Erumbi S Rangarajan1, Tina Izard. 1. Department of Cancer Biology, Scripps Research Institute, Jupiter, Florida, USA.
Abstract
The F-actin-binding cytoskeletal protein α-catenin interacts with β-catenin-cadherin complexes and stabilizes cell-cell junctions. The β-catenin-α-catenin complex cannot bind F-actin, whereas interactions of α-catenin with the cytoskeletal protein vinculin appear to be necessary to stabilize adherens junctions. Here we report the crystal structure of nearly full-length human α-catenin at 3.7-Å resolution. α-catenin forms an asymmetric dimer where the four-helix bundle domains of each subunit engage in distinct intermolecular interactions. This results in a left handshake-like dimer, wherein the two subunits have remarkably different conformations. The crystal structure explains why dimeric α-catenin has a higher affinity for F-actin than does monomeric α-catenin, why the β-catenin-α-catenin complex does not bind F-actin, how activated vinculin links the cadherin-catenin complex to the cytoskeleton and why α-catenin but not inactive vinculin can bind F-actin.
The F-actin-binding cytoskeletal protein α-catenin interacts with β-catenin-cadherin complexes and stabilizes cell-cell junctions. The β-catenin-α-catenin complex cannot bind F-actin, whereas interactions of α-catenin with the cytoskeletal protein vinculin appear to be necessary to stabilize adherens junctions. Here we report the crystal structure of nearly full-length human α-catenin at 3.7-Å resolution. α-catenin forms an asymmetric dimer where the four-helix bundle domains of each subunit engage in distinct intermolecular interactions. This results in a left handshake-like dimer, wherein the two subunits have remarkably different conformations. The crystal structure explains why dimeric α-catenin has a higher affinity for F-actin than does monomeric α-catenin, why the β-catenin-α-catenin complex does not bind F-actin, how activated vinculin links the cadherin-catenin complex to the cytoskeleton and why α-catenin but not inactive vinculin can bind F-actin.
The formation and stabilization of cell-cell (adherens) junctions is essential
for the development, architecture, maintenance, and function of tissues in higher
organisms. Adherens junctions are directed by the cadherin receptor family of single
transmembrane-pass glycoproteins, which interact in a homotypic fashion through the
agency of their calcium-binding ectodomains[1-4]. Clustering of these
receptors stabilizes adherens junctions and remodels the actin cytoskeleton, and this
response requires the interaction of the intracellular tail domains of cadherin
receptors to the adaptor protein β-catenin. In turn, β-catenin binds to
the F-actin binding cytoskeletal protein α-catenin to form a ternary
cadherin-β-catenin-α-catenin complex[5-7]. Accordingly,
α-catenin is necessary for mechanical connections between the
E-cadherin–β-catenin complex and the cortical actomyosin
network[8,9], and loss of α-catenin disrupts adherens
junctions and disables connections of the cadherin-β-catenin complex to the
actin cytoskeleton[10-14].α-Catenin is a homodimer that binds to F-actin, suggesting that the
ternary cadherin–β-catenin–α-catenin complex forms
direct links to the actin network. However, monomeric but not dimeric α-catenin
binds to the E-cadherin–β-catenin complex, binding of β-catenin
peptide disrupts the N-terminal α-catenin homodimer, and
reconstituted cadherin–β-catenin–α-catenin complexes do
not bind to F-actin[15-17]. Thus, α-catenin stabilizes adherens
junctions by other means and its additional binding partners have been implicated in
this response, in particular the cytoskeletal proteins vinculin[18-20] and
eplin[21] that also bind to
F-actin. For example, vinculin is necessary to stabilize adherens junctions and
force-dependent unfurling of α-catenin has been suggested to recruit vinculin to
adherens junctions to stabilize these complexes[19]. Furthermore, β-catenin competes with α-catenin
for binding to vinculin suggesting that β-catenin also recruits vinculin to
adherens junctions[18,22].α-Catenin is a 906 residue polypeptide that has been reported to harbor
four functional domains: an N-terminal homodimerization and
β-catenin binding domain[23], an
α-actinin and vinculin binding domain (VBD)[22,24], an M-fragment that
can form cross-linked dimers and that can bind to l-afadin[25], and a C-terminal F-actin
binding domain[7,26] that can also bind to the tight junction protein
ZO-1[27,28]. The crystal structure of the
N-terminal domain suggested that α-catenin was a symmetrical
dimer, where dimerization occurs via two-fold related interactions of two
α-helices from each subunit, and the structure of a chimera of this domain with
β-catenin binding peptide established that β-catenin binding disrupts
this dimer[29]. The crystal structure of
the isolated M-fragment in the central portion of the protein revealed that this is
comprised of two tandem four-helix bundles[30,31].To resolve its structure, regulation, and function, here we determined the
structure of nearly full-length human α-catenin (lacking its
N-terminal residues 1–81) at 3.7 Å resolution. The
structure revealed that α-catenin is an asymmetric dimer and suggests that
asymmetry drives its functions in controlling binding to F-actin, and in its
interactions with activated vinculin. Further, our studies revealed that the activated
vinculin–α-catenin complex was a 2:2 heterotetramer, thus explaining how
vinculin stabilizes adherens junctions.
Results
Overall fold of human α-catenin
We solved the human α-catenin crystal structure to 3.7 Å
resolution (Table 1) by establishing a
particular crystal dehydration protocol described in the Supplementary Methods and by
identifying a heavy metal cluster that was compatible with the crystallization
conditions. The crystal structure revealed that α-catenin is an
all-helical asymmetric dimer that is comprised of four domains of helix bundles
(Fig. 1a). The
N-terminal domain (residues 82–262) of each subunit has
two helix bundle domains that resembled the conformation seen in the crystal
structure of this domain alone[29], consisting of two antiparallel α-helices where the
second α-helix was shared by the following four-helix bundle. The VBD
(residues 277–393)[19,20,28,32,33] was a four-helix bundle that harbored
the two α-helical vinculin binding sites (VBS) of α-catenin,
where the residues that direct the interaction with vinculin were buried within
this four-helix bundle. The M-fragment (residues 390–631) was comprised
of tandem four-helix bundle domains as noted previously[30,31], yet they adopted a much more compact and vinculin-like
conformation in α-catenin, where the two four-helix bundle domains were
rotated by 95°–135° relative to the more open V-shape
conformation (that had helix bundle-helix bundle angles of about
70°–90° versus about 45° in the
full-length structure) seen in the isolated M-fragment structures (Supplementary Fig. 1).
Finally, the F-actin binding domain of α-catenin was a five-helix bundle
that resembled the vinculin tail domain that also bound to F-actin (Fig. 1b)[34,35]. However, the
termini of these C-terminal tail domains of α-catenin
and vinculin were quite distinct. First, the N-terminus of the
vinculin tail domain folded back towards the end of α-helix H1, while
the N-terminus of the F-actin binding domain of
α-catenin interacted with and displaced the H2-H3 loop. Second, the
C-terminus of the α-catenin F-actin binding domain
adopted two distinct conformations in subunits A and B that were oriented in
opposite directions, and only the conformation of subunit A was similar to that
of vinculin (Fig. 1b). These differences
could contribute, in part, to the distinct F-actin binding properties of the two
proteins, where α-catenin can bind to F-actin whereas vinculin binding
requires activation by severing of the head-tail clamp that keeps it in its
inactive state[36-38].
Table 1
X-ray Data Reduction and Crystallographic Refinement Statistics
Native data were collected at a wavelength of 1 Å at APS/ANL beamline
22BM and derivative data at a wavelength of 1.07 Å at SSRL beamline
11-1. The anomalous completeness for the derivative was 0.98 overall and 1 in
the highest resolution shell with a multiplicity of 2.6 and 2.5, respectively.
The final model, comprising 1,519 residues, has a correlation coefficient of
0.93. Some loop regions (residues 265-270, 292-297, 354-361, 600-607, 706-710,
and 799-810 in subunit A and residues 262-273, 354-362, 600-607, and 846-852 in
subunit B) have moderate to very weak electron densities, compared to other
regions of the model. The following regions (residues 636-665 and 859-906 in
subunit A and residues 638-664 and 874-906 in subunit B) were not modeled due to
missing electron density.
Native
2Na2O·P2O5·12WO3
X-ray Data Collection
Space group
P32
P32
Unit cell dimensions
a = b,
c
145.6, 145.6 Å, 139 Å
144.7 Å, 139.9 Å
α = β,
γ
90°, 120°
90°, 120°
Resolution [Å]
(last shell)
139.08–3.66
(3.86–3.66)
46.68–5.58 (5.6–5.58)
R-merge (last shell)
0.077 (0.491)
0.066 (0.537)
Average/σ(I) (last
shell)
15.1 (3.6)
24.7 (2.9)
Completeness (last shell)
0.99 (1)
0.99 (1)
Redundancy (last shell)
5.8 (5.8)
5.2 (5)
Crystallographic
Refinement
Resolution, overall
23.21 Å – 3.66
Å
No. reflections, working set (test
set)
34,383 (1,823)
R-factor
(R-free)
0.217 (0.241)
No. of protein atoms
11,704
No. of sulfate atoms
10
Average B-factor, protein (sulfate)
126.5 Å2 (172.1
Å2)
R.m.s.d. from ideal
geometry
Bond lengths
0.008 Å
Bond angles
0.99°
Figure 1
α-Catenin structure. (a) α-Catenin harbors four
distinct domains: the N-terminal dimerization domain (DD), the
vinculin binding domain (VBD), the M-fragment (M), and the F-actin binding
domain (FABD). F-actin binding domain α-helices are labeled H1 through
H5 as are the termini. Subunit B is shown. (b) Superposition of the
F-actin binding domain of the two subunits in the asymmetric unit onto the
vinculin tail domain. α-Catenin terminal residues are labeled and
‘N’ and ‘C’ indicate vinculin termini,
respectively.
The α-catenin asymmetric dimer
The α-catenin dimer was about 130 Å in its longest
dimension and its architecture resembled that of an asymmetric left handshake
(Fig. 2, Supplementary Fig. 2), where the
thumbs were the helix bundles of the N-terminus, the palms are
the M-fragment, and the fingers were the F-actin binding domain and the VBD.
Superposition of both molecules within the dimer underscored the asymmetry and
distinct orientations of the two subunits (subunit A and subunit B), where there
was a large r.m.s.d. of about 4.8 Å, and of even 3.2
Å without the F-actin binding domain (residues 82–631). In
contrast, the individual domains of the two subunits superimposed relatively
well (0.8 Å for the VBD and M-fragment [residues
277–631]; 0.6 Å for the M-fragment [residues
390–631]; and 0.5 Å for the N-terminal
domain [residues 82–262]), indicating that there is
intrinsically high flexibility within the polypeptide chain. This dynamic nature
may account for the ability of α-catenin to switch between its two
oligomeric states.
Figure 2
α-Catenin is a dimer that resembles a left handshake. (a)
Views onto the distinct F-actin binding domain of subunits A (top panel) and B
(bottom panel) are shown. Subunit A is shown in cyan, subunit B in grey, the
five α-helices of the respective F-actin binding domains are colored
spectrally (H1, red; H2, orange; H3 yellow; H4, green; H5, blue). The F-actin
binding domain α-helices H0 and the respective termini as well as the
respective α-helices of the VBD (α1 through α4) are
indicated. (b) View onto the markedly different intermolecular
interactions of the VBD shown in blue and yellow for subunits A (cyan) and B
(grey), respectively. The dimer ‘stands’ on the
N-terminal dimerization domains in this view.
Interestingly, the structure of the N-terminal
dimerization domain as found in the nearly full-length α-catenin dimer
more closely resembled its conformation in the
β-catenin-α-catenin chimera (PDB 1dow)[29]
versus the isolated domain (PDB 1dov) in its unbound state
(r.m.s.d. of 1.6 Å versus 2.1
Å). This was particularly the case for the subunit B conformation of
α-catenin, which superimposed onto this chimera with
r.m.s.d. of about 1.5 Å compared to superposition
onto the unbound N-terminal dimerization domain (2.2
Å). In contrast, subunit A superimposed similarly onto either structure.
Collectively, this architecture resulted in a more open conformation for the B
subunit of α-catenin.Except for the second four-helix bundle of the M-fragment (residues
508–630), which stuck out in the α-catenin dimer, all helix
bundles engaged in extensive interdomain interactions and contributed to the
overall marked asymmetry of the molecule. For example, the first two
α-helices of the VBD of subunit B bound to the second and third
α-helices of the VBD in subunit A (Fig.
2b). Further, unlike the structure of the M-fragment alone where the
two four-helix bundles were purported to interact[30,31], neither of these bundles interacted in the asymmetric
α-catenin dimer.Notably, the orientation of the F-actin binding domain markedly differed
in the two subunits of the α-catenin dimer. Specifically, while the
orientation of the F-actin binding domain in the A subunit generally resembled
that seen in vinculin, the F-actin binding domain in subunit B was rotated about
166° compared to its orientation in subunit A (Supplementary Fig. 3).
Specifically, in subunit A the F-actin binding domain α-helices H4 and
H5 interacted with the VBD, α-helix H3 interacted with the M-fragment,
and its N-terminus interacted with the
N-terminal four-helix bundle of the N-terminal
dimerization domain of subunit B (residues 146–262). Further, the
C-terminus of the F-actin binding domain of subunit A
interacted with the second four-helix bundle of the M-fragment of subunit B
(Fig. 2a). In contrast, in the more
open subunit B, the N-terminus of the F-actin binding domain
interacted with the second four-helix bundle of the M-fragment of subunit A,
α-helix H4 was in contact with the VBD, and the
C-terminus bound the second four-helix bundle of the
dimerization domain (Fig. 2b). Finally,
asymmetry did not seem to be driven by crystallization and crystal contacts, as
the F-actin binding domains in particular of subunit B did not engage in any
crystal contacts and those present in subunit A seemed too minor to affect its
conformation.The closely related vinculin protein harbored five domains that were
also comprised of four- or five-helix bundles (Vh1, Vh2, Vh3, Vt2 and the
F-actin binding domain)[39,40]. A comparison of the
full-length structures of α-catenin and vinculin indicated that their
helix bundle domains are conserved with the exception that α-catenin
lacked an equivalent Vh2 domain (Supplementary Fig. 3). Furthermore,
in the α-catenin structure, the F-actin binding domain was oriented much
differently, in particular for the flipped conformation in subunit B. These
features likely explain the distinct F-actin binding properties of the two
proteins, where α-catenin but not inactive vinculin can bind to
F-actin.
β-Catenin binding disrupts dimerization and F-actin binding
α-Catenin interacts with the E-cadherin-β-catenin
complex at adherens junctions via binding to the N-terminal
α-helix of β-catenin. Superposition of the α-catenin
structure onto the β-catenin-α-catenin chimera[29] and onto the full-length
β-catenin structure[41]
revealed the consequences of the β-catenin interaction on
α-catenin structure and function (Fig.
3). As shown experimentally, β-catenin and α-catenin
bound as a 1:1 complex, where β-catenin binding displaced the two
N-terminal α-catenin α-helices, thus
disrupting the α-catenin dimer, which had a much higher affinity for
F-actin[15]. The exact
F-actin binding site of α-catenin has, however, not been defined other
than that residues 864–906 were necessary for the interaction[42]. Importantly, the
β-catenin-α-catenin model clearly showed that β-catenin
sterically hinders F-actin binding by the α-catenin dimer. Specifically,
the C-terminus of α-catenin that is essential for
F-actin binding was too close to β-catenin in subunit A (about 25
Å, Fig. 3a) to accommodate F-actin
and indeed was in direct contact, via at least one electrostatic interaction,
with β-catenin in subunit B (Fig.
3b). Indeed, a portion of the 864–906 F-actin binding site of
α-catenin (residues 865–869) was positioned to facilitate
interactions with β-catenin in subunit B (Fig. 3b). Thus, our structure explains how α-catenin can
bind to either F-actin or β-catenin but not to both at the same
time.
Figure 3
Model of the α-catenin–β-catenin heterodimer based on the
crystal structures of β-catenin (PDB 2z6g shown as a cartoon and
surface, both in green), the α-catenin-β-catenin chimera (PDB
1dow shown as a cartoon in pink), and α-catenin subunits A or B shown as
a cartoon in (a) cyan or (b) grey, respectively, and
as a grey surface. The α-catenin F-actin binding domain
α-helices are colored spectrally. A red sphere is shown for the last
α-catenin residue (858 in A and 873 in B) indicating the region involved
in F-actin binding (residues 859–906). Only α-catenin residues
57–82 of the α-catenin–β-catenin chimera
structure are shown (pink).
F-actin binding
The F-actin binding site in the closely related vinculin tail domain of
vinculin was masked in its closed-clamp inactive conformer but was released and
was fully accessible to F-actin following severing of the vinculin head-tail
interactions[43].
Superposition of the F-actin binding domain of vinculin onto our
α-catenin structure revealed that different surfaces were buried and
exposed in these two cytoskeletal proteins (Fig.
4). For example, the N-terminus of α-helices
H4 and the C-terminus of α-helix H5 were buried in
inactive vinculin via interactions with its Vt2 domain, whereas these regions
were largely solvent exposed in the F-actin binding domain of subunit A of
α-catenin. Further, the N-terminus of α-helices
H3 and the C-terminus of α-helix H4 were buried in
inactive vinculin by interactions with its head domain, yet were solvent exposed
in subunit B of α-catenin (Fig. 4).
Thus, the α-catenin structure also explains how full-length
α-catenin can bind to F-actin while vinculin cannot.
Figure 4
The F-actin binding domain surfaces of vinculin and dimeric α-catenin are
distinct. F-actin binding domain surfaces engaging in interdomain interactions
of each α-catenin molecule (subunit A, blue; subunit B, green) and of
the vinculin tail domain Vt (red) are shown (grey, solvent exposed). The first
panels show the Vt surfaces and cartoon while the second panels the
α-catenin surface and cartoon of subunits A or B (in a and
b), respectively. (a) The
N-terminal (indicated by ‘+’)
α-helix H4 and C-terminal (indicated by
‘-’) H5 regions are buried in the F-actin binding domain of
vinculin via interactions with its Vt2 domain but they are solvent exposed in
subunit A of the α-catenin dimer. (b) The
N-terminal (+) α-helix H3 and
C-terminal (-) H4 regions are buried in the F-actin binding
domain of vinculin by interactions with its N-terminal
four-helix bundle but are solvent exposed in subunit B of the α-catenin
dimer.
α-Catenin residues 864–906, some of which
(861–906 in subunit A and 876–906 in subunit B) were disordered
in our structure, are essential for F-actin binding[42]. The dimeric α-catenin structure
showed that the C-terminus of subunit B was held in its
position via extensive intermolecular interactions with the
N-terminal dimerization domain of subunit A (Fig. 2a). As a monomer (e.g.,
following β-catenin binding) these interactions were thus lost.
Interestingly, F-actin had also been reported to bind to the
N-terminal 228 residues of α-catenin with similar
affinity[44]. Given that
only dimeric α-catenin bound efficiently to F-actin and that this
head-tail interface was lost in monomeric α-catenin, a surface that
extends across both domains is perhaps the long-sought F-actin binding site.
Thus, asymmetry also explains how dimeric but not monomeric α-catenin
binds F-actin.
The α-catenin–vinculin interactions
Vinculin was also necessary for stabilizing adherens junctions[19] and force-activated
α-catenin had been suggested to bind and recruit vinculin to adherens
junctions[18-20]. However, our studies have established
that only pre-activated vinculin was capable of binding to α-catenin, as
the Vh1 domain that binds to both α-catenin and to the vinculin tail
domain to hold vinculin in its closed clamp conformation had a higher affinity
for the vinculin tail domain than for the VBD of α-catenin[20]. The structure of the VBD
four-helix bundle within nearly full-length α-catenin presented herein,
and that of VBD in complex with the vinculin Vh1 domain[20], confirmed that, as proposed[19,20], the VBD unfurled when bound to activated vinculin. On
a sizing column, the vinculin head (residues 1–840) in complex with
α-catenin eluted well before dimeric α-catenin, indicating that
the α-catenin–vinculin formed a 2:2 complex (Fig. 5a). Interestingly, as shown by native gel shift
assays and immunoblotting, the asymmetric nature of the α-catenin dimer
was also manifest in its interaction with vinculin, where the α-catenin
dimer first bound to one vinculin molecule before then forming the 2:2 complex
(Fig. 5b). Thus, activated vinculin
unfurls dimeric α-catenin and this 2:2 heterotetrameric complex is fully
competent to bind to F-actin[20].
Figure 5
Asymmetry also directs interactions of α-catenin with vinculin.
(a) Size exclusion chromatography showing the UV absorbance
profile as measured at 280 nm (without units, not indicated)
versus the elution volume of the vinculin head (VH) domain
(residues 1–840) alone (black trace), α-catenin (residues
82–906) alone (blue trace), and the α-catenin–VH complex
(red trace). The α-catenin–VH complex elutes well before dimeric
α-catenin (184,164 Da) indicating that α-catenin remains as a
dimer following complex formation with VH. Complex formation was saturated with
excess VH (92,251 Da) eluting separately. (b) Native gel analyses
(top panel) of ∼10 μM His-tagged α-catenin
(α-cat) alone (lane 1) and with increasing amounts of VH (2.5
μM, 5 μM, 10 μM, 20 μM, 30 μM, and 50
μM for lanes 2–7, respectively), and ∼10 μM VH
alone (lane 8). Note that a 2:1 α-catenin–VH complex initially
appears and with increasing amounts of VH the formation of the 2:2
α-catenin–VH complex saturates. Lower panel,
anti-His Western blotting shows that α-catenin is present in all
complexes.
Discussion
α-Catenin binds to F-actin and bundles actin filaments[44] and also binds to several F-actin
binding proteins[24,27,30,45-47]. However, binding studies with purified recombinant
proteins, as well as measurements of protein dynamics in cells, have clearly
established that α-catenin cannot simultaneously bind to β-catenin
and F-actin and that the oligomeric state of α-catenin dictates which
partner it binds to[15]. These
findings were difficult to reconcile with earlier work[28,48-50] but a plausible explanation was
provided by the fact that E-cadherin-α-catenin fusions were used in earlier
studies[16]. Our structural
data now provide mechanistic evidence that explains why α-catenin binding to
F-actin and β-catenin is indeed mutually exclusive. Specifically, the
structure shows that binding of β-catenin disrupts the intermolecular
interactions of the four-helix bundle of the N-terminus of one
subunit of α-catenin with a region of the C-terminus of the
other subunit that holds the asymmetric dimer together and that are necessary for
binding to F-actin.The mechanism by which α-catenin binds to F-actin has been a
conundrum for the field, as extensive mutagenesis of the C-terminal
F-actin binding domain has failed to define the F-actin binding motif[42]. While in cells there are likely
contributions from other partners such as vinculin that also bind to F-actin, the
fact remains that recombinant dimeric α-catenin alone binds avidly to
F-actin. Notably, asymmetry also explains the F-actin binding functions of the
α-catenin dimer and why monomeric α-catenin binds to F-actin rather
poorly[15]. Specifically,
our structure reveals that the F-actin binding surface is likely created by
intermolecular interactions of the tail of α-catenin with a four-helix
bundle of its N-terminus, which is lost in monomeric or
β-catenin-bound α-catenin. This finding also reconciles reports of
F-actin binding by both the N-terminus and
C-terminus of α-catenin[44]. Only the structure of the α-catenin dimer in
complex with F-actin will allow one to fully define the mechanism of F-actin
binding.Recombinant full-length vinculin cannot link pre-existing cadherin-catenin
complexes and actin filaments as determined by actin pelleting assays in the
presence of all four proteins[15].
However, this is the expected outcome since vinculin is in its closed conformation,
which cannot bind to either F-actin or to α-catenin. However, at adherens
junctions, vinculin is in its activated, open conformation[51], a scenario that would allow it to bind to
α-catenin at adherens junctions, and to facilitate interactions of
α-catenin with the actin network. The fact that the vinculin tail domain
readily displaced α-catenin from pre-existing complexes comprised of
α-catenin and the vinculin head domain (i.e., vinculin
lacking its F-actin binding domain)[13,20,24] establishes that vinculin must be
pre-activated at adherens junctions to interact with dimeric α-catenin and
to stabilize adherens junctions (Supplementary Fig. 4). Finally, activated vinculin also appears to
directly bind to cadherin receptors in cells[22], and since the α-catenin dimer is competent to bind
to activated vinculin, vinculin may serve as a scaffold that tethers both
α-catenin and cadherin receptors, as well as F-actin.
Online Methods
Crystallization
Human α-catenin (residues 82–906) was expressed in
E. coli and purified as described[20] and dialyzed into 20 mM Tris-HCl (pH 8),
150 mM NaCl, and 5 mM DTT, and concentrated to 25 mg/ml. Initial trigonal
crystals were obtained from either 0.9 M
(NH4)2SO4, 0.25 M NaCl, and 0.1 M Tris-HCl
(pH 7) or 0.9 M Na/K phosphate (pH 6.8) and 0.3 M sodium formate that diffracted
X-rays at various synchrotron beam lines (11-1 at Stanford Synchrotron Radiation
Laboratory, SSRL, or 22ID and 22BM at the Advanced Photon Source at Argonne
National Laboratory, APS/ANL) to about 6 Å Bragg spacings. Conventional
strategies failed to improve the diffraction but ultimately systematic
dehydration of human α-catenin crystals grown from 0.9 M Na/K phosphate
and 0.2 M sodium formate in 2 to 3.5 M Na/K phosphate (pH 6.8) in the presence
of glycerol or polyethylene glycol 3350 resulted in diffraction beyond 4
Å. Dehydration was only successful for crystals that were harvested
within one week that were 0.15 to 0.3 mm in size, as dehydration did not improve
diffraction of larger or smaller crystals. Best diffraction, up to 3.2 Å
Bragg spacings, was obtained from crystals that were dehydrated with 3 M Na/K
phosphate and 5% polyethylene glycol 3350 for one week. However,
significant anisotropy and sensitivity to X-rays limited data collection beyond
3.7 Å Bragg spacings.
X-ray data collection and processing
Native and phosphotungstate derivate X-ray diffraction data were
collected on beamlines 22BM at APS/ANL and 11-1 at SSRL, respectively, and
integrated and scaled using autoProc[52], which uses XDS[53] and SCALA[54] as the data reduction engine. Data reduction statistics are
provided in Table 1.
Structure determination and crystallographic refinement
Molecular replacement was unsuccessful using crystal structures of the
dimerization domain (residues 82–262; PDB 1dov) or the M-fragment
(residues 377–631; PDB 1h6g), or homology models for the VBD or F-actin
binding domain as search models. Selenomethionine labeled α-catenin
crystals did not grow beyond 0.05 mm and their diffraction was limited to 8
Å Bragg spacings. Derivatization was also limited due to the high
concentration of phosphate in the crystallization reservoir, which caused
standard heavy atoms, such as Pt, Hg, and Au, to precipitate. This precipitation
was overcome to some degree by short (10 min) soaking times with high
concentrations (10 mM) of heavy metals such as K2PtCl4.
However, this significantly affected the diffraction and anomalous signal
detection. Sodium phosphotungstate was eventually identified as a suitable heavy
atom due to its solubility in phosphate conditions.Crystals were incubated for 24 hr in a low phosphate condition (0.2 M
NaK/phosphate, 2.5 M sodium formate, and 0.7 M sodium malonate, pH 7) to avoid
competition of phosphate from the reservoir. Effective heavy atom incorporation
was accomplished via short soaking times (15 min) in a 10 mM phosphotungstate
solution containing 0.2 M Na/K phosphate, 2.5 M sodium formate, and 0.7 M sodium
malonate (pH 7), then back soaked for 10 min in 0.2 M Na/K phosphate, 2.5 M
sodium formate, and 0.7 M sodium malonate (pH 7), and mounted without including
any additional cryoprotectant. X-ray diffraction data were obtained at SSRL beam
line 11-1 near the L-II absorption edge of tungsten (1.07 Å) to 5.6
Å Bragg spacings.Determination of the heavy atom substructure was performed using the
program autoSHARP[55]. Two
tungsten cluster sites with peak heights of 1 and 0.44 and a correlation of
0.207 were located from which phases (with a figure of merit of 0.15) were
obtained to 5.6 Å (Supplementary Table 1). The resulting electron density map provided
clear definition of the various α-catenin domains but did not allow
chain tracing. SIRAS using autoSHARP allowed phase extension to 4.3 Å
resolution and manual building of α-helices and placement of the high
resolution dimerization domain and M-fragment structures into the experimental
4.3 Å SIRAS electron density map. The resulting model was used as a
search model for molecular replacement with the program MOLREP[56] to position the dimer and
further refine to 3.7 Å using the native X-ray diffraction data.
Iterative cycles of model building were performed using Coot[57] and maximum likelihood crystallographic
refinement using autoBUSTER[58]
by imposing target restraints using the high resolution structures. The model
was improved by local non-crystallographic symmetry through LSSR[59]. Model bias was minimized by
model building into composite omit maps. Map sharpening was performed in
Coot[57] to ensure the
directionality and identity of the α-helices. The quality of the final
model assessment using MolProbity[60] resulted in no outliers and over 95% of the amino
acid residues in the favored region of the Ramachandran plot. Refinement
statistics are provided in Table 1.
Size exclusion chromatography
α-Catenin (residues 82–906), VH (residues
1–840), and α-catenin plus a 2.5 molar excess of VH were loaded
onto a superdex 200 10/300GL (GE Healthcare) analytical chromatography column
equilibrated in 20 mM Tris-HCl (pH 8), 150 m M NaCl, and 5 mM DTT. Fractions
were analyzed on a 10–15% gradient PHAST gel with native buffer
strips.
Native gel shift assays and immunoblotting
Samples (in 20 mM Tris-HCl, pH 8, 150 mM NaCl, 5 mM DDT) were incubated
for 1 hr at 4 °C. Increasing concentrations of VH (0 μM, 2.5
μM, 5 μM, 10 μM, 20 μM, 30 μM, and 50
μM) were titrated to purified His-tagged α-catenin (∼10
μM) and the resultant complex was analyzed using a
10–15% gradient PHAST gel with native buffer strips. The bands
were visualized by coomassie blue staining. α-Catenin was detected with
an anti-His antibody.
Authors: Phillip W Miller; Sabine Pokutta; Jennyfer M Mitchell; Jayanth V Chodaparambil; D Nathaniel Clarke; W James Nelson; William I Weis; Scott A Nichols Journal: J Biol Chem Date: 2018-06-07 Impact factor: 5.157
Authors: Bela Farago; Iain D Nicholl; Shen Wang; Xiaolin Cheng; David J E Callaway; Zimei Bu Journal: Proc Natl Acad Sci U S A Date: 2021-03-30 Impact factor: 11.205
Authors: Hyunook Kang; Injin Bang; Kyeong Sik Jin; Boyun Lee; Junho Lee; Xiangqiang Shao; Jonathon A Heier; Adam V Kwiatkowski; W James Nelson; Jeff Hardin; William I Weis; Hee-Jung Choi Journal: J Biol Chem Date: 2017-03-15 Impact factor: 5.157
Authors: Iain D Nicholl; Tsutomu Matsui; Thomas M Weiss; Christopher B Stanley; William T Heller; Anne Martel; Bela Farago; David J E Callaway; Zimei Bu Journal: Biophys J Date: 2018-07-11 Impact factor: 4.033