Home
Browse
Search
Statistics
About
Usage
PMID: 17043148
Csanady L, Nairn AC, Gadsby DC
Thermodynamics of CFTR channel gating: a spreading conformational change initiates an irreversible gating cycle.
J Gen Physiol. 2006 Nov;128(5):523-33. Epub 2006 Oct 16.,
[PubMed]
Sentences
No.
Mutations
Sentence
Comment
9
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 17043148:9:134
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 17043148:9:123
status:
NEW
view ABCC7 p.Lys1250Arg details
∆H‡ for reversal of the channel opening step, estimated from closure of ATP hydrolysis-deficient NBD2 mutant
K1250R
and
K1250A
channels, and from unlocking of WT channels locked open with ATP+AMPPNP, was 43 ± 2, 39 ± 4, and 37 ± 6 kJ/mol, respectively.
Login to comment
41
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 17043148:41:145
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 17043148:41:134
status:
NEW
view ABCC7 p.Lys1250Arg details
M AT E R I A L S A N D M E T H O D S Molecular Biology pGEMHE-WT was constructed as previously described (Chan et al., 2000), and the
K1250R
and
K1250A
mutations introduced using QuikChange (Stratagene) as previously described (Vergani et al., 2003, 2005).
Login to comment
88
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 17043148:88:150
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 17043148:88:139
status:
NEW
view ABCC7 p.Lys1250Arg details
S2-S4 show parallel macroscopic current and temperature records illustrating temperature dependence of closure of partially phosphorylated
K1250R
and
K1250A
, and of AMPPNP-locked WT, CFTR, respectively, recorded at -80 to -20 mV between 25°C and 31°C. Fig. S5 demonstrates that exposure to millimolar levels of the hydrolysis products ADP+Pi does not cause opening of prephosphorylated WT CFTR channels.
Login to comment
89
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 17043148:89:76
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 17043148:89:88
status:
NEW
view ABCC7 p.Lys1250Arg details
Fig. S6 shows the predicted energetic profile of CFTR gating obtained using
K1250A
, not
K1250R
(as in Fig. 6), as a model for nonhydrolytic channel closure.
Login to comment
105
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 17043148:105:81
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 17043148:105:70
status:
NEW
view ABCC7 p.Lys1250Arg details
Temperature Dependence of Closing Rate of Hydrolysis-deficient Mutant
K1250R
and
K1250A
CFTR Channels To estimate ∆H‡ for channel closing when the normal route for channel closure via ATP hydrolysis was unavailable, we studied the temperature dependence of the closing rate of two channel constructs in which the composite NBD2 site was made catalytically inactive by mutation of the conserved NBD2 Walker A lysine, K1250.
Login to comment
106
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 17043148:106:13
status:
NEW
view ABCC7 p.Lys1250Ala details
The mutation
K1250A
has been shown to abolish ATPase activity of purified CFTR (Ramjeesingh et al., 1999).
Login to comment
107
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 17043148:107:164
status:
NEW
view ABCC7 p.Lys1250Arg details
In another ABC ATPase, P-glycoprotein, the Lys-to-Arg mutation of either Walker A lysine abolishes ATP hydrolysis (Lerner-Marmarosh et al., 1999), and in CFTR, the
K1250R
mutation prolongs open burst durations by >20-fold (compare Vergani et al., 2005), consistent with abolished, or greatly diminished, ATP hydrolysis.
Login to comment
108
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 17043148:108:24
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 17043148:108:11
status:
NEW
view ABCC7 p.Lys1250Arg details
Closure of
K1250R
or of
K1250A
mutant CFTR channels is too slow to allow kinetic analysis of individual gating events and so it was assayed as current decay after sudden removal of ATP.
Login to comment
110
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 17043148:110:18
status:
NEW
view ABCC7 p.Lys1250Arg details
Prephosphorylated
K1250R
CFTR channels in macropatches were repeatedly opened by brief exposures to 2 mM MgATP at temperatures alternating between 25°C and °51فC (Fig. 3 A), or 25°C and °13فC (Fig. S2).
Login to comment
113
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 17043148:113:12
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 17043148:113:156
status:
NEW
view ABCC7 p.Lys1250Ala details
Because the
K1250A
mutation greatly diminishes the affinity for ATP binding (Vergani et al., 2003), 10 mM MgATP was used to repeatedly activate macroscopic
K1250A
currents at temperatures alternating between 25°C and either °51فC (Fig. 4 A) or °13فC (Fig. S3).
Login to comment
114
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 17043148:114:271
status:
NEW
view ABCC7 p.Lys1250Arg details
The Eyring plot (Fig. 4 B) of the normalized closing rates obtained from single exponential fits (Fig. 4 A, smooth lines) to the decaying currents after ATP removal yielded a ∆H‡ for nonhydrolytic closure of 39 ± 4 kJ/mol, similar to that obtained for
K1250R
channels (Fig. 3 B).
Login to comment
115
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 17043148:115:185
status:
NEW
view ABCC7 p.Lys1250Arg details
Interestingly, whereas open burst duration of WT channels was greater than twofold longer in the presence of PKA than shortly after its withdrawal, the average closing time constant of
K1250R
at 25°C, equivalent to its mean open burst duration, was only slightly longer (Fig. 3 A; Fig. S2) upon removal of PKA+ATP (7.3 ± 0.8 s, n = 12) than upon removal of just ATP (5.7 ± 0.4 s, n = 30).
Login to comment
116
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 17043148:116:192
status:
NEW
view ABCC7 p.Lys1250Arg details
But, because the fall in Po that signals partial dephosphorylation of WT channels upon PKA removal occurs so rapidly (i.e., in 2-3 s; Csanády et al., 2000), the phosphorylation status of
K1250R
channels after removal of ATP+PKA, during their gradual closure, which takes tens of seconds (compare Fig. 3 A, current segments fitted by magenta lines), is uncertain.
Login to comment
117
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 17043148:117:4
status:
NEW
view ABCC7 p.Lys1250Ala details
For
K1250A
channels, the closing time constant after simultaneous removal of ATP and PKA was rarely assessed (τ = 38 ± 4 s, n = 3), and is not easily compared with that after removal of just ATP (τ = 25 ± 2 s, n = 29), as the latter usually progressively shortened during an experiment (τ = 29 ± 3 s, n = 18, for the first decay from each Figure 1.
Login to comment
130
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 17043148:130:61
status:
NEW
view ABCC7 p.Lys1250Arg details
Temperature dependence of gating of partially phosphorylated
K1250R
CFTR.
Login to comment
131
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 17043148:131:70
status:
NEW
view ABCC7 p.Lys1250Arg details
(A) Macroscopic current trace (top) from 000,2ف
K1250R
CFTR channels at -20 mV, with simultaneously recorded temperature (bottom).
Login to comment
135
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 17043148:135:60
status:
NEW
view ABCC7 p.Lys1250Arg details
(B) Eyring plot of normalized closing rates ( ˆk ) of
K1250R
CFTR channels upon ATP removal, fitted by a straight line to obtain ∆H‡ value shown; closing rates, obtained as 1/τ from single-exponential fits, as in A, were normalized to their average values in bracketing control segments at 25°C. Figure 4.
Login to comment
136
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 17043148:136:61
status:
NEW
view ABCC7 p.Lys1250Ala details
Temperature dependence of gating of partially phosphorylated
K1250A
CFTR.
Login to comment
137
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 17043148:137:45
status:
NEW
view ABCC7 p.Lys1250Ala details
(A) Macroscopic current recording (top) from
K1250A
CFTR channels with simultaneously recorded temperature (bottom).
Login to comment
140
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 17043148:140:60
status:
NEW
view ABCC7 p.Lys1250Ala details
(B) Eyring plot of normalized closing rates ( ˆk ) of
K1250A
CFTR channels upon ATP removal, fitted by a straight line to obtain ∆H‡; closing rates, obtained as 1/τ from single-exponential fits, as in A, were normalized to their average values in bracketing control segments at 25°C.
Login to comment
145
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 17043148:145:276
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 17043148:145:265
status:
NEW
view ABCC7 p.Lys1250Arg details
From an Eyring plot of normalized unlocking rates (Fig. 5 B), the rough estimate of ∆H‡ for unlocking from AMPPNP of partially phosphorylated WT CFTR was 37 ± 6 kJ/ mol, similar to the value obtained above for closure of partially phosphorylated
K1250R
and
K1250A
channels opened by just ATP (Fig. 3 B and Fig. 4 B).
Login to comment
166
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 17043148:166:36
status:
NEW
view ABCC7 p.Lys1250Arg details
We chose NBD2 catalytic site mutant
K1250R
as one model for nonhydrolytic closure because the mutation conserves charge in the anticipated catalytic interface, and, in P-glycoprotein, the corresponding K-to-R mutation essentially abolishes ATP hydrolysis (Lerner-Marmarosh et al., 1999).
Login to comment
167
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 17043148:167:23
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 17043148:167:177
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 17043148:167:119
status:
NEW
view ABCC7 p.Lys1250Arg details
We selected the mutant
K1250A
as a second model for nonhydrolytic closure because it displays much slower closure than
K1250R
(e.g., Vergani et al., 2003, 2005) and because the
K1250A
mutation abolishes ATP hydrolysis by CFTR (Ramjeesingh et al., 1999).
Login to comment
179
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 17043148:179:127
status:
NEW
view ABCC7 p.Lys1250Arg details
Second, because ∆H‡ is high (117 kJ/mol) for opening, but small for nonhydrolytic closure (e.g., 43 kJ/mol using
K1250R
as a model), α Δ O-CH must be large (+74 kJ/mol; Fig. 6 A, red line).
Login to comment
180
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 17043148:180:96
status:
NEW
view ABCC7 p.Lys1250Arg details
Third, in contrast, α Δ O-CG is estimated to be rather small (e.g., -1 kJ/mol using
K1250R
as a model; Fig. 6 A, blue line), which in turn suggests that α Δ O-CS is large ( α Δ O-CT S ≈ 75 kJ/mol; Fig. 6 A, green line).
Login to comment
182
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 17043148:182:151
status:
NEW
view ABCC7 p.Lys1250Arg details
Also, independent evidence that α Δ O-CG ≈ 0 is provided by the observation that steady-state Po ≈ 0.5 for the nonhydrolytic
K1250R
mutant, which is presumed to gate at thermodynamic equilibrium (Vergani et al., 2005).
Login to comment
187
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 17043148:187:117
status:
NEW
view ABCC7 p.Lys1250Arg details
The paucity of ATPase measurements for CFTR mutants means that we cannot be certain that the charge-sparing mutation
K1250R
abolishes ATP hydrolysis in CFTR, even though the equivalent mutation in P-glycoprotein abolishes ATP hydrolysis (Lerner-Marmarosh et al., 1999).
Login to comment
188
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 17043148:188:33
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 17043148:188:173
status:
NEW
view ABCC7 p.Lys1250Arg details
The charge-neutralizing mutation
K1250A
, on the other hand,doesabrogateATPhydrolysisinCFTR(Ramjeesingh et al., 1999) and yields an open burst state more stable than that of
K1250R
(Vergani et al., 2003, 2005).
Login to comment
189
ABCC7 p.Lys1250Ala
X
ABCC7 p.Lys1250Ala 17043148:189:30
status:
NEW
view ABCC7 p.Lys1250Ala details
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 17043148:189:49
status:
NEW
view ABCC7 p.Lys1250Arg details
But using the closing rate of
K1250A
(instead of
K1250R
) channels as a model for nonhydrolytic closure, and hence for reversal of channel opening, yields barrier values for this step (∆H‡ = 39 kJ/mol and Δ maxG‡ = 81 kJ/mol) that are onlyslightlydifferentfromthoseestimatedusingK1250R.
Login to comment
191
ABCC7 p.Glu1371Gln
X
ABCC7 p.Glu1371Gln 17043148:191:33
status:
NEW
view ABCC7 p.Glu1371Gln details
Even for the Walker B Glu mutant
E1371Q
CFTR channels, which display the most stable open-burst state observed for CFTR (closing time constant 004ف s; Vergani et al., 2005), corresponding to Δ maxG‡ = 88 kJ/mol, if ∆H‡ is assumed 04ف kJ/mol (its experimental determination would be a formidable task), the model predicts α Δ O-CG = -12 kJ/ mol, and again a similar overall energy profile.
Login to comment
202
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 17043148:202:224
status:
NEW
view ABCC7 p.Lys1250Arg details
Forward (left to right) ∆H‡ values were obtained from slopes of Eyring plots for WT opening and closing rates (Fig. 1 C), ∆H‡ for the reversal of opening reflects the slope of the Eyring plot for
K1250R
closing rate (Fig. 3B).
Login to comment
203
ABCC7 p.Lys1250Arg
X
ABCC7 p.Lys1250Arg 17043148:203:156
status:
NEW
view ABCC7 p.Lys1250Arg details
Corresponding Δ maxG‡ values were computed as RT ln(kBT/(kh)), by substituting the rates of WT opening (0.3 s-1) and closure (3.9 s-1), and of
K1250R
closure (0.2 s-1), for k.
Login to comment