ABCC7 p.Val345Lys
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PMID: 23083715
[PubMed]
El Hiani Y et al: "Tuning of CFTR chloride channel function by location of positive charges within the pore."
No.
Sentence
Comment
49
conductance (Fig. 2, B and C), especially in Q98K (conductance 75 5 1% of WT, n &#bc; 6) and V345K (64 5 3% of WT, n &#bc; 9), and in no case was conductance increased by the addition of a second positive charge.
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ABCC7 p.Val345Lys 23083715:49:93
status: NEW55 Additional mutations in a K95Q background to transplant the positive charge to pore-lining positions in TM1 (Q98K) or TM6 (I344K, V345K, M348K, and A349K) partially restored NPPB block (Fig. 3), although in no case was the block as strong as for the WT.
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ABCC7 p.Val345Lys 23083715:55:130
status: NEW56 The rank order of the apparent strength of NPPB block was WT > K95Q/V345K > K95Q/I344K > K95Q/Q98K ~ K95Q/ M348K ~ K95Q/A349K (Fig. 3 B).
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ABCC7 p.Val345Lys 23083715:56:68
status: NEW60 As shown in Fig. 4, block by Pt(NO2)4 2 was significantly strengthened in each of the mutants Q98K, I344K, V345K, M348K, and A349K, as well as in the previously unstudied S341K.
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ABCC7 p.Val345Lys 23083715:60:108
status: NEW61 At 0 mV membrane potential, the apparent Kd for Pt(NO2)4 2 block was in the rank order V345K (3.3 5 0.9 mM, n &#bc; 7) % I344K (4.5 5 0.7 mM, n &#bc; 6) < S341K (26.6 5 1.8 mM, n &#bc; 7) < M348K (80.9 5 7.2 mM, n &#bc; 5) % Q98K (95.4 5 11.0 mM, n &#bc; 6) % A349K (117.4 5 7.7 mM, FIGURE 2 Single-channel conductance is restored by moving the positive charge from K95.
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ABCC7 p.Val345Lys 23083715:61:88
status: NEW74 Blocker voltage dependence was also significantly changed in most mutants, with the effective blocker valence (zd) being significantly increased in M348K and significantly decreased in Q98K, V345K, and A349K (Fig. 4 F).
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ABCC7 p.Val345Lys 23083715:74:191
status: NEW82 Interestingly, whereas the conductance of I344H (at pH 5.5) was not significantly different from that of I344K (p > 0.37; Fig. 2 C), the conductance of V345H (pH 5.5) was ~20% greater than that of V345K (p < 0.002).
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ABCC7 p.Val345Lys 23083715:82:197
status: NEW90 However, although a single positive charge is necessary, the addition of a second positive charge to this region of the pore (as in the point mutants Q98K, I344K, V345K, M348K, and A349K) failed to increase conductance above WT levels (Fig. 2), as previously observed for S1141K (8).
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ABCC7 p.Val345Lys 23083715:90:163
status: NEW99 In fact, the addition of a second positive charge in Q98K, I344K, V345K, M348K, and A349K led to a small, but significant, decrease in conductance (Fig. 2 C).
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ABCC7 p.Val345Lys 23083715:99:66
status: NEW103 Furthermore, the notion that charge is not the only factor that influences conductance is supported by the fact that the conductance of V345K was significantly less than that of V345H when measured at pH 5.5, where the histidine side chain is expected to bear a positive charge.
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ABCC7 p.Val345Lys 23083715:103:136
status: NEW105 The weakening of blocker binding seen in K95Q is partially reversed by the second site mutations I344K and V345K, and to a lesser extent Q98K, M348K, and A349K.
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ABCC7 p.Val345Lys 23083715:105:107
status: NEW146 Again this appears to be a relatively nonsite-specific effect of positive charge, since all mutants studied (Q98K, S341K, I344K, V345K, M348K, and A349K) led to significant increase in apparent affinity of Pt(NO2)4 2 block (Fig. 4), as did S1141K (8).
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ABCC7 p.Val345Lys 23083715:146:129
status: NEW147 Most striking were I344K and V345K, which led to an ~70-fold and ~95-fold increase in apparent affinity, respectively (Fig. 4 E).
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ABCC7 p.Val345Lys 23083715:147:29
status: NEW151 The cartoon model of Fig. 1 suggests that it is proximity to the endogenous positive charge at K95, at least in terms of location along the axis of the pore, that determines the ability of introduced positive charges to strengthen Pt(NO2)4 2 block, since I344K and V345K (Fig. 4), together with S1141K (8), give the most potent block.
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ABCC7 p.Val345Lys 23083715:151:266
status: NEW
PMID: 24671572
[PubMed]
Linsdell P et al: "State-dependent blocker interactions with the CFTR chloride channel: implications for gating the pore."
No.
Sentence
Comment
6
Interestingly, mutations in the pore that weakened (K95Q) or strengthened (I344K, V345K) interactions with Pt(NO2)4 2- altered blocker effects both on Cl-permeation and on channel gating, suggesting that both these effects are a consequence of Pt(NO2)4 2- interaction with a single site within the pore.
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ABCC7 p.Val345Lys 24671572:6:82
status: NEW31 Furthermore, when the number of positive charges lining this part of the inner vestibule is increased from one (as in wild type) to two (for example in the channel mutants I344K, V345K, and S1141K), blocker potency is increased [8, 36].
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ABCC7 p.Val345Lys 24671572:31:179
status: NEW43 Where the properties of different channel pore variants (wild type, K95Q, I344K, V345K) have been directly compared in wild type and E1371Q backgrounds, the wild-type background is referred to as "1371E" to indicate that the endogenous glutamate residue is present at this position.
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ABCC7 p.Val345Lys 24671572:43:81
status: NEW109 Removal of the key endogenous positive charge (using the K95Q mutation) greatly weakens Pt(NO2)4 2- block (Fig. 3(B-D)), whereas addition of a second pore-lining positive charge (in I344K or V345K) dramatically strengthens open-channel block (Fig. 3(B-D)).
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ABCC7 p.Val345Lys 24671572:109:191
status: NEW110 Interestingly, not only blocker binding affinity (Fig. 3(D)) but also blocker voltage dependence (Fig. 3(E)) appeared correlated with the number of positively charged lysine side chains lining the inner vestibule of the pore; both I344K/E1371Q and V345K/E1371Q gave very strong, very strongly voltage-dependent block (Fig. 3(A, C-E)).
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ABCC7 p.Val345Lys 24671572:110:248
status: NEW113 In contrast, the strong inhibitory effects of Pt(NO2)4 2- on both I344K- and V345K-containing channels were observed in both E1371Q and 1371E backgrounds (Fig. 4(B)).
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ABCC7 p.Val345Lys 24671572:113:77
status: NEW114 Most strikingly, however, the very strong voltage dependence of block seen in both I344K/E1371Q and V345K/E1371Q (Fig. 3) was not observed in I344K/1371E and V345K/1371E channels that were allowed to open and close normally; instead, block was very strong but almost completely voltage-independent (Fig. 4).
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ABCC7 p.Val345Lys 24671572:114:100
status: NEWX
ABCC7 p.Val345Lys 24671572:114:158
status: NEW115 In many ways, these results with I344K and V345K recapitulate the results observed when comparing wild type and E1371Q channels (Fig. 1); block is weaker in E1371Q-containing channels (Fig. 4(C)), and blocker voltage dependence is greatly decreased (Fig. 4(D)).
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ABCC7 p.Val345Lys 24671572:115:43
status: NEW119 Gating of I344K and V345K channels was affected by Pt(NO2)4 2- in a similar manner to those of wild-type channels, but at much lower concentrations.
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ABCC7 p.Val345Lys 24671572:119:20
status: NEW122 Investigation of the effect of different concentrations of Pt(NO2)4 2- on the PO of wild type, I344K and V345K channels (Fig. 5(C)) confirms a dramatic increase in the apparent potency with which Pt(NO2)4 2- ions interact with these channel pore mutants.
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ABCC7 p.Val345Lys 24671572:122:105
status: NEW123 Effect of extracellular Clon Pt(NO2)4 2- block As a consequence of the striking difference in voltage-dependence of block of I344K and V345K-containing channels studied in 1371E (Fig. 4) or E1371Q backgrounds (Fig. 3), there was an unusual "cross-over" effect in the relationship between the KD for Pt(NO2)4 2- block and voltage (Fig. 4(B)), suggesting that block is stronger in 1371E than in E1371Q channels at positive voltages, but weaker in 1371E at the most negative voltages studied.
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ABCC7 p.Val345Lys 24671572:123:135
status: NEW126 Under these conditions, cross-over of the KD-voltage relationship was observed for wild type and I344K channels, whereas for V345K channels block was now stronger in E1371Q channels at all voltages studied.
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ABCC7 p.Val345Lys 24671572:126:125
status: NEW135 Under these ionic conditions, the E1371Q mutation increased the apparent affinity of block (Fig. 7(A, B)), an effect that was especially strong in I344K and V345K channels and at hyperpolarized voltages.
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ABCC7 p.Val345Lys 24671572:135:157
status: NEW136 This contrasts with what was found under high [Cl- ] conditions, where the E1371Q mutation decreased the affinity of block, especially in I344K and V345K (Fig. 4(C)).
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ABCC7 p.Val345Lys 24671572:136:148
status: NEW146 However, [Cl- ] has little effect on the voltage dependence of block (Fig. 7(E)), which is already very strong in I344K/E1371Q and V345K/E1371Q channels (Figs. 4(D) and 7(C)).
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ABCC7 p.Val345Lys 24671572:146:131
status: NEW148 The strong effect of [Cl- ] on the strength of block of I344K and V345K is abolished (Fig. 7(D)), and high [Cl- ] actually reduces the strong apparent voltage dependence of block in these same mutants (Fig. 7(E)).
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ABCC7 p.Val345Lys 24671572:148:66
status: NEW150 (A) Example currents recorded from inside out patches each containing two active CFTR channels, either I344K (top) or V345K (bottom).
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ABCC7 p.Val345Lys 24671572:150:118
status: NEW152 All closed state is indicated by the line to the left. Note that V345K exhibits a significantly reduced single-channel current amplitude, as described and quantified previously [8].
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ABCC7 p.Val345Lys 24671572:152:65
status: NEW155 (C) Effect of different concentrations of Pt(NO2)4 2- on the PO of wild type, I344K and V345K channels as indicated.
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ABCC7 p.Val345Lys 24671572:155:88
status: NEW165 Mean of data from 5 to 11 patches Pt(NO2)4 2-binding within the inner vestibule of the pore, since they are weakened by the K95Q mutation and strengthened in I344K and V345K (Fig. 3(C)), as described previously [8, 36].
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ABCC7 p.Val345Lys 24671572:165:169
status: NEW172 Thus, effects on gating are apparently lost in K95Q (Fig. 4(B)), and are substantially strengthened by mutations (I344K, V345K) that increase the strength of binding inside the pore (Figs. 4 and 5).
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ABCC7 p.Val345Lys 24671572:172:121
status: NEW175 However, these two effects appear unable to explain the overall effects of Pt(NO2)4 2- in I344K and V345K (Figs. 4(B) and 6(C)), or effects on wild type under low extracellular [Cl- ] conditions (Fig. 6(C)).
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ABCC7 p.Val345Lys 24671572:175:100
status: NEW187 Perhaps supporting the former hypothesis, this putative stimulatory effect of Pt(NO2)4 2- does appear to be positively correlated with strong open-channel block, i.e., it is not observed in K95Q but is prominent in I344K and V345K channels that show strong binding, and at negative voltages that promote open-channel block (Fig. 6).
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ABCC7 p.Val345Lys 24671572:187:225
status: NEW200 Interestingly, this apparent knock-off effect is greatly strengthened in I344K/E1371Q and V345K/E1371Q (Fig. 7(D)), suggesting Fig. 8 Schematic summary of the effects of Pt(NO2)4 2- .
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ABCC7 p.Val345Lys 24671572:200:90
status: NEW
PMID: 25673337
[PubMed]
Rubaiy HN et al: "Location of a permeant anion binding site in the cystic fibrosis transmembrane conductance regulator chloride channel pore."
No.
Sentence
Comment
79
e Mean KD values for Au(CN)2 - block for these channel constructs, as well as the additional positive charge mutants V345K/ E1371Q and S1141K/E1371Q, obtained as described in Fig. 1. f Relationship between the observed KD values for Au(CN)2 - block (at -100 mV) and the expected number of fixed positive charges in the pore inner vestibule in different channel constructs.
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ABCC7 p.Val345Lys 25673337:79:117
status: NEW90 Consistent with this, mutation of any of these three residues to lysine (I344K, V345K, S1141K) led to a significant strengthening of Au(CN)2 - block (Fig. 3d-f), with mean KD values at -100 mV being reduced by 18-fold (I344K/E1371Q), 17-fold (V345K/E1371Q) and 7-fold (S1141K/E1371Q), respectively.
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ABCC7 p.Val345Lys 25673337:90:80
status: NEWX
ABCC7 p.Val345Lys 25673337:90:243
status: NEW