ABCC7 p.His1375Ala

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PMID: 21576373 [PubMed] Szollosi A et al: "Mutant cycles at CFTR's non-canonical ATP-binding site support little interface separation during gating."
No. Sentence Comment
27 Although both mutations H1348A and H1375A produced dramatic changes in hydrolytic and nonhydrolytic channel closing rates, in the corresponding double mutants these changes proved mostly additive with those caused by mutation T460S, suggesting little change in energetic coupling between either positions 460-1348 or positions 460-1375 during gating.
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ABCC7 p.His1375Ala 21576373:27:35
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36 M AT E R I A L S A N D M E T H O D S Molecular biology pGEMHE-WT (Chan et al., 2000), carrying the coding sequence of human WT CFTR, was used as a template for mutants T460S, L1353M, H1348A, H1375A, T460S/L1353M, T460S/H1348A, and T460S/H1375A.
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ABCC7 p.His1375Ala 21576373:36:191
status: NEW
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ABCC7 p.His1375Ala 21576373:36:237
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102 Fitting the relaxation time course after ATP removal for the nonhydrolytic H1375A/K1250R and T460S/H1375A/K1250R constructs consistently required a double exponential with two slow time constants (each in the seconds range), suggesting two populations of open-channel bursts (see Fig. 9 A).
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ABCC7 p.His1375Ala 21576373:102:75
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ABCC7 p.His1375Ala 21576373:102:99
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195 Energetic coupling between positions 460 and 1375 is little changed during gating To study interactions between positions 460 and 1375, we compared the effects of mutation T460S in H1375A and WT backgrounds. For single channels gating under normal hydrolytic conditions (Fig. 8 A, top), mutation H1375A also slowed closure (to 1.3 ± 0.1 s1 ; n = 6; Fig. 8 B, left, blue bar), similarly to what was observed for H1348A (see Fig. 6 B, left, blue bar).
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ABCC7 p.His1375Ala 21576373:195:181
status: NEW
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ABCC7 p.His1375Ala 21576373:195:296
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197 The increased open probability of T460S/H1375A relative to that of H1375A (Fig. 8 C, in Fig. 6 B, left), just as that of T460S relative to WT (compare red and black bar in Fig. 2 B).
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ABCC7 p.His1375Ala 21576373:197:40
status: NEW
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ABCC7 p.His1375Ala 21576373:197:67
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215 Because for both H1375A/K1250R green vs. blue bar) attested to an increased opening rate in the double mutant (Fig. 8 D, left, green vs. blue bar).
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ABCC7 p.His1375Ala 21576373:215:17
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225 (A) Representative single-channel current traces from prephosphorylated H1375A and T460S/H1375A CFTR channels gating in 2 mM ATP. Downward deflection indicates inward current.
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ABCC7 p.His1375Ala 21576373:225:72
status: NEW
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ABCC7 p.His1375Ala 21576373:225:89
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226 (B; left) Closing rates of H1375A (blue bar) and T460S/H1375A (green bar), defined as the inverse of the mean burst duration (see Materials and methods).
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ABCC7 p.His1375Ala 21576373:226:27
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ABCC7 p.His1375Ala 21576373:226:55
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229 (C) Noise analysis was used to estimate Po for H1375A (blue bar) and T460S/H1375A (green bar).
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ABCC7 p.His1375Ala 21576373:229:47
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ABCC7 p.His1375Ala 21576373:229:75
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230 (D; left) Opening rates of H1375A (blue bar) and T460S/H1348A (green bar), obtained using the estimate for Po (see C) and closing rate (see B).
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ABCC7 p.His1375Ala 21576373:230:27
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241 An alteration and T460S/H1375A/K1250R adequate fitting of the relaxation time course after ATP removal consistently required a double exponential with two slow time constants (each in the seconds range; Fig. 9 A), average steady-state closing rate was estimated from a double-exponential fit as described in Materials and methods.
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ABCC7 p.His1375Ala 21576373:241:24
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242 Unexpectedly, when the H1375A mutation was introduced into the K1250R background, average nonhydrolytic closing rate was not slowed, but rather slightly accelerated (Fig. 9 A, blue bar).
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ABCC7 p.His1375Ala 21576373:242:23
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244 Finally, by noise analysis (Fig. 9 C), mutation T460S reduced Po in the H1375A/K1250R background (compare green vs. blue bars in Fig. 9 D, left) to a similar extent as it did in the single-mutant K1250R background (compare red vs. black bars in Fig. 5 C), yielding a Gint(open-closed) not significantly different from zero (Fig. 9 D; P = 0.15).
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ABCC7 p.His1375Ala 21576373:244:72
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248 (A) Representative normalized decay time courses of macroscopic currents for H1375A/K1250R and T460S/H1375A/K1250R CFTR after the removal of 2 mM ATP. Solid blue and green lines are fitted bi-exponentials.
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ABCC7 p.His1375Ala 21576373:248:77
status: NEW
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ABCC7 p.His1375Ala 21576373:248:101
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249 Fitted parameters were 1 = 2.8 s, 2 = 11 s, A1 = 0.77, and A2 = 0.23 for the H1375A/ K1250R trace, and 1 = 2.8 s, 2 = 15 s, A1 = 0.82, and A2 = 0.18 for the T460S/H1375A/ K1250R trace.
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ABCC7 p.His1375Ala 21576373:249:93
status: NEW
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ABCC7 p.His1375Ala 21576373:249:195
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253 (C) Noise analysis for estimation of Po for H1375A (blue symbols) and T460S/H1375A (green symbols); each symbol represents one patch.
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ABCC7 p.His1375Ala 21576373:253:44
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ABCC7 p.His1375Ala 21576373:253:76
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254 (D; left) Mean ± SEM Po for H1375A (blue bar) and T460S/H1375A (green bar).
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ABCC7 p.His1375Ala 21576373:254:33
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ABCC7 p.His1375Ala 21576373:254:61
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277 In contrast to the simple interpretation of the effects of the above two mutations, the functional consequences of the H1375A mutation are more complex.
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ABCC7 p.His1375Ala 21576373:277:119
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281 Although the H1375A phenotypes are not easily interpretable, altogether our findings are generally consistent with evidence from other studies of mutations in site 1, which suggest that protein-nucleotide and protein-protein interactions at composite site 1 contribute to the stability of the open-state dimer (Vergani et al., 2003; Bompadre et al., 2005; Cai et al., 2006; Zhou et al., 2006; Tsai et al., 2009).
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ABCC7 p.His1375Ala 21576373:281:13
status: NEW
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