PMID: 20876359

Szollosi A, Vergani P, Csanady L
Involvement of F1296 and N1303 of CFTR in induced-fit conformational change in response to ATP binding at NBD2.
J Gen Physiol. 2010 Oct;136(4):407-23., [PubMed]
Sentences
No. Mutations Sentence Comment
18 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:18:42
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Arg1358Ala
X
ABCC7 p.Arg1358Ala 20876359:18:54
status: NEW
view ABCC7 p.Arg1358Ala details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:18:34
status: NEW
view ABCC7 p.Phe1296Ser details
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. Login to comment
19 ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:19:265
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:19:266
status: NEW
view ABCC7 p.Lys1250Arg details
Thermodynamic mutant cycles were built on several kinetic parameters that characterize individual steps in the gating cycle, such as apparent affinities for ATP, open probabilities in the absence of ATP, open probabilities in saturating ATP in a mutant background (K1250R), which precludes ATP hydrolysis, as well as the rates of nonhydrolytic closure. Login to comment
28 ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:28:141
status: NEW
view ABCC7 p.Lys1250Arg details
M AT E R I A L S A N D M E T H O D S Molecular biology CFTR mutants were constructed by using either pGEMHE-WT (Chan et al., 2000) or pGEMHE-K1250R (Vergani et al., 2005) as template. Login to comment
72 ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:72:280
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:72:295
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:72:314
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:72:359
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:72:142
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:72:161
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:72:307
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:72:352
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:72:134
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:72:154
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:72:288
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:72:344
status: NEW
view ABCC7 p.Phe1296Ser details
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). Login to comment
105 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:105:57
status: NEW
view ABCC7 p.Asn1303Gln details
By elongating the side chain at site 2, the substitution N1303Q might interfere with potential H bonds linking residue 1303 to either 1296 or 1358. Login to comment
109 ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:109:148
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:109:163
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:109:178
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:109:204
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:109:96
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:109:115
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:109:171
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:109:197
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:109:88
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:109:108
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:109:156
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:109:190
status: NEW
view ABCC7 p.Phe1296Ser details
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). Login to comment
111 ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:111:55
status: NEW
view ABCC7 p.Lys1250Arg details
Fig. S6 illustrates apparent affinities for ATP in the K1250R background. Login to comment
112 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:112:108
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Arg1358Ala
X
ABCC7 p.Arg1358Ala 20876359:112:90
status: NEW
view ABCC7 p.Arg1358Ala details
ABCC7 p.Arg1358Ala
X
ABCC7 p.Arg1358Ala 20876359:112:101
status: NEW
view ABCC7 p.Arg1358Ala details
Fig. S7 shows example macroscopic current traces to illustrate the apparent affinities of R1358A and R1358A/N1303Q for ATP. Login to comment
113 ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:113:108
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:113:134
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:113:100
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:113:127
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:113:93
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:113:120
status: NEW
view ABCC7 p.Phe1296Ser details
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. Login to comment
118 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:118:111
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:118:134
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:118:99
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:118:127
status: NEW
view ABCC7 p.Phe1296Ser details
(A-D) Inward chloride currents recorded in patches excised from resting oocytes expressing WT (A), F1296S (B), N1303Q (C), and F1296S/N1303Q (D) CFTR. Login to comment
122 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:122:80
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:122:99
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:122:307
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:122:350
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:122:72
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:122:92
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:122:288
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:122:343
status: NEW
view ABCC7 p.Phe1296Ser details
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. Login to comment
127 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:127:164
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:127:216
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:127:153
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:127:209
status: NEW
view ABCC7 p.Phe1296Ser details
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. Login to comment
129 ABCC7 p.Arg1358Ala
X
ABCC7 p.Arg1358Ala 20876359:129:37
status: NEW
view ABCC7 p.Arg1358Ala details
To perturb site 3, we chose mutation R1358A, which is likely to prevent a possible hydrogen-bonding interaction between the R1358 and N1303 side chains. Login to comment
131 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:131:41
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:131:60
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:131:33
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:131:53
status: NEW
view ABCC7 p.Phe1296Ser details
(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. Login to comment
132 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:132:55
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:132:81
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:132:41
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:132:74
status: NEW
view ABCC7 p.Phe1296Ser details
(B) Estimation of Po;max for WT (black), F1296S (red), N1303Q (blue), and F1296S/N1303Q (green) by stationary noise analysis. Login to comment
138 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:138:163
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:138:183
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:138:310
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:138:155
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:138:175
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:138:303
status: NEW
view ABCC7 p.Phe1296Ser details
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). Login to comment
140 ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:140:101
status: NEW
view ABCC7 p.Lys1250Arg details
Because openings in the absence of ATP must necessarily be nonhydrolytic, the NBD2 Walker A mutation K1250R, known to abolish ATP hydrolysis in ABC proteins (Lerner-Marmarosh et al., 1999; Payen et al., 2005), is not expected to affect this spontaneous gating. Login to comment
141 ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:141:62
status: NEW
view ABCC7 p.Lys1250Arg details
To test this idea, we studied the same mutant cycle also in a K1250R background (Fig. 4). Login to comment
142 ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:142:17
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:142:32
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:142:51
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:142:44
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:142:25
status: NEW
view ABCC7 p.Phe1296Ser details
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. Login to comment
146 ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:146:169
status: NEW
view ABCC7 p.Lys1250Arg details
Although Figure 4.  The stabilizing site-1-site-2 interaction that facilitates channel opening in the absence of ATP is preserved in the ATP hydrolysis-deficient K1250R mutant. Login to comment
147 ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:147:29
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:147:44
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:147:59
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:147:85
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:147:52
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:147:78
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:147:37
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:147:71
status: NEW
view ABCC7 p.Phe1296Ser details
(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). Login to comment
148 ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:148:29
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:148:52
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:148:73
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:148:106
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:148:66
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:148:99
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:148:45
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:148:92
status: NEW
view ABCC7 p.Phe1296Ser details
(B) Estimation of Po;max for K1250R (black), F1296S/K1250R (red), N1303Q/K1250R (blue), and F1296S/N1303Q/K1250R (green) by stationary noise analysis. Login to comment
150 ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:150:128
status: NEW
view ABCC7 p.Lys1250Arg details
(D) Thermodynamic mutant cycle built on Po;bas/(1Po;bas) values; notation as in Fig. 3 D. analogous constructs in the K1250R background (Fig. S4, A and B). Login to comment
152 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:152:42
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:152:125
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ala
X
ABCC7 p.Phe1296Ala 20876359:152:35
status: NEW
view ABCC7 p.Phe1296Ala details
ABCC7 p.Phe1296Ala
X
ABCC7 p.Phe1296Ala 20876359:152:114
status: NEW
view ABCC7 p.Phe1296Ala details
Again, Po;bas of the double mutant F1296A/N1303Q was 10-fold larger than that of WT or the single mutants F1296A and N1303Q (Fig. S5, A-C), producing a negative Gint for the mutant cycle built on Po;bas/(1Po;bas) values (Fig. S5 D), even though in this case the overall free energy change (1.18 ± 0.84 kT) could not be claimed significantly different from zero because of the smaller Po;bas values obtained for WT in this set of experiments (Fig. S5 C, black). Login to comment
155 ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:155:128
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:155:121
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:155:114
status: NEW
view ABCC7 p.Phe1296Ser details
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. Login to comment
157 ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:157:95
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:157:96
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:157:88
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:157:89
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:157:81
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:157:82
status: NEW
view ABCC7 p.Phe1296Ser details
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). Login to comment
160 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:160:140
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:160:160
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:160:132
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:160:152
status: NEW
view ABCC7 p.Phe1296Ser details
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. Login to comment
161 ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:161:33
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:161:56
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:161:77
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:161:110
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:161:70
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:161:103
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:161:49
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:161:96
status: NEW
view ABCC7 p.Phe1296Ser details
(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. Login to comment
168 ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:168:25
status: NEW
view ABCC7 p.Lys1250Arg details
Interestingly, Po;max of K1250R (0.68 ± 0.06; n = 6) was only slightly affected by the substitutions at sites 1 and 2, and even these small changes were mostly additive (Fig. 5 A; compare Fig. S4 B), such that a mutant cycle built on Po;max/(1Po;max) yielded a Gint of zero (0.03 ± 0.14 kT; Fig. 5 B; compare Fig. S4 C). Login to comment
171 ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:171:4
status: NEW
view ABCC7 p.Lys1250Arg details
The K1250R mutation itself is known to prolong open-channel burst durations by 20-30-fold (Vergani et al., 2005; Csanády et al., 2006) due to the slow rate of dissociation of the ATP-bound NBD dimer in the absence of ATP hydrolysis. Login to comment
172 ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:172:82
status: NEW
view ABCC7 p.Lys1250Arg details
Consistent with those reports, upon the sudden removal of ATP, we saw macroscopic K1250R currents decline with a time constant of 8 s (Fig. 5 C, black single-exponential fit In a nonhydrolytic background, interaction between sites 1 and 2 is similar for ATP-bound closed and open states, but changes after ATP removal Because the interaction between sites 1 and 2 changes during ATP-independent spontaneous openings (Figs. 3 D and 4 D), we wondered whether the same interaction also plays a role in normal, ATP-dependent channel opening. Login to comment
175 ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:175:182
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:175:183
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:175:229
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:175:230
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:175:244
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:175:245
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:175:260
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:175:261
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:175:286
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:175:287
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:175:252
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:175:253
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:175:279
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:175:280
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:175:237
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:175:238
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:175:272
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:175:273
status: NEW
view ABCC7 p.Phe1296Ser details
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. Login to comment
176 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:176:96
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:176:129
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:176:76
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:176:122
status: NEW
view ABCC7 p.Phe1296Ser details
(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. Login to comment
177 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:177:128
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:177:154
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:177:114
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:177:147
status: NEW
view ABCC7 p.Phe1296Ser details
(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). Login to comment
184 ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:184:136
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:184:355
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:184:36
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:184:348
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:184:21
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:184:340
status: NEW
view ABCC7 p.Phe1296Ser details
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). Login to comment
186 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:186:47
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Arg1358Ala
X
ABCC7 p.Arg1358Ala 20876359:186:29
status: NEW
view ABCC7 p.Arg1358Ala details
ABCC7 p.Arg1358Ala
X
ABCC7 p.Arg1358Ala 20876359:186:40
status: NEW
view ABCC7 p.Arg1358Ala details
(A) Representative traces of R1358A and R1358A/N1303Q currents illustrating segments in 0 mM ATP and bracketing segments in 2 mM ATP. Dotted lines show zero current level. Login to comment
187 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:187:55
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:187:81
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Arg1358Ala
X
ABCC7 p.Arg1358Ala 20876359:187:41
status: NEW
view ABCC7 p.Arg1358Ala details
ABCC7 p.Arg1358Ala
X
ABCC7 p.Arg1358Ala 20876359:187:74
status: NEW
view ABCC7 p.Arg1358Ala details
(B) Estimation of Po;max for WT (black), R1358A (red), N1303Q (blue), and R1358A/N1303Q (green) by stationary noise analysis. Login to comment
188 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:188:81
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Arg1358Ala
X
ABCC7 p.Arg1358Ala 20876359:188:42
status: NEW
view ABCC7 p.Arg1358Ala details
ABCC7 p.Arg1358Ala
X
ABCC7 p.Arg1358Ala 20876359:188:74
status: NEW
view ABCC7 p.Arg1358Ala details
Estimated Po;max was 0.62 ± 0.05 for R1358A and 0.36 ± 0.04 for R1358A/N1303Q. Login to comment
191 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:191:128
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:191:154
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Arg1358Ala
X
ABCC7 p.Arg1358Ala 20876359:191:114
status: NEW
view ABCC7 p.Arg1358Ala details
ABCC7 p.Arg1358Ala
X
ABCC7 p.Arg1358Ala 20876359:191:147
status: NEW
view ABCC7 p.Arg1358Ala details
(E) ATP-dependent current fractions (II0)/(ImaxI0) plotted as a function of [ATP] for WT (black), R1358A (red), N1303Q (blue), and R1358A/N1303Q (green). Login to comment
195 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:195:92
status: NEW
view ABCC7 p.Asn1303Gln details
channels retained substantial basal activity after ATP removal (Fig. 7 A; traces for WT and N1303Q are illustrated in Fig. 3 A). Login to comment
196 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:196:271
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:196:298
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Arg1358Ala
X
ABCC7 p.Arg1358Ala 20876359:196:253
status: NEW
view ABCC7 p.Arg1358Ala details
ABCC7 p.Arg1358Ala
X
ABCC7 p.Arg1358Ala 20876359:196:264
status: NEW
view ABCC7 p.Arg1358Ala details
Combining Po;bas/Po;max, obtained from current segments in 0 mM and bracketing periods in 2 mM ATP with Po;max estimated for the 2-mM ATP segments using stationary noise analysis (Fig. 7 B), provided Po;bas estimates (Fig. 7 C) that were higher in both R1358A and R1358A/N1303Q compared with WT or N1303Q. Login to comment
199 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:199:188
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Arg1358Ala
X
ABCC7 p.Arg1358Ala 20876359:199:170
status: NEW
view ABCC7 p.Arg1358Ala details
ABCC7 p.Arg1358Ala
X
ABCC7 p.Arg1358Ala 20876359:199:181
status: NEW
view ABCC7 p.Arg1358Ala details
We also investigated a possible change in coupling between sites 2 and 3 upon ATP binding by studying [ATP] dependence of macroscopic currents (sample current traces for R1358A and R1358A/N1303Q are shown in Fig. S7, A and B). Login to comment
200 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:200:138
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Arg1358Ala
X
ABCC7 p.Arg1358Ala 20876359:200:131
status: NEW
view ABCC7 p.Arg1358Ala details
ABCC7 p.Arg1358Ala
X
ABCC7 p.Arg1358Ala 20876359:200:239
status: NEW
view ABCC7 p.Arg1358Ala details
Fitting the [ATP] dose-response curve of the ATP-sensitive current fractions (Fig. 7 E) yielded a slightly increased KPo value for R1358A/N1303Q (inset), but for the calculated KrCO values (Fig. 7 F), a similar trend was apparent even for R1358A. Login to comment
205 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:205:287
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:205:524
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:205:544
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:205:279
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:205:516
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:205:536
status: NEW
view ABCC7 p.Phe1296Ser details
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. Login to comment
209 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:209:78
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:209:163
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:209:67
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:209:156
status: NEW
view ABCC7 p.Phe1296Ser details
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). Login to comment
213 ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:213:13
status: NEW
view ABCC7 p.Lys1250Arg details
Thus, in the K1250R background, apparent ATP affinities were three- to fourfold decreased (Fig. S6, A and B), corresponding to six- to ninefold increased values of KrCO (Fig. S6 C), but a mutant cycle built on the latter values yielded a Gint not significantly different from zero (Fig. S6 D). Login to comment
214 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:214:405
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Arg1358Ala
X
ABCC7 p.Arg1358Ala 20876359:214:376
status: NEW
view ABCC7 p.Arg1358Ala details
Truncation of the site-3 arginine side chain promotes spontaneous, ATP-independent opening regardless of the side chain at site 2 To determine the functional importance of site 3 within our triad of target residues (Fig. 1), we investigated functional coupling between sites 2 (position 1303) and 3 (position 1358) by comparing the effects of removal of the R1358 side chain (R1358A) in either a WT or an N1303Q background. Login to comment
215 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:215:78
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:215:80
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Arg1358Ala
X
ABCC7 p.Arg1358Ala 20876359:215:60
status: NEW
view ABCC7 p.Arg1358Ala details
ABCC7 p.Arg1358Ala
X
ABCC7 p.Arg1358Ala 20876359:215:62
status: NEW
view ABCC7 p.Arg1358Ala details
ABCC7 p.Arg1358Ala
X
ABCC7 p.Arg1358Ala 20876359:215:71
status: NEW
view ABCC7 p.Arg1358Ala details
ABCC7 p.Arg1358Ala
X
ABCC7 p.Arg1358Ala 20876359:215:73
status: NEW
view ABCC7 p.Arg1358Ala details
Interestingly, after prephosphorylation by 300 nM PKA, both R1358A and R1358A/N1303Q result from formation of a stabilizing interaction in state B (or breaking of a destabilizing interaction present in state A). Login to comment
227 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:227:119
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:227:138
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:227:111
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:227:131
status: NEW
view ABCC7 p.Phe1296Ser details
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). Login to comment
228 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:228:247
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:228:295
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:228:240
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:228:284
status: NEW
view ABCC7 p.Phe1296Ser details
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). Login to comment
242 ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 20876359:242:241
status: NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 20876359:242:54
status: NEW
view ABCC7 p.Asp1370Asn details
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 20876359:242:249
status: NEW
view ABCC7 p.Glu1371Ser details
ABCC7 p.Glu1371Gln
X
ABCC7 p.Glu1371Gln 20876359:242:261
status: NEW
view ABCC7 p.Glu1371Gln details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:242:233
status: NEW
view ABCC7 p.Lys1250Arg details
Although for WT CFTR and for the nonhydrolytic mutant D1370N these two parameters are in rough agreement (Csanády et al., 2010), such comparisons have not yet been done for several other NBD2mutantsdefectiveinATPhydrolysis(e.g.,K1250R, K1250A, E1371S, and E1371Q). Login to comment
268 ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:268:85
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:268:50
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:268:43
status: NEW
view ABCC7 p.Phe1296Ser details
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. Login to comment
269 ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:269:202
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:269:228
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:269:120
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:269:221
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:269:112
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:269:213
status: NEW
view ABCC7 p.Phe1296Ser details
(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). Login to comment
272 ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:272:78
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:272:71
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:272:64
status: NEW
view ABCC7 p.Phe1296Ser details
in an unchanged Po;max (Fig. 8 B), just as we have observed for F1296S/N1303Q/K1250R (Fig. 5 A). Login to comment
274 ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:274:77
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:274:103
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:274:69
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:274:96
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:274:62
status: NEW
view ABCC7 p.Phe1296Ser details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:274:89
status: NEW
view ABCC7 p.Phe1296Ser details
Such predicted time courses are summarized in Fig. S8 for WT, F1296S/N1303Q, K1250R, and F1296S/N1303Q/K1250R. Login to comment
275 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:275:78
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:275:71
status: NEW
view ABCC7 p.Phe1296Ser details
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). Login to comment
276 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:276:275
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:276:268
status: NEW
view ABCC7 p.Phe1296Ser details
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. Login to comment
281 ABCC7 p.Arg1358Ala
X
ABCC7 p.Arg1358Ala 20876359:281:65
status: NEW
view ABCC7 p.Arg1358Ala details
The observed facilitation of spontaneous channel openings by the R1358A mutation (Fig. 7 C) therefore likely reflects loss of a stabilizing interaction in the C1 state between R1358 and a residue other than N1303. Login to comment
286 ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:286:21
status: NEW
view ABCC7 p.Lys1250Arg details
nonhydrolytic mutant K1250R (Fig. 5 C, black). Login to comment
287 ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:287:111
status: NEW
view ABCC7 p.Lys1250Arg details
The Po;max values of 0.6 measured for the long-burst nonhydrolytic mutants (Fig. 5 A) suggest that the K1250R mutation, in addition to abrogating ATP hydrolysis, also slows maximal opening rate. Login to comment
288 ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:288:39
status: NEW
view ABCC7 p.Lys1250Arg details
We therefore modeled the effect of the K1250R mutation by simultaneously setting rate O2→C1 to zero and rate C4→O2 to 0.2 s1 (Fig. 8 A, magenta). Login to comment
291 ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:291:176
status: NEW
view ABCC7 p.Lys1250Arg details
Parameters Po;bas and KPo calculated for Scheme 2 using the rates plotted in black in Fig. 8 A, as well as Po;max and relax calculated using the two rates adjusted for K1250R (Fig. 8 A, magenta), are in good agreement with the measured values (Fig. 8 B, left column, measured values are shown in parentheses below each calculated parameter). Login to comment
293 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:293:44
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:293:55
status: NEW
view ABCC7 p.Phe1296Ser details
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). Login to comment
295 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:295:40
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:295:33
status: NEW
view ABCC7 p.Phe1296Ser details
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. Login to comment
297 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:297:145
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:297:138
status: NEW
view ABCC7 p.Phe1296Ser details
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). Login to comment
298 ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 20876359:298:186
status: NEW
view ABCC7 p.Lys1250Arg details
ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:298:179
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:298:172
status: NEW
view ABCC7 p.Phe1296Ser details
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). Login to comment
300 ABCC7 p.Asn1303Gln
X
ABCC7 p.Asn1303Gln 20876359:300:166
status: NEW
view ABCC7 p.Asn1303Gln details
ABCC7 p.Phe1296Ser
X
ABCC7 p.Phe1296Ser 20876359:300:159
status: NEW
view ABCC7 p.Phe1296Ser details
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). Login to comment