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PMID: 22966014
Jih KY, Sohma Y, Hwang TC
Nonintegral stoichiometry in CFTR gating revealed by a pore-lining mutation.
J Gen Physiol. 2012 Oct;140(4):347-59. Epub 2012 Sep 10.,
[PubMed]
Sentences
No.
Mutations
Sentence
Comment
33
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:33:145
status:
NEW
view ABCC7 p.Arg352Cys details
When mutating the positively charged arginine at position 352 (located in the sixth transmembrane segment, TM6) to cysteine, the mutant channel (
R352C
-CFTR) features two distinct open states with unequal conductance (Bai et al., 2010; compare Cui et al., 2008).
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34
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:34:145
status:
NEW
view ABCC7 p.Arg352Cys details
When mutating the positively charged arginine at position 352 (located in the sixth transmembrane segment, TM6) to cysteine, the mutant channel (
R352C
-CFTR) features two distinct open states with unequal conductance (Bai et al., 2010; compare Cui et al., 2008).
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43
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 22966014:43:95
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:43:85
status:
NEW
view ABCC7 p.Glu1371Ser details
For example, the drastic effect of nonhydrolyzable ATP analogues or mutations (e.g.,
E1371S
or
K1250A
) that abolish ATP hydrolysis on the open time supports the notion that ATP hydrolysis is coupled to channel Figure 1.ߓ An updated model illustrating the relationship between an opening/closing cycle of the gate and ATP consumption in CFTR` s NBDs.
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44
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 22966014:44:95
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:44:85
status:
NEW
view ABCC7 p.Glu1371Ser details
For example, the drastic effect of nonhydrolyzable ATP analogues or mutations (e.g.,
E1371S
or
K1250A
) that abolish ATP hydrolysis on the open time supports the notion that ATP hydrolysis is coupled to channel Figure 1. An updated model illustrating the relationship between an opening/closing cycle of the gate and ATP consumption in CFTR` s NBDs.
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70
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:70:47
status:
NEW
view ABCC7 p.Arg352Cys details
Fig. S1 shows the closed-time distribution for
R352C
-CFTR. Fig. S2 presents dwell-time distributions for O1 and O2 states.
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71
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:71:48
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:71:89
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Trp401Phe
X
ABCC7 p.Trp401Phe 22966014:71:40
status:
NEW
view ABCC7 p.Trp401Phe details
Fig. S1 shows the closed- time distribut
ion f
or
R352C
-CFTR. Fig. S2 presents dwell-time d
istri
butions for O1 and O2 states.
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72
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:72:89
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Trp401Phe
X
ABCC7 p.Trp401Phe 22966014:72:40
status:
NEW
view ABCC7 p.Trp401Phe details
Fig. S3 demonstrates the effects of the
W401F
mutation on the single-channel kinetics of
R352C
-CFTR.
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73
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:73:77
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:73:231
status:
NEW
view ABCC7 p.Arg352Cys details
R E S U L T S Unique pattern of single-channel gating transitions in Cysless/
R352C
-CFTR During our previous studies in scanning the pore-lining residues in the sixth transmembrane segment of TMDs (TM6), a unique feature of Cysless/
R352C
-CFTR caught our attentions.
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74
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:74:77
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:74:231
status:
NEW
view ABCC7 p.Arg352Cys details
R E S U L T S Unique pattern of single-channel gating transitions in Cysless/
R352C
-CFTR During our previous studies in scanning the pore-lining residues in the sixth transmembrane segment of TMDs (TM6), a unique feature of Cysless/
R352C
-CFTR caught our attentions.
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79
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:79:85
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:79:78
status:
NEW
view ABCC7 p.Glu1371Ser details
Consistent with this idea, ATP only induces CO1C transitions in
E1371S
/
R352C
-CFTR, a hydrolysis-deficient mutant.
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80
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:80:4
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:80:87
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:80:80
status:
NEW
view ABCC7 p.Glu1371Ser details
Cons
isten
t with this idea, ATP only induces C→O1→C transitions in
E1371S
/
R352C
-CFTR, a hydrolysis-deficient mutant.
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81
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:81:4
status:
NEW
view ABCC7 p.Arg352Cys details
The
R352C
mutant channel becomes a precious tool, as it allows us to distinguish the prehydrolytic (O1) and post-hydrolytic (O2) open states and thus to "visualize" ATP hydrolysis taking place within each opening burst.
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103
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:103:25
status:
NEW
view ABCC7 p.Arg352Cys details
Figure 2.ߓ Cysless/
R352C
-CFTR reveals two different open states with distinct conductance level.
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104
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:104:26
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:104:101
status:
NEW
view ABCC7 p.Arg352Cys details
Figure 2. Cysless/
R352C
-CFTR reveals two different open states with distinct conductance leve
l.
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105
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:105:101
status:
NEW
view ABCC7 p.Arg352Cys details
(A) Five representative traces and amplitude histograms from a patch that contained only one Cysless/
R352C
-CFTR channel.
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106
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:106:68
status:
NEW
view ABCC7 p.Arg352Cys details
(B) Four representative traces and amplitude histograms for Cysless/
R352C
-CFTR recorded in a condition similar to that in A, except that both pipette and perfusion solution contain 375 mM Cl&#e032; (see Materials and methods for details).
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107
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:107:68
status:
NEW
view ABCC7 p.Arg352Cys details
(B) Four representative traces and amplitude histograms for Cysless/
R352C
-CFTR recorded in a condition similar to that in A, except that both pipette and perfusion solution contain 375 mM Cl (see Materials and methods for details).
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111
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:111:0
status:
NEW
view ABCC7 p.Arg352Cys details
R352C
-CFTR channels is that a higher percentage of CO1O2C transitions were present under the WT background (Table 1).
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112
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:112:0
status:
NEW
view ABCC7 p.Arg352Cys details
R352C
-CFTR channels is that a higher percentage of C→O1→O2→C transitions were present under the WT background (Table 1).
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113
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:113:174
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:113:153
status:
NEW
view ABCC7 p.Glu1371Ser details
To further test our hypothesis that the dominant O1O2 transition versus O2O1 transition is the result of ATP hydrolysis, we engineered the
E1371S
mutation into
R352C
-CFTR to abolish ATP hydrolysis (Vergani et al., 2003; Bompadre et al., 2005b) and recorded ATP-dependent opening events.
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114
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:114:176
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:114:155
status:
NEW
view ABCC7 p.Glu1371Ser details
To further test our hypothesis that the dominant O1→O2 transition versus O2→O1 transition is the result of ATP hydrolysis, we engineered the
E1371S
mutation into
R352C
-CFTR to abolish ATP hydrolysis (Vergani et al., 2003; Bompadre et al., 2005b) and recorded ATP-dependent opening events.
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115
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:115:103
status:
NEW
view ABCC7 p.Glu1371Ser details
This lack of transitions to the O2 state for ATP-induced opening bursts is not caused by the mutation,
E1371S
, eliminating the O2 state, because in the absence of ATP, the channel opens predominantly into bursts of a larger conductance level corresponding to that of the O2 state (Fig. 3 C).
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116
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:116:103
status:
NEW
view ABCC7 p.Glu1371Ser details
This lack of transitions to the O2 state for ATP-induced opening bursts is not caused by the mutation,
E1371S
, eliminating the O2 state, because in the absence of ATP, the channel opens predominantly into bursts of a larger conductance level corresponding to that of the O2 state (Fig. 3 C).
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124
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:124:96
status:
NEW
view ABCC7 p.Arg352Cys details
They showed that in addition to O1 and O2 (named s1 and s2, respectively, in Cui et al., 2008),
R352C
-CFTR occasionally transits to a full conductance level that is not different from that of WT-CFTR.
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125
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:125:96
status:
NEW
view ABCC7 p.Arg352Cys details
They showed that in addition to O1 and O2 (named s1 and s2, respectively, in Cui et al., 2008),
R352C
-CFTR occasionally transits to a full conductance level that is not different from that of WT-CFTR.
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129
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:129:107
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:129:198
status:
NEW
view ABCC7 p.Arg352Cys details
ATP hydrolysis drives the O1O2 transition Although our initial observations were made with Cys-less/
R352C
-CFTR, this unique pattern of gating transitions was also seen when we introduced the
R352C
mutation into the WT background (Fig. 3 A and Table 1).
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130
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:130:31
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:130:107
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:130:198
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:130:199
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:130:354
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:130:510
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Trp401Phe
X
ABCC7 p.Trp401Phe 22966014:130:516
status:
NEW
view ABCC7 p.Trp401Phe details
ATP hydrolysis drives the O1&#x
2192;
O2 transition Although our initial observations were made with Cysless/
R352C
-CFTR, this unique pattern of gating transitions was also seen when we introduced the
R352C
mutation into the WT background (Fig. 3 A and Table 1).
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131
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:131:31
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:131:199
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:131:355
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:131:512
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Trp401Phe
X
ABCC7 p.Trp401Phe 22966014:131:518
status:
NEW
view ABCC7 p.Trp401Phe details
One notable difference between
R352C
- and Cysless/ Ta b l e 1 Summary of opening events by different gating patterns in three CFTR mutants Gating topology O1-O2 O1 O2 O2-O1 (O1-O2) n # Total Cysless/
R352C
2.75 mM ATP 100 µM ATP 720 (45%) 663 (56%) 290 (18%) 216 (18%) 175 (11%) 137 (12%) 42 (3%) 32 (3%) 375 (23%) 128 (11%) 1,602 (100%) 1,176 (100%)
R352C
2.75 mM ATP 100 µM ATP 834 (55%) 1,246 (59%) 301 (20%) 406 (19%) 173 (11%) 281 (13%) 39 (3%) 45 (2%) 169 (11%) 121 (6%) 1,516 (100%) 2,099 (100%)
R352C
/
W401F
2.75 mM ATP 100 µM ATP 733 (44%) 1,189 (54%) 326 (19%) 367 (17%) 122 (7%) 337 (15%) 28 (2%) 60 (3%) 474 (28%) 232 (11%) 1,683 (100%) 2,185 (100%) Five different gating patterns are illustrated on the top of the table.
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139
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:139:36
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:139:46
status:
NEW
view ABCC7 p.Arg352Cys details
Table 1 shows that for both Cysless/
R352C
and
R352C
mutant channels, CO1O2C is the prevailing transition; thus, most gating events indeed follow the long-held one-to-one stoichiometry between the gating cycle and ATP hydrolysis cycle.
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140
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:140:36
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:140:46
status:
NEW
view ABCC7 p.Arg352Cys details
Table 1 shows that for both Cysless/
R352C
and
R352C
mutant channels, C→O1→O2→C is the prevailing transition; thus, most gating events indeed follow the long-held one-to-one stoichiometry between the gating cycle and ATP hydrolysis cycle.
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141
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:141:98
status:
NEW
view ABCC7 p.Arg352Cys details
A simplified scheme (Scheme 1) summarizes the idea that the gating transition pattern observed in
R352C
-CFTR represents a cyclic steady state in which ATP hydrolysis drives a "clockwise" movement around the state diagram (compare Richard and Miller, 1990; Gunderson and Kopito, 1995).
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142
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:142:98
status:
NEW
view ABCC7 p.Arg352Cys details
A simplified scheme (Scheme 1) summarizes the idea that the gating transition pattern observed in
R352C
-CFTR represents a cyclic steady state in which ATP hydrolysis drives a "clockwise" movement around the state diagram (compare Richard and Miller, 1990; Gunderson and Kopito, 1995).
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143
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:143:83
status:
NEW
view ABCC7 p.Arg352Cys details
(A) Four representative traces and amplitude histograms show the gating pattern of
R352C
-CFTR channel in the presence of 2.75 mM ATP.
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144
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:144:83
status:
NEW
view ABCC7 p.Arg352Cys details
(A) Four representative traces and amplitude histograms show the gating pattern of
R352C
-CFTR channel in the presence of 2.75 mM ATP.
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145
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:145:61
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:145:67
status:
NEW
view ABCC7 p.Glu1371Ser details
(B and C) Representative traces and amplitude histograms for
R352C
/
E1371S
-CFTR in the presence (B) or absence (C) of 2.75 mM ATP.
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146
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:146:61
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:146:67
status:
NEW
view ABCC7 p.Glu1371Ser details
(B and C) Representative traces and amplitude histograms for
R352C
/
E1371S
-CFTR in the presence (B) or absence (C) of 2.75 mM ATP.
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149
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:149:168
status:
NEW
view ABCC7 p.Arg352Cys details
However, these nondiscernible closures, if they exist, are not the same as the original closed state (C in Scheme 1) for the following reasons: (a) the closed state of
R352C
-CFTR marked with stars in Fig. 2 assumes a very long lifetime (1 s [Fig. S1] vs. 300-400 ms for WT-CFTR); thus, the probability of having this state with a lifetime of <3 ms buried in an opening burst is extremely small (<0.003); (b) for this idea to be valid, one has to propose that ATP can open this presumed brief closed channel at a rate that is two to three orders faster than it does to the original closed state; and (c) as shown in the next section, multiple rounds of O1→O2 transitions can take place within an opening burst in conditions when the O2 state is stabilized, a theme predicted by Scheme 2.
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153
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:153:61
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:153:72
status:
NEW
view ABCC7 p.Arg352Cys details
This idea is first supported simply by comparing the Cysless/
R352C
- and
R352C
-CFTR results shown in Table 1.
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154
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:154:12
status:
NEW
view ABCC7 p.Arg352Cys details
The Cysless/
R352C
mutant channel has an O2 state that is about four times as long as that in that hydrolysis of more than one ATP molecule does take place within an opening burst.
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163
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:163:26
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:163:40
status:
NEW
view ABCC7 p.Arg352Cys details
Opening events of Cysless/
R352C
- (A) or
R352C
-CFTR (B) containing one (events 1, 3, and 4 in A, and 1-4 in B) or more (events 2 and 5 in A, and 5 in B) O1→O2 transitions.
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164
ABCC7 p.Ile344Cys
X
ABCC7 p.Ile344Cys 22966014:164:142
status:
NEW
view ABCC7 p.Ile344Cys details
Events were extracted from traces in Figs. 2 B and 3 A. Chosen events were specified in boxes and numbered in Figs. 2 B and 3 A. in Cysless/
I344C
-CFTR, these long ATP-independent openings should show up as the larger O2 state, and that, in the presence of ATP, an opening burst could contain numerous O1→O2 transitions.
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165
ABCC7 p.Ile344Cys
X
ABCC7 p.Ile344Cys 22966014:165:86
status:
NEW
view ABCC7 p.Ile344Cys details
Chosen events were specified in boxes and numbered in Figs. 2 B and 3 A. in Cysless/
I344C
-CFTR, these long ATP-independent openings should show up as the larger O2 state, and that, in the presence of ATP, an opening burst could contain numerous O1O2 transitions.
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166
ABCC7 p.Arg352Gln
X
ABCC7 p.Arg352Gln 22966014:166:18
status:
NEW
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ABCC7 p.Ile344Cys
X
ABCC7 p.Ile344Cys 22966014:166:51
status:
NEW
view ABCC7 p.Ile344Cys details
We introduced the
R352Q
mutation into the Cysless/
I344C
-CFTR channel.
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167
ABCC7 p.Arg352Gln
X
ABCC7 p.Arg352Gln 22966014:167:18
status:
NEW
view ABCC7 p.Arg352Gln details
ABCC7 p.Arg352Gln
X
ABCC7 p.Arg352Gln 22966014:167:41
status:
NEW
view ABCC7 p.Arg352Gln details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:167:92
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Ile344Cys
X
ABCC7 p.Ile344Cys 22966014:167:35
status:
NEW
view ABCC7 p.Ile344Cys details
ABCC7 p.Ile344Cys
X
ABCC7 p.Ile344Cys 22966014:167:51
status:
NEW
view ABCC7 p.Ile344Cys details
Before MESET modif
icati
on, Cysless/
I344C
/
R352Q
muta
nt ch
annels behaved similarly as Cysless/
R352C
-CFTR in the presence of ATP (Fig. 5 A).
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168
ABCC7 p.Arg352Gln
X
ABCC7 p.Arg352Gln 22966014:168:41
status:
NEW
view ABCC7 p.Arg352Gln details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:168:92
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Ile344Cys
X
ABCC7 p.Ile344Cys 22966014:168:35
status:
NEW
view ABCC7 p.Ile344Cys details
Before MESET modification, Cysless/
I344C
/
R352Q
mutant channels behaved similarly as Cysless/
R352C
-CFTR in the presence of ATP (Fig. 5 A).
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170
ABCC7 p.Arg352Gln
X
ABCC7 p.Arg352Gln 22966014:170:42
status:
NEW
view ABCC7 p.Arg352Gln details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:170:169
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Ile344Cys
X
ABCC7 p.Ile344Cys 22966014:170:36
status:
NEW
view ABCC7 p.Ile344Cys details
After MTSET modification of Cysless/
I344C
/
R352Q
, we indeed observed robust ATP-independent openings (Fig. 5 B) with an open lifetime of 1.03 ± 0.30 s (n = 10), the
R352C
-CFTR (Fig. S2).
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171
ABCC7 p.Arg352Gln
X
ABCC7 p.Arg352Gln 22966014:171:42
status:
NEW
view ABCC7 p.Arg352Gln details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:171:122
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:171:168
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Ile344Cys
X
ABCC7 p.Ile344Cys 22966014:171:36
status:
NEW
view ABCC7 p.Ile344Cys details
Correspondingly, the percentage of o
penin
g
burs
ts encompassing more than one O1→O2 transition is higher in Cysless/
R352C
(Table 1).
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172
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:172:121
status:
NEW
view ABCC7 p.Arg352Cys details
Correspondingly, the percentage of opening bursts encompassing more than one O1O2 transition is higher in Cysless/
R352C
(Table 1).
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174
ABCC7 p.Ile344Cys
X
ABCC7 p.Ile344Cys 22966014:174:51
status:
NEW
view ABCC7 p.Ile344Cys details
In Bai et al. (2010), we showed that after Cysless/
I344C
-CFTR is modified by MTSET, the open probability of this CFTR mutant in the presence of ATP becomes virtually 1 (Bai et al., 2010).
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175
ABCC7 p.Ile344Cys
X
ABCC7 p.Ile344Cys 22966014:175:51
status:
NEW
view ABCC7 p.Ile344Cys details
In Bai et al. (2010), we showed that after Cysless/
I344C
-CFTR is modified by MTSET, the open probability of this CFTR mutant in the presence of ATP becomes virtually 1 (Bai et al., 2010).
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177
ABCC7 p.Arg352Gln
X
ABCC7 p.Arg352Gln 22966014:177:66
status:
NEW
view ABCC7 p.Arg352Gln details
ABCC7 p.Ile344Cys
X
ABCC7 p.Ile344Cys 22966014:177:60
status:
NEW
view ABCC7 p.Ile344Cys details
Representative traces and amplitude histograms for Cysless/
I344C
/
R352Q
-CFTR under these conditions: (A) in the presence of 2.75 mM ATP; (B-C) after MTSET modification, in the absence (B) or presence (C) of 2.75 mM ATP.
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178
ABCC7 p.Arg352Gln
X
ABCC7 p.Arg352Gln 22966014:178:66
status:
NEW
view ABCC7 p.Arg352Gln details
ABCC7 p.Ile344Cys
X
ABCC7 p.Ile344Cys 22966014:178:60
status:
NEW
view ABCC7 p.Ile344Cys details
Representative traces and amplitude histograms for Cysless/
I344C
/
R352Q
-CFTR under these conditions: (A) in the presence of 2.75 mM ATP; (B-C) after MTSET modification, in the absence (B) or presence (C) of 2.75 mM ATP.
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179
ABCC7 p.Arg352Gln
X
ABCC7 p.Arg352Gln 22966014:179:55
status:
NEW
view ABCC7 p.Arg352Gln details
ABCC7 p.Ile344Cys
X
ABCC7 p.Ile344Cys 22966014:179:49
status:
NEW
view ABCC7 p.Ile344Cys details
(E) The amplitude of O1 and O2 states of Cysless/
I344C
/
R352Q
-CFTR before (the left bar) or after (the right bar) being modified by MTSET.
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180
ABCC7 p.Arg352Gln
X
ABCC7 p.Arg352Gln 22966014:180:55
status:
NEW
view ABCC7 p.Arg352Gln details
ABCC7 p.Ile344Cys
X
ABCC7 p.Ile344Cys 22966014:180:49
status:
NEW
view ABCC7 p.Ile344Cys details
(E) The amplitude of O1 and O2 states of Cysless/
I344C
/
R352Q
-CFTR before (the left bar) or after (the right bar) being modified by MTSET.
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181
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:181:18
status:
NEW
view ABCC7 p.Arg352Cys details
P < 0.05. with
R352C
-CFTR (Fig. 3), this double mutant also exhibits a preferred order of the gating transition.
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182
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:182:18
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:182:130
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Trp401Phe
X
ABCC7 p.Trp401Phe 22966014:182:124
status:
NEW
view ABCC7 p.Trp401Phe details
Quantitative analy
sis o
f gating events indeed demonstrates a higher percentage of gating events with reentry transitions in
W401F
/
R352C
-CFTR (Table 1).
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183
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:183:130
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Trp401Phe
X
ABCC7 p.Trp401Phe 22966014:183:124
status:
NEW
view ABCC7 p.Trp401Phe details
Quantitative analysis of gating events indeed demonstrates a higher percentage of gating events with reentry transitions in
W401F
/
R352C
-CFTR (Table 1).
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184
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:184:28
status:
NEW
view ABCC7 p.Arg352Cys details
The results reveal that the
R352C
mutation significantly shortens the total open time (150 ms [Fig. S2] vs. 400 ms for WT-CFTR ; Vergani et al., 2003; Bompadre et al., 2005a).
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185
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:185:28
status:
NEW
view ABCC7 p.Arg352Cys details
The results reveal that the
R352C
mutation significantly shortens the total open time (&#e07a;150 ms [Fig. S2] vs. &#e07a;400 ms for WT-CFTRÊf;; Vergani et al., 2003; Bompadre et al., 2005a).
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186
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:186:57
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Trp401Phe
X
ABCC7 p.Trp401Phe 22966014:186:51
status:
NEW
view ABCC7 p.Trp401Phe details
Prolonged O1 and O2 dwell times were also found in
W401F
/
R352C
-CFTR, but to a lesser extent.
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187
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:187:57
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:187:73
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Trp401Phe
X
ABCC7 p.Trp401Phe 22966014:187:26
status:
NEW
view ABCC7 p.Trp401Phe details
ABCC7 p.Trp401Phe
X
ABCC7 p.Trp401Phe 22966014:187:51
status:
NEW
view ABCC7 p.Trp401Phe details
The effect of Cysless and
W401F
mutations in prolon
ging
t
he op
en time of
R352C
mutant channels is consistent with the observations made for the same mutants in the WT background (Bai et al., 2010; Tsai et al., 2010a).
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188
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:188:51
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:188:73
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Trp401Phe
X
ABCC7 p.Trp401Phe 22966014:188:26
status:
NEW
view ABCC7 p.Trp401Phe details
D I S C U S S I O N An acc
ident
al discovery of the
R352C
mutation grants
us th
e opportunity to actually "see"-in real time-ATP hydrolysis taking place during CFTR gating as the ordered transition between two distinct levels of open channel conductance (O1 and O2) indicates an input of the free energy from ATP hydrolysis.
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189
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:189:51
status:
NEW
view ABCC7 p.Arg352Cys details
D I S C U S S I O N An accidental discovery of the
R352C
mutation grants us the opportunity to actually "see"-in real time-ATP hydrolysis taking place during CFTR gating as the ordered transition between two distinct levels of open channel conductance (O1 and O2) indicates an input of the free energy from ATP hydrolysis.
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194
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:194:33
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:194:214
status:
NEW
view ABCC7 p.Arg352Cys details
After we made our discovery with
R352C
-CFTR, we recorded WT-CFTR under conditions described in these early reports, but did which is approximately fivefold longer than the mean lifetime of the O2 state for Cysless/
R352C
-CFTR (Fig. S2).
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195
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:195:33
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:195:214
status:
NEW
view ABCC7 p.Arg352Cys details
After we made our discovery with
R352C
-CFTR, we recorded WT-CFTR under conditions described in these early reports, but did which is approximately fivefold longer than the mean lifetime of the O2 state for Cysless/
R352C
-CFTR (Fig. S2).
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206
ABCC7 p.Trp401Phe
X
ABCC7 p.Trp401Phe 22966014:206:0
status:
NEW
view ABCC7 p.Trp401Phe details
W401F
mutation promotes O2→O1 transition In our latest paper (Jih et al., 2012), using nonhydrolyzable ATP analogues (pyrophosphate or adenylyl-imidodi- phosphate) as baits, we captured a post-hydrolytic state (state X), which, like the O2 state in this paper, can reenter the prehydrolytic open state (O1) upon ATP binding to the vacant ABP2.
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208
ABCC7 p.Trp401Phe
X
ABCC7 p.Trp401Phe 22966014:208:0
status:
NEW
view ABCC7 p.Trp401Phe details
ABCC7 p.Trp401Phe
X
ABCC7 p.Trp401Phe 22966014:208:48
status:
NEW
view ABCC7 p.Trp401Phe details
Inter
estingly, a conservative mutation in NBD1 (
W401F
, both W and F are aromatic amino acids) can enhance the responsiveness of state X to ATP as well as nonhydrolyzable ATP analogues for reasons yet to be elucidated.
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209
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:209:173
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:209:246
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Trp401Phe
X
ABCC7 p.Trp401Phe 22966014:209:155
status:
NEW
view ABCC7 p.Trp401Phe details
ABCC7 p.Trp401Phe
X
ABCC7 p.Trp401Phe 22966014:209:240
status:
NEW
view ABCC7 p.Trp401Phe details
Nevertheless, the striking functional similarities between state X in Jih et al. (2012) and the O2 state in this paper prompt us to test the effect of the
W401F
mutation on
R352C
-CFTR. Fig. S3 shows a representative single-channel trace of
W401F
/
R352C
-CFTR.
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210
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:210:37
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Trp401Phe
X
ABCC7 p.Trp401Phe 22966014:210:48
status:
NEW
view ABCC7 p.Trp401Phe details
Compared state C is nearly 1 s for
R352C
-CFTR.
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211
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:211:173
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:211:246
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Trp401Phe
X
ABCC7 p.Trp401Phe 22966014:211:155
status:
NEW
view ABCC7 p.Trp401Phe details
ABCC7 p.Trp401Phe
X
ABCC7 p.Trp401Phe 22966014:211:240
status:
NEW
view ABCC7 p.Trp401Phe details
Nevertheless, the striking functional similarities between state X in Jih et al. (2012) and the O2 state in this paper prompt us to test the effect of the
W401F
mutation on
R352C
-CFTR. Fig. S3 shows a representative single-channel trace of
W401F
/
R352C
-CFTR.
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212
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:212:37
status:
NEW
view ABCC7 p.Arg352Cys details
Compared state C is nearly 1 s for
R352C
-CFTR.
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228
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:228:24
status:
NEW
view ABCC7 p.Arg352Cys details
Nonetheless, the mutant
R352C
does offer the advantage of observing transitions between the O1 and O2 states with a much better temporal resolution necessary for a more thorough microscopic kinetic analysis.
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230
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:230:24
status:
NEW
view ABCC7 p.Arg352Cys details
Nonetheless, the mutant
R352C
does offer the advantage of observing transitions between the O1 and O2 states with a much better temporal resolution necessary for a more thorough microscopic kinetic analysis.
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254
ABCC7 p.Thr1246Asn
X
ABCC7 p.Thr1246Asn 22966014:254:281
status:
NEW
view ABCC7 p.Thr1246Asn details
Indeed, mutations of the amino acid residue that directly interacts with ATP have been reported to decrease the opening rate in an ATP-dependent manner (Zhou et al., 2006); further, mutations located at the NBD dimer interface have also been shown to lower the opening rate (e.g.,
T1246N
in Vergani et al., 2005).
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255
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:255:83
status:
NEW
view ABCC7 p.Arg352Cys details
Here, we show that mutating R352 leads to a reduced opening rate (1 s1 for
R352C
-CFTR vs. 2.5 s1 for WT-CFTR; Vergani et al., 2003; Bompadre et al., 2005a).
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256
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:256:18
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Thr1246Asn
X
ABCC7 p.Thr1246Asn 22966014:256:281
status:
NEW
view ABCC7 p.Thr1246Asn details
Figure 7.
R352C
shorten the locked-open time of hydrolytic-deficient CFTR mutant.
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257
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:257:47
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:257:82
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:257:98
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:257:30
status:
NEW
view ABCC7 p.Glu1371Ser details
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:257:53
status:
NEW
view ABCC7 p.Glu1371Ser details
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:257:77
status:
NEW
view ABCC7 p.Glu1371Ser details
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:257:111
status:
NEW
view ABCC7 p.Glu1371Ser details
ABCC7 p.Thr1246Asn
X
ABCC7 p.Thr1246Asn 22966014:257:70
status:
NEW
view ABCC7 p.Thr1246Asn details
ABCC7 p.Thr1246Asn
X
ABCC7 p.Thr1246Asn 22966014:257:104
status:
NEW
view ABCC7 p.Thr1246Asn details
Macroscopic current traces of
E1371S
-CFTR (A),
R352C
/
E1371S
-CFTR (B),
T1246N
/
E1371S-CFT
R (C), and
R352C
/
T1246N
/
E1371S
-CFTR (D).
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258
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:258:17
status:
NEW
view ABCC7 p.Arg352Cys details
Figure 7.ߓ
R352C
shorten the locked-open time of hydrolytic-deficient CFTR mutant.
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259
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:259:47
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:259:98
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:259:202
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:259:306
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:259:30
status:
NEW
view ABCC7 p.Glu1371Ser details
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:259:53
status:
NEW
view ABCC7 p.Glu1371Ser details
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:259:77
status:
NEW
view ABCC7 p.Glu1371Ser details
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:259:111
status:
NEW
view ABCC7 p.Glu1371Ser details
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:259:159
status:
NEW
view ABCC7 p.Glu1371Ser details
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:259:209
status:
NEW
view ABCC7 p.Glu1371Ser details
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:259:258
status:
NEW
view ABCC7 p.Glu1371Ser details
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:259:319
status:
NEW
view ABCC7 p.Glu1371Ser details
ABCC7 p.Thr1246Asn
X
ABCC7 p.Thr1246Asn 22966014:259:70
status:
NEW
view ABCC7 p.Thr1246Asn details
ABCC7 p.Thr1246Asn
X
ABCC7 p.Thr1246Asn 22966014:259:104
status:
NEW
view ABCC7 p.Thr1246Asn details
ABCC7 p.Thr1246Asn
X
ABCC7 p.Thr1246Asn 22966014:259:251
status:
NEW
view ABCC7 p.Thr1246Asn details
ABCC7 p.Thr1246Asn
X
ABCC7 p.Thr1246Asn 22966014:259:312
status:
NEW
view ABCC7 p.Thr1246Asn details
The current relaxation was fit
ted wi
th a single
-expo
n
ential
function r
esulti
n
g in t
he relaxation t
ime c
o
nstant
for ea
ch mutant: 65.6 ± 10.1 s (n = 8) for
E1371S
-CFTR, 4.9 ± 0.8 s (n = 12) for
R352C
/
E1371S
-CFTR, 7.8 ± 1.6 s (n = 7) for
T1246N
/
E1371S
-CFTR, and 2.27 ± 0.27 s (n = 6) for
R352C
/
T1246N
/
E1371S
-CFTR.
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261
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:261:200
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:261:302
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:261:26
status:
NEW
view ABCC7 p.Glu1371Ser details
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:261:158
status:
NEW
view ABCC7 p.Glu1371Ser details
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:261:207
status:
NEW
view ABCC7 p.Glu1371Ser details
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:261:255
status:
NEW
view ABCC7 p.Glu1371Ser details
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:261:315
status:
NEW
view ABCC7 p.Glu1371Ser details
ABCC7 p.Thr1246Asn
X
ABCC7 p.Thr1246Asn 22966014:261:248
status:
NEW
view ABCC7 p.Thr1246Asn details
ABCC7 p.Thr1246Asn
X
ABCC7 p.Thr1246Asn 22966014:261:308
status:
NEW
view ABCC7 p.Thr1246Asn details
*, P < 0.05 compared with
E1371S
; #, P < 0.05 between two designated data.
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263
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:263:26
status:
NEW
view ABCC7 p.Glu1371Ser details
*, P < 0.05 compared with
E1371S
; #, P < 0.05 between two designated data.
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266
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:266:61
status:
NEW
view ABCC7 p.Arg352Cys details
In conclusion, capitalizing on the unique gating features of
R352C
-CFTR, we were able to visualize ATP hydrolysis in real time for CFTR by simply monitoring single-channel current traces.
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268
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:268:61
status:
NEW
view ABCC7 p.Arg352Cys details
In conclusion, capitalizing on the unique gating features of
R352C
-CFTR, we were able to visualize ATP hydrolysis in real time for CFTR by simply monitoring single-channel current traces.
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292
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:292:191
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Thr1246Asn
X
ABCC7 p.Thr1246Asn 22966014:292:94
status:
NEW
view ABCC7 p.Thr1246Asn details
It follows that mutations that decrease the rate of NBD dimerization (CATP→CAD), e.g.,
T1246N
in Vergani et al. (2005), or those that reduce the rate for CAD→O1 (presumably the
R352C
mutation), will accelerate the decay rate of macroscopic currents in hydrolysis-deficient mutants upon ATP washout.
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293
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:293:35
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:293:133
status:
NEW
view ABCC7 p.Glu1371Ser details
ABCC7 p.Thr1246Asn
X
ABCC7 p.Thr1246Asn 22966014:293:45
status:
NEW
view ABCC7 p.Thr1246Asn details
Here, in Fig. 7, we show that both
R352C
and
T1246N
mutations significantly shorten the locked-open time of the hydrolytic-deficient
E1371S
-CFTR (Fig. 7).
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294
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:294:189
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Thr1246Asn
X
ABCC7 p.Thr1246Asn 22966014:294:93
status:
NEW
view ABCC7 p.Thr1246Asn details
ABCC7 p.Thr1246Asn
X
ABCC7 p.Thr1246Asn 22966014:294:132
status:
NEW
view ABCC7 p.Thr1246Asn details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 22966014:294:139
status:
NEW
view ABCC7 p.Lys1250Arg details
Notably, this result is somewhat different from that shown in Vergani et al. (2005) in which
the cu
rrent relaxation is prolonged in
T1246N
/
K1250R
- CFTR.
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295
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:295:35
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:295:133
status:
NEW
view ABCC7 p.Glu1371Ser details
ABCC7 p.Thr1246Asn
X
ABCC7 p.Thr1246Asn 22966014:295:45
status:
NEW
view ABCC7 p.Thr1246Asn details
Here, in Fig. 7, we show that both
R352C
and
T1246N
mutations significantly shorten the locked-open time of the hydrolytic-deficient
E1371S
-CFTR (Fig. 7).
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296
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:296:70
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Thr1246Asn
X
ABCC7 p.Thr1246Asn 22966014:296:80
status:
NEW
view ABCC7 p.Thr1246Asn details
ABCC7 p.Thr1246Asn
X
ABCC7 p.Thr1246Asn 22966014:296:132
status:
NEW
view ABCC7 p.Thr1246Asn details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 22966014:296:139
status:
NEW
view ABCC7 p.Lys1250Arg details
Nonetheless, the locked-open time is further shortened when combining
R352C
and
T1246N
mutations together (Fig. 7, D and E), suggest
ing th
a
t the
two mutations affects two different kinetic steps as described above.
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298
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:298:70
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Thr1246Asn
X
ABCC7 p.Thr1246Asn 22966014:298:80
status:
NEW
view ABCC7 p.Thr1246Asn details
Nonetheless, the locked-open time is further shortened when combining
R352C
and
T1246N
mutations together (Fig. 7, D and E), suggesting that the two mutations affects two different kinetic steps as described above.
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