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PMID: 9089437
Cheung M, Akabas MH
Locating the anion-selectivity filter of the cystic fibrosis transmembrane conductance regulator (CFTR) chloride channel.
J Gen Physiol. 1997 Mar;109(3):289-99.,
[PubMed]
Sentences
No.
Mutations
Sentence
Comment
9
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 9089437:9:64
status:
NEW
view ABCC7 p.Arg352Cys details
Furthermore, the electrical distance calculations indicate that
R352C
is closer to the extracellular end of the channel than either of the adjacent residues. We speculate that the cytoplasmic end of the M6 segment may loop back into the channel narrowing the lumen and thereby forming both the major resistance to current flow and the anion-selectivity filter.
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19
ABCC7 p.Arg347His
X
ABCC7 p.Arg347His 9089437:19:12
status:
NEW
view ABCC7 p.Arg347His details
Mutation of
Arg347 to His
resulted in pH-dependent anomalous mole-fraction effects, indicating that the positive charge at this position was important and that Arg347 was at or near one of the anion-binding sites (Tabcharani et al., 1993).
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20
ABCC7 p.Arg347Glu
X
ABCC7 p.Arg347Glu 9089437:20:13
status:
NEW
view ABCC7 p.Arg347Glu details
The mutation
R347E
, however, had little or no effect on the halide permeability or conductance sequences (Anderson et al., 1991b).
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21
ABCC7 p.Lys335Glu
X
ABCC7 p.Lys335Glu 9089437:21:26
status:
NEW
view ABCC7 p.Lys335Glu details
In contrast, the mutation
K335E
changed the halide permeability and/or conductance sequences (Anderson et al., 1991b) but did not alter the anomalous mole-fraction effects (Tabcharani et al., 1993).
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71
ABCC7 p.Thr351Cys
X
ABCC7 p.Thr351Cys 9089437:71:14
status:
NEW
view ABCC7 p.Thr351Cys details
Activation of
T351C
mutant and effect of MTSEAϩ.
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72
ABCC7 p.Thr351Cys
X
ABCC7 p.Thr351Cys 9089437:72:91
status:
NEW
view ABCC7 p.Thr351Cys details
(A) Illustration of the activation of the CFTR-induced current in an oocyte expressing the
T351C
mutant under two-electrode voltage clamp.
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102
ABCC7 p.Thr351Cys
X
ABCC7 p.Thr351Cys 9089437:102:25
status:
NEW
view ABCC7 p.Thr351Cys details
2 and 3 A for the mutant
T351C
.
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107
ABCC7 p.Arg347Cys
X
ABCC7 p.Arg347Cys 9089437:107:343
status:
NEW
view ABCC7 p.Arg347Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 9089437:107:1752
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Gln353Cys
X
ABCC7 p.Gln353Cys 9089437:107:1917
status:
NEW
view ABCC7 p.Gln353Cys details
ABCC7 p.Arg334Cys
X
ABCC7 p.Arg334Cys 9089437:107:926
status:
NEW
view ABCC7 p.Arg334Cys details
ABCC7 p.Lys335Cys
X
ABCC7 p.Lys335Cys 9089437:107:1089
status:
NEW
view ABCC7 p.Lys335Cys details
ABCC7 p.Thr351Cys
X
ABCC7 p.Thr351Cys 9089437:107:1587
status:
NEW
view ABCC7 p.Thr351Cys details
ABCC7 p.Leu333Cys
X
ABCC7 p.Leu333Cys 9089437:107:753
status:
NEW
view ABCC7 p.Leu333Cys details
ABCC7 p.Ile331Cys
X
ABCC7 p.Ile331Cys 9089437:107:83
status:
NEW
view ABCC7 p.Ile331Cys details
ABCC7 p.Ser341Cys
X
ABCC7 p.Ser341Cys 9089437:107:1421
status:
NEW
view ABCC7 p.Ser341Cys details
ABCC7 p.Ile344Cys
X
ABCC7 p.Ile344Cys 9089437:107:333
status:
NEW
view ABCC7 p.Ile344Cys details
ABCC7 p.Phe337Cys
X
ABCC7 p.Phe337Cys 9089437:107:1255
status:
NEW
view ABCC7 p.Phe337Cys details
We did not measure the reaction rate constants for the most extracellular residue,
I331C
, because we thought that it was unlikely that the reaction rates would be voltage dependent given the absence of voltage dependence at the adjacent, more cytoplasmic residues. We also did not measure the reaction rate constants for the mutants
I344C
and
R347C
because, although MTSEAϩ reacted with these residues, MTSES- and MTSETϩ did not react with these k ψ( )( )ln k Ψ 0=( )( ) zFδ RT/( )-ln ψ= t a b l e i Second-order Rate Constants for the Reaction of the MTS Reagents with the Water-exposed Cysteine Mutants k ES (M-1s-1) k EA (M-1s-1) k ET (M-1s-1) mutant -25 mV -50 mV -75 mV -25 mV -50 mV -75 mV -25 mV -50 mV -75 mV
L333C
71 Ϯ 3(3) 71 Ϯ 20(2) 71 Ϯ 23(3) 320 Ϯ 89(2) 320 Ϯ 128(2) 333 Ϯ 139(3) 952 Ϯ 136(2) 1,000 Ϯ 350(2) 1,053 Ϯ 443(2)
R334C
48 Ϯ 14(2) 48 Ϯ 6(3) 44 Ϯ 8(4) 145 Ϯ 32(2) 163 Ϯ 7(2) 182 Ϯ 21(3) 444 Ϯ 49(2) 454 Ϯ 124(2) 588 Ϯ 95(3)
K335C
36 Ϯ 20(3) 23 Ϯ 11(3) 27 Ϯ 16(3) 222 Ϯ 80(3) 121 Ϯ 51(4) 107 Ϯ 30(3) 217 Ϯ 111(3) 235 Ϯ 28(3) 217 Ϯ 95(4)
F337C
91 Ϯ 17(2) 80 Ϯ 22(3) 71 Ϯ 20(4) 222 Ϯ 74(2) 222 Ϯ 86(3) 285 Ϯ 81(3) 740 Ϯ 246(3) 740 Ϯ 82(2) 714 Ϯ 51(2)
S341C
56 Ϯ 18(3) 56 Ϯ 40(2) 43 Ϯ 12(3) 93 Ϯ 6(3) 110 Ϯ 22(3) 138 Ϯ 34(3) 690 Ϯ 356(3) 556 Ϯ 246(3) 800 Ϯ 224(4)
T351C
100 Ϯ 25(5) 57 Ϯ 6(3) 26 Ϯ 9(6) 146 Ϯ 30(4) 195 Ϯ 42(4) 296 Ϯ 18(3) 308 Ϯ 47(10) 392 Ϯ 78(6) 769 Ϯ 89(5)
R352C
42 Ϯ 4(3) 26 Ϯ 4(5) 21 Ϯ 6(4) 105 Ϯ 76(3) 137 Ϯ 46(3) 205 Ϯ 58(2) 417 Ϯ 138(4) 800 Ϯ 128(2) 952 Ϯ 408(2)
Q353C
125 Ϯ 23(4) 51 Ϯ 12(4) 42 Ϯ 8(4) 83 Ϯ 24(4) 116 Ϯ 42(4) 160 Ϯ 92(3) 189 Ϯ 48(6) 220 Ϯ 48(3) 625 Ϯ 273(4) residues and therefore we could not determine the charge selectivity at these positions.2 The reaction rate constants that we have measured are between 10-and 500-fold slower than the rates of reaction with sulfhydryls in free solution (Table II) (Stauffer and Karlin, 1994).
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112
ABCC7 p.Leu333Cys
X
ABCC7 p.Leu333Cys 9089437:112:334
status:
NEW
view ABCC7 p.Leu333Cys details
Furthermore, the voltage dependence of the rates of reaction of MTSES- is opposite to the voltage t a b l e i i Second-order Rate Constants at Holding Potential ϭ 0 mV and Ratios of Rate Constants at V ϭ 0 mV (kmtses/kmtset) 1 2* k0,MTSES 3* k0,MTSET 4‡ k0,MTSES 5§ kES/kET Mutant (M-1 S-1) (M-1 S-1) k0,MTSET
L333C
2-MEʈ 4300 51000 0.08 1 L333 68 828 0.08 1 R334 53 376 0.14 2 K335 47 455 0.1 1 F337 96 991 0.1 1 S341 72 727 0.1 1 T351 250 219 1.14 14 R352 48 324 0.15 2 Q353 213 102 2.09 26 *Columns 2, 3 are the rate constants for MTSES- and MTSETϩ at V ϭ 0 mV.
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115
ABCC7 p.Leu333Cys
X
ABCC7 p.Leu333Cys 9089437:115:58
status:
NEW
view ABCC7 p.Leu333Cys details
The same ratio is observed for the rates of reaction with
L333C
indicating that there is no charge selectivity for the reaction with this residue.
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116
ABCC7 p.Leu333Cys
X
ABCC7 p.Leu333Cys 9089437:116:150
status:
NEW
view ABCC7 p.Leu333Cys details
§Column 5 is the anion to cation selectivity ratio derived by dividing the data in Column 4 by the ratio obtained for the rates of reaction with
L333C
.
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117
ABCC7 p.Leu333Cys
X
ABCC7 p.Leu333Cys 9089437:117:152
status:
NEW
view ABCC7 p.Leu333Cys details
The ratio of the rate constants (kmtses/kmtset) for reaction with an exposed cysteine relative to the ratio of the rate constants for the reaction with
L333C
gives a measure of the anion to cation selectivity at the level of an exposed cysteine.
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120
ABCC7 p.Arg347Cys
X
ABCC7 p.Arg347Cys 9089437:120:59
status:
NEW
view ABCC7 p.Arg347Cys details
2In the course of these experiments we discovered that the
R347C
construct that we had used previously contained a large truncation, deleting most of the R-domain to the COOH terminus.
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121
ABCC7 p.Arg347Cys
X
ABCC7 p.Arg347Cys 9089437:121:38
status:
NEW
view ABCC7 p.Arg347Cys details
In the full length CFTR construct the
R347C
mutant is accessible to MTSEAϩ which causes 19% inhibition, however, MTSES- and MTSETϩ do not react with this mutant.
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123
ABCC7 p.Thr351Cys
X
ABCC7 p.Thr351Cys 9089437:123:95
status:
NEW
view ABCC7 p.Thr351Cys details
Experiments illustrating data used to determine rates of reaction of the MTS reagents with the
T351C
mutant.
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129
ABCC7 p.Thr351Cys
X
ABCC7 p.Thr351Cys 9089437:129:114
status:
NEW
view ABCC7 p.Thr351Cys details
(B) The natural log of the rate constants, k, for MTSES- (circles) and MTSETϩ (triangles) reacting with the
T351C
mutant are plotted as a function of voltage.
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134
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 9089437:134:123
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Leu333Cys
X
ABCC7 p.Leu333Cys 9089437:134:55
status:
NEW
view ABCC7 p.Leu333Cys details
ABCC7 p.Ser341Cys
X
ABCC7 p.Ser341Cys 9089437:134:64
status:
NEW
view ABCC7 p.Ser341Cys details
Note that the electrical distance to the residues from
L333C
to
S341C
is close to zero and that the electrical distance to
R352C
is smaller than the electrical distance to the adjacent residues.
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148
ABCC7 p.Thr351Cys
X
ABCC7 p.Thr351Cys 9089437:148:111
status:
NEW
view ABCC7 p.Thr351Cys details
In Fig. 3 B the natural log of the rate constants for the reactions of MTSES- and MTSETϩ with the mutant
T351C
are plotted as a function of membrane potential.
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154
ABCC7 p.Gln353Cys
X
ABCC7 p.Gln353Cys 9089437:154:53
status:
NEW
view ABCC7 p.Gln353Cys details
ABCC7 p.Thr351Cys
X
ABCC7 p.Thr351Cys 9089437:154:43
status:
NEW
view ABCC7 p.Thr351Cys details
The distance from the extracellular end to
T351C
and
Q353C
is significantly greater than to the other residues (P Ͻ 0.05).
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155
ABCC7 p.Leu333Cys
X
ABCC7 p.Leu333Cys 9089437:155:20
status:
NEW
view ABCC7 p.Leu333Cys details
lar residue tested,
L333C
, the ratio of the rates of reaction of MTSES-/MTSETϩ is also 0.08 (Table II, column 4); this suggests that there is no charge selectivity for access of the MTS reagents to this residue from the extracellular solution.
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156
ABCC7 p.Leu333Cys
X
ABCC7 p.Leu333Cys 9089437:156:187
status:
NEW
view ABCC7 p.Leu333Cys details
To account for this difference in the intrinsic rates of reaction of the two MTS reagents, we divided the ratio of the rates at a given residue by the ratio of the rates of reaction with
L333C
.
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162
ABCC7 p.Thr351Cys
X
ABCC7 p.Thr351Cys 9089437:162:68
status:
NEW
view ABCC7 p.Thr351Cys details
The major site of charge selectivity appears to be in the region of
T351C
and Q353C where the anion to cation selectivity rises to between 15 and 25 (Fig. 5).
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173
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 9089437:173:60
status:
NEW
view ABCC7 p.Arg352Cys details
We now show that based on the measured electrical distances
R352C
appears to be closer to the extracellular end of the channel than either of the adjacent residues.
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180
ABCC7 p.Gln353Cys
X
ABCC7 p.Gln353Cys 9089437:180:302
status:
NEW
view ABCC7 p.Gln353Cys details
ABCC7 p.Thr351Cys
X
ABCC7 p.Thr351Cys 9089437:180:292
status:
NEW
view ABCC7 p.Thr351Cys details
By measuring the relative rates of reaction of anionic and cationic MTS reagents with water-exposed cysteines in and flanking the M6 segment we have shown that a major determinant of anion selectivity occurs near the cytoplasmic end of the channel; access of the negatively charged MTSES- to
T351C
and
Q353C
is favored over the positively charged MTSETϩ (Fig. 5).
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183
ABCC7 p.Gln353Cys
X
ABCC7 p.Gln353Cys 9089437:183:92
status:
NEW
view ABCC7 p.Gln353Cys details
ABCC7 p.Thr351Cys
X
ABCC7 p.Thr351Cys 9089437:183:82
status:
NEW
view ABCC7 p.Thr351Cys details
Consistent with this, the reaction rate constants for the reaction of MTSES- with
T351C
and
Q353C
are larger than the rates with other channel-lining residues (Table II, column 2).
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185
ABCC7 p.Gln353Cys
X
ABCC7 p.Gln353Cys 9089437:185:41
status:
NEW
view ABCC7 p.Gln353Cys details
ABCC7 p.Thr351Cys
X
ABCC7 p.Thr351Cys 9089437:185:31
status:
NEW
view ABCC7 p.Thr351Cys details
The arginine that lies between
T351C
and
Q353C
, Arg352, appears to be a major determinant of the anion selectivity in this region; when cysteine is substituted for the arginine at position 352 the selectivity is similar to that observed in the rest of the channel (Fig. 5).
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186
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 9089437:186:117
status:
NEW
view ABCC7 p.Arg352Cys details
If other residues in this region were the main determinants of anion selectivity, then, the anion selectivity of the
R352C
mutant should have been similar to that of the adjacent residues.
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187
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 9089437:187:50
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Gln353Cys
X
ABCC7 p.Gln353Cys 9089437:187:121
status:
NEW
view ABCC7 p.Gln353Cys details
ABCC7 p.Thr351Cys
X
ABCC7 p.Thr351Cys 9089437:187:111
status:
NEW
view ABCC7 p.Thr351Cys details
Based on our measurements of electrical distance,
R352C
is closer to the extracellular end of the channel than
T351C
and
Q353C
(Fig. 4, see below).
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188
ABCC7 p.Gln353Cys
X
ABCC7 p.Gln353Cys 9089437:188:186
status:
NEW
view ABCC7 p.Gln353Cys details
ABCC7 p.Thr351Cys
X
ABCC7 p.Thr351Cys 9089437:188:177
status:
NEW
view ABCC7 p.Thr351Cys details
Thus, ions passing from the extracellular end of the channel would first encounter Arg352, which we infer forms part of the charge-selectivity filter, before they could reach
T351C
or
Q353C
; thereby accounting for the greater anion selectivity we observed at these residues.
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191
ABCC7 p.Gln353Cys
X
ABCC7 p.Gln353Cys 9089437:191:82
status:
NEW
view ABCC7 p.Gln353Cys details
ABCC7 p.Thr351Cys
X
ABCC7 p.Thr351Cys 9089437:191:72
status:
NEW
view ABCC7 p.Thr351Cys details
The increase in the reaction rate constants for MTSES- with the mutants
T351C
and
Q353C
(Table II, column 2) is consistent with these residues being near an anion binding site which increases the dwell time of MTSES- in this region of the channel thereby effectively increasing the reaction rate constants.
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192
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 9089437:192:143
status:
NEW
view ABCC7 p.Arg352Cys details
A further suggestion that Arg352 is important in charge selectivity is the increase in the reaction rate of the cationic MTSETϩ with the
R352C
mutant as compared to the adjacent residues (Table II, column 3).
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193
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 9089437:193:36
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 9089437:193:219
status:
NEW
view ABCC7 p.Arg352Cys details
Removing the positive charge in the
R352C
mutant may increase the ability of cations to enter this region near the cytoplasmic end of the channel, thereby accounting for the increase rate of reaction of MTSETϩ at
R352C
compared to the adjacent residues.
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200
ABCC7 p.Gln353Cys
X
ABCC7 p.Gln353Cys 9089437:200:114
status:
NEW
view ABCC7 p.Gln353Cys details
ABCC7 p.Thr351Cys
X
ABCC7 p.Thr351Cys 9089437:200:104
status:
NEW
view ABCC7 p.Thr351Cys details
The ability of the cationic MTS reagents to move past the anion-selectivity filter, i.e., to react with
T351C
and
Q353C
, is consistent with the lack of ideal anion selectivity that has been reported by others.
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204
ABCC7 p.Lys335Glu
X
ABCC7 p.Lys335Glu 9089437:204:47
status:
NEW
view ABCC7 p.Lys335Glu details
ABCC7 p.Lys95Asp
X
ABCC7 p.Lys95Asp 9089437:204:38
status:
NEW
view ABCC7 p.Lys95Asp details
Based on the effects of the mutations
K95D
and
K335E
on halide selectivity sequences, Anderson et al. (1991b) concluded that Lys95 and Lys335 were determinants of halide selectivity.
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205
ABCC7 p.Arg347Glu
X
ABCC7 p.Arg347Glu 9089437:205:56
status:
NEW
view ABCC7 p.Arg347Glu details
ABCC7 p.Arg1030Glu
X
ABCC7 p.Arg1030Glu 9089437:205:66
status:
NEW
view ABCC7 p.Arg1030Glu details
Curiously, neither of these mutations nor the mutations
R347E
and
R1030E
were reported to alter the Cl- to Naϩ permeability ratio (PCl/PNa), and the latter two mutations had minimal effects on halide permeability or conductance ratios (Anderson et al., 1991b).
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206
ABCC7 p.Lys335Glu
X
ABCC7 p.Lys335Glu 9089437:206:17
status:
NEW
view ABCC7 p.Lys335Glu details
Furthermore, the
K335E
mutation had no effect on anomalous mole-fraction effects suggesting that Lys335 is not part of an anion binding site in the channel (Tabcharani et al., 1993).
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210
ABCC7 p.Gln353Cys
X
ABCC7 p.Gln353Cys 9089437:210:72
status:
NEW
view ABCC7 p.Gln353Cys details
ABCC7 p.Thr351Cys
X
ABCC7 p.Thr351Cys 9089437:210:62
status:
NEW
view ABCC7 p.Thr351Cys details
Note the marked increase in anion selectivity at the residues
T351C
and
Q353C
.
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234
ABCC7 p.Arg352Cys
X
ABCC7 p.Arg352Cys 9089437:234:131
status:
NEW
view ABCC7 p.Arg352Cys details
ABCC7 p.Thr351Cys
X
ABCC7 p.Thr351Cys 9089437:234:97
status:
NEW
view ABCC7 p.Thr351Cys details
The electrical distances from the extracellular end of the channel to these three residues, with
T351C
being more cytoplasmic than
R352C
, is also inconsistent with an ␣-helical secondary structure (Fig. 4).
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