ABCC7 p.Tyr1219Trp

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PMID: 16966475 [PubMed] Zhou Z et al: "The two ATP binding sites of cystic fibrosis transmembrane conductance regulator (CFTR) play distinct roles in gating kinetics and energetics."
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105 A more conserved mutation (Y1219W) does not change the K1/2 value significantly.
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ABCC7 p.Tyr1219Trp 16966475:105:27
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122 (A) Normalized ATP dose-response relationships of WT (black line, Michaelis-Menten fit from Fig. 1 D), Y1219W (brown), Y1219F (pink), Y1219I (blue), and Y1219G (green line, Michaelis-Menten fit from Fig. 1 D).
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ABCC7 p.Tyr1219Trp 16966475:122:103
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124 K1/2 values are 0.13 ± 0.02 mM (Y1219W), 0.46 ± 0.06 mM (Y1219F), and 0.94 ± 0.20 mM (Y1219I), respectively.
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ABCC7 p.Tyr1219Trp 16966475:124:37
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PMID: 18391167 [PubMed] Chen TY et al: "CLC-0 and CFTR: chloride channels evolved from transporters."
No. Sentence Comment
786 A more conservative mutation (Y1219W), however, did not change the K0.5 value significantly.
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ABCC7 p.Tyr1219Trp 18391167:786:30
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PMID: 20628841 [PubMed] Shimizu H et al: "A stable ATP binding to the nucleotide binding domain is important for reliable gating cycle in an ABC transporter CFTR."
No. Sentence Comment
19 The degree of dose-response shift, a descending order of Y1218G, Y1219I, Y1219F and Y1219W, seemed to depend on the similarity of chemical properties, e.g., hydrophobicity and p bond by aromatic ring, of the side chains introduced by the mutations to tyrosine.
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ABCC7 p.Tyr1219Trp 20628841:19:84
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59 Figure 2b compares macroscopic current relaxations for Y1219G, Y1219I, Y1219F and Y1219W mutants.
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ABCC7 p.Tyr1219Trp 20628841:59:82
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60 Although a slow phase of current decay can be seen with Y1219G and Y1219I, this second phase is hardly discernable for the Y1219W mutant.
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ABCC7 p.Tyr1219Trp 20628841:60:123
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65 b A representative current trace of WT-CFTR channel showing immediate closing upon a rapid removal of ATP somewhere between Y1219W and Y1219I.
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ABCC7 p.Tyr1219Trp 20628841:65:125
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67 The time constants of the initial fast phase for all the Y1219 mutants are within hundreds of milliseconds (sfast: 504 &#b1; 76 ms, n = 5 for Y1219G; 450 &#b1; 44 ms, n = 7 for Y1219I; 571 &#b1; 142 ms, n = 4 for Y1219F; 513 &#b1; 66 ms, n = 5 for Y1219W) and there is not significant difference in the fast time constant among these Y1219 mutants (Fig. 2b).
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ABCC7 p.Tyr1219Trp 20628841:67:248
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68 On the other hand, the time constants of the slow component for Y1219F and Y1219W are shorter than those of Y1219G and Y1219I (Fig. 3a).
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ABCC7 p.Tyr1219Trp 20628841:68:75
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69 More importantly, the fraction of the slow component (Fig. 3b) shows a gradual decrease as the mutation becomes less 'preserved` (Y1219G [ Y1219I [ Y1219F [ Y1219W).
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ABCC7 p.Tyr1219Trp 20628841:69:157
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70 It should be noted that, for technical reasons (detailed in ''Discussion``), our calculation of the fraction of the slow component is somewhat overestimated for Y1219F and Y1219W.
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ABCC7 p.Tyr1219Trp 20628841:70:172
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71 The actual values for Y1219F and Y1219W are lower than those shown in Fig. 3b.
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ABCC7 p.Tyr1219Trp 20628841:71:33
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80 b Macroscopic current relaxations upon ATP wash-out for Y1219G, Y1219I, Y1219F and Y1219W.
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ABCC7 p.Tyr1219Trp 20628841:80:83
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82 The time constant and the fraction of the slow component are summarized in Fig. 3. c Single channel recording of Y1219G-CFTR showing a long opening even after ATP removal 35 30 25 20 15 10 5 0 Y1219G Y1219I Y1219F Y1219W 0.5 0.4 0.3 0.2 0.1 0.0 Y1219G Y1219I Y1219F Y1219W A slow / (A slow + A fast ) c4; slow (s) A B Fig. 3 Kinetic parameters of macroscopic current relaxations for Y1219G, Y1219I, Y1219F and Y1219W.
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ABCC7 p.Tyr1219Trp 20628841:82:214
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ABCC7 p.Tyr1219Trp 20628841:82:266
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ABCC7 p.Tyr1219Trp 20628841:82:413
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83 a Time constants of the slow component of the current relaxation for the Y1219 mutants. Y1219G: n = 5; Y1219I: n = 7; Y1219F: n = 4; and Y1219W: n = 5. b Fraction of the slow component (Aslow/Aslow ?
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ABCC7 p.Tyr1219Trp 20628841:83:137
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84 Afast) for the Y1219 mutants. Y1219G: n = 5; Y1219I: n = 7; Y1219F: n = 4; and Y1219W: n = 5 ATP because of their similar rate-limiting hydrolyzing rates [11].
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ABCC7 p.Tyr1219Trp 20628841:84:79
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132 Although the results with Y1219G and Y1219I mutations are quantified accurately, this may not be the case with the data for Y1219F and Y1219W.
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ABCC7 p.Tyr1219Trp 20628841:132:135
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133 First, like WT-CFTR, the slow component for Y1219W is too obscure for reliable curve fitting.
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ABCC7 p.Tyr1219Trp 20628841:133:44
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162 If different mutations at Y1219 can affect the entry rate and the exit rate differently as shown in Table 2, this hypothesis may explain most of the results Table 1 Parameter sets (s-1 ) for the ''kiss and run`` hypothesis kCO1 kO1C kO1O2 kO2C Y1219G 3 or 0a 3 2 9 10-2 3.8 9 10-2 Y1219I : : 1.3 9 10-2 : Y1219F : : 1.1 9 10-2 : Y1219W : : 4 9 10-3 : a kCO1 was set to 3 s-1 for simulating the ''with ATP`` condition and 0 s-1 for simulating the ''after the ATP washout`` condition.
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ABCC7 p.Tyr1219Trp 20628841:162:329
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166 b Representative reproduced macroscopic current relaxations mimicking those in Y1219G (red), Y1219I (green), Y1219F (cyan) and Y1219W (blue).
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ABCC7 p.Tyr1219Trp 20628841:166:127
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