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PMID: 12508051
Vergani P, Nairn AC, Gadsby DC
On the mechanism of MgATP-dependent gating of CFTR Cl- channels.
J Gen Physiol. 2003 Jan;121(1):17-36.,
[PubMed]
Sentences
No.
Mutations
Sentence
Comment
4
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:4:204
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:4:185
status:
NEW
view ABCC7 p.Lys464Ala details
ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:4:214
status:
NEW
view ABCC7 p.Asp1370Asn details
The rate of opening to a burst (1/ib) was a saturable function of [MgATP], but apparent affinity was reduced by mutations in either of CFTR`s nucleotide binding domains (NBDs):
K464A
in NBD1, and
K1250A
or
D1370N
in NBD2.
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7
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:7:30
status:
NEW
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ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:7:38
status:
NEW
view ABCC7 p.Asp1370Asn details
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 12508051:7:50
status:
NEW
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NBD2 catalytic site mutations
K1250A
,
D1370N
, and
E1371S
were found to prolong open bursts.
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9
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:9:65
status:
NEW
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However, when hydrolysis at NBD2 was impaired, the NBD1 mutation
K464A
shortened the prolonged open bursts.
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32
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:32:44
status:
NEW
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ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:32:103
status:
NEW
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ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:32:260
status:
NEW
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ABCC7 p.Asp572Asn
X
ABCC7 p.Asp572Asn 12508051:32:245
status:
NEW
view ABCC7 p.Asp572Asn details
However, in CFTR the Walker A NBD2 mutation
K1250A
abolished ATP hydrolysis, whereas the NBD1 mutation
K464A
simply reduced overall hydrolytic activity (Ramjeesingh et al., 1999); and biochemical studies of Walker B aspartate mutations in CFTR (
D572N
in NBD1,
D1370N
in NBD2) have not yet been performed.
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34
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:34:10
status:
NEW
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ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:34:216
status:
NEW
view ABCC7 p.Lys464Ala details
ABCC7 p.Gln552His
X
ABCC7 p.Gln552His 12508051:34:234
status:
NEW
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ABCC7 p.Gln552Ala
X
ABCC7 p.Gln552Ala 12508051:34:223
status:
NEW
view ABCC7 p.Gln552Ala details
Thus, the
K1250A
mutation dramatically prolonged burst duration, suggesting that hydrolysis at NBD2 might be coupled to burst termination (Carson et al., 1995; Gunderson and Kopito, 1995), whereas the NBD1 mutations
K464A
,
Q552A
, and
Q552H
somewhat slowed channel opening to a burst, suggesting that NBD1 might be a site of ATP interactions governing opening (Carson et al., 1995; Carson and Welsh 1995).
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41
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:41:203
status:
NEW
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ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:41:193
status:
NEW
view ABCC7 p.Lys464Ala details
ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:41:247
status:
NEW
view ABCC7 p.Asp1370Asn details
We studied in detail the dependence of channel gating on [MgATP], gating in the presence of poorly hydrolyzable nucleotide analogs, as well as the effects of mutating residues in the Walker A (
K464A
and
K1250A
) and Walker B motifs (in particular,
D1370N
in NBD2).
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52
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:52:127
status:
NEW
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ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:52:143
status:
NEW
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ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:52:137
status:
NEW
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ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:52:240
status:
NEW
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ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:52:250
status:
NEW
view ABCC7 p.Asp1370Asn details
Amounts of cRNA injected were adjusted to vary the level of expression: up to 40 ng/oocyte was required for high expression of
K1250A
or
K464A
/
K1250A
mutant channels, whereas 0.1-0.25 ng/oocyte sufficed for single channel recordings of WT,
K464A
, or
D1370N
channels.
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85
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:85:496
status:
NEW
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We do not report absolute values for ib and rCO in these cases, but only values relative to some other experimental condition applied to the same patch, and these should be relatively insensitive to N. Thus, for MgATP dose-response curves (Fig. 2), rates were normalized to those in bracketing segments at 5 mM MgATP; for the poorly hydrolyzable nucleotides, rates were normalized to those obtained in the same patches at 10 M (Figs. 7 and 11) or 50 M MgATP (Fig. 8); for
K1250A
mutant openings in 10 M MgATP, rates were normalized to those in nominally MgATP-free bath solution.
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89
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:89:65
status:
NEW
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ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:89:71
status:
NEW
view ABCC7 p.Asp1370Asn details
T A B L E I Kinetic Parameters of WT and Mutant CFTR Channels WT
K464A
D1370N
mean Ϯ SEM n mean Ϯ SEM n mean Ϯ SEM n (A) 5 mM MgATP ϩ 300 nM PKA b 644 Ϯ 63 30 620 Ϯ 58 21 3,768 Ϯ 499 21 ib 1,671 Ϯ 172 30 2,760 Ϯ 439 21 3,588 Ϯ 414 21 1,552 Ϯ 170 19 2,438 Ϯ 483 12 2,849 Ϯ 491 12 F 19.3 Ϯ 2.0 30 20.8 Ϯ 2.1 21 49.9 Ϯ 4.3 21 nF 0.57 Ϯ 0.06 30 0.50 Ϯ 0.06 21 2.76 Ϯ 0.25 21 rCO 0.75 Ϯ 0.06 30 0.50 Ϯ 0.05 21 0.38 Ϯ 0.05 21 0.77 Ϯ 0.08 19 0.54 Ϯ 0.08 12 0.47 Ϯ 0.07 12 rOC 1.95 Ϯ 0.15 30 1.92 Ϯ 0.15 21 0.43 Ϯ 0.07 21 (B) 5 mM MgATP b 338 Ϯ 22 18 309 Ϯ 23 8 1,748 Ϯ 215 17 ib 4,506 Ϯ 497 18 6,752 Ϯ 1314 8 9,503 Ϯ 1440 17 4,454 Ϯ 1382 5 6,928 Ϯ 1666 6 7,584 Ϯ 1967 9 F 23.5 Ϯ 3.2 18 16.1 Ϯ 2.2 8 51.5 Ϯ 6.0 17 nF 0.42 Ϯ 0.05 18 0.39 Ϯ 0.06 8 1.40 Ϯ 0.13 17 rCO 0.27 Ϯ 0.03 18 0.18 Ϯ 0.03 8 0.16 Ϯ 0.03 17 0.33 Ϯ 0.09 5 0.18 Ϯ 0.03 6 0.22 Ϯ 0.05 9 rOC 3.28 Ϯ 0.21 18 3.43 Ϯ 0.25 8 0.75 Ϯ 0.09 17 (C) 50 M MgATP b 355 Ϯ 44 12 323 Ϯ 136 4 1,433 Ϯ 381 4 F 27.3 Ϯ 5.2 12 22.1 Ϯ 4.4 4 46.2 Ϯ 10.8 4 nF 0.38 Ϯ 0.05 12 0.45 Ϯ 0.11 4 1.91 Ϯ 0.34 4 (D) 5 mM MgAMPPNP b 1,619 Ϯ 232 32 271 Ϯ 52 8 F 59.5 Ϯ 6.6 32 26.8 Ϯ 7.7 8 nF 2.40 Ϯ 0.26 32 0.38 Ϯ 0.10 8 Kinetic parameters were obtained using a maximum likelihood simultaneous fit to dwell-time histograms at all conductance levels (Csanády, 2000).
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94
ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:94:65
status:
NEW
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The significance of the slight prolongation of F for the
D1370N
mutant and for WT in 5 mM MgAMPPNP is unknown, but the rate rOF remained 1-2 s-1 for all conditions and mutants tested.
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113
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:113:54
status:
NEW
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ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:113:64
status:
NEW
view ABCC7 p.Asp1370Asn details
(B and C) Representative traces for prephosphorylated
K464A
and
D1370N
channels.
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114
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:114:143
status:
NEW
view ABCC7 p.Lys464Ala details
ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:114:170
status:
NEW
view ABCC7 p.Asp1370Asn details
Relative opening (D) and closing (E) rates (mean Ϯ SEM, 2 Յ n Յ 7) from analysis of records as in A-C for WT (blue circles),
K464A
(red triangles), and
D1370N
(green squares) channels at 10 M Յ [MgATP] Յ 5 mM, plotted on semilogarithmic axes.
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116
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:116:159
status:
NEW
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ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:116:170
status:
NEW
view ABCC7 p.Asp1370Asn details
Curves in D show Michaelis-Menten fits, yielding K0.5 of 56 Ϯ 5, 807 Ϯ 185, 391 Ϯ 118 M, and rCOmax of 1.02, 1.16, and 1.08, for WT,
K464A
, and
D1370N
, respectively.
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123
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:123:23
status:
NEW
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ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:123:309
status:
NEW
view ABCC7 p.Lys464Ala details
ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:123:59
status:
NEW
view ABCC7 p.Asp1370Asn details
ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:123:320
status:
NEW
view ABCC7 p.Asp1370Asn details
Compared with WT, both
K464A
(Walker A lysine in NBD1) and
D1370N
(Walker B aspartate in NBD2) mutant CFTR channels opened less frequently at low [MgATP] (e.g., 50 M; Figs. 2, A-D), and this defect could be largely overcome by raising the [MgATP], so that, at saturating [MgATP], opening rates of WT,
K464A
, and
D1370N
channels differed by less than a factor of two (Table I).
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125
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:125:222
status:
NEW
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ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:125:232
status:
NEW
view ABCC7 p.Asp1370Asn details
As expected (see below) for channels in which opening rate, but not closing rate, is sensitive to [MgATP], the dependence of Po on [MgATP] was not very different from that of rCO, shown in Fig. 2 D, for WT (see Fig. 3 C),
K464A
, or
D1370N
channels.
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126
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:126:93
status:
NEW
view ABCC7 p.Lys1250Ala details
Similar kinetic analysis of patches containing few channels proved technically difficult for
K1250A
CFTR (NBD2 Walker A lysine mutant) due to the extremely prolonged bursts (see Fig. 6 C, below), which precluded collection of enough events to reliably estimate absolute values of rCO or Po.
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127
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:127:82
status:
NEW
view ABCC7 p.Lys1250Ala details
So we recorded macroscopic current in patches with hundreds or thousands of WT or
K1250A
channels (Fig. 3, A and B), and determined relative Po as a function of [MgATP] (Fig. 3 C) by normalizing current amplitude at each test [MgATP] to that during bracketing exposures at 5 mM MgATP (Fig. 3, A and B).
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128
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:128:14
status:
NEW
view ABCC7 p.Lys1250Ala details
The curve for
K1250A
was strongly shifted to higher [MgATP] and was still not saturated at 10 mM MgATP.
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132
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:132:14
status:
NEW
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Therefore, in
K1250A
, as in WT CFTR, it is only the dependence of channel opening rate on [MgATP] that underlies the [MgATP] dependence of Po.
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134
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:134:111
status:
NEW
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ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:134:210
status:
NEW
view ABCC7 p.Lys1250Ala details
In fact, this relationship implies that the effective dissociation constant for MgATP activation of opening of
K1250A
channels is likely even larger than is apparent in Fig. 3 C because the other effect of the
K1250A
mutation, marked slowing of channel closure from bursts, would by itself shift the Po versus [MgATP] curve to lower [MgATP], opposite to our experimental observation.
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137
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:137:4
status:
NEW
view ABCC7 p.Lys1250Ala details
The
K1250A
mutation strongly shifts the [MgATP] dependence of Po to higher [MgATP].
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140
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:140:27
status:
NEW
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(B) Macroscopic current of
K1250A
channels was reduced Ն2-fold on lowering [MgATP] from 5 to 1 mM.
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144
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:144:108
status:
NEW
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ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:144:213
status:
NEW
view ABCC7 p.Lys1250Ala details
Michaelis fit parameters for WT: Po max ϭ 1.04 Ϯ 0.01, K0.5 ϭ 57 Ϯ 2 M; for
K1250A
: Po max ϭ 2.45 Ϯ 0.88, K0.5 ϭ 6.5 Ϯ 4.8 mM; for display, WT (circles) and
K1250A
(inverted triangles) data (mean Ϯ SD, 3 Յ n Յ9) were renormalized to these Po max values.
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145
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:145:75
status:
NEW
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Because 10 mM, the highest [MgATP] used, was still far from saturating for
K1250A
channels, the fit for this mutant is less accurate, evident from large errors on fit parameters.
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151
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:151:128
status:
NEW
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Catalytic Site Mutations at NBD1 Do Not Alter Channel Closing from Normal, MgATP-elicited Bursts The average rate of closure of
K464A
mutant CFTR channels from open bursts was closely similar to that of WT CFTR under comparable conditions (Figs. 4, A-F, and 5, A, B, and E); it was likewise approximately independent of [MgATP] (Fig. 2 E, red triangles) and it was similarly reduced roughly twofold by strong phosphorylation (Fig. 4, D and E; Table I).
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152
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:152:50
status:
NEW
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Also like WT, the burst duration distributions of
K464A
mutant channels were well described by single exponential functions (Fig. 4, D-F).
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154
ABCC7 p.Asp572Asn
X
ABCC7 p.Asp572Asn 12508051:154:124
status:
NEW
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ABCC7 p.Ser573Glu
X
ABCC7 p.Ser573Glu 12508051:154:269
status:
NEW
view ABCC7 p.Ser573Glu details
The mean closing rate from bursts was not substantially altered by these NBD1 mutations (compare Fig. 5 E and Table I): for
D572N
, rOC(5 mM MgATP ϩ PKA) ϭ 1.4 Ϯ 0.2 s-1 (n ϭ 9), and rOC(5 mM MgATP) ϭ 3.1 Ϯ 0.6 s-1 (n ϭ 3); for
S573E
, rOC(5 mM MgATP ϩ PKA) ϭ 2.2 Ϯ 0.3 s-1 (n ϭ 7).
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156
ABCC7 p.Asp572Asn
X
ABCC7 p.Asp572Asn 12508051:156:10
status:
NEW
view ABCC7 p.Asp572Asn details
Thus, for
D572N
CFTR, rCO(5 mM MgATP ϩ PKA) ϭ 0.34 Ϯ 0.1 s-1 (n ϭ 9), and rCO(5 mM MgATP) ϭ 0.35 Ϯ 0.1 s-1 (n ϭ 3), although these values ("total" estimates, see materials and methods) likely overestimate true opening rate, as the somewhat lower maximal Po (0.18 vs. 0.29 for WT) of this mutant precluded Figure 4.
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157
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:157:58
status:
NEW
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Burst duration distributions are similar for WT (A-C) and
K464A
(D-F) channels under comparable conditions, as indicated (PKA present for left column only).
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160
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:160:9
status:
NEW
view ABCC7 p.Lys464Ala details
Only for
K464A
at M MgATP (F) could the likelihood be significantly increased by including a second component, though with a shorter (but not longer; Ikuma and Welsh, 2000) mean: 1 ϭ 30 ms, a1 ϭ 0.17; 2 ϭ 263 ms, a2 ϭ 0.83; increase in log likelihood, ⌬LL ϭ 8.3; number of bursts fitted, M ϭ 263; giving (⌬LL - ln(2M) ϭ 2.0).
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161
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:161:390
status:
NEW
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The small differences between means at mM and M MgATP (B vs. C, E vs. F) may be only apparent, as the mean b, estimated by multichannel kinetic fits, from these same stretches of record at M MgATP is not significantly different from that during intervening stretches in 5 mM MgATP (for WT: bM/b5mM ϭ 1.03 Ϯ 0.07, n ϭ 9; for
K464A
: bM/b5mM ϭ 0.95 Ϯ 0.13, n ϭ 7).
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162
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:162:50
status:
NEW
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ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:162:60
status:
NEW
view ABCC7 p.Asp1370Asn details
(G and H) Representative traces showing gating of
K464A
and
D1370N
channels at 15 M MgATP (after PKA removal).
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163
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:163:20
status:
NEW
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Prolonged bursts of
K464A
channels (Ikuma and Welsh, 2000) are not evident.
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164
ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:164:70
status:
NEW
view ABCC7 p.Asp1370Asn details
Though variability among the four patches containing sufficiently few
D1370N
channels precluded pooling the data for burst distribution analysis, in none of those patches (analyzed separately) did introduction of a second component significantly improve the maximum likelihood fit.
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166
ABCC7 p.Ser573Glu
X
ABCC7 p.Ser573Glu 12508051:166:4
status:
NEW
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For
S573E
channels, rCO(5 mM MgATP ϩ PKA) ϭ 0.9 Ϯ 0.2 s-1 (n ϭ 7, total estimate) and 1 Ϯ 0.2 s-1 (n ϭ 4, best estimate).
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168
ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:168:0
status:
NEW
view ABCC7 p.Asp1370Asn details
ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:168:247
status:
NEW
view ABCC7 p.Asp1370Asn details
D1370N
channels closed 4-5-fold more slowly than WT CFTR (Figs. 2 E and 6, A vs. B; Table I), and this reduced closing rate was constant at all [MgATP] tested (Figs. 2 E and 4 H), although, as for WT CFTR, strong phosphorylation slowed closing of
D1370N
channels roughly twofold (Table I).
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169
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:169:4
status:
NEW
view ABCC7 p.Lys1250Ala details
The
K1250A
mutation more dramatically slowed channel closing from bursts, resulting in prolonged bursts lasting tens of seconds (Fig. 6 C; cf. Carson et al., 1995; Gunderson and Kopito, 1995; Ramjeesingh et al., 1999; Zeltwanger et al., 1999).
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170
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:170:101
status:
NEW
view ABCC7 p.Lys1250Ala details
Analysis of the macroscopic current relaxation upon nucleotide withdrawal in patches containing many
K1250A
channels indicates that their average burst duration was 08ف s in the presence of PKA (see below, Fig. 10, E and G) but 04ف s after PKA had been removed (Fig. 3 B), at least two orders of magnitude longer than bursts of WT channels under the same conditions (Fig. 3, A vs. B; Fig. 6, A vs. C).
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171
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:171:19
status:
NEW
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ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:171:185
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:171:30
status:
NEW
view ABCC7 p.Asp1370Asn details
ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:171:221
status:
NEW
view ABCC7 p.Asp1370Asn details
Moreover, for both
K1250A
and
D1370N
mutants, this macroscopic current decay followed a single exponential time course, implying the presence of a single population of open bursts (for
K1250A
, see Figs. 3 B and 10 E; for
D1370N
, decay time constants were: [after 5 mM MgATP ϩ PKA] ϭ 6.4 Ϯ 1.6 s, n ϭ 6; [after 5 mM MgATP] ϭ 2.2 Ϯ 0.5 s, n ϭ 7; [after 300 M MgATP] ϭ 1.9 Ϯ 0.3 s, n ϭ 8; cf. Table I).
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179
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:179:20
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:179:8
status:
NEW
view ABCC7 p.Asp1370Asn details
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 12508051:179:36
status:
NEW
view ABCC7 p.Glu1371Ser details
WT (A),
D1370N
(B),
K1250A
(C), and
E1371S
(D) CFTR channels were activated by 5 mM MgATP plus PKA as indicated: burst termination (-4.0فpA downward steps) after nucleotide washout was slowed for NBD2 mutants, relative to WT.
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180
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:180:55
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 12508051:180:66
status:
NEW
view ABCC7 p.Glu1371Ser details
Note persistence of brief (intraburst) closures during
K1250A
and
E1371S
bursts, long after nucleotide withdrawal.
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183
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:183:30
status:
NEW
view ABCC7 p.Lys464Ala details
ABCC7 p.Asp572Asn
X
ABCC7 p.Asp572Asn 12508051:183:80
status:
NEW
view ABCC7 p.Asp572Asn details
ABCC7 p.Ser573Glu
X
ABCC7 p.Ser573Glu 12508051:183:44
status:
NEW
view ABCC7 p.Ser573Glu details
Patches contained one WT (A),
K464A
(B), or
S573E
(D) channel, or more than one
D572N
(C) channel.
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184
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:184:115
status:
NEW
view ABCC7 p.Lys464Ala details
ABCC7 p.Asp572Asn
X
ABCC7 p.Asp572Asn 12508051:184:122
status:
NEW
view ABCC7 p.Asp572Asn details
ABCC7 p.Ser573Glu
X
ABCC7 p.Ser573Glu 12508051:184:133
status:
NEW
view ABCC7 p.Ser573Glu details
(E) Summary of mean (ϮSEM) b values at 5 mM MgATP and 300 nM PKA (n ϭ 30, 21, 9, and 7 for WT,
K464A
,
D572N
, and
S573E
, respectively).
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218
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:218:46
status:
NEW
view ABCC7 p.Lys464Ala details
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:218:94
status:
NEW
view ABCC7 p.Lys464Ala details
Closing from Locked-open Bursts Is Faster for
K464A
Mutants than for WT Channels Although the
K464A
mutation did not alter open burst duration of channels exposed to MgATP (Figs. 2 E, 4, and 5), regardless of phosphorylation status (Fig. 4; Table I), it did significantly reduce the duration of certain unusually prolonged bursts.
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222
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:222:4
status:
NEW
view ABCC7 p.Lys464Ala details
For
K464A
channels, on the other hand (Fig. 10 B), the slow component comprised a somewhat smaller fraction (as ϭ 0.63 Ϯ 0.04, n ϭ 16, Fig. 10 C) of the current Figure 8.
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227
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:227:59
status:
NEW
view ABCC7 p.Lys464Ala details
The smaller fractional amplitude of the slow component for
K464A
channels can be explained by this observed shortening of their locked-open bursts without the mutation markedly altering the frequency of entry into such bursts.
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232
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:232:27
status:
NEW
view ABCC7 p.Lys464Ala details
The analogous estimate for
K464A
channels gives an average of 1 locking in every 6ف openings.
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234
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:234:95
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:234:4
status:
NEW
view ABCC7 p.Lys464Ala details
The
K464A
mutation also shortened (Fig. 10, E-G) the similarly prolonged bursts of NBD2 mutant
K1250A
channels exposed to MgATP alone (Fig. 6 C).
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235
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:235:148
status:
NEW
view ABCC7 p.Lys1250Ala details
The control record (Fig. 10 E) illustrates the slow decay of macroscopic current after washout of MgATP and PKA from a patch containing hundreds of
K1250A
CFTR Figure 9.
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242
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:242:4
status:
NEW
view ABCC7 p.Lys464Ala details
The
K464A
mutation speeds exit from locked open burst states.
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244
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:244:41
status:
NEW
view ABCC7 p.Lys464Ala details
(B) Current decay is much faster for the
K464A
mutant in the same conditions.
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245
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:245:186
status:
NEW
view ABCC7 p.Lys464Ala details
Blue fit lines in A and B show only the slow components of double exponential fits, with s ϭ 67.8s, as ϭ 0.92 for WT, and s ϭ 8.7s, as ϭ 0.79 for
K464A
.
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246
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:246:127
status:
NEW
view ABCC7 p.Lys464Ala details
(C and D) Summaries of fractional amplitude, as (C), and time constant, s (D), of the slow component from 18 WT and 16
K464A
experiments.
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247
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:247:193
status:
NEW
view ABCC7 p.Lys464Ala details
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:247:370
status:
NEW
view ABCC7 p.Lys464Ala details
In controls with no MgAMPPNP, closure after exposure to MgATP and PKA yielded ϭ 1.9 Ϯ 0.2 s (n ϭ 35) for WT and ϭ 1.0 Ϯ 0.1 s (n ϭ 34) for
K464A
, and both constructs sometimes showed a small amplitude slower component: for WT, s ϭ 7.6 Ϯ 1.7 s, as ϭ 0.1 Ϯ 0.03 (in 13/35 patches); for
K464A
, s ϭ 5.9 Ϯ 0.8 s, as ϭ 0.24 Ϯ 0.04 (20/24 patches).
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248
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:248:16
status:
NEW
view ABCC7 p.Lys1250Ala details
(E) Macroscopic
K1250A
currents, activated by 5 mM MgATP ϩ PKA, decay slowly on nucleotide withdrawal.
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249
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:249:121
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:249:163
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:249:19
status:
NEW
view ABCC7 p.Lys464Ala details
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:249:157
status:
NEW
view ABCC7 p.Lys464Ala details
(F) The additional
K464A
mutation accelerates channel closure from bursts: for the traces shown, ϭ 71.7s (
K1250A
) and ϭ 29.7s (
K464A
/
K1250A
).
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250
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:250:33
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:250:52
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:250:46
status:
NEW
view ABCC7 p.Lys464Ala details
(G) Mean time constants of all 9
K1250A
and 9
K464A
/
K1250A
relaxations, each well fit by a single exponential.
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253
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:253:32
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:253:240
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:253:26
status:
NEW
view ABCC7 p.Lys464Ala details
However, in double mutant
K464A
/
K1250A
CFTR channels (Fig. 10 F) the current relaxation time constant ( ϭ 36 Ϯ 4 s, n ϭ 9), and hence the mean open-burst dwell time, was less than half that of channels bearing the
K1250A
mutation alone (Fig. 10 G).
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254
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:254:89
status:
NEW
view ABCC7 p.Lys464Ala details
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:254:154
status:
NEW
view ABCC7 p.Lys464Ala details
Closing from Bursts During Activation by Poorly Hydrolyzable Analogs Alone Is Faster for
K464A
Mutants than for WT Channels Like WT CFTR (Fig. 7), mutant
K464A
channels could be opened by millimolar concentrations of the analogs MgAMPPNP or MgATP␥S alone (Fig. 11), with rates of opening to bursts of 1.5 Ϯ 0.2% (n ϭ 4) at 0.5 mM and 2.9 Ϯ 0.3% (n ϭ 4) at 5 mM MgAMPPNP, and 5.0 Ϯ 0.6% (n ϭ 8) at 2 mM MgATP␥S, of the maximal rate at saturating [MgATP], values not very different from those for WT channels under the same conditions.
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255
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:255:96
status:
NEW
view ABCC7 p.Lys464Ala details
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:255:126
status:
NEW
view ABCC7 p.Lys464Ala details
However, the 5-10-fold prolongation of WT bursts by these analogs (Fig. 7 A) was not evident in
K464A
channels (Fig. 11): for
K464A
channels opened by MgAMPPNP or MgATP␥S alone, the mean b values were only 1.1 Ϯ 0.2 (n ϭ 8) or 2.2 Ϯ 0.5 (n ϭ 8) times larger, respectively, than at 10 M MgATP.
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256
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:256:32
status:
NEW
view ABCC7 p.Lys464Ala details
Because this consequence of the
K464A
mutation is manifest during exposure to essentially nonhydrolyzable ATP analogs it cannot be ascribed to any failure of the mutant channel to hydrolyze nucleotide at the NBD1 catalytic site, but instead must be attributed to the alteration of NBD1 structure per se. D I S C U S S I O N We may draw several conclusions from these analyses of gating kinetics of WT and of NBD mutant CFTR channels, in the presence of MgATP and/or of poorly-hydrolyzable analogs: (a) nucleotide binds at both NBD1 and NBD2 catalytic sites before channel opening; (b) the slow opening transition, after nucleotide binding, is highly sensitive to the structures of the beta-␥ phosphate bridging group and of the ␥ phosphate; (c) no further nucleotide binding is required to terminate an open burst; (d) hydrolysis of the nucleotide at NBD2 precedes normal, rapid closing from bursts; (e) if that hydrolysis is prevented, the structure of the NBD1 catalytic site and of the nucleotide bound there can modulate rate of exit from the resulting prolonged (locked) open burst.
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266
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:266:73
status:
NEW
view ABCC7 p.Lys464Ala details
ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:266:89
status:
NEW
view ABCC7 p.Asp1370Asn details
Our results show that mutations within the Walker motifs of either NBD1 (
K464A
) or NBD2 (
D1370N
, Figure 11.
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267
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:267:28
status:
NEW
view ABCC7 p.Lys464Ala details
Gating of prephosphorylated
K464A
channels by poorly hydrolyzable ATP analogs, as indicated.
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268
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:268:22
status:
NEW
view ABCC7 p.Lys464Ala details
Unlike WT (Fig. 7 A),
K464A
burst duration was not increased during exposure to MgAMPPNP (A and B, b ϭ 270 Ϯ 50 ms, n ϭ 8), and was only slightly increased during exposure to ATP␥S (C, b ϭ 655 Ϯ 170 ms, n ϭ 8), compared with bursts in MgATP (b ϭ 276 Ϯ 21 ms, n ϭ 16) in the same patches.
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269
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:269:49
status:
NEW
view ABCC7 p.Lys464Ala details
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:269:289
status:
NEW
view ABCC7 p.Lys464Ala details
Note that, due to the lower apparent affinity of
K464A
for MgATP (Fig. 2), the relative opening rate of mutant channels at 10 M MgATP averaged only 2.3 Ϯ 0.8% (n ϭ 3) of that in saturating MgATP (compared with %11ف for WT), so the opening rate of
K464A
channels was similar in the presence of millimolar concentrations of the poorly hydrolyzable analogs or of 10 M MgATP.
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270
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:270:0
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:270:129
status:
NEW
view ABCC7 p.Lys464Ala details
ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:270:139
status:
NEW
view ABCC7 p.Asp1370Asn details
K1250A
) reduce the apparent affinity of the MgATP binding site(s) involved in channel opening (Figs. 2 and 3), but (at least for
K464A
and
D1370N
) affect the maximal opening rate little (Table I).
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275
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:275:130
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:275:124
status:
NEW
view ABCC7 p.Lys464Ala details
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:275:162
status:
NEW
view ABCC7 p.Lys464Ala details
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:275:201
status:
NEW
view ABCC7 p.Lys464Ala details
Accordingly, although no major difference in [␣32P]8-azidoATP photolabeling at 0ЊC was detected between WT and
K464A
/
K1250A
(Carson et al., 1995) or
K464A
CFTR (Vergani et al., 2002), the
K464A
mutation alone greatly reduced photolabeling of NBD1 by M [␣32P]8-azidoATP at 37ЊC (Aleksandrov et al., 2002) and virtually abolished stable (i.e., surviving extensive post-incubation washing) photolabeling at 30ЊC (unpublished data).
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280
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:280:130
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:280:359
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:280:108
status:
NEW
view ABCC7 p.Lys464Ala details
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:280:325
status:
NEW
view ABCC7 p.Lys464Ala details
ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:280:118
status:
NEW
view ABCC7 p.Asp1370Asn details
ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:280:347
status:
NEW
view ABCC7 p.Asp1370Asn details
Therefore, the simplest interpretation of the reduced apparent affinity with which MgATP elicits opening of
K464A
and
D1370N
(and
K1250A
) mutants compared with WT is that the mutations impair nucleotide binding at two different sites, such that at subsaturating [MgATP] channel opening is limited by MgATP binding at NBD1 in
K464A
, but at NBD2 in
D1370N
(and
K1250A
).
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286
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:286:124
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:286:105
status:
NEW
view ABCC7 p.Lys464Ala details
ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:286:112
status:
NEW
view ABCC7 p.Asp1370Asn details
Allosteric interactions between CFTR`s two NBDs (compare Powe et al., 2002) could, therefore, permit the
K464A
,
D1370N
, and
K1250A
mutations to all affect the same binding site.
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291
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:291:96
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:291:122
status:
NEW
view ABCC7 p.Asp1370Asn details
Moreover, covalent modification of the NBD2 Walker A sequence (Cotten and Welsh, 1998), and the
K1250A
(Fig. 3 C) and the
D1370N
(Fig. 2 D) mutations (9-8ف Å apart; e.g., Hung et al., 1998), all reduce apparent affinity for MgATP activation of opening.
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293
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:293:81
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:293:69
status:
NEW
view ABCC7 p.Asp1370Asn details
Most likely, therefore, the rightward shift in [MgATP] dependence of
D1370N
(and
K1250A
) open- ing rate reflects the lower affinity of a binding step, required for channel opening, at NBD2 itself.
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297
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:297:57
status:
NEW
view ABCC7 p.Lys464Ala details
However, we cannot rule out that, at low [MgATP], mutant
K464A
CFTR channels might open to bursts with only NBD2 occupied by nucleotide.
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298
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:298:234
status:
NEW
view ABCC7 p.Lys464Ala details
ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:298:43
status:
NEW
view ABCC7 p.Asp1370Asn details
In fact, although opening rates for WT and
D1370N
mutant CFTR channels (Fig. 2 D, blue and green symbols) are satisfactorily described by the Michaelis equation (i.e., opening limited by binding to a single site) the opening rates of
K464A
channels (Fig. 2 D, red symbols) at low (Յ50 M) [MgATP] are slightly higher than expected.
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299
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:299:71
status:
NEW
view ABCC7 p.Lys464Ala details
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:299:234
status:
NEW
view ABCC7 p.Lys464Ala details
If confirmed, these results would be consistent with the right-shifted
K464A
[MgATP]-rCO curve reflecting principally a reduced nucleotide affinity at NBD1 (now lower than the affinity at NBD2) and a low, but nonzero, opening rate of
K464A
mutant CFTR channels with nucleotide bound only at the unmodified NBD2 site.
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300
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:300:197
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:300:265
status:
NEW
view ABCC7 p.Lys464Ala details
ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:300:185
status:
NEW
view ABCC7 p.Asp1370Asn details
Therefore, present evidence suggests that nucleotide normally binds to both of WT CFTR`s NBDs before the channel opens, and that opening is limited by nucleotide binding at NBD2 in WT,
D1370N
, and
K1250A
CFTR channels, but probably by nucleotide binding at NBD1 in
K464A
CFTR channels.
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305
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:305:342
status:
NEW
view ABCC7 p.Lys464Ala details
But, by directly comparing gating of the same channels, in the same patch, during exposure to MgAMPPNP, MgAMPPCP, or MgATP␥S, and to MgATP, we find that at concentrations of these analogs expected to be saturating (Figs. 7 and 8; see also Weinreich et al., 1999; Aleksandrov et al., 2001, 2002) the opening rates of WT (Figs. 7-9) and
K464A
(Fig. 11) channels are only %5ف of that reached at saturating [MgATP].
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311
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:311:12
status:
NEW
view ABCC7 p.Lys464Ala details
Whereas the
K464A
mutation in NBD1 has been reported to reduce 02ف fold the ATPase activity of purified CFTR (Ramjeesingh et al., 1999), we find that the same mutation diminishes maximal opening rate by only Ͻ50%, similar to effects of other NBD1 catalytic site mutations (Figs. 2 and 5).
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316
ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:316:33
status:
NEW
view ABCC7 p.Asp1370Asn details
ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:316:157
status:
NEW
view ABCC7 p.Asp1370Asn details
For example, our measurements of
D1370N
CFTR gating show a twofold reduction in maximal opening rate (Table I), but no ATPase measurements are available for
D1370N
CFTR.
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318
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:318:78
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:318:166
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:318:449
status:
NEW
view ABCC7 p.Lys1250Ala details
On the other hand, ATPase measurements on purified CFTR have shown that the
K1250A
mutation abolished ATP hydrolysis (Ramjeesingh et al., 1999), whereas opening of
K1250A
channels was impaired, but not abolished, at normal [MgATP] (Carson et al., 1995; Gunderson and Kopito, 1995; Ramjeesingh et al., 1999; Powe et al., 2002); indeed, the greatly reduced apparent affinity for MgATP we observed (Fig. 3 C) implies that the maximal opening rate of
K1250A
may be several-fold greater than that measured at 1-2 mM MgATP.
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324
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:324:149
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:324:131
status:
NEW
view ABCC7 p.Lys464Ala details
ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:324:138
status:
NEW
view ABCC7 p.Asp1370Asn details
We found no clear dependence of burst duration on [MgATP] (10 M to 5 mM) in WT CFTR (Figs. 2 E, 3 A, and 4, B and C) or in
K464A
,
D1370N
, or
K1250A
mutant channels (Figs. 2 E, 3 B, and 4, E-H), indicating that all ATP binding events precede channel opening and no further binding to the open channel is needed to complete the gating cycle.
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326
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:326:76
status:
NEW
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This [MgATP] dependence of burst duration was reported to be exaggerated in
K1250A
mutant channels, in which brief bursts were observed at 10 M MgATP and only at higher concentrations did the characteristic (e.g., Fig. 6 C, above) prolonged bursts appear (Zeltwanger et al., 1999; Ikuma and Welsh, 2000; Powe et al., 2002).
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327
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:327:48
status:
NEW
view ABCC7 p.Lys1250Ala details
Though we occasionally observed brief bursts in
K1250A
channels at 10 M MgATP (not illustrated), these were very rare, with a frequency of occurrence not demonstrably different from that in nominally MgATP-free bath solution (rCO10 M/rCObath soln ϭ 0.72 Ϯ 0.12, n ϭ 6).
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328
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:328:22
status:
NEW
view ABCC7 p.Lys1250Ala details
Thus, brief bursts of
K1250A
channels might reflect infrequent nucleotide-independent events, unrelated to the physiological gating cycle of WT channels, an interpretation consistent with those brief bursts surviving mutation of the Walker A lysine in either, or both, NBDs (Zeltwanger et al., 1999; Ikuma and Welsh, 2000; Powe et al., 2002).
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329
ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:329:27
status:
NEW
view ABCC7 p.Asp1370Asn details
ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:329:264
status:
NEW
view ABCC7 p.Asp1370Asn details
Moreover, our finding that
D1370N
channels at low (15 M) [MgATP] both enter and exit bursts more slowly on average than WT channels (Figs. 2, D-E, and 4 H) demonstrates that this single NBD2 mutation impacts every gating cycle, regardless of the fact that
D1370N
channels have an intact WT NBD1 sequence.
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362
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:362:182
status:
NEW
view ABCC7 p.Lys464Ala details
However, the scheme as drawn suggests tight coupling between channel gating and ATP hydrolysis, which is inconsistent with the largely unaltered gating of the catalytically impaired
K464A
mutant (with ATPase Vmax apparently reduced -02فfold; Ramjeesingh et al., 1999).
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366
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:366:107
status:
NEW
view ABCC7 p.Lys464Ala details
ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:366:169
status:
NEW
view ABCC7 p.Asp1370Asn details
Even higher levels of steady state phosphorylation could prolong normal hydrolytic bursts (Table I, WT and
K464A
), as well as nonhydrolytic locked-open bursts (Table I,
D1370N
; Fig. 10 A vs. Fig. 9; Fig. 3 B vs. Fig. 10 E), by stabilizing the open burst states more than the transition states for both possible pathways (forward or backward; Fig. 12 A) for terminating the burst.
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369
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 12508051:369:216
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:369:243
status:
NEW
view ABCC7 p.Lys464Ala details
But when hydrolysis (at NBD2) was prevented, by supplying nucleotide resistant to hydrolysis (Figs. 9, and 10, A-D; Fig. 7 vs. Fig. 11), by adding VO4 (Vergani et al., 2002), or by mutating the NBD2 Walker A lysine (
K1250A
; Fig. 10, E-G), the
K464A
mutation resulted in less prolonged bursts.
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370
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:370:60
status:
NEW
view ABCC7 p.Lys464Ala details
Very similar reduction of locked-open burst duration by the
K464A
mutation has been described recently in NIH3T3 and CHO cells (Powe et al., 2002).
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379
ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:379:183
status:
NEW
view ABCC7 p.Asp1370Asn details
Unfortunately, the difficulty of collecting adequate numbers of CFTR`s relatively infrequent gating events, combined with the lack of biochemical information on CFTR mutants (whether
D1370N
is capable of ATP hydrolysis, for instance), precludes extraction of the many (Ն7) rate constants from fits to data, even for a scheme as simple as the one in Fig. 12 A.
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381
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:381:21
status:
NEW
view ABCC7 p.Lys464Ala details
The influence of the
K464A
mutation seen in Fig. 2 D (also on Po) is then mimicked simply by an -05فfold acceleration of the MgATP dissociation rate from NBD1, together with the Ͻ2-fold observed reduction in maximal opening rate (Table IB).
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382
ABCC7 p.Asp1370Asn
X
ABCC7 p.Asp1370Asn 12508051:382:29
status:
NEW
view ABCC7 p.Asp1370Asn details
Similarly, the effect of the
D1370N
mutation seen in Fig. 2 D (and on Po) can be mimicked by an -01فfold acceleration of the MgATP dissociation rate from NBD2 with the Ͻ2-fold observed reduction in maximal opening rate (Table IB), and (assuming that hydrolysis is abolished) by appropriate speeding of nonhydrolytic closing.
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639
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:639:63
status:
NEW
view ABCC7 p.Lys464Ala details
Effects on CFTR Cl- channel gating of Walker A lysine mutation
K464A
imply allosteric interaction between NBDs.
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646
ABCC7 p.Lys464Ala
X
ABCC7 p.Lys464Ala 12508051:646:62
status:
NEW
view ABCC7 p.Lys464Ala details
Effects on CFTR Cl-channel gating of Walker A lysine mutation
K464A
imply allosteric interaction between NBDs.
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