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). Login to comment
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). Login to comment
43 ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 22966014:43:95
status: NEW
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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. Login to comment
44 ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 22966014:44:95
status: NEW
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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. Login to comment
70 ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:70:47
status: NEW
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Fig. S1 shows the closed-time distribution for R352C-CFTR. Fig. S2 presents dwell-time distributions for O1 and O2 states. Login to comment
71 ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:71:48
status: NEW
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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 distribution for R352C-CFTR. Fig. S2 presents dwell-time distributions for O1 and O2 states. Login to comment
72 ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:72:89
status: NEW
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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. Login to comment
73 ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:73:77
status: NEW
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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. Login to comment
74 ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:74:77
status: NEW
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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. Login to comment
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 C࢐O1࢐C transitions in E1371S/R352C-CFTR, a hydrolysis-deficient mutant. Login to comment
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
Consistent with this idea, ATP only induces C→O1→C transitions in E1371S/R352C-CFTR, a hydrolysis-deficient mutant. Login to comment
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. Login to comment
103 ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:103:25
status: NEW
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Figure 2.ߓ Cysless/R352C-CFTR reveals two different open states with distinct conductance level. Login to comment
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 level. Login to comment
105 ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:105:101
status: NEW
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(A) Five representative traces and amplitude histograms from a patch that contained only one Cysless/R352C-CFTR channel. Login to comment
106 ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:106:68
status: NEW
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(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). Login to comment
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). Login to comment
111 ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:111:0
status: NEW
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R352C-CFTR channels is that a higher percentage of C࢐O1࢐O2࢐C transitions were present under the WT background (Table 1). Login to comment
112 ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:112:0
status: NEW
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R352C-CFTR channels is that a higher percentage of C→O1→O2→C transitions were present under the WT background (Table 1). Login to comment
113 ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:113:174
status: NEW
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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 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. Login to comment
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. Login to comment
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). Login to comment
116 ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:116:103
status: NEW
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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). Login to comment
124 ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:124:96
status: NEW
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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. Login to comment
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. Login to comment
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 O1࢐O2 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). Login to comment
130 ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:130:31
status: NEW
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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→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). Login to comment
131 ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:131:31
status: NEW
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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. Login to comment
139 ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:139:36
status: NEW
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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, 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. Login to comment
140 ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:140:36
status: NEW
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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. Login to comment
141 ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:141:98
status: NEW
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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). Login to comment
142 ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:142:98
status: NEW
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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). Login to comment
143 ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:143:83
status: NEW
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(A) Four representative traces and amplitude histograms show the gating pattern of R352C-CFTR channel in the presence of 2.75 mM ATP. Login to comment
144 ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:144:83
status: NEW
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(A) Four representative traces and amplitude histograms show the gating pattern of R352C-CFTR channel in the presence of 2.75 mM ATP. Login to comment
145 ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:145:61
status: NEW
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ABCC7 p.Glu1371Ser
X
ABCC7 p.Glu1371Ser 22966014:145:67
status: NEW
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(B and C) Representative traces and amplitude histograms for R352C/E1371S-CFTR in the presence (B) or absence (C) of 2.75 mM ATP. Login to comment
146 ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:146:61
status: NEW
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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. Login to comment
149 ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:149:168
status: NEW
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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. Login to comment
153 ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:153:61
status: NEW
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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. Login to comment
154 ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:154:12
status: NEW
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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. Login to comment
163 ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 22966014:163:26
status: NEW
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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. Login to comment
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. Login to comment
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 O1࢐O2 transitions. Login to comment
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. Login to comment
167 ABCC7 p.Arg352Gln
X
ABCC7 p.Arg352Gln 22966014:167:18
status: NEW
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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
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Before MESET modification, Cysless/I344C/R352Q mutant channels behaved similarly as Cysless/R352C-CFTR in the presence of ATP (Fig. 5 A). Login to comment
168 ABCC7 p.Arg352Gln
X
ABCC7 p.Arg352Gln 22966014:168:41
status: NEW
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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
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Before MESET modification, Cysless/I344C/R352Q mutant channels behaved similarly as Cysless/R352C-CFTR in the presence of ATP (Fig. 5 A). Login to comment
170 ABCC7 p.Arg352Gln
X
ABCC7 p.Arg352Gln 22966014:170:42
status: NEW
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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). Login to comment
171 ABCC7 p.Arg352Gln
X
ABCC7 p.Arg352Gln 22966014:171:42
status: NEW
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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 opening bursts encompassing more than one O1→O2 transition is higher in Cysless/R352C (Table 1). Login to comment
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 O1࢐O2 transition is higher in Cysless/R352C (Table 1). Login to comment
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). Login to comment
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). Login to comment
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. Login to comment
178 ABCC7 p.Arg352Gln
X
ABCC7 p.Arg352Gln 22966014:178:66
status: NEW
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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. Login to comment
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. Login to comment
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. Login to comment
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. Login to comment
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 analysis of gating events indeed demonstrates a higher percentage of gating events with reentry transitions in W401F/R352C-CFTR (Table 1). Login to comment
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). Login to comment
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). Login to comment
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). Login to comment
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. Login to comment
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 prolonging the open 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). Login to comment
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 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. Login to comment
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. Login to comment
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). Login to comment
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). Login to comment
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. Login to comment
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
Interestingly, 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. Login to comment
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. Login to comment
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. Login to comment
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. Login to comment
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. Login to comment
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. Login to comment
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. Login to comment
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). Login to comment
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 s1 for R352C-CFTR vs. 2.5 s1 for WT-CFTR; Vergani et al., 2003; Bompadre et al., 2005a). Login to comment
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. Login to comment
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-CFTR (C), and R352C/T1246N/E1371S-CFTR (D). Login to comment
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. Login to comment
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 fitted with a single-exponential function resulting in the relaxation time constant for each 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. Login to comment
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. Login to comment
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. Login to comment
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. Login to comment
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. Login to comment
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. Login to comment
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). Login to comment
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 current relaxation is prolonged in T1246N/K1250R- CFTR. Login to comment
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). Login to comment
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), suggesting that the two mutations affects two different kinetic steps as described above. Login to comment
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. Login to comment