 |
PDBsum entry 1eoe
|
|
|
|
 |
|
|
|
|
|
|
|
|
|
|
|
 |
|
|
|
 |
 |
 |
 |
 |
 |
 |
 |
 |
 |
 |
 |
 |
 |
 |
|
|
|
|
|
|
|
|
|
|
Membrane protein
|
PDB id
|
|
|
|
1eoe
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
 |
Contents |
 |
|
|
|
|
|
|
|
|
|
* Residue conservation analysis
|
|
|
|
|
References listed in PDB file
|
 |
|
Key reference
|
 |
|
Title
|
 |
Voltage dependent activation of potassium channels is coupled to t1 domain structure.
|
 |
|
Authors
|
 |
S.J.Cushman,
M.H.Nanao,
A.W.Jahng,
D.Derubeis,
S.Choe,
P.J.Pfaffinger.
|
 |
|
Ref.
|
 |
Nat Struct Biol, 2000,
7,
403-407.
[DOI no: ]
|
 |
|
PubMed id
|
 |
|
 |
 |
|
Abstract
|
 |
|
The T1 domain, a highly conserved cytoplasmic portion at the N-terminus of the
voltage-dependent K+ channel (Kv) alpha-subunit, is responsible for driving and
regulating the tetramerization of the alpha-subunits. Here we report the
identification of a set of mutations in the T1 domain that alter the gating
properties of the Kv channel. Two mutants produce a leftward shift in the
activation curve and slow the channel closing rate while a third mutation
produces a rightward shift in the activation curve and speeds the channel
closing rate. We have determined the crystal structures of T1 domains containing
these mutations. Both of the leftward shifting mutants produce similar
conformational changes in the putative membrane facing surface of the T1 domain.
These results suggest that the structure of the T1 domain in this region is
tightly coupled to the channel's gating states.
|
 |
 |
 |
|
 |
|
 |
Figure 1.
Figure 1. Location of T1 domain point mutations. A model of a
Kv channel1 is depicted based on known structures. Only two
subunits on opposite sides of the Kv channel are shown for
clarity. The T1 domain2, 3 is shown to scale below the TM pore
region, which is depicted based on the structure of the KcsA
channel4. An N-terminal inactivation ball structure^1, based on
the NMR structure of the Shaw type Kv channel Kv3.4 (Raw3)
inactivation ball44 is shown to scale connected to one of the T1
subunits. Regions for which no structural information is
available are given as black linking segments (segment A links
the N-terminal inactivation ball to the T1 domain; B is the T1
to S1 linker; C is the S4 to S5 linker and segment D links the
S6 to the C-terminus). S1 -S6 are the proposed Kv, only S5 and
S6 are modeled here. The four-fold symmetry axis at the center
of the hypothetical Kv channel is vertical and indicated by
arrow 1. The backbone conformation of the T1 subunit chain is
shown in color gradually changing from blue (N-terminus) to
white (C-terminus). The model depicts a 'right side up'
relationship between the T1 domain and the transmembrane
domains. An 'upside down' relationship would have the darker
N-terminal regions of the T1 domain near the TM pore region. The
two side chains where mutations have been introduced are
highlighted: Val 135, blue; Asn 136, green. Potential pathways
for ions to reach the TM pore are between the T1 domain and the
TM pore (arrow 2) or up the aqueous central cavity at the axis
of symmetry (arrow 1). The narrowest part of the T1 cavity along
the four fold axis is formed by Asn 136 (green). This figure was
prepared using Setor45.
|
 |
Figure 3.
Figure 3. Analysis of T1 domain tetramer stability. a,
Fractional elution of Aplysia Kv1.1 wild type untagged
N-terminal cytoplasmic domains from immobilized tetramers,
formed by coassembly with otherwise identical His[6]-tagged
protein. Tetramers were immobilized by binding of the His[6]
squence to metal affinity resin. Elutions were performed under
constant flow using standard buffer conditions at 4 °C (blue
circle) and at 22 °C (red square). Curves are exponential decay
fits to the data, with one exponential term for 4 °C and two
exponential terms for 22 °C. The time constant is 5 h n 3
s.e.m.
for all data points. b, Dissociation of monomers in 3 M urea.
Data were best fit with three exponentials with time constants
ranging from 2 min to 4 h at 22 °C (red square) and 9 min to 7 h
at 4 °C (blue circle). n 3
s.e.m
for all data points. c, Stability of mutant T1 tetramers as
determined by urea denaturation. The unfolding free energy of
wild type, V135R, N136A and N136D mutants are estimated to be
11.1, 10.2, 9.8 and 7.4 kcal mol-1, respectively. d, Correlation
of the energetic effects of T1 mutations on channel gating
properties with the change in unfolding free energy of the T1
domain. The functional  G
for the change in activation midpoint is proportional to the
shift in V[1/2] by the factor z[G]F, where z[G] is the gating
charge that is moved across the lipid bilayer during channel
activation gating and F is Faraday constant. The functional  G
is proportional to ln ( [mutant]/
[wildtype])
by the factor -RT, for the changes in gate closing time measured
at -50 mV. Slopes and intercepts of the regression lines are:
2.2 mV kcal-1 mol-1 and -24.56 mV for the change in half
activation; and -0.18 kcal-1 mol-1 and 2.05 mV for the change in
ln ( [mutant]/
[wildtype])
measured at -50 mV.
|
 |
|
 |
 |
|
The above figures are
reprinted
by permission from Macmillan Publishers Ltd:
Nat Struct Biol
(2000,
7,
403-407)
copyright 2000.
|
 |
|
|
|
|
 |