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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.
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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.
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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.
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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).
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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.
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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).
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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.
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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.
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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.
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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.
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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.
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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
.
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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.
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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.
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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.
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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).
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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.
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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).
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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.
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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.
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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).
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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.
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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/(1Po;bas) values; notation as in Fig. 3 D. analogous constructs in the
K1250R
background (Fig. S4, A and B).
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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/(1Po;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).
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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.
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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/(1Po;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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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.
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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.
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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/(1Po;max) yielded a Gint of zero (0.03 ± 0.14 kT; Fig. 5 B; compare Fig. S4 C).
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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.
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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.
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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.
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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.
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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 (II0)/(ImaxI0) plotted as a function of [ATP] for WT (black),
F1296S
(red),
N1303Q
(blue), and
F1296S
/
N1303Q
(green).
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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).
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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.
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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.
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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
.
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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 (II0)/(ImaxI0) plotted as a function of [ATP] for WT (black),
R1358A
(red),
N1303Q
(blue), and
R1358A
/
N1303Q
(green).
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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).
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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
.
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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).
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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
.
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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.
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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).
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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).
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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.
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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 a
nd
R1358A/N1303Q
result from formation of a stabilizing interaction in state B (or breaking of a destabilizing interaction present in state A).
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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/(1Po;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/(1Po;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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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).
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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
).
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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.
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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).
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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).
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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
.
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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).
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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
.
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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.
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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).
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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.
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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 s1 (Fig. 8 A, magenta).
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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).
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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).
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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.
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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).
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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).
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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).
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