ABCC7 p.Phe1296Ser

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PMID: 20876359 [PubMed] Szollosi A et al: "Involvement of F1296 and N1303 of CFTR in induced-fit conformational change in response to ATP binding at NBD2."
No. Sentence Comment
18 We expressed wild-type as well as F1296S, N1303Q, and R1358A mutant CFTR in Xenopus oocytes and studied these channels using macroscopic inside-out patch recordings.
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72 In this study, the average durations of stationary segments of record used for estimating Po;max were 40-50 s for the wild-type (WT), F1296S, N1303Q, and F1296S/N1303Q constructs (estimated single-channel cycle times 1.25 s in saturating ATP; Fig. 8 A), but 100-130 s for K1250R, F1296S/K1250R, and N1303Q/K1250R, and 220 s for F1296S/ N1303Q/K1250R (estimated single-channel cycle times 13 s in saturating ATP; Fig. 8 A).
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ABCC7 p.Phe1296Ser 20876359:72:134
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ABCC7 p.Phe1296Ser 20876359:72:154
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ABCC7 p.Phe1296Ser 20876359:72:288
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109 Figs. S3 and S4 show verification of Po;max estimates in single-channel patches for WT, F1296S, N1303Q, and F1296S/N1303Q (Fig. S3), as well as for K1250R, F1296S/K1250R, N1303Q/K1250R, and F1296S/N1303Q/K1250R (Fig. S4).
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ABCC7 p.Phe1296Ser 20876359:109:88
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ABCC7 p.Phe1296Ser 20876359:109:108
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ABCC7 p.Phe1296Ser 20876359:109:156
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113 Fig. S8 depicts predicted Po time courses in response to the addition/removal of ATP for WT, F1296S/N1303Q, K1250R, and F1296S/N1303Q/K1250R, calculated using Scheme 2.
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ABCC7 p.Phe1296Ser 20876359:113:93
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118 (A-D) Inward chloride currents recorded in patches excised from resting oocytes expressing WT (A), F1296S (B), N1303Q (C), and F1296S/N1303Q (D) CFTR.
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ABCC7 p.Phe1296Ser 20876359:118:99
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122 Phosphorylation dependence of channel activity is largely unchanged for F1296S, N1303Q, and F1296S/N1303Q CFTR mutants, whereas the double mutant displays significantly increased ATP-independent activity Similarly to WT CFTR (Fig. 2 A), in patches excised from resting oocytes expressing F1296S (Fig. 2 B), N1303Q (Fig. 2 C), or double mutant F1296S/N1303Q (Fig. 2 D) CFTR channels, we observed very low channel activity upon the application of 2 mM ATP, but robust macroscopic currents could be activated for all three constructs by the subsequent addition of 300 nM PKA to the bath solution.
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ABCC7 p.Phe1296Ser 20876359:122:72
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ABCC7 p.Phe1296Ser 20876359:122:92
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ABCC7 p.Phe1296Ser 20876359:122:288
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127 This pattern of coevolution between sites 1 and 2 suggests that possible functional interactions between the two residues, perturbed by single mutations F1296S and N1303Q, might be restored in a double mutant F1296S/N1303Q.
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ABCC7 p.Phe1296Ser 20876359:127:153
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131 (A) Representative traces of WT, F1296S, N1303Q, and F1296S/N1303Q currents illustrating segments in 0 mM ATP and bracketing segments in 2 mM ATP. Dotted lines show zero current level.
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ABCC7 p.Phe1296Ser 20876359:131:33
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132 (B) Estimation of Po;max for WT (black), F1296S (red), N1303Q (blue), and F1296S/N1303Q (green) by stationary noise analysis.
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ABCC7 p.Phe1296Ser 20876359:132:41
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138 maximal open probabilities were little changed in all three mutant constructs (0.22 ± 0.02, 0.32 ± 0.04, and 0.33 ± 0.03, respectively, for F1296S, N1303Q, and F1296S/ N1303Q) compared with WT (0.35 ± 0.03) (Fig. 3 B), open probability in zero ATP was 10-fold higher for the F1296S/N1303Q double mutant than for WT or the two single mutants (Fig. 3 C).
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ABCC7 p.Phe1296Ser 20876359:138:155
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ABCC7 p.Phe1296Ser 20876359:138:175
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142 Indeed, although K1250R, F1296S/K1250R, and N1303Q/K1250R ATP removal rapidly abolished currents for both single mutants just as for WT (Fig. 2, A-C), in the case of the double mutant, a constitutive basal activity persisted even after ATP removal (Fig. 2 D, magnified in inset) and did not vanish even over the time course of several minutes.
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147 (A) Representative traces of K1250R, F1296S/K1250R, N1303Q/K1250R, and F1296S/N1303Q/K1250R currents illustrating segments in 0 mM ATP and bracketing segments in 2 mM ATP. Dotted lines show zero current level (determined for the triple mutant similarly to that in Fig. S2).
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ABCC7 p.Phe1296Ser 20876359:147:37
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148 (B) Estimation of Po;max for K1250R (black), F1296S/K1250R (red), N1303Q/K1250R (blue), and F1296S/N1303Q/K1250R (green) by stationary noise analysis.
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ABCC7 p.Phe1296Ser 20876359:148:45
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155 constructs showed hardly detectable basal activity, a markedly elevated spontaneous activity was observed for the F1296S/N1303Q/K1250R triple mutant (Fig. 4 A), persisting even minutes after ATP washout.
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ABCC7 p.Phe1296Ser 20876359:155:114
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157 Similarly to their hy-drolytic counterparts, Po;bas was 10-fold higher in F1296S/N1303Q/K1250R compared with the other three constructs, and the mutant cycle built on the closed-open equilibrium constant Po;bas/(1Po;bas) yielded a Gint of 2.36 ± 0.58 kT (Fig. 4 D)-again, significantly different from zero (P < 0.01).
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ABCC7 p.Phe1296Ser 20876359:157:81
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160 Conventional dwell-time analysis of such records yielded Po;max values similar to those obtained by noise analysis both for the WT, F1296S, N1303Q, and F1296S/ N1303Q constructs (Fig. S3, A and B), and for the Figure 5.  Energetic coupling between sites 1 and 2 changes between ATP-bound open and ATP-free closed states, but not between ATP-bound closed and open states.
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ABCC7 p.Phe1296Ser 20876359:160:132
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161 (A) Summary of Po;max values for K1250R (black), F1296S/K1250R (red), N1303Q/K1250R (blue), and F1296S/N1303Q/K1250R (green) obtained from the data presented in Fig. 4 B.
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ABCC7 p.Phe1296Ser 20876359:161:49
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ABCC7 p.Phe1296Ser 20876359:161:96
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175 Thus, to test for a possible change in interaction between sites 1 and 2 during ATP-driven reversible opening and closure, we repeated the mutant cycle analysis in the nonhydrolytic K1250R background, comparing Po;max values for K1250R, F1296S/K1250R, N1303Q/ K1250R, and F1296S/N1303Q/K1250R (Fig. 5 A), Figure 6.  ATP binding affects energetic coupling between sites 1 and 2 in closed channels.
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ABCC7 p.Phe1296Ser 20876359:175:237
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ABCC7 p.Phe1296Ser 20876359:175:238
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176 (A) [ATP] dependence of macroscopic currents was assayed for WT (top left), F1296S (top right), N1303Q (bottom left), and F1296S/N1303Q (bottom right) channels by exposure to various test [ATP] bracketed by exposures to 2 mM ATP.
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ABCC7 p.Phe1296Ser 20876359:176:76
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ABCC7 p.Phe1296Ser 20876359:176:122
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177 (B) ATP-dependent current fractions (II0)/(ImaxI0) plotted as a function of [ATP] for WT (black), F1296S (red), N1303Q (blue), and F1296S/N1303Q (green).
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ABCC7 p.Phe1296Ser 20876359:177:114
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ABCC7 p.Phe1296Ser 20876359:177:147
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184 Although neither the F1296S nor the N1303Q mutation, when introduced one at a time, affected the time constant of current relaxation of K1250R upon ATP removal (Fig. 5 C, red and blue fit lines and bars), this relaxation time constant (relax) was prolonged by approximately fourfold, to 31 ± 5 s (n = 10), in the triple mutant F1296S/ N1303Q/K1250R (Fig. 5 C, green fit line and bar).
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ABCC7 p.Phe1296Ser 20876359:184:21
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ABCC7 p.Phe1296Ser 20876359:184:340
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205 For instance, in TAP1, the site-1 phenylalanine backbone forms an H bond with the asparagine at site 2 (corresponding to N1303 in CFTR`s NBD2) when ATP is bound to the protein (Procko et al., 2006), whereas in the ADP-bound form Right-shift in ATP dependence of opening rate for F1296S/ N1303Q indicates a change in interaction between sites 1 and 2 upon ATP binding to closed channels To test whether the site-1-site-2 interaction was affected by ATP binding, we evaluated the apparent affinity for ATP to open WT, F1296S, N1303Q, and F1296S/ N1303Q channels.
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ABCC7 p.Phe1296Ser 20876359:205:279
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ABCC7 p.Phe1296Ser 20876359:205:516
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209 Just as for KPo, the resulting KrCO values were slightly lower for F1296S and N1303Q than for WT, but approximately twofold increased for the double mutant F1296S/N1303Q (Fig. 6 C).
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ABCC7 p.Phe1296Ser 20876359:209:67
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ABCC7 p.Phe1296Ser 20876359:209:156
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227 Phenotypic pattern of single and double mutants at site 1 and 2 suggests toggle switch mechanism Using mutants F1296S, N1303Q, and F1296S/N1303Q, we studied the interaction between sites 1 and 2 in the form of mutant cycles built on (a) ATP-independent spontaneous activity (i.e., Po;bas/(1Po;bas)) both in hydrolysis-competent (Fig. 3 D) and (b) in catalytically inactive (Fig. 4 D) background; (c) ATP-dependent maximal activity (i.e., Po;max/(1Po;max)) (Fig. 5 B) and (d) de- activationrateuponATPremoval(Fig.5D)ofcatalytically incompetent constructs; and (e) apparent affinity for ATP to open the channels (Fig. 6 D).
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ABCC7 p.Phe1296Ser 20876359:227:111
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ABCC7 p.Phe1296Ser 20876359:227:131
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228 Interestingly, although four of the above five mutant cycles (Figs. 3 D, 4 D, 5 D, and 6 D) yielded Gint significantly different from zero, in each case this was due to a significantly altered phenotype in the double mutant F1296S/N1303Q, whereas the single mutations F1296S and N1303Q did not measurably affect gating (Figs. 3-6).
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ABCC7 p.Phe1296Ser 20876359:228:240
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268 The two rates assumed to be changed by the F1296S/N1303Q double mutation, and by the K1250R mutation, are shown in red and magenta, respectively, belowtheWTrates.
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ABCC7 p.Phe1296Ser 20876359:268:43
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269 (B)Tablesummarizingparam- eters Po;bas and KPo predicted by Scheme 2 for WT (using the rates in black in A) and F1296S/ N1303Q (using the two rates in red in A), as well as Po;max and relax for K1250R and F1296S/ N1303Q/K1250R (using the rates printed in magenta for steps C4→O2 and O2→C1).
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ABCC7 p.Phe1296Ser 20876359:269:112
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272 in an unchanged Po;max (Fig. 8 B), just as we have observed for F1296S/N1303Q/K1250R (Fig. 5 A).
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ABCC7 p.Phe1296Ser 20876359:272:64
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274 Such predicted time courses are summarized in Fig. S8 for WT, F1296S/N1303Q, K1250R, and F1296S/N1303Q/K1250R.
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ABCC7 p.Phe1296Ser 20876359:274:62
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275 Thus, this alteration of only two analogous rates in the double mutant F1296S/N1303Q is sufficient to account for all of our data on site-1-site-2 interactions (Figs. 1-6).
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276 Because S-Q (and A-Q) pairings are also quite frequent alternatives of the most typical F-N pairing at these two sites (Fig. 1 A), it is conceivable that the site-1-site-2 interaction postulated for states C2, C4, O1, and O2 in WT can also be formed to some extent in F1296S/N1303Q.
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293 The lack of phenotype in the single mutants N1303Q and F1296S can be accounted for by assuming stabilizing F-X and N-Y interactions in states C1 and C3 replaced by a stabilizing F-N interaction in states C2 and C4 (retained in O1 and O2) in WT CFTR (illustrated in the cartoon in Fig. 8 A).
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ABCC7 p.Phe1296Ser 20876359:293:55
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295 In contrast, the double mutation F1296S/N1303Q removes two stabilizing interactions (F-X and N-Y) in states C1 and C3, but only one such interaction (F-N) in states C2, C4, O1, and O2.
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297 Indeed, a 160-fold decrease in rate C2→C1 (Fig. 8 A, red) increases Po;bas by 10-fold (Fig. 8 B) to the level we have observed for F1296S/N1303Q (Fig. 3 C).
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ABCC7 p.Phe1296Ser 20876359:297:138
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298 A comparable (100-fold) decrease in rate C4→C3 (Fig. 8 A, red) reproduces the approximately fourfold prolonged relax (Fig. 8 B) we have observed for F1296S/N1303Q/K1250R (Fig. 5 C).
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300 Moreover, the reduction in rate C4→C3 has no impact on maximal opening rate, and hence on Po;max, consistent with our observation for the double mutant F1296S/N1303Q (Fig. 3 B).
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ABCC7 p.Phe1296Ser 20876359:300:159
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PMID: 24058550 [PubMed] Dawson JE et al: "Allosteric coupling between the intracellular coupling helix 4 and regulatory sites of the first nucleotide-binding domain of CFTR."
No. Sentence Comment
265 ATP-independent channel opening has been enhanced by Cys, Ser, and Pro mutations of K978 in the ICDs [15] and F1296S/N1303Q and R1358A in NBD2 [60].
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ABCC7 p.Phe1296Ser 24058550:265:110
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