login to comment
161 ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22923500:161:132
status: NEW
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ABCC7 p.Ile1131Cys
X
ABCC7 p.Ile1131Cys 22923500:161:82
status: NEW
view ABCC7 p.Ile1131Cys details
This result is most likely a reflection of an increase in the open probability of I1131C CFTR channels similar to that observed for R352C CFTR by Bai et al., (2010). Login to comment
162 ABCC7 p.Phe337Cys
X
ABCC7 p.Phe337Cys 22923500:162:75
status: NEW
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The subsequent application of [Au(CN)2]afa; almost completely abolished F337C CFTR conductance. Login to comment
163 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:163:94
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Phe337Cys
X
ABCC7 p.Phe337Cys 22923500:163:80
status: NEW
view ABCC7 p.Phe337Cys details
C and D, time courses of the decreases in normalized conductance as a result of F337C (C) and T338C (D) modifications with [Au(CN)2]afa; . Login to comment
164 ABCC7 p.Ser341Cys
X
ABCC7 p.Ser341Cys 22923500:164:0
status: NEW
view ABCC7 p.Ser341Cys details
S341C CFTR is reactive toward channel permeant reagents, like [Ag(CN)2]- , but the reactions are not irreversible at this position, a requirement for implementation of the post-GlyH-101 washout protocol. Login to comment
165 ABCC7 p.Phe337Cys
X
ABCC7 p.Phe337Cys 22923500:165:8
status: NEW
view ABCC7 p.Phe337Cys details
For the F337C CFTR, the abscissa represents cumulative [Au(CN)2]afa; exposure time. Login to comment
166 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:166:8
status: NEW
view ABCC7 p.Thr338Cys details
For the T338C CFTR, the abscissa represents cumulative [Au(CN)2]afa; exposure (exposure time afb; [Au(CN)2]afa; concentration used). Login to comment
167 ABCC7 p.Phe337Cys
X
ABCC7 p.Phe337Cys 22923500:167:26
status: NEW
view ABCC7 p.Phe337Cys details
The reaction rate for the F337C CFTR before activation of the channels was b03;20 times slower than the rate after activation. Login to comment
168 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:168:17
status: NEW
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The rate for the T338C CFTR was almost 30 times slower before activation. Login to comment
170 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:170:58
status: NEW
view ABCC7 p.Phe342Ala details
The EC50 of GlyH-101 is reduced approximately 200-fold in F342A CFTR The binding pose predicted for GlyH-101 drew our attention to another residue predicted to lie within the pore bottleneck, F342. Login to comment
171 ABCC7 p.Phe337Cys
X
ABCC7 p.Phe337Cys 22923500:171:49
status: NEW
view ABCC7 p.Phe337Cys details
The second-order reaction rate constants for the F337C CFTR before and after activation were 1.5 and 26 Mafa;1 safa;1 , respectively. Login to comment
172 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:172:49
status: NEW
view ABCC7 p.Thr338Cys details
The second-order reaction rate constants for the T338C CFTR before and after activation were 1.2 afb; 102 and 3.0 afb; 103 Mafa;1 safa;1 , respectively. Login to comment
174 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:174:19
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:174:42
status: NEW
view ABCC7 p.Phe342Ala details
We analyzed GlyH-101 binding to wt and F342A CFTR channels using the MM-GB/SA method as described by Guimaraes and Cardozo, (2008). Login to comment
175 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:175:41
status: NEW
view ABCC7 p.Phe342Ala details
In order to predict the structure of the F342A CFTR/GlyH-101 complex, the phenylalanine at position 342 of wt CFTR was mutated to alanine in silico (see Methods) and GlyH-101 was docked to the mutant CFTR using IFD (supplemental PDB file 3). Login to comment
177 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:177:42
status: NEW
view ABCC7 p.Phe342Ala details
The estimated parameter values for wt and F342A are collected in Table 2. Login to comment
178 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:178:105
status: NEW
view ABCC7 p.Phe342Ala details
ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:178:142
status: NEW
view ABCC7 p.Phe342Ala details
The calculation predicts that the free energy of binding of GlyH-101, ΔGbind, is more negative for F342A CFTR than for wt CFTR, that is F342A CFTR binds GlyH-101 more tightly than does wt CFTR. Login to comment
179 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:179:193
status: NEW
view ABCC7 p.Phe342Ala details
Decomposition of the total binding free energy according to the terms listed in Equation 1 reveals that the predicted energy difference arises mainly from reduction of the strain energy of the F342A CFTR (EPTN), consistent with the notion that the side chain of F342 in the wt CFTR channel causes an unfavorable steric clash with GlyH-101. Login to comment
181 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:181:124
status: NEW
view ABCC7 p.Phe342Ala details
The calculated free energies of GlyH-101 binding were -7.43 and -8.54 kcal/mol for wt CFTR and -11.8 and -12.6 kcal/mol for F342A CFTR with and without the membrane respectively. Login to comment
182 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:182:82
status: NEW
view ABCC7 p.Phe342Ala details
The experimental results collected in Figure 8A show that dose-dependent block of F342A CFTR by GlyH-101, as predicted by the MM-GB/SA analysis, exhibited an EC50(0) that was dramatically reduced (5.2 ± 0.83 nM; n = 3) compared to that of wt CFTR (1.1 ± 0.11 µM; n = 4; Figure 1C), consistent with a substantial increase in binding affinity for the blocker that was brought about by eliminating the bulky phenylalanine side chain. Login to comment
183 ABCC7 p.Arg334Cys
X
ABCC7 p.Arg334Cys 22923500:183:92
status: NEW
view ABCC7 p.Arg334Cys details
ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:183:46
status: NEW
view ABCC7 p.Phe342Ala details
The substantially higher apparent affinity of F342A CFTR for GlyH-101 implies a dramatic slowing of the off-rate for the bound blocker. Login to comment
188 ABCC7 p.Arg334Cys
X
ABCC7 p.Arg334Cys 22923500:188:27
status: NEW
view ABCC7 p.Arg334Cys details
Beck et al. (2008) studied R334C CFTR channels expressed in X. laevis oocytes by using a protocol similar to that used here, but they failed to detect increased reactivity toward externally applied 2-aminoethylmethanethiosulfonate in the activated state. Login to comment
196 ABCC7 p.Arg334Cys
X
ABCC7 p.Arg334Cys 22923500:196:29
status: NEW
view ABCC7 p.Arg334Cys details
Time courses of reactions of R334C (an engineered cysteine at position 334) with 10 òe;M [Au(CN)2]afa; (A) or 250 nM MTSETaf9; (B). Login to comment
197 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:197:111
status: NEW
view ABCC7 p.Phe342Ala details
ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:197:241
status: NEW
view ABCC7 p.Phe342Ala details
ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:197:296
status: NEW
view ABCC7 p.Phe342Ala details
Using their data, the k`on for wt CFTR was calculated to be 1.6 x 107 M-1 s-1 , a value similar to the k`on of F342A CFTR (2.3 × 107 M-1 s-1 ) determined in the current study, again indicating that the difference in EC50 between wt and F342A CFTR is due to the slow off rate of GlyH-101 for F342A CFTR. Login to comment
198 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:198:130
status: NEW
view ABCC7 p.Phe342Ala details
The binding free energy based on the observed EC50, estimated as RTln(EC50), is -8.12 kcal/mol for wt CFTR and -11.3 kcal/mol for F342A CFTR. Login to comment
199 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:199:212
status: NEW
view ABCC7 p.Phe342Ala details
These empirical values are qualitatively consistent with the computed free energies, obtained with the MM-GB/SA technique using the proposed model of GlyH-101 binding (Figure 2), for wt CFTR (-7.43 kcal/mol) and F342A CFTR (-11.8 kcal/mol). Login to comment
201 ABCC7 p.Arg334Cys
X
ABCC7 p.Arg334Cys 22923500:201:71
status: NEW
view ABCC7 p.Arg334Cys details
For both [Au(CN)2]afa; and MTSETaf9; , the reaction rate for the R334C CFTR before activation of the channels was faster than the rate after activation. Login to comment
204 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:204:78
status: NEW
view ABCC7 p.Thr338Cys details
and 1-min applications of 5 òe;M [Au(CN)2]afa; to an oocyte expressing T338C CFTR. Login to comment
205 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:205:340
status: NEW
view ABCC7 p.Thr338Cys details
A similar procedure, in which [Au(CN)2]afa; was applied during brief exposures of the oocyte to GlyH-101 and the extent of the reaction was estimated from the conductance recovered after washout of the blocker, is illustrated in Fig. 5B. Inspection of the response to the first, 30-s exposure revealed that the extent of modification of T338C CFTR conductance by [Au(CN)2]afa; was markedly reduced when the reagent was applied in the presence of the blocker. Login to comment
206 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:206:62
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Phe337Cys
X
ABCC7 p.Phe337Cys 22923500:206:52
status: NEW
view ABCC7 p.Phe337Cys details
Figure 5, C and D, summarizes the inhibition of the F337C and T338C CFTRs by [Au(CN)2]afa; in the presence and absence of GlyH-101. Login to comment
209 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:209:22
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:209:104
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Phe337Cys
X
ABCC7 p.Phe337Cys 22923500:209:94
status: NEW
view ABCC7 p.Phe337Cys details
Second, alkylation of T338C CFTR with IAM, which results in covalent addition of an acetamide moiety predicted by the model to create a steric clash with GlyH-101, significantly reduced the apparent binding affinity of GlyH-101. Login to comment
210 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:210:23
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Phe337Cys
X
ABCC7 p.Phe337Cys 22923500:210:27
status: NEW
view ABCC7 p.Phe337Cys details
In contrast, alkylation of F337C CFTR with IAM is not predicted by the molecular model to cause a steric clash and does not markedly alter GlyH-101 block. Login to comment
211 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:211:145
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:211:167
status: NEW
view ABCC7 p.Phe342Ala details
Finally, when a predicted steric clash between the side chain of F342 and the naphthalene tail of the bound blocker was removed by mutating the residue to an alanine (F342A), the apparent blocker affinity was increased by more than 200-fold, a change that was consistent with free energies of binding estimated using a MM-GB/SA approach. Login to comment
215 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:215:23
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Phe337Cys
X
ABCC7 p.Phe337Cys 22923500:215:9
status: NEW
view ABCC7 p.Phe337Cys details
C and D, F337C (C) and T338C (D) CFTR channels were protected by 10 òe;M GlyH-101 from reactions with [Au(CN)2]afa; . Login to comment
217 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:217:70
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Phe337Cys
X
ABCC7 p.Phe337Cys 22923500:217:4
status: NEW
view ABCC7 p.Phe337Cys details
The F337C CFTR was reacted with 600 òe;M [Au(CN)2]afa; and the T338C CFTR was reacted with 5 òe;M [Au(CN)2]afa; in the presence and absence of 10 òe;M GlyH-101. Login to comment
220 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:220:34
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:220:70
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:220:203
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:220:231
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Glu1371Gln
X
ABCC7 p.Glu1371Gln 22923500:220:209
status: NEW
view ABCC7 p.Glu1371Gln details
ABCC7 p.Phe337Cys
X
ABCC7 p.Phe337Cys 22923500:220:56
status: NEW
view ABCC7 p.Phe337Cys details
The state-dependent reactivity of T338C CFTR observed in the current study is consistent with the finding of Beck et al., (2008) that MTSES- reacts slightly faster with a high open probability mutant T338C/E1371Q CFTR than with T338C/wt CFTR.2 Mornon et al., (2009) created a homology model of CFTR based on the inward-facing conformation of a prokaryotic transporter, MsbA (Ward et al., 2007) (PDB code: 3B5X). Login to comment
224 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:224:106
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Phe337Cys
X
ABCC7 p.Phe337Cys 22923500:224:96
status: NEW
view ABCC7 p.Phe337Cys details
A conformational change of this sort would be consistent with the state-dependent reactivity of F337C and T338C CFTR observed in the current study. Login to comment
225 ABCC7 p.Arg334Cys
X
ABCC7 p.Arg334Cys 22923500:225:412
status: NEW
view ABCC7 p.Arg334Cys details
ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:225:137
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Phe337Cys
X
ABCC7 p.Phe337Cys 22923500:225:47
status: NEW
view ABCC7 p.Phe337Cys details
The MsbA-based model of Mornon et al., (2009) also predicts that the side chain of R334 protrudes into the external aqueous environment, and when R334 is mutated to a cysteine in the MsbA-based model of Mornon et al., (2009) using Maestro (version 9.1, Schrödinger LLC), the reactive thiolate is clearly accessible from the extracellular solution (Figure 9C), consistent with the closed state reactivity of R334C observed in the current study and by Zhang et al., (2005). Login to comment
226 ABCC7 p.Arg334Cys
X
ABCC7 p.Arg334Cys 22923500:226:46
status: NEW
view ABCC7 p.Arg334Cys details
ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:226:59
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Phe337Cys
X
ABCC7 p.Phe337Cys 22923500:226:49
status: NEW
view ABCC7 p.Phe337Cys details
On the other hand, the mechanism that renders R334C CFTR unreactive in the conducting state of CFTR is not clear. Login to comment
228 ABCC7 p.Arg334Cys
X
ABCC7 p.Arg334Cys 22923500:228:4
status: NEW
view ABCC7 p.Arg334Cys details
The R334C mutation may cause a significant conformational change to the CFTR protein (not captured in our MD simulation), as suggested by Zhou et al., (2007), that renders the engineered cysteine inaccessible in the conducting state of CFTR. Login to comment
231 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:231:88
status: NEW
view ABCC7 p.Thr338Cys details
As a test for the role of charge-charge interactions, we compared the protection of the T338C CFTR against reactions with MTSETaf9; and MTSESafa; . Login to comment
232 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:232:49
status: NEW
view ABCC7 p.Thr338Cys details
The results summarized in Fig. 6 showed that the T338C CFTR was protected by GlyH-101 from negatively charged MTSESafa; but not from positively charged MTSETaf9; , indicating that the charge on the blocker is a major determinant of the protective effect at this position. Login to comment
234 ABCC7 p.Ile1131Cys
X
ABCC7 p.Ile1131Cys 22923500:234:36
status: NEW
view ABCC7 p.Ile1131Cys details
We also studied the reaction of the I1131C CFTR with MTSESafa; . Login to comment
237 ABCC7 p.Ile1131Cys
X
ABCC7 p.Ile1131Cys 22923500:237:16
status: NEW
view ABCC7 p.Ile1131Cys details
ABCC7 p.Ile1131Cys
X
ABCC7 p.Ile1131Cys 22923500:237:101
status: NEW
view ABCC7 p.Ile1131Cys details
No occlusion of I1131C was observed with 10 òe;M GlyH-101, despite more than 80% blockade of the I1131C CFTR current. Login to comment
238 ABCC7 p.Ile1131Cys
X
ABCC7 p.Ile1131Cys 22923500:238:50
status: NEW
view ABCC7 p.Ile1131Cys details
The rate of reaction between MTSESafa; and the I1131C CFTR was actually somewhat greater in the presence of GlyH-101 (Fig. 7A). Login to comment
239 ABCC7 p.Ile1131Cys
X
ABCC7 p.Ile1131Cys 22923500:239:52
status: NEW
view ABCC7 p.Ile1131Cys details
The rates of reactions of charged reagents with the I1131C CFTR would be influenced by the relative positions of nearby charges, which might change slightly upon GlyH-101 binding. Login to comment
242 ABCC7 p.Ile1131Cys
X
ABCC7 p.Ile1131Cys 22923500:242:99
status: NEW
view ABCC7 p.Ile1131Cys details
The presence of negative charges near Ile1131 is consistent with the observed slow reaction of the I1131C CFTR with MTSESafa; (20 Mafa;1 safa;1 ) (Fig. 7), which is more than 100-fold less than the rate seen with a cysteine at position 338 (3.3 afb; 103 Mafa;1 safa;1 ) (Fig. 6). Login to comment
243 ABCC7 p.Ile1131Cys
X
ABCC7 p.Ile1131Cys 22923500:243:84
status: NEW
view ABCC7 p.Ile1131Cys details
As reported previously (Norimatsu et al., 2012), the macroscopic conductance of the I1131C CFTR was increased by deposition of the negatively charged sulfonic acid group through reaction with MTSESafa; . Login to comment
244 ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22923500:244:137
status: NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Ile1131Cys
X
ABCC7 p.Ile1131Cys 22923500:244:82
status: NEW
view ABCC7 p.Ile1131Cys details
This result is most likely a reflection of an increase in the open probability of I1131C CFTR channels, similar to that observed for the R352C CFTR (Bai et al., 2010). Login to comment
247 ABCC7 p.Ser341Cys
X
ABCC7 p.Ser341Cys 22923500:247:4
status: NEW
view ABCC7 p.Ser341Cys details
The S341C CFTR is reactive toward channel-permeant reagents such as [Ag(CN)2]afa; but the reactions at this position are not irreversible, which is a requirement for implementation of the post-GlyH-101 washout protocol. Login to comment
250 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:250:23
status: NEW
view ABCC7 p.Thr338Cys details
GlyH-101 protection of T338C (an engineered cysteine at position 338) from MTSESafa; but not from MTSETaf9; . Login to comment
251 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:251:7
status: NEW
view ABCC7 p.Thr338Cys details
A, the T338C CFTR was reacted with 5 òe;M MTSESafa; in the presence and absence of 10 òe;M GlyH-101. Data points represent mean afe; S.E.M. (n afd; 3). Login to comment
255 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:255:194
status: NEW
view ABCC7 p.Thr338Cys details
The second-order reaction rate constants for MTSESafa; in the presence and absence of 10 òe;M GlyH-101 were 1.2 afb; 103 and 3.3 afb; 103 Mafa;1 safa;1 , respectively. B, the T338C CFTR was reacted with 50 òe;M MTSETaf9; in the presence and absence of 10 òe;M GlyH-101. Data points represent mean afe; S.E.M. (n afd; 3). Login to comment
262 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:262:57
status: NEW
view ABCC7 p.Phe342Ala details
The GlyH-101 EC50 Is Reduced Approximately 200-Fold with F342A CFTR. Login to comment
267 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:267:39
status: NEW
view ABCC7 p.Phe342Ala details
We analyzed GlyH-101 binding to wt and F342A CFTR channels by using the MM-GB/SA method described by Guimara dc;es and Cardozo (2008). Login to comment
268 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:268:32
status: NEW
view ABCC7 p.Phe342Ala details
To predict the structure of the F342A CFTR-GlyH-101 complex, the phenylalanine at position 342 of the wt CFTR was mutated to alanine in silico (see Materials and Methods) and GlyH-101 was docked to the mutant CFTR by using IFD techniques (Supplemental PDB File 3). Login to comment
270 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:270:42
status: NEW
view ABCC7 p.Phe342Ala details
The estimated parameter values for wt and F342A CFTRs are presented in Table 2. Login to comment
271 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:271:111
status: NEW
view ABCC7 p.Phe342Ala details
ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:271:157
status: NEW
view ABCC7 p.Phe342Ala details
The calculations suggested that the free energy of binding of GlyH-101, èc;Gbind, is more negative for the F342A CFTR than for the wt CFTR, that is, the F342A CFTR binds GlyH-101 more tightly than does the wt CFTR. Login to comment
273 ABCC7 p.Ile1131Cys
X
ABCC7 p.Ile1131Cys 22923500:273:40
status: NEW
view ABCC7 p.Ile1131Cys details
A, time courses of the reactions of the I1131C CFTR with 1 mM MTSESafa; in the presence and absence of 10 òe;M GlyH-101. Data points represent mean afe; S.E.M. (n afd; 3). Login to comment
274 ABCC7 p.Ile1131Cys
X
ABCC7 p.Ile1131Cys 22923500:274:25
status: NEW
view ABCC7 p.Ile1131Cys details
Covalent labeling of the I1131C CFTR with MTSESafa; resulted in increases in conductance. Login to comment
278 ABCC7 p.Ile1131Cys
X
ABCC7 p.Ile1131Cys 22923500:278:47
status: NEW
view ABCC7 p.Ile1131Cys details
The EC50 at 0 mV for GlyH-101 blockade for the I1131C CFTR was 0.86 afe; 0.016 òe;M (n afd; 3). Login to comment
279 ABCC7 p.Ser341Cys
X
ABCC7 p.Ser341Cys 22923500:279:40
status: NEW
view ABCC7 p.Ser341Cys details
B, time courses of the reactions of the S341C CFTR with 1 mM NEM in the presence and absence of 10 òe;M GlyH-101. Data points represent mean afe; S.E.M. (n afd; 3). Login to comment
280 ABCC7 p.Ser341Cys
X
ABCC7 p.Ser341Cys 22923500:280:25
status: NEW
view ABCC7 p.Ser341Cys details
Covalent labeling of the S341C CFTR with NEM resulted in reductions in conductance. Login to comment
284 ABCC7 p.Ser341Cys
X
ABCC7 p.Ser341Cys 22923500:284:47
status: NEW
view ABCC7 p.Ser341Cys details
The EC50 at 0 mV for GlyH-101 blockade for the S341C CFTR was 0.89 afe; 0.056 òe;M (n afd; 3). Login to comment
285 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:285:118
status: NEW
view ABCC7 p.Phe342Ala details
TABLE 2 GlyH-101 binding free energy, èc;Gbind, and its components estimated through MM-GB/SA analysis for wt and F342A CFTRs, without and with a membrane Analyses were performed with eq. 1, èc;Gbind afd; èc;Elig af9; èc;Gsolv afa; Tèc;Sconf af9; Evdw af9; Ees af9; èc;EPTN, where èc;Elig and èc;EPTN are changes (upon ligand binding) in the intramolecular strains of the ligand and protein, respectively, èc;Gsolv is the total desolvation penalty for the ligand and protein, Tèc;Sconf is the ligand conformational penalty, and Evdw and Ees are the van der Waals and electrostatic energies, respectively. Login to comment
286 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:286:205
status: NEW
view ABCC7 p.Phe342Ala details
ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:286:261
status: NEW
view ABCC7 p.Phe342Ala details
ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:286:346
status: NEW
view ABCC7 p.Phe342Ala details
ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:286:402
status: NEW
view ABCC7 p.Phe342Ala details
ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:286:437
status: NEW
view ABCC7 p.Phe342Ala details
CFTR èc;Elig èc;EPTN Evdw af9; Ees af9; èc;Gsolv afa;Tèc;Sconf èc;Gbind kcal/mol kcal/mol kcal/mol kcal/mol kcal/mol Without membrane wt 4.68 6.89 afa;21.2 1.05 afa;8.54 F342A 3.90 4.04 afa;21.6 1.05 afa;12.6 wt afa; F342A 0.78 2.85 0.42 0.0 4.0 With membrane wt 4.68 6.88 afa;19.8 1.05 afa;7.23 F342A 3.92 4.05 afa;20.4 1.05 afa;11.4 wt afa; F342A 0.76 2.82 0.54 0.0 4.1 the F342A CFTR (EPTN), consistent with the notion that the side chain of Phe342 in the wt CFTR channel causes an unfavorable steric clash with GlyH-101. Login to comment
288 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:288:156
status: NEW
view ABCC7 p.Phe342Ala details
The calculated free energies of GlyH-101 binding were afa;7.43 and afa;8.54 kcal/mol for the wt CFTR and afa;11.8 and afa;12.6 kcal/mol for the F342A CFTR with and without the membrane, respectively. Login to comment
289 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:289:89
status: NEW
view ABCC7 p.Phe342Ala details
The experimental results presented in Fig. 8A showed that dose-dependent blockade of the F342A CFTR by GlyH-101, as predicted by the MM-GB/SA analysis, exhibited an EC50(0) that was dramatically reduced (5.2 afe; 0.83 nM; n afd; 3), compared with that of the wt CFTR (1.1 afe; 0.11 òe;M; n afd; 4) (Fig. 1C), which is consistent with a substantial increase in binding affinity for the blocker with elimination of the bulky phenylalanine side chain. Login to comment
290 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:290:50
status: NEW
view ABCC7 p.Phe342Ala details
The substantially higher apparent affinity of the F342A CFTR for GlyH-101 suggests dramatic slowing of the off-rate for the bound blocker. Login to comment
304 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:304:175
status: NEW
view ABCC7 p.Phe342Ala details
ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:304:328
status: NEW
view ABCC7 p.Phe342Ala details
ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:304:398
status: NEW
view ABCC7 p.Phe342Ala details
With the data reported by those authors, the kb18; on for the wt CFTR was calculated to be 1.6 afb; 107 Mafa;1 safa;1 , a value similar to the kb18; on for the F342A CFTR (2.3 afb; 107 Mafa;1 safa;1 ) determined in the current study, which indicates that the difference in EC50 values between the wt and F342A CFTRs is attributable to the slow off-rate of GlyH-101 with the F342A CFTR. Login to comment
305 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:305:166
status: NEW
view ABCC7 p.Phe342Ala details
The binding free energy values based on the observed EC50 values, estimated as RTln(EC50), were afa;8.12 kcal/mol for the wt CFTR and afa;11.3 kcal/mol for the F342A CFTR. Login to comment
306 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:306:226
status: NEW
view ABCC7 p.Phe342Ala details
These empirical values are qualitatively consistent with the computed free energies obtained by applying the MM-GB/SA technique to the proposed model of GlyH-101 binding (Fig. 2) for the wt CFTR (afa;7.43 kcal/mol) and the F342A CFTR (afa;11.8 kcal/mol). Login to comment
317 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:317:26
status: NEW
view ABCC7 p.Thr338Cys details
Second, alkylation of the T338C CFTR with iodoacetamide, which results in covalent addition of an acetamide moiety that is predicted by the model to create a steric clash with GlyH-101, significantly reduced the apparent binding affinity of GlyH-101. Login to comment
318 ABCC7 p.Phe337Cys
X
ABCC7 p.Phe337Cys 22923500:318:31
status: NEW
view ABCC7 p.Phe337Cys details
In contrast, alkylation of the F337C CFTR with iodoacetamide was not predicted by the molecular model to cause a steric clash and did not alter GlyH-101 blockade markedly. Login to comment
319 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:319:177
status: NEW
view ABCC7 p.Phe342Ala details
Finally, when a predicted steric clash between the side chain of Phe342 and the naphthalene tail of the bound blocker was removed through mutation of the residue to an alanine (F342A), the apparent blocker affinity was increased more than 200-fold, a change consistent with the free energies of binding estimated using a MM-GB/SA approach. Login to comment
322 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:322:0
status: NEW
view ABCC7 p.Phe342Ala details
F342A CFTR transmembrane currents. Login to comment
323 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:323:0
status: NEW
view ABCC7 p.Phe342Ala details
F342A CFTR channels were expressed in Xenopus laevis oocytes, and transmembrane currents were measured at clamped voltages by using a two-electrode, voltage-clamp technique. Login to comment
324 ABCC7 p.Phe342Ala
X
ABCC7 p.Phe342Ala 22923500:324:55
status: NEW
view ABCC7 p.Phe342Ala details
A, the voltage dependence of the GlyH-101 EC50 for the F342A CFTR is consistent with the Woodhull model (Woodhull, 1973; Tikhonov and Magazanik, 1998), in a manner similar to that of wt CFTR (Fig. 1). Login to comment
346 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:346:38
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:346:225
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:346:259
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Glu1371Gln
X
ABCC7 p.Glu1371Gln 22923500:346:232
status: NEW
view ABCC7 p.Glu1371Gln details
The state-dependent reactivity of the T338C CFTR that was observed in the current study is consistent with the finding by Beck et al. (2008) that MTSESafa; reacted slightly faster with a mutant with high open probability (T338C/ E1371Q CFTR) than with the T338C/wt CFTR.2 Mornon et al. (2009) created a homology model of the CFTR that was based on the inward-facing conformation of the prokaryotic transporter MsbA (PDB code 3B5X) (Ward et al., 2007). Login to comment
350 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:350:110
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Phe337Cys
X
ABCC7 p.Phe337Cys 22923500:350:100
status: NEW
view ABCC7 p.Phe337Cys details
A conformational change of this sort would be consistent with the state-dependent reactivity of the F337C and T338C CFTRs observed in the current study. Login to comment
352 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:352:50
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Glu1371Gln
X
ABCC7 p.Glu1371Gln 22923500:352:56
status: NEW
view ABCC7 p.Glu1371Gln details
Wang and Linsdell (2012) studied reactions of the T338C/E1371Q CFTR with MTSESafa; and [Au(CN)2]afa; and suggested that the reaction of an engineered cysteine at position 338 with externally applied reagents was favored in the closed state. Login to comment
353 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:353:173
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:353:206
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Glu1371Gln
X
ABCC7 p.Glu1371Gln 22923500:353:179
status: NEW
view ABCC7 p.Glu1371Gln details
However, this observation conflicts with that by Beck et al. (2008), who reported that MTSESafa; reacted slightly faster with a double-mutant with high open probability (T338C/E1371Q CFTR) than with the T338C/wt CFTR. Login to comment
354 ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:354:49
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:354:62
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Thr338Cys
X
ABCC7 p.Thr338Cys 22923500:354:190
status: NEW
view ABCC7 p.Thr338Cys details
ABCC7 p.Glu1371Gln
X
ABCC7 p.Glu1371Gln 22923500:354:68
status: NEW
view ABCC7 p.Glu1371Gln details
We observed reaction rates for MTSESafa; with T338C/wt and T338C/E1371Q CFTRs that were similar to those observed by Beck et al. (2008) (data not shown), which supports the idea that the T338C CFTR reacts in the open state. Login to comment
356 ABCC7 p.Arg334Cys
X
ABCC7 p.Arg334Cys 22923500:356:21
status: NEW
view ABCC7 p.Arg334Cys details
Cells expressing the R334C CFTR were preincubated with MTSESafa; with and without an activating cocktail of forskolin and IBMX, and the reaction, which was inferred on the basis of changes in the rectification ratio of the CFTR I-V curve, was observed only with cells exposed to the activating cocktail. Login to comment
368 ABCC7 p.Arg334Cys
X
ABCC7 p.Arg334Cys 22923500:368:205
status: NEW
view ABCC7 p.Arg334Cys details
with Maestro 9.1 (Schro &#a8;dinger) in the MsbA-based model, the reactive thiolate is clearly accessible from the extracellular solution (Fig. 9C), which is consistent with the closed-state reactivity of R334C observed in the current study and in the study by Zhang et al. (2005). Login to comment
369 ABCC7 p.Arg334Cys
X
ABCC7 p.Arg334Cys 22923500:369:31
status: NEW
view ABCC7 p.Arg334Cys details
The mechanism that renders the R334C CFTR unreactive in the conducting state is not clear. Login to comment
371 ABCC7 p.Arg334Cys
X
ABCC7 p.Arg334Cys 22923500:371:4
status: NEW
view ABCC7 p.Arg334Cys details
The R334C mutation may cause significant conformational changes in the CFTR protein (that are not captured in our MD simulation), as suggested by Zhou et al. (2007), which render the engineered cysteine inaccessible in the conducting state of the CFTR. Login to comment