ABCC7 p.Asp993Arg

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PMID: 10026154 [PubMed] Cotten JF et al: "Cystic fibrosis-associated mutations at arginine 347 alter the pore architecture of CFTR. Evidence for disruption of a salt bridge."
No. Sentence Comment
154 We studied the conductance properties of the following double mutants: R347D/D924R, R347D/D993R, and R347E/E1104R.
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ABCC7 p.Asp993Arg 10026154:154:90
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155 The R347D/D993R and R347E/E1104R mutants each had two conductance states with pHc-dependent behavior (Fig. 5).
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ABCC7 p.Asp993Arg 10026154:155:10
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156 For R347D/D993R the increased entry into the OB state was apparent as a shoulder on the amplitude histogram at pHc 5.5.
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ABCC7 p.Asp993Arg 10026154:156:10
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157 Accordingly, for R347D/D993R and R347E/E1104R the current variance in the open state increased with decreasing pHc (Fig. 5B).
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ABCC7 p.Asp993Arg 10026154:157:23
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158 Qualitatively, the lifetimes of the OL and OB conductance states in the R347D/D993R and R347E/E1104R were similar to that of the R347D and R347E mutants, respectively. The amplitude of the OL state was larger for both of these double mutants as compared with the single mutants (Figs.
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ABCC7 p.Asp993Arg 10026154:158:78
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179 A, single-channel current tracings from excised, inside-out membrane patches containing R347E/E1104R, R347D/D924R, and R347D/D993R.
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ABCC7 p.Asp993Arg 10026154:179:125
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181 B, current variance of R347E/E1104R, R347D/D924R, and R347D/D993R at the indicated pHc was collected as in Fig. 3.
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ABCC7 p.Asp993Arg 10026154:181:60
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209 Consistent with this, mutation of D993R and E1104R in MSD2 increased the relative amplitude of the OL conductance state in the context of Arg-347 mutations.
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ABCC7 p.Asp993Arg 10026154:209:34
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PMID: 18421494 [PubMed] Cui G et al: "Mutations at arginine 352 alter the pore architecture of CFTR."
No. Sentence Comment
8 Wild-type-like properties were rescued in R352E/D993R-CFTR, suggesting that R352 and D993 in the wild-type channel may interact to stabilize pore architecture.
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ABCC7 p.Asp993Arg 18421494:8:48
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9 Finally, R352A-CFTR was sensitive to modification by externally applied MTSEA+ , while wild-type and R352E/D993R-CFTR were not.
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ABCC7 p.Asp993Arg 18421494:9:107
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162 Slope conductances are summarized in Table 1 Table 1 Slope conductancea (in pS) of the f state of WT-CFTR and multiple single and double mutants CFTR n Negative VM Positive VM WT 7 6.82 ± 0.03 6.97 ± 0.06 R352A 6 6.80 ± 0.06 7.85 ± 0.07*, ** R352Q 6 5.29 ± 0.02* 6.28 ± 0.05*, ** R352K 5 6.87 ± 0.03 6.86 ± 0.01 R352E 5 3.78 ± 0.01* 6.03 ± 0.01*, ** R352E/E873R 6 3.84 ± 0.01* 5.64 ± 0.01*, ** R352E/ E1104R 6 4.36 ± 0.01* 5.86 ± 0.02*, ** R352E/D993R 5 5.90 ± 0.02* 6.44 ± 0.01*, ** D993R 7 8.27 ± 0.05* 7.13 ± 0.07** a Slope conductance indicates single-channel conductance calculated from 0 to +100 mV (positive VM) or to -100 mV (negative VM) by linear regression * P B 0.001 compared to the equivalent slope conductance in WT-CFTR, ** P B 0.001 compared to the slope conductance in the same mutant at negative VM reflects the loss of anion binding properties within the core of the permeation pathway, which contributes to the tight binding of SCN (Smith et al. 1999).
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ABCC7 p.Asp993Arg 18421494:162:516
status: NEW
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ABCC7 p.Asp993Arg 18421494:162:564
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166 Our present results suggest -300 -50 300 50 Br -100 100 NO3 Cl SCN pA mVBr NO3 SCN Cl -300 -50 300 50 Br -100 100 NO3 Cl SCNC pA mVBr NO3 SCN Cl R352E -4000 -50 4000 50 -100 100 -800 -50 800 50 -100 100 -6000 -50 6000 50 -100 100 A pA -50 800 50 -100 100 A SCN Br Cl NO3 NO3 Br Cl SCN Br NO3 SCN Cl Br NO3 SCN Cl -800 mV pA mV pA mV pA mV NO3 Br Cl SCN Br NO3 SCN Cl Br NO3 SCN Cl Br NO3 SCN Cl -4000 -50 4000 50 -100 100 D -800 -50 800 50 -100 100 E D993R -6000 -50 6000 50 -100 100 WT pA -50 800 50 -100 100 B SCN Br Cl NO3 NO3 Br Cl SCN Br NO3 SCN Cl Br NO3 SCN Cl -800 mV pA mV pA mV pA mV NO3 Br Cl SCN Br NO3 SCN Cl Br NO3 SCN Cl Br NO3 SCN Cl R352A R352K R352E/ Fig. 5 Mutations at R352 alter anion selectivity.
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ABCC7 p.Asp993Arg 18421494:166:451
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167 Representative inside-out macropatches, recorded in the presence of cytoplasmic Cl- or Cl- plus substitute anions, with voltage ramps between -100 and +100 mV, are shown for (A) WT-CFTR, (B) R352A-CFTR, (C) R352E-CFTR, (D) R352K-CFTR and (E) the double mutant R352E/D993R-CFTR.
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ABCC7 p.Asp993Arg 18421494:167:266
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171 Solutions were at pH 7.45 and are labeled as follows: 150 mM Cl- (black), 130 mM Cl- plus 20 mM NO3 - (purple), 130 mM Cl- plus 20 mM Br- (green) and 130 mM Cl- plus 20 mM SCN- (red) Table 2 Relative permeabilities of some anions in WT-CFTR and R352-CFTR mutants * Significant difference compared with WT-CFTR, P \ 0.05; ** Significant difference compared with R352A, P \ 0.05 CFTR n SCN Br NO3 WT 6 4.11 ± 0.17 1.45 ± 0.04 1.51 ± 0.02 R352A 10 4.18 ± 0.65 1.35 ± 0.21 1.70 ± 0.29 R352E 6 5.18 ± 0.32* 1.47 ± 0.08 1.64 ± 0.43 R352K 7 4.05 ± 0.12 1.52 ± 0.01 1.59 ± 0.03** R352E/D993R 6 3.62 ± 0.06* 1.48 ± 0.04 1.59 ± 0.02** Table 3 Relative conductances of some anions in WT-CFTR and R352-CFTR mutants CFTR n SCN Br NO3 WT 6 0.16 ± 0.02 0.67 ± 0.04 0.84 ± 0.04 R352A 10 1.59 ± 0.12* 1.31 ± 0.08* 1.59 ± 0.14* R352E 6 2.73 ± 0.31*, ** 1.49 ± 0.22* 1.54 ± 0.12* R352K 7 1.12 ± 0.08*, ** 0.99 ± 0.02*, ** 1.73 ± 0.26* R352E/ D993R 7 0.61 ± 0.05*, ** 0.98 ± 0.03*, ** 1.26 ± 0.13* Relative conductance was measured at VM = Vrev -25 mV * Significant difference compared with WT-CFTR, P\0.05; ** Significant difference compared with R352A, P\0.05 that loss of positive charge at position 352 destroyed the overall pore architecture, which subsequently changed the anion selectivity characteristics as seen in R352A- and R352E-CFTR.
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ABCC7 p.Asp993Arg 18421494:171:638
status: NEW
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ABCC7 p.Asp993Arg 18421494:171:1058
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199 We studied the conductance properties of CFTR channels bearing the following mutations: R352E, R352E/E873R, R352E/ D993R and R352E/E1104R.
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ABCC7 p.Asp993Arg 18421494:199:115
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202 R352E/D993R-CFTR, in contrast, exhibited stability of the full conductance state similar to that seen in WT-CFTR and R352K-CFTR (Fig. 1); transitions to the s1 and s2 states were rare events in this double mutant.
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ABCC7 p.Asp993Arg 18421494:202:6
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205 The slope conductance of R352E/D993R-CFTR was slightly lower than that of WT-CFTR, although linearity of the i-V relation was mostly retained.
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ABCC7 p.Asp993Arg 18421494:205:31
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206 These data suggested that the D993R mutation at least partly compensated for the R352E mutation, although the double mutant R352E/ D993R-CFTR did not fully recapitulate the behavior of WT-CFTR.
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ABCC7 p.Asp993Arg 18421494:206:30
status: NEW
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ABCC7 p.Asp993Arg 18421494:206:131
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208 If D993 served as the interaction partner of R352, we would expect that block of R352E/D993R-CFTR would be similar to that 0.4 pA 2 s 0.4 pA 2 s 0.2 pA 2 s 0.2 pA 2 s c s1 s2 f c s1 s2 f c s1 s2 f c f R352E R352E/E873R R352E/E1104R R352E/D993R 0 4000 #ofevents 0.0 -0.4 -0.8 0.0 -0.4 -0.8 3000 #ofevents 0 #ofevents 0.0 -0.4 -0.8 3000 0 Currents (pA) 0.0 -0.4 0 2500#ofevents -0.8 fc s1 s2 s1 s2 s1 s2 0.4 pA 2 s 0.4 pA 2 s 0.2 pA 2 s 0.2 pA 2 s c s1 s2 f c s1 s2 f c s1 s2 f c f R352E R352E/E873R R352E/E1104R R352E/D993R 0.4 pA 2 s 0.4 pA 2 s 0.4 pA 2 s 0.4 pA 2 s 0.2 pA 2 s 0.2 pA 2 s 0.2 pA 2 s 0.2 pA 2 s c s1 s2 f c s1 s2 f c s1 s2 f c f R352E R352E/E873R R352E/E1104R R352E/D993R B C D A 0 4000 #ofevents 0.0 -0.4 -0.8 0 4000 #ofevents 0.0 -0.4 -0.8 0.0 -0.4 -0.8 3000 #ofevents 0 0.0 -0.4 -0.8 3000 #ofevents 0 #ofevents 0.0 -0.4 -0.8 3000 0 Currents (pA) #ofevents 0.0 -0.4 -0.8 3000 0 #ofevents 0.0 -0.4 -0.8 3000 0 Currents (pA) 0.0 -0.4 0 2500#ofevents -0.8 fc s1 s2 s1 s2 s1 s2 Fig. 7 Single-channel current tracings of R352E-CFTR and double mutants from excised inside-out patches (left) and resulting all-points amplitude histograms (right) under the same experimental conditions as in Fig. 1.
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ABCC7 p.Asp993Arg 18421494:208:87
status: NEW
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ABCC7 p.Asp993Arg 18421494:208:238
status: NEW
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ABCC7 p.Asp993Arg 18421494:208:517
status: NEW
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ABCC7 p.Asp993Arg 18421494:208:682
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210 There are four current levels indicating the c, s1, s2 and f states in all but the revertant mutant R352E/ D993R-CFTR, which only exhibited the c and f states.
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ABCC7 p.Asp993Arg 18421494:210:107
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213 Figure 8B shows macropatch currents from R352E/D993R-CFTR in the presence and absence of 200 lM glipizide; time-dependent block was rescued in this double mutant.
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ABCC7 p.Asp993Arg 18421494:213:47
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215 This result suggested that the revertant double mutation, R352E/ D993R, recovered the time-dependent block by glipizide but did not completely recover the sensitivity to glipizide characteristic of WT-CFTR. This may reflect the difference in side chain volumes between aspartic and glutamic acids; the volume of a glutamic acid side chain is 20% larger than that of an aspartic acid side chain (Creighton 1993), which may result in a different pore structure.
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ABCC7 p.Asp993Arg 18421494:215:65
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216 To further explore the characteristics of R352E/D993R-CFTR, we studied anion selectivity between Cl- and four substitute monovalent anions.
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ABCC7 p.Asp993Arg 18421494:216:48
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218 Overall, both relative permeability and relative conductance values for WTand R352E/ D993R-CFTR were similar (Tables 2, 3).
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ABCC7 p.Asp993Arg 18421494:218:85
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219 R352E/D993R- CFTRcurrentsexhibitedthesameanionpermeabilitysequence as WT-CFTR: SCN- [NO3 - C Br- [Cl- (although PSCN/ PCl was clearly reduced in the double mutant).
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ABCC7 p.Asp993Arg 18421494:219:6
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220 R352E/D993R-CFTR exhibited relative conductances to SCN- and Br- intermediate between that of WT-CFTR and R352A-CFTR (Table 3).
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ABCC7 p.Asp993Arg 18421494:220:6
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221 These results also suggested that R352A-CFTR and R352E/D993R-CFTR have different pore architecture and that the selectivity properties of the pore of the double mutant might be slightly different from that of WT-CFTR.
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ABCC7 p.Asp993Arg 18421494:221:55
status: NEW
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222 The D993R Mutation Alone also Altered the Pore Architecture of CFTR D993 is localized to TM9 of CFTR, which has not been suggested to be a pore lining domain (McCarty 2000).
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ABCC7 p.Asp993Arg 18421494:222:4
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223 Because the data presented thus far suggested that D993 serves as the interacting partner of R352, we predicted that the D993R mutation alone would change channel activity in a manner similar to that of the R352E, -A or -Q mutation.
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ABCC7 p.Asp993Arg 18421494:223:121
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224 We studied D993R-CFTR with single-channel recording techniques using the same conditions as in Fig. 1.
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ABCC7 p.Asp993Arg 18421494:224:11
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225 D993R-CFTR exhibited instability of the open state, with frequent transitions between all three open conductance levels (Fig. 9A, B); these three open states were even less stable than those of R352A-CFTR.
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ABCC7 p.Asp993Arg 18421494:225:0
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226 The slope conductance of the f state in D993R-CFTR was larger than that of WT-CFTR and indicated slight inward rectification (Fig. 9C, Table 1).
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ABCC7 p.Asp993Arg 18421494:226:40
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227 These results suggest that the D993R mutation alone also destroyed pore architecture in a manner similar to that of the charge-destroying mutations at R352.
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ABCC7 p.Asp993Arg 18421494:227:31
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232 Hence, it is likely that MTSEA+ modified one (or more) of the endogenous cysteines, which B WT-CFTR R352E/D993R R352E R352E/E873R R352E/E1104R WT-CFTR R352E/D993R R352E R352E/E873R R352E/E1104R mV -100 -50 50 100 -0.8 -0.4 0.4 0.8 pA 100 ms 0.2 nA A WT-CFTR R352E/D993R R352E R352E/E873R R352E/E1104R WT-CFTR R352E/D993R R352E R352E/E873R R352E/E1104R mV -100 -50 50 100 -0.8 -0.4 0.4 0.8 pA WT-CFTR R352E/D993R R352E R352E/E873R R352E/E1104R WT-CFTR R352E/D993R R352E R352E/E873R R352E/E1104R WT-CFTR R352E/D993R R352E R352E/E873R R352E/E1104R WT-CFTR R352E/D993R R352E R352E/E873R R352E/E1104R mV -100 -50 50 100 -0.8 -0.4 0.4 0.8 pA 100 ms 0.2 nA Fig. 8 The double mutant R352E/D993R-CFTR recovers WT-like channel behavior.
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ABCC7 p.Asp993Arg 18421494:232:106
status: NEW
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ABCC7 p.Asp993Arg 18421494:232:157
status: NEW
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ABCC7 p.Asp993Arg 18421494:232:264
status: NEW
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ABCC7 p.Asp993Arg 18421494:232:315
status: NEW
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ABCC7 p.Asp993Arg 18421494:232:406
status: NEW
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ABCC7 p.Asp993Arg 18421494:232:457
status: NEW
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ABCC7 p.Asp993Arg 18421494:232:508
status: NEW
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ABCC7 p.Asp993Arg 18421494:232:559
status: NEW
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ABCC7 p.Asp993Arg 18421494:232:681
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233 (A) Single channel i-V relationships are shown for full conductance states of WT-, R352E-, R352E/E873R-, R352E/ E1104R- and R352E/D993R-CFTR.
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ABCC7 p.Asp993Arg 18421494:233:130
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235 (B) Block of R352E/ D993R-CFTR macropatch currents by glipizide (200 lM) is time-dependent.
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ABCC7 p.Asp993Arg 18421494:235:20
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239 If this were true, we would expect that the revertant double mutant, R352E/D993R-CFTR, would not respond to MTSEA+ .
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ABCC7 p.Asp993Arg 18421494:239:75
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244 In contrast, R352E/ D993R-CFTR was insensitive to exposure to MTSEA+ , which resulted in only a 1.08 ± 0.02-fold increase in current (n = 6), thus indicating that the double mutant exhibited WT-like behavior.
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ABCC7 p.Asp993Arg 18421494:244:20
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250 These results strongly suggested that the loss of the positively charged side chain at position 352 shifted the pore architecture in such a way as to destabilize the full open state, 0.2 pA 2 s c s1 s2 f 0.2 pA 2 s c s1 s2 f Currents (pA) 0.0 -0.4 -0.8 2000 4000 6000 #ofevents mV -100 -50 50 100 -1.0 -0.5 0.5 1.0 WT-CFTR D993R pA 0.2 pA 2 s c s1 s2 f 0.2 pA 2 s c s1 s2 f A CB Currents (pA) 0.0 -0.4 -0.8 2000 4000 6000 #ofevents Currents (pA) 0.0 -0.4 -0.8 2000 4000 6000 #ofevents mV -100 -50 50 100 -1.0 -0.5 0.5 1.0 WT-CFTR D993R pA mV -100 -50 50 100 -1.0 -0.5 0.5 1.0 WT-CFTR D993R WT-CFTR D993R pA Fig. 9 Mutation D993R alone had effects similar to those of the charge-reversing mutations at R352.
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ABCC7 p.Asp993Arg 18421494:250:323
status: NEW
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ABCC7 p.Asp993Arg 18421494:250:530
status: NEW
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ABCC7 p.Asp993Arg 18421494:250:584
status: NEW
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ABCC7 p.Asp993Arg 18421494:250:598
status: NEW
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ABCC7 p.Asp993Arg 18421494:250:623
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251 Representative single-channel current tracing (A), all-points amplitude histogram (B) and i-V relationship for the f conductance state (C) are shown for the D993R mutant.
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ABCC7 p.Asp993Arg 18421494:251:157
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253 In c, points show mean ± SEM for n = 7 observations, and error bars are smaller than the symbols; lines are from linear regression WT 1 A 200 s Isoproterenol 0.4 A 100 s 0.4 A 100 s R352A R352E/D993R MTSEA MTSEA MTSEA WT 1 A 200 s Isoproterenol 0.4 A 100 s 0.4 A 100 s R352A R352E/D993R MTSEA MTSEA MTSEA Fig. 10 Mutation R352A results in appearance of sensitivity to a cysteine-modifying reagent.
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ABCC7 p.Asp993Arg 18421494:253:199
status: NEW
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ABCC7 p.Asp993Arg 18421494:253:286
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254 Oocytes expressing WT-CFTR (top trace), R352A-CFTR (middle trace) or R352E/D993R-CFTR (bottom trace), along with the b2-adrenergic receptor, were studied by two-electrode voltage clamp.
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ABCC7 p.Asp993Arg 18421494:254:75
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258 Second, we identified the interaction partner as D993 by use of double mutants; R352E/E873R-CFTR and R352E/E1104R-CFTR exhibited permeation properties similar to those of R352E-CFTR, while R352E/D993R-CFTR behaved more like WT-CFTR.
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ABCC7 p.Asp993Arg 18421494:258:195
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261 As predicted, D993R-CFTR exhibited instability of the open state similar to that seen in R352E-CFTR.
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ABCC7 p.Asp993Arg 18421494:261:14
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295 Stability of the open state was retained in the case of a charge-conserving mutation, R352K, and in the double mutant R352E/D993R-CFTR.
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ABCC7 p.Asp993Arg 18421494:295:124
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297 Compared to WT-CFTR, R352E/D993R-CFTR channels exhibited lower slope conductance, weakened block by glipizide, and altered selectivity between Cl- and SCN- .
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ABCC7 p.Asp993Arg 18421494:297:27
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301 We conclude that the double mutant R352E/D993R-CFTR retains the interaction between these residues but does not fully mimic the behavior of WT-CFTR, suggesting that permeation properties in the CFTR chloride channel are very sensitive to small changes in pore structure.
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ABCC7 p.Asp993Arg 18421494:301:41
status: NEW
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PMID: 19020075 [PubMed] Jordan IK et al: "Evolutionary and functional divergence between the cystic fibrosis transmembrane conductance regulator and related ATP-binding cassette transporters."
No. Sentence Comment
95 Isolated bursts of channel activity from oocytes expressing WT-CFTR, R352E-CFTR, R352E/E1104R-CFTR, and R352E/D993R-CFTR.
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ABCC7 p.Asp993Arg 19020075:95:110
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100 In contrast, WT-CFTR channels, and channels bearing the revertant mutation R352E/D993R, primarily exhibit transitions to the full conductance level.
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ABCC7 p.Asp993Arg 19020075:100:81
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131 In contrast, approximately wild-type channel behavior is retained in R352K-CFTR and the charge-swapping double mutant, R352E/D993R-CFTR (Fig. 3).
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ABCC7 p.Asp993Arg 19020075:131:125
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PMID: 19754156 [PubMed] Alexander C et al: "Cystic fibrosis transmembrane conductance regulator: using differential reactivity toward channel-permeant and channel-impermeant thiol-reactive probes to test a molecular model for the pore."
No. Sentence Comment
306 Conversely, Cui et al. (41) reported that substitution of a positive charge at position 993 (D993R) increased single-channel conductance for inward current above that of wt CFTR.
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ABCC7 p.Asp993Arg 19754156:306:93
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PMID: 22160394 [PubMed] Cui G et al: "Differential contribution of TM6 and TM12 to the pore of CFTR identified by three sulfonylurea-based blockers."
No. Sentence Comment
144 These functional characteristics were returned to approximately their wildtype behavior in R352E/D993R-CFTR, perhaps because the salt bridge was retained in this second-site reversion [12].
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ABCC7 p.Asp993Arg 22160394:144:97
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PMID: 23709221 [PubMed] Cui G et al: "Two salt bridges differentially contribute to the maintenance of cystic fibrosis transmembrane conductance regulator (CFTR) channel function."
No. Sentence Comment
21 However, subconductance states are dominant events with short burst durations in CFTR channels bearing known salt bridge mutations, such as R352A, R347H, D993R, and D924R (13, 14).
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ABCC7 p.Asp993Arg 23709221:21:154
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105 Similar results were found for D993R-CFTR, but nearly wild type-like behavior, including stable openings to the f state, was recovered in the R352E/D993R double mutant (see Fig. 3A).
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ABCC7 p.Asp993Arg 23709221:105:31
status: NEW
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ABCC7 p.Asp993Arg 23709221:105:148
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109 We therefore hypothesized that Arg347 might also interact with Asp993 to rescue the CFTR channel pore to a stable f state and tested this hypothesis in three double mutants; TABLE 1 Summary of the effects of mutations studied Mutant Main features of open bursts Impact on f state R347A Emphasizes s1 state, brief transitions to s2 and f Can reach f but not stable R347D Emphasizes s1 state, no transitions to s2 and f Cannot reach f D924R Brief transitions to all conductance levels Can reach f but not stable R347K Wild type-like Wild type-like R347D/D924R Emphasizes s2 state, rare and brief transitions to f Can reach f but not stable R352E Opens to all 3 levels; s1 much more stable than in WT, s2 unstable, f unstable Can reach f but not stable D993R Opens to all 3 levels, but none are stable Can reach f but not stable R352E/D993R Wild type-like, with increased transitions to s1 and s2; slightly reduced single-channel conductance Wild type-like R352E/D924R Opens to all 3 levels, but none are stable Can reach f but not stable R347D/D993R Very stable s2; rare and brief transitions to both s1 and f Can reach f but not stable R347A/R352A Opens to all 3 levels; s1 much more stable than in WT, s2 unstable, f unstable Can reach f but not stable R347D/D924R/D993R Opens to all 3 levels; s1 much more stable than in WT, s2 relatively stabilized, f unstable Can reach f but not stable R347D/D924R/R352E/D993R Primarily flickers between s2 and f; s1 much more stable than in WT, slightly reduced single channel conductance Can reach f but not stable FIGURE 3.
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ABCC7 p.Asp993Arg 23709221:109:750
status: NEW
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ABCC7 p.Asp993Arg 23709221:109:832
status: NEW
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ABCC7 p.Asp993Arg 23709221:109:1042
status: NEW
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ABCC7 p.Asp993Arg 23709221:109:1265
status: NEW
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ABCC7 p.Asp993Arg 23709221:109:1408
status: NEW
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111 A, representative current samples of R352E/D993R-, R352E/D924R-, and R347D/D993R-CFTR recorded from excised inside-out patches with the same conditions as Fig. 2 (n afd; 3-6 for each mutant).
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ABCC7 p.Asp993Arg 23709221:111:43
status: NEW
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ABCC7 p.Asp993Arg 23709221:111:75
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114 As noted above, R352E/D993R exhibited a prominent full open state similar to WT-CFTR (13), suggesting that the R352E/D993R salt bridge can fully rescue the CFTR channel pore to normal behavior (aside from a slight decrease in single channel conductance).
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ABCC7 p.Asp993Arg 23709221:114:22
status: NEW
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ABCC7 p.Asp993Arg 23709221:114:117
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115 Whereas the single channel behavior of R352E/D924R was similar to that of R352E alone, with multiple unstable open states, suggesting that Arg352 and Asp924 do not interact, R347D/D993R was much more like R347D/D924R, with the s2 state dominant (compare Figs. 3 and 2).
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ABCC7 p.Asp993Arg 23709221:115:180
status: NEW
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116 R347D/ D993R-CFTR is able to transition to the f state but sojourns there are even more brief than those seen for the R347D/ D924R.
X
ABCC7 p.Asp993Arg 23709221:116:7
status: NEW
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122 Similarly, in the R347D/D993R mutant, the positive charge at Arg347 is no longer available to interact with Asp924 .
X
ABCC7 p.Asp993Arg 23709221:122:24
status: NEW
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124 This was tested in the triple mutant R347D/D924R/D993R (Fig. 4, A and B).
X
ABCC7 p.Asp993Arg 23709221:124:49
status: NEW
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125 Unlike the two double mutants described above (R347D/D924R and R347D/ D993R), the triple mutant exhibited roughly equal occupancy of s1,s2,andfstates;theoccupancyofthes2statewasnotasstableas in either double mutant.
X
ABCC7 p.Asp993Arg 23709221:125:70
status: NEW
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141 However, the quadruple mutant R347D/D924R/D993R/R352E did not completely rescue WT behavior (Fig. 4, A and B).
X
ABCC7 p.Asp993Arg 23709221:141:42
status: NEW
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146 Representative current samples of R347A/R352A-, R347D/D924R/D993R-, and R347D/D924R/D993R/R352E-CFTR were recorded under the same conditions as in Fig. 3 (n afd; 5-6 for each mutant) (A).
X
ABCC7 p.Asp993Arg 23709221:146:60
status: NEW
X
ABCC7 p.Asp993Arg 23709221:146:84
status: NEW
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