There is a growing interest in engineering proteins whose function can be controlled with the spatial and temporal precision of light. Here, we present a novel example of a functional light-triggered switch in the Ca-dependent cell-cell adhesion protein E-cadherin, created using a mechanism-based design strategy. We report an 18-fold change in apparent Ca(2+) binding affinity upon illumination. Our results include a detailed examination of functional switching via linked changes in Ca(2+) binding and cadherin dimerization. This design opens avenues toward controllable tools that could be applied to many long-standing questions about cadherin's biological function in cell-cell adhesion and downstream signaling.
There is a growing interest in engineering proteins whose function can be controlled with the spatial and temporal precision of light. Here, we present a novel example of a functional light-triggered switch in the Ca-dependent cell-cell adhesion protein E-cadherin, created using a mechanism-based design strategy. We report an 18-fold change in apparent Ca(2+) binding affinity upon illumination. Our results include a detailed examination of functional switching via linked changes in Ca(2+) binding and cadherin dimerization. This design opens avenues toward controllable tools that could be applied to many long-standing questions about cadherin's biological function in cell-cell adhesion and downstream signaling.
There has been considerable
interest in light-based control of biological systems,[1] and successful applications include light-modulation of
neuronal ion channels,[2] light-switchable
signaling proteins,[5] and light-controlled
protein targeting.[6] Light-based methods
offer titratable, precise spatial and temporal regulation that has
been demonstrated in vitro,[7] in cell culture,[6,8] and in whole animals.[9] Most examples of light-based control fall into
one of two categories: (a) those that are genetically encoded using
a recombinantly produced protein borrowed from nature,[6] and (b) those created via targeted insertion of amino acids
into a protein sequence and subsequent reaction with them of an exogenously
introduced photoisomerizable small molecule, typically azobenzene
based.[10] Azobenzene and related molecules
undergo a reversible cis–trans isomerization
when exposed to specific wavelengths of light, and this change in
molecular shape can be coupled to changes in protein function. While
in (a) the functional design is already provided naturally, one is
limited both by the function (e.g., modulation of protein–protein
binding, tuning fluorescence intensity) already encoded by the natural
gene and by the requirement to fuse the natural protein with the protein
to be modulated. In contrast, the designs in (b) allow many types
of functional modulation, such as changes in agonist binding, protein–protein
binding, and protein folding. In this work, we used a new strategy
where changes in protein–ion affinity couple to protein dimerization,
in the cell–cell adhesion protein cadherin (Figure 1A).
Figure 1
(A) A cartoon showing
the basis of our design. As designed, our
photoswitch reduces Ca2+ binding affinity, which, in turn,
reduces homodimer affinity. (B) BSBCA undergoes a reversible cis/trans
isomerization when illuminated with specific wavelengths of light.
(C) EC12 structure showing the region targeted for photoswitchability.
Labels indicate the design considerations. (D) Photoswitchability
and reversibility measured by absorbance after many cycles of illumination
of X-EC12.
Cadherins are a key family of Ca-dependent
cell–cell adhesion
proteins and are divided into several subtypes, including the most
commonly studied subtype, the classical cadherins. Classical cadherins,
which include E-, N-, P-, R-, and C-cadherin,[11] are composed of an intracellular domain, a transmembrane helix,
and five, repeated, extracellular domains labeled EC1 (N-terminal,
membrane distal) to EC5 (C-terminal, membrane proximal), along with
three Ca2+ binding sites present in the loops at each extracellular
domain boundary.[12,13] Calcium binding is required for
cadherin function, as depletion of Ca2+ disrupts cadherin-mediated
cell adhesion;[14] the presence of Ca2+ is suggested to rigidify the cadherin structure, allowing
it to multimerize.[15] Knockdowns of cadherin
significantly slow cell–cell adhesion,[16] and in a classic experiment, cadherin-free, nonadherent cells transfected
with cadherin acquire morphological similarities to naturally adherent
cells.[18]Our approach to creating
a light-switchable cadherin aimed to modulate
its Ca2+ binding affinity. Because Ca2+ binding
is essential for cadherin multimerization, we reasoned that reversibly
changing Ca2+ binding affinity would be an effective way
to also modulate cadherin adhesive function (Figure 1A). We designed cysteine residues into the protein to serve
as conjugation sites for an azobenzene-based photoisomerizable chromophore,
BSBCA (Figure 1B). BSBCA has been used in previous
applications,[7,20] demonstrating
reversible switching between the cis and trans states when exposed to 370 nm (near UV) and 550 nm
(green) light, respectively.[7] Our strategy
involved conjugating both ends of the chromophore to the Ca-binding
loops between cadherin domains EC1 and EC2, as these Ca2+ sites have previously been shown to be most critical for function.[13] In addition, because the Ca2+ binding
sites are located in loop regions and bind Ca2+ with relatively
weak affinities near 20 μM,[22] we
reasoned it would be easier to induce conformational changes affecting
Ca2+ binding there than in more rigid secondary structural
elements or well-packed core regions of the protein.Because
BSBCA spontaneously cross-links cysteine residues,[23] the design challenge presented here can be generalized
as the problem of finding the best pair of residues to mutate to cysteine.
In practice, however, an enormous number of pairs are possible, the
overwhelming majority of which are likely to be nonfunctional. We
took a sequential and computational approach to identifying likely
functional pairs (Figure S1 and Supporting Information
[SI]). First, we used the program Rosetta[24] to computationally mutate all residues in four representative
E-cadherin structures (PDB identifiers: 1FF5, 1EDH, 2O72, and 1Q1P) to alanine (the simplest mutation) and
then calculated the predicted change in fold stability using a protocol
we developed previously.[25,26] Residues with predicted
destabilization >1 kcal/mol were not considered, as mutations to
these
residues were presumed to be disruptive. Next, we narrowed the pairs
to those that would be geometrically compatible with the small molecule.
We calculated pairwise Cβ–Cβ distances between the residues remaining using the 1FF5 structure and kept
those pairs that fell in the range 17–20 Å (appropriate
for the BSBCA trans isomer). Finally, the remaining
pairs were ranked for an additional set of structural and geometric
constraints (Figure 1C and SI). Eleven
high-ranking pairs (Table S1) were cloned,
expressed, and tested for conjugability (Figure
S2), photoswitchability, and functionality (SI). One pair, K129C/D138C (Figure 1C, red residues) showed the best switchability and functionality,
and was further characterized in detail.(A) A cartoon showing
the basis of our design. As designed, our
photoswitch reduces Ca2+ binding affinity, which, in turn,
reduces homodimer affinity. (B) BSBCA undergoes a reversible cis/trans
isomerization when illuminated with specific wavelengths of light.
(C) EC12 structure showing the region targeted for photoswitchability.
Labels indicate the design considerations. (D) Photoswitchability
and reversibility measured by absorbance after many cycles of illumination
of X-EC12.We focused on, and expressed,
the first two domains of E-cadherin
(EC12), because they contain the homodimeric binding interfaces[27] and are the specificity determining domains,[28] making them most principally responsible for
cadherin’s function. Additionally, the shortened EC12 construct
can be readily produced in high yields in E. coli. EC12 contains a single native cysteine residue, which we mutated
to alanine (C9A), previously shown not to affect cadherin function.[29]Characterization of photoswitchable Ca2+ binding
affinity.
(A) Ca2+ binding as monitored by mass spectrometry. While
WT and trans X-EC12 bound three Ca2+ ions
specifically, cis X-EC12 showed considerably weaker,
predominantly nonspecific binding (Figure S4 and
SI). Fits are based on a model of a single class of binding
site for a maximum of three specifically bound Ca2+ ions.
(B) The half-life of the cis state as a function
of Ca2+ concentration, as measured by absorbance. Error
bars are +1 SD from three independent experiments.We first sought to show that K129C/D138C conjugated
with trans BSBCA (termed X-EC12) could undergo isomerization
to cis. Unconjugated BSBCA in the trans state has an absorbance peak near 370 nm that decreases when illuminated
at this wavelength, resulting in a population that is 80–90% cis; subsequent illumination at 500–550 nm will reverse
the isomerization and produce a population that is >90% trans. Illuminating our conjugated protein (X-EC12) at 365
nm with a hand-held
LED showed the characteristic reduction in absorbance of the trans state. The reverse isomerization (pan-visual illumination,
including 500–550 nm bands) also behaved as expected, leading
to a reappearance of the absorbance band of the trans state. We illuminated X-EC12 for 10 complete UV-green illumination
cycles without any apparent loss of absorbance or switchability (Figure 1D); the switchability was also titratable via shorter
illumination times (Figure S3).We
next tested whether isomerization changes Ca2+ binding
affinity. To do so, we used a previously described mass spectrometry
based assay[22] to directly measure the Ca2+ binding affinity of WT C9A as well as trans and cis X-EC12 (Figures 2A and S4; these assays used a cadherin
concentration of 2 μM, significantly below a previously measured
homodimeric Kd of WT cadherin (98.6 ±
15.5 μM),[27] to avoid potential complications
due to cadherin dimerization). If isomerization alters Ca2+ binding, the cis X-EC12 should have weaker affinity
than trans. In addition, because EC12 binds three
Ca2+ ions, any of which could be interfered with, a decrease
in apparent cooperativity as measured by the Hill coefficient (Nh) would be expected. WT C9A cadherin specifically
bound three Ca2+ ions with a dissociation constant Kd = 28.5 ± 1.9 μM (throughout the
text, errors are the boundaries of a 95% confidence interval unless
otherwise indicated) and extensive cooperativity with Nh = 2.85 ± 0.47, close to previously reported numbers[22] of Kd = 20 ±
0.7 μM and Nh = 2.6 ± 0.2. Trans X-EC12 showed 2-fold weaker affinity and less cooperativity,
with Kd = 55.2 ± 5.8 μM and Nh= 1.80 ± 0.35, but also bound three Ca2+ ions. In contrast, Ca2+ binding to cis X-EC12 was dominated by nonspecific binding. By using quadruple
and higher Ca-bound states from trans X-EC12 (Figure S5) as a reference for nonspecific binding,
we subtracted the estimated contribution of nonspecific Ca2+ binding from the measured average Ca2+ occupancy for cis X-EC12 (SI). The resulting
line shows significantly reduced binding compared to trans. (A quantitative fit was not possible due to required Ca2+ concentrations being higher than the dynamic range of the assay.)
Figure 2
Characterization of photoswitchable Ca2+ binding
affinity.
(A) Ca2+ binding as monitored by mass spectrometry. While
WT and trans X-EC12 bound three Ca2+ ions
specifically, cis X-EC12 showed considerably weaker,
predominantly nonspecific binding (Figure S4 and
SI). Fits are based on a model of a single class of binding
site for a maximum of three specifically bound Ca2+ ions.
(B) The half-life of the cis state as a function
of Ca2+ concentration, as measured by absorbance. Error
bars are +1 SD from three independent experiments.
To more directly measure the Ca2+ binding of cis X-EC12, we turned to a different assay that determined
the cis half-life as a function of Ca2+ concentration. One general caveat inherant to azobenzene-based strategies
is that switching to the cis state is generally incomplete;
i.e., the cis state always contains a minor trans population.[10,23] However, the entirety
of any change observed in half-life experiments is due only to the cis subpopulation, allowing measurement of pure cis properties unaffected by the small fraction that remains trans. Therefore, if chromophore isomerization significantly
affects Ca2+ binding in our conjugated constructs, with
stronger binding of Ca2+ to trans X-EC12,
by thermodynamic coupling we would expect to see a change in the cis X-EC12 half-life with Ca2+ (Figure 2B). The cis state is thermodynamically
unstable, and cis BSBCA relaxes back to the stable trans state in the dark with a half-life of ∼20 min
at 25 °C,[23] although conjugation to
proteins can alter chromophore half-lives.[7,31] By
observing the increase in absorbance at 370 nm during relaxation of
our conjugated constructs back to trans, one can
compute the half-life of the process (Figures S6 and S7; SI; these assays used a protein concentration
of 12 μM to minimize potential changes in half-life due to protein
dimerization). The half-life should decrease with increasing Ca2+ concentration as trans X-EC12 becomes stabilized
by Ca2+ binding. As expected, we observed a half-life decrease
from ∼72 to 28 min, with an EC50 of 996 ± 135
μM Ca2+. This represents a nearly 18-fold change
in apparent Ca2+ binding affinity from the 55 μM
for trans X-EC12 (mass spectrometry analysis, Figure 2A).We also observed a cooperative transition
in half-life duration,
with a measured Nh of 2.4 ± 0.74.
In showing interdependence between isomerization and Ca2+ binding, these results indicate that, as expected, isomerization
of the chromophore significantly weakens Ca2+ binding.
In addition, the observed cooperative nature indicates multiple Ca2+ ions are binding simultaneously during the transition from cis to trans, hinting that the cis state likely weakens multiple binding sites.Characterization
of photoswitch homodimeric binding. (A) Homodimeric
binding monitored in SPR as a function of Ca2+ concentration.
The data were fit to a Hill equation. Faded points contain significant
nonspecific binding and were not used in the fits. Responses between
flow cells were scaled to minimize a least-squares difference, and
then mean values were normalized such that the fit value at [Ca2+] = ∞ was 1.0 (SI). Error
bars are ±1 SD of the three active flow cells in the instrument
after scaling and normalization. Inset shows fits at low Ca2+ concentrations. (B) Homodimeric binding monitored in SPR at 1 mM
Ca2+, after repeated illumination cycles. Responses between
flow cells were scaled to minimize a least-squares difference. Error
bars are ±1 SD of the three active flow cells in the instrument
after scaling.After successfully demonstrating
photoswitchable Ca2+ binding in our engineered cadherin,
we next asked whether the change
in Ca2+ binding affinity also results in the expected change
in protein binding activity. We used surface plasmon resonance (SPR)
to measure protein homodimerization as a function of Ca2+ concentration (Figures 3, S8, and S9; SI). In this assay, similar to that of Harrison
et al.,[27] biotinylated WT C9A cadherin
was immobilized to the SPR chip and WT C9A, trans or cis X-EC12 were flowed over it. Direct measurements
of both Ca2+ affinity and homodimeric protein affinity
in SPR are difficult due to solution homodimers competing with those
on the surface, reducing the effective protein concentration; to minimize
solution homodimerization, we used a protein concentration (40 μM)
below the Kd for homodimerization of WT
EC12 cadherin.[27] Additionally, cis measurements are of mixed populations due to the inability
of reaching full conversion to the cis state and
some thermal relaxation to trans during the experiment,
limiting the observable fold change in affinity (SI). We observed a Ca2+ binding EC50 for WT C9A cadherin, as measured by a single Hill fit, of 72.0 μM
(with mean fit values and ±2 SD error, as measured by a bootstrapping
analysis of the data, of 71.2 ± 14 μM; see SI and Figures S10, S11) and Nh = 2.24 (2.45 ± 1.7). In comparison, trans X-EC12 has an EC50 of 156 μM (170 ± 33 μM),
with Nh = 1.38 (1.28 ± 0.28). These
EC50 values are higher than those measured in the mass
spectrometry assay (Figure 2A), which is due
to cadherin binding multiple Ca2+ ions to function, causing
any measured EC50 to necessarily be, at a minimum, a multiple
of the protein concentration used, which here was 40 μM. Strikingly, cis X-EC12 showed substantially weakened binding (Figure 3A), with EC50 = 619 μM (611 ±
180 μM) and Nh = 0.76 (0.77 ±
0.15), demonstrating a nearly 4-fold change in Ca2+ affinity
under these conditions. (Note: nonspecific protein binding to the
SPR chip appeared at Ca2+ concentrations >2 mM for WT
C9A
and trans X-EC12; see SI.) The change in protein–protein binding was also reversible
as measured over multiple illumination cycles with 40 μM protein
and 1 mM Ca2+ (Figure 3B).
Figure 3
Characterization
of photoswitch homodimeric binding. (A) Homodimeric
binding monitored in SPR as a function of Ca2+ concentration.
The data were fit to a Hill equation. Faded points contain significant
nonspecific binding and were not used in the fits. Responses between
flow cells were scaled to minimize a least-squares difference, and
then mean values were normalized such that the fit value at [Ca2+] = ∞ was 1.0 (SI). Error
bars are ±1 SD of the three active flow cells in the instrument
after scaling and normalization. Inset shows fits at low Ca2+ concentrations. (B) Homodimeric binding monitored in SPR at 1 mM
Ca2+, after repeated illumination cycles. Responses between
flow cells were scaled to minimize a least-squares difference. Error
bars are ±1 SD of the three active flow cells in the instrument
after scaling.
An alternative explanation for the observed decrease in the SPR
signal upon isomerization to the cis state could
be an increase in cis homodimerization in solution,
reducing the effective concentration of X-EC12 cadherin monomers available
to bind to the WT cadherin immobilized on the chip. To exclude that
possibility, we analyzed X-EC12 cadherin homodimerization via gel
filtration. The observed decrease in the dimer/monomer ratio after
UV illumination additionally confirms the expected weaker cis homodimerization upon illumination (Figure S12).Questions remain about the structure of
the functional cadherin
multimers, including evidence that cadherin forms strand-swapped dimers.[27,32,33] While we cannot directly determine
the structure of the interacting species formed in our SPR experiments,
each set of SPR traces for a given cadherin variant can be fit to
a single off rate returning to baseline levels, even at higher Ca2+ concentrations (Figure S13).
This behavior is consistent with a single dimer type formed for each
assayed cadherin variant.Taken together, our results demonstrate
the successful design of
a reversibly photoswitchable cadherin. When illuminated with light,
its Ca2+ binding affinity changes from 56 to 996 μM,
a nearly 18-fold change, and this change in affinity is coupled to
a change in protein–protein binding. One constraint on our
current design is the inability of BSBCA and other currently available
chromophores to switch completely to cis. Several
new chromophores have become available[31,35,37] that possess either more complete isomerization or
longer half-lives that could allow for isolation and use of the pure cis state.When applied in cell culture experiments,
the light-modulatable
cadherin could help answer several outstanding questions about cadherin’s
function. One way to introduce this engineered molecule into a cellular
context is via cadherin-coated substrata. Coated substrata have been
used to study cell–cell adhesion[38] and stem cell pluripotency.[40] Creation of coated surfaces allows spatial control
of cadherin patterning and fine control over cadherin concentration,
which could help maximize the switchability of cadherin-mediated adhesion.[38]Although interest in photoswitchable proteins
has increased in
recent years, relatively few examples exist in the literature, perhaps
because finding good cysteine attachment points remains difficult.
Compared to high-throughput and other library techniques, we were
able to create a successful conjugate using a rational design strategy
and a small library of constructs. In our design, we chose to focus
on modulating loop structures that may have a lower activation energy
barrier to transition compared to more rigid parts of protein domains.
While not all proteins could be modified in this way, we believe our
combined rational/computational selection method and our focus on
loops can be generalized to create other photoswitchable designs.
Authors: Marina Blanco-Lomas; Subhas Samanta; Pedro J Campos; G Andrew Woolley; Diego Sampedro Journal: J Am Chem Soc Date: 2012-04-16 Impact factor: 15.419
Authors: Nicolas Borghi; Molly Lowndes; Venkat Maruthamuthu; Margaret L Gardel; W James Nelson Journal: Proc Natl Acad Sci U S A Date: 2010-06-21 Impact factor: 11.205
Authors: Yi I Wu; Daniel Frey; Oana I Lungu; Angelika Jaehrig; Ilme Schlichting; Brian Kuhlman; Klaus M Hahn Journal: Nature Date: 2009-08-19 Impact factor: 49.962