Summary
Here, using single-molecule FRET, we reveal previously hidden conformations of the ankyrin-repeat domain of AnkyrinR, a giant adaptor molecule that anchors integral membrane proteins to the spectrin-actin cytoskeleton through simultaneous binding of multiple partner proteins. We show that the ankyrin repeats switch between high-FRET and low-FRET states, controlled by an unstructured “safety pin” or “staple” from the adjacent domain of AnkyrinR. Opening of the safety pin leads to unravelling of the ankyrin repeat stack, a process that will dramatically affect the relative orientations of AnkyrinR binding partners and, hence, the anchoring of the spectrin-actin cytoskeleton to the membrane. Ankyrin repeats are one of the most ubiquitous molecular recognition platforms in nature, and it is therefore important to understand how their structures are adapted for function. Our results point to a striking mechanism by which the order-disorder transition and, thereby, the activity of repeat proteins can be regulated.
Highlights
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Single-molecule FRET reveals previously hidden conformations of AnkyrinR
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We show that ankyrin repeats of AnkyrinR switch between high- and low-FRET states
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Switching is controlled by an unstructured “safety pin” from an adjacent subdomain
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The results suggest that the order-disorder transition regulates AnkyrinR activity
Using single-molecule FRET, Tsytlonok et al. reveal previously hidden conformations of AnkyrinR. The ankyrin repeats of AnkyrinR switch between two FRET states, and the switching is controlled by an unstructured “safety pin” from an adjacent subdomain. Therefore, the order-disorder transition regulates AnkyrinR activity.
Introduction
Single-molecule measurements can resolve the complexity that is inherent in protein energy landscapes but obscured in ensemble experiments because of sample averaging. Such studies of small single-domain proteins and miniproteins have yielded fundamental insights into folding mechanisms (Chung and Eaton, 2013; Ferreon et al., 2009; Kuzmenkina et al., 2005; Laurence et al., 2005; Nath et al., 2012; Nettels et al., 2007; Sherman and Haran, 2006). In other respects, however, new information will be limited if single-molecule analysis is applied only to small proteins because such proteins generally populate just two states, the native and denatured states, and, therefore, all that can be observed is the exchange between them. Large, multidomain proteins have been subjected to little single-molecule folding experiments other than force-probe characterization of their mechanics (Bertz et al., 2010; Kotamarthi et al., 2013; Shank et al., 2010; Wang et al., 2012). Tandem-repeat proteins such as ankyrin, tetratricopeptide, and HEAT repeats will be particularly interesting targets for single-molecule analysis because of a fundamental property distinguishing them from globular proteins, namely the copopulation of multiple, partly folded intermediates under equilibrium unfolding conditions and the accessibility of multiple pathways in the unfolding kinetics (Ferreiro et al., 2005; Lowe and Itzhaki, 2007; Tripp and Barrick, 2008; Werbeck and Itzhaki, 2007; Werbeck et al., 2008). This feature arises from the modular nature of repeat-protein structures and the high level of similarity between the modules at both sequence and structural levels. However, it is very difficult to detect such degeneracy experimentally because of limitations of scale; small repeat proteins have been the focus of most studies to date, and yet giant repeat proteins have much greater potential for heterogeneity. We reasoned, therefore, that single-molecule Förster resonance energy transfer (smFRET) between a series of fluorescent donor-acceptor dye pairs along the repeat stack would allow direct visualization of the spectrum of conformations accessible to this special class of proteins.
D34 is a 426-residue 12-ankyrin-repeat fragment from the giant multidomain protein AnkyrinR (Michaely et al., 2002) (Figure 1A), one of a family of molecular adaptors that mediate the attachment of integral membrane proteins to the spectrin-actin cytoskeleton (Bennett and Healy, 2009). The membrane-binding domain of AnkyrinR forms a superhelical spiral comprising 24 ankyrin repeats that can be divided into four subdomains, D1–D4 (of which D34 is subdomains D3 and D4). Experimental and computational studies suggest that ion transporters bind on one side of the 24-ankyrin repeat stack and that clathrin and cell adhesion molecules bind on the other side (Grey et al., 2012; Kim et al., 2011; Michaely and Bennett, 1995; Michaely et al., 2002). The ankyrin-repeat membrane-binding domain is followed by the spectrin-binding domain (SBD), and an extended loop of the latter domain is found to pack against the five most C-terminal ankyrin repeats in the crystal structure of D34 (Figure 1A). It has been proposed that the interaction between the two domains serves to orientate the multiple AnkyrinR binding partners relative to one another and, thereby, position the spectrin-actin cytoskeleton to the membrane surface.
Previous ensemble experiments showed that D34 unfolds via an intermediate state in which the six C-terminal ankyrin repeats are folded and the six N-terminal ankyrin repeats are unfolded (Werbeck and Itzhaki, 2007; Werbeck et al., 2008). The data also hinted tantalizingly at the presence of other partly folded states under mildly denaturing conditions. Here, smFRET analysis reveals a previously hidden complexity in the conformational ensemble of D34. Under native conditions, we find that, although the N-terminal subdomain of D34 is compact and homogeneously folded, the C-terminal subdomain populates two states in roughly equal proportions, one having high FRET and the other low FRET. Upon truncation of the SBD loop, the high-FRET state is no longer detected, and only the low-FRET state is observed, indicating that the loop acts as a molecular “staple” to control the structure of the C-terminal repeats. The results show that both folded and partially unfolded forms of the protein are present even under native conditions, adding another layer of complexity to the already rich spectrum of conformational states that make up the energy landscape of D34 and pointing to an interesting mechanism by which the folding and, thereby, the function of tandem-repeat proteins can be regulated. This mechanism could be also be exploited to regulate the binding properties of designed ankyrin-repeat proteins, which are currently in development as alternatives to therapeutic antibodies (Stumpp and Amstutz, 2007).
Results
Design of D34 Variants along the Repeat Array
D34 comprises residues 402–827 from AnkyrinR, corresponding to the 12 C-terminal ankyrin repeats of the 24-ankyrin-repeat membrane-binding domain and an unstructured loop from the SBD that folds back onto the ankyrin repeats (Figure 1A). It has two solvent-exposed cysteine residues at positions 475 and 530 (the residues numbers used here correspond to those in the full-length protein) in the third and fifth ankyrin repeats, respectively (ANK3-5), whose Cα atoms are separated by 25 Å and which we used for labeling with the FRET dye pair. To monitor the behavior of the C-terminal repeats and of the repeats in the middle of the protein, three further constructs were designed in which one or both of the wild-type cysteine residues were mutated to serine, and serine residues at other positions were mutated to cysteine: ANK5-8 (having cysteines at positions 530 and 655), ANK8-12 (C655 and C780), and ANK9-12 (C665 and C764), with 45, 50, and 25 Å between the Cα atoms of the two cysteine residues, respectively (Figure 1). The stabilities of the double-cysteine variants were determined using urea-induced unfolding measured by tryptophan fluorescence, and they were found to be only slightly less stable than the wild-type (see Supplemental Experimental Procedures, Figure S1C, and Table S1, available online, for further details). Next, the effect of labeling on the stability of the wild-type and the double-cysteine variants was analyzed using urea-induced unfolding and measuring of donor and acceptor fluorescence, and the labeling was found to have only small effects on stability (see Supplemental Experimental Procedures, Figure S1D, and Table S2 for further details).
We tested the integrity of the fluorescence emission of the dyes in the FRET construct by measuring the fluorescence lifetime of the fluorophores (Supplemental Experimental Procedures and Figure S2). The Förster’s distance value for the FRET pair was then calculated to be 56 Å (Invitrogen), if random orientation of the dyes’ dipoles (κ2 = 2/3) is assumed. We then confirmed this assumption by measuring the fluorescence anisotropies for each double-cysteine variant and all labeled single-cysteine variants (Table S3). The values are notably lower than the limiting anisotropy, indicating that the orientation of the FRET-pair dyes can be considered random.
Single-Molecule FRET and TCCD Measurements Reveal Heterogeneity in the C-Terminal Subdomain of D34, with Both Compact and Noncompact States Copopulated under Native Conditions
We applied two-color coincidence detection (TCCD)/FRET to probe the conformations of ANK3-5, ANK5-8, ANK8-12, and ANK9-12. In TCCD experiments, two (blue and red) overlapping laser beams simultaneously excited a dilute (50 pM) solution of the D34 molecules as they diffused through the confocal volume one molecule at a time. Donor and acceptor fluorescence bursts are detected in coincidence when they originate from the same molecule, therefore allowing direct quantification of the number of molecules with both donor and acceptor fluorophores on them. In FRET, the donor fluorophores were excited with only the blue laser to measure the separation between the dye pairs because the measured simultaneous bursts depend on the conformation of an individual species as it passes through the confocal volume.
Data analysis for both TCCD and FRET measurements was carried out using a coincidence criterion described in detail previously (Orte et al., 2008; Ye et al., 2012). The data for each D34 sample were analyzed using a common donor channel threshold value determined automatically by maximizing the association quotient in the TCCD experiment (Clarke et al., 2007), whereas the acceptor channel thresholds were determined independently. This ensured that both the FRET and TCCD measurements of each sample resulted in approximately equal burst rates in the donor channel. The combined use of TCCD and FRET measurements allows the estimation of the proportion of molecules that were in non-FRET conformations. The use of the coincidence technique allows the detection of both compact (high-FRET) and noncompact (low-FRET) species while isolating singly labeled D34 molecules from the data. Different conformations are detectable, and their relative changes in the population as conditions are changed can be evaluated.
smFRET experiments were performed first under native conditions (50 mM Tris-HCl buffer (pH 8), 150 mM NaCl, 1 mM EDTA, and 0.001% Tween20). The FRET efficiency histogram for wild-type D34 (ANK3-5) is shown in Figure 1B (ANK3-5 FRET Efficiency). The high FRET efficiency is consistent with the small distance between the cysteine residues in the crystal structure (25 Å between the two Cα atoms). FRET efficiency histograms are not well described by Gaussian distributions, especially at very high or very low FRET efficiencies (Wallace et al., 2000). FRET data are better represented by a lognomal distribution using the Z parameter defined as Z = ln(IA/ID), where IA and ID are the acceptor and donor fluorescence intensities, respectively, having been corrected to account for background and crosstalk. The Z parameter histograms for FRET and TCCD measurements of ANK3-5 are shown in Figure 1B. The TCCD Z parameter histogram shows a relatively broad distribution of events. In contrast, the FRET Z parameter histogram measured by single-laser (blue) excitation shows one narrow peak with Z values around 1 (corresponding to a FRET efficiency of 0.83), suggesting that there is a homogeneous population for ANK3-5 under native conditions. It should be noted that the lifetime measurements of single-cysteine variants labeled with the donor only show partial quenching of the dye at position C475 when the protein is under native conditions (Supplemental Experimental Procedures and Figure S2). This additional quenching could potentially contribute to heterogeneity and broadening of the single-molecule FRET histograms. However, given that the FRET efficiency under these conditions is high, the energy transfer is the faster of the two processes (energy transfer and quenching), and, therefore, the quenching does not compete.
The FRET efficiency histogram of ANK5-8 shows a broad distribution of events peaking at a low efficiency of ∼0.4 (Figure 1B). This result was not surprising given that the two cysteine residues are separated by a relatively large distance (45 Å between the Cα atoms). As with ANK3-5, the TCCD and FRET data for ANK5-8 are better represented by Z parameter histograms. The FRET and TCCD Z parameter histograms each show one peak at Z values of approximately −1 (a FRET efficiency of 0.4) and 0.5, respectively. The distance between the two cysteine residues in ANK8-12 (50 Å) is slightly larger than that in ANK5-8 (45 Å). The FRET efficiency histogram for ANK8-12 shows a unimodal distribution of events with a peak at FRET efficiency of 0.55 (Figure 1B), which is somewhat higher than that observed for ANK5-8. The higher FRET efficiency despite a larger interdye distance may simply reflect the likely dynamic nature of the protein structure compared with the one that is “frozen” in the crystal structure. Specifically, previous folding studies by our group (Werbeck and Itzhaki, 2007; Werbeck et al., 2008) as well as limited proteolysis experiments (Michaely and Bennett, 1993) and steered molecular dynamics simulations (Sotomayor et al., 2005) have shown that each six-repeat half of D34 is a stable subdomain and that the interaction between the two subdomains (i.e., between ANK6 and ANK7) is disrupted first before global unfolding occurs. The dye pair in the ANK5-8 construct span these two subdomains, and if, as suggested by these previous studies, there is some unzipping of the intersubdomain interface occurring even under native conditions, then we would expect, on average, the dyes to be further apart than what the static distance measured in the crystal structure indicates. In contrast, the dyes in ANK8-12 lie within a single subdomain, and, therefore, their separation may be more accurately reflected by the crystallographic values.
The two cysteine residues of ANK9-12 are in close proximity (25 Å), like those of ANK3-5. However, the histograms obtained for ANK9-12 are very different from those for ANK3-5 (Figure 1B). The FRET efficiency histogram for ANK9-12 can be fitted to a high-FRET subpopulation at a value of 0.9 and a low-FRET subpopulation at 0.55. Moreover, in contrast to the FRET Z histograms obtained for ANK3-5 and ANK5-8, the ANK9-12 FRET Z parameter histogram shows two clear subpopulations at −0.1 (a FRET efficiency of 0.6) and 1.5 (a FRET efficiency of 0.9), in agreement with the FRET efficiency histogram. In summary, the FRET efficiency and Z parameter histograms suggest that the N-terminal subdomain of D34 is homogenous and compactly folded, whereas the C-terminal subdomain is heterogeneous under native conditions, with a subpopulation of approximately 50% that is not compactly folded. Unlike ANK9-12, no high-FRET population is observed or expected for ANK8-12 because the separation of the dyes is much greater. We focused most of our subsequent analysis on the two variants, ANK3-5 and ANK9-12, in which the cysteine residues are sufficiently close for there to be high-FRET species.
The C-Terminal Subdomain Becomes More Compact upon Addition of Sodium Sulfate
Kosmotrope Na2SO4 has been found to stabilize the compact states of proteins (e.g., Pugh et al., 2010). We therefore examined the effect of Na2SO4 on the conformational ensemble of D34 using the ANK3-5 and ANK9-12 proteins. In red, in Figure S3A, we show their FRET Z parameter histograms in the presence of 400 mM Na2SO4. Na2SO4 does not have a significant effect on the histogram of ANK3-5. For ANK9-12, by contrast, there is a significant shift in molecules from the low-FRET subpopulation to the high-FRET subpopulation that is most evident in the TCCD histogram. Now the ratio of low-FRET to high-FRET species is ∼30:70 rather than ∼50:50. These experiments are consistent with the population of a noncompact state for the C-terminal subdomain of D34 under native conditions (discussed further subsequently).
Single-Molecule Equilibrium Denaturation Measurements by TCCD Detects All Events in the Denatured State
Single-molecule urea-induced equilibrium unfolding experiments were performed next (see Figure 2 for low and high urea concentrations and Figure S3 for the complete set of urea concentrations). As discussed earlier, the histograms do not follow simple Gaussian distribution, and, therefore, the Z parameter histogram was applied. For ANK3-5, the FRET Z parameter histogram, which shows a peak at a Z value of ∼1 at 0 M urea, becomes broader at urea concentrations of 1.5, 2, and 2.5 M. These data can be fitted to Gaussian with two peaks at Z values around 1 and −1. Above 3 M urea, only the peak with the Z value of −1 is observed. These results are consistent with unfolding of the protein leading to separation of the dye pairs. The transition between high and low Z values is similar to the unfolding transition measured by dye fluorescence in bulk experiments (Figure S1D; Table S2) and is also in agreement with the lifetime measurements as a function of urea (Figure S2). The results are consistent with a cooperative mode of unfolding for the N-terminal subdomain of D34, as observed previously in ensemble experiments (Werbeck and Itzhaki, 2007).
We noticed that the total number of FRET events decreased with increasing urea concentration (see Figure 2B, 1c). To establish the origins of this behavior, we next performed equilibrium denaturation experiments with TCCD using two-laser (blue and red) excitation of the samples. The advantage of TCCD is that, by exciting both dyes simultaneously and applying the coincidence criteria, molecules with very low FRET efficiencies are not thresholded out of the analysis. Therefore, TCCD permits the assessment of the number of dual-labeled molecules, even those showing very low FRET efficiency (less than 0.2). Using TCCD, we now observe that the total number of molecules is constant and does not change with urea concentration (Figure 2B, 2c). Therefore, the decrease in the number of FRET events compared with the number of TCCD events clearly indicates that the unfolding is increasing the population of a very low FRET state. This was confirmed by measurement of the FRET efficiency of the unfolded protein using time-resolved fluorescence lifetime measurements (Figure S2E), which showed FRET efficiencies below 0.25 at 7 M urea for all of the constructs. The same behavior was also observed for ANK5-8, ANK8-12, and ANK9-12 (Figure 2B). Urea denaturation experiments were also performed in the presence of 400 mM Na2SO4 (red histograms in Figure S3A). With Na2SO4, the urea-dependent decrease in the number of FRET events is shifted to a higher urea concentration (Figure S3B), consistent with the stabilizing effect of Na2SO4 on D34.
Deletion of the C-Terminal Tail Results in Only the Low-FRET State for the C-Terminal Subdomain
We speculated that the conformational heterogeneity observed for the C-terminal subdomain under native conditions is related to the unstructured SBD loop (tail) that is packed against the five most C-terminal ankyrin repeats of D34 in the crystal structure (Figure 1A). To investigate the role of the tail, we made a truncated variant of ANK9-12 in which the tail was deleted at residue S799, ANK9-12Δ. The truncated variant is destabilized relative to the nontruncated variant (Figure S1C), as shown previously (Werbeck and Itzhaki, 2007). We confirmed, by circular dichroism and analytical gel filtration, that the protein is monomeric and retains a substantial helical structure and compactness, and, therefore, we can assume that at least the N-terminal subdomain is not perturbed by the deletion of the C-terminal tail. The protein was labeled successfully, and the FRET Z parameter histogram is shown in Figure 1B. It is strikingly different from that of ANK9-12 because only a low-FRET state is observed for ANK9-12Δ, and there is no high-FRET state detectable. Moreover, upon addition of Na2SO4, the histogram is shifted to higher FRET, as also observed for ANK9-12 (Figure S3). These results are consistent with the hypothesis that the tail exists in two different conformations, one packed against the ankyrin repeats, resulting in a fully folded and compact C-terminal subdomain, and the other unpacked from the ankyrin repeats, resulting in partial unfolding of the ankyrin repeats and to an expanded form. The kosmotrope Na2SO4 shifts the equilibrium between these two conformations to the more compact one.
Discussion
We used single-molecule FRET to systematically probe the energy landscape of D34. To quantify the changes in the populations of the different FRET states at increasing denaturant concentrations, we used both TCCD with two-laser excitation of the samples and smFRET using only single-laser (blue) excitation. Using the TCCD method, we found that the total number of molecules was constant across the range of urea concentrations, whereas this number decreased gradually with increasing urea concentration when smFRET measurement was used. These results underline the importance of using the two techniques in combination to fully understand the biophysical properties of a protein because TCCD permits the assessment of the number of dual-labeled molecules, even those showing very low FRET.
Previous ensemble analysis showed that the unfolding of D34 is a complex and multistep process in which the unfolding of the N-terminal subdomain occurs cooperatively, whereas the C-terminal subdomain unravels in a noncooperative manner (Werbeck and Itzhaki, 2007). Moreover, protein engineering suggest that mutations modulate the energy landscape of D34 so that different unfolding intermediates become dominant. The single-molecule analysis described here adds a further layer of complexity. The results show that the “native state” of D34 is not a homogeneous species. Although the N-terminal subdomain is homogeneous and compactly folded, there is a heterogeneous ensemble of conformations of the C-terminal subdomain. Two roughly equal populations are present under native conditions, one with a high FRET efficiency and one with a low FRET efficiency. Moreover, a variant in which the protein is truncated before the tail showed only the low-FRET species. These results indicate that the low-FRET population arises from the detachment of the unstructured tail from the C-terminal ankyrin repeats and consequent unravelling of the ankyrin stack (Figure 3A).
The properties of D34 revealed here are particularly significant in view of the biological function of Ankyrins (Figure 3B). The three vertebrate Ankyrins, AnkyrinR, AnkyrinB, and AnkyrinG, are critical for normal physiology, and dysfunction is associated with numerous human diseases, including cardiac and neurological disorders (Bennett and Healy, 2009). They are very large proteins comprising an N-terminal membrane-binding domain (MBD), a central SBD, a death domain of poorly defined function, and a highly variable C-terminal regulatory domain. The MBD is composed of 24 ankyrin repeats forming a superhelical spiral that can be divided into four subdomains, D1–D4. D34 corresponds to D3 and D4 from AnkyrinR. The MBD and SBD are not independent of one another. Rather, they interact via an unstructured segment from the latter domain that was found in the crystal structure of D34 to fold back and pack against the D4 subdomain (Michaely et al., 2002), and a similar “linker” has been identified in AnkyrinB and AnkyrinG and has been shown to modulate the membrane-protein recognition of the ankyrin repeats. By binding membrane-spanning proteins via the ankyrin repeats of the MBD and spectrin via the SBD, Ankyrins anchor the membrane surface to the spectrin-actin cytoskeleton. There are no structures of the ankyrin repeats in complex with their binding partners. However, computational and experimental analyses suggest that the exceptionally long groove of the ankyrin superhelix allows a diverse range of membrane proteins, including ion transport, cell adhesion, and membrane trafficking molecules, to bind (Davis et al., 1989; Grey et al., 2012; Kim et al., 2011; Michaely and Bennett, 1995; Michaely et al., 2002). Ankyrins appear to have evolved an extraordinarily complex set of autoregulatory mechanisms that may work in a combinatorial fashion to coordinate the activities of the different domains, modulating subcellular localization and membrane protein-binding specificities and, thereby, greatly diversifying their functions (Figure 3B). First, the C-terminal regulatory domain interacts intramolecularly with the MBD to negatively modulate the latter’s affinity for its binding partners through an as yet unknown allosteric mechanism (Davis et al., 1992; Figure 3B, i). Second, the Ank genes are subject to varied and tissue-specific mRNA splicing events that result in heterogeneous populations of Ankyrin polypeptides (Cunha et al., 2008; Hall and Bennett, 1987; Lux et al., 1990). Notable are splicing that removes the C-terminal regulatory domain, leading to alleviation of its repressive effect on the MBD (Figure 3B, ii), and splicing within the MBD that removes exons encoding individual ankyrin repeats, which will alter the molecular recognition capabilities of this domain (Figure 3B, iii).
Our single-molecule analysis reveals a third, distinct mechanism by which Ankyrin function can be regulated (Figure 3B, iv). We show that the unstructured segment of the SBD acts as a staple or safety pin that induces the folding of the ankyrin repeats of the D4 subdomain. Under native conditions, this safety pin is in the open position for ∼50% of the molecules (and likely at an even higher percentage at body temperature), and the ankyrin repeats are consequently partly unfolded, a process that will dramatically affect the positioning of membrane proteins to the spectrin-based cytoskeleton. The disordered nature of these ankyrin repeats will also modulate the interactions of the MBD with its binding partners. Interestingly, alternative exons have been identified close to this region between the MBD and SBD, which would further modulate the properties of the ankyrin repeats (Cunha et al., 2008; Hall and Bennett, 1987; Lux et al., 1990).
The absence of sequence-distant contacts likely affords repeat proteins extreme flexibility and particular molecular recognition capabilities (Ferreiro et al., 2005; Sivanandan and Naganathan, 2013), consistent with the proposal that they are a distinct class midway between globular structured proteins and intrinsically disordered proteins (Forwood et al., 2010). An example is IκBα, the two C-terminal ankyrin repeats of which possess features of intrinsic disorder (Lamboy et al., 2011, 2013). These repeats are found to fold upon binding to its partner, NFκB (Truhlar et al., 2006). A distinct way to regulate the order-disorder transition of repeat proteins is revealed in our study of AnkyrinR. Here it is the intramolecular association of the C-terminal ankyrin repeats with the adjacent domain that induces folding, thereby providing an additional level of control with which this complex adaptor molecule anchors membrane proteins to the underlying cytoskeleton.
Experimental Procedures
Production of Dye-Labeled D34 Wild-Type and Mutants
Site-directed mutagenesis of D34 and expression and purification of wild-type and mutants were performed as described previously (Werbeck and Itzhaki, 2007). Wild-type D34 has two solvent-exposed cysteine residues at positions C475 and C530 (the residues numbers used here correspond to those in the full-length protein) in the third and fifth ankyrin repeats (referred to as ANK3-5). Labeling with Alexa Fluor 488 and Alexa Fluor 647 was performed as described in the Supplemental Experimental Procedures. The bulk fluorescence behavior of the double-labeled protein upon excitation at 485 nm was analyzed as a function of urea concentration (Supplemental Experimental Procedures). The fluorescence intensity of the donor increased and that of the acceptor decreased with increasing urea concentration (Figures S1B and S1D), as expected for a decrease in FRET between the two fluorophores upon unfolding. Next, mutant variants were created with one or both of the wild-type cysteine residues mutated to serine and cysteine residues introduced at other positions to probe other regions of the structure. These were expressed, purified, and labeled as for the wild-type. They showed similar bulk fluorescence behavior as the wild-type (Figure S1D). Anisotropy and fluorescence lifetime measurements were performed to check that the labeled proteins were suitable for single-molecule FRET measurements (Supplemental Experimental Procedures).
Single-Molecule Fluorescence Measurements: smFRET, TCCD, and PAX
smFRET, dual laser excitation in TCCD, and periodic acceptor excitation (PAX) measurements were performed using a homebuilt laser confocal microscope. The instrumentation, data acquisition, and data analysis have been described in detail previously, including validation of the TCCD/FRET measurements by PAX (Ye et al., 2012), and are summarized in the Supplemental Experimental Procedures. PAX measurements were performed on ANK9-12 to confirm that there was no threshold bias in the TCCD/FRET measurements and similar FRET efficiencies and populations were obtained.
Author Contributions
L.S.I. and D.K. conceived the research. M.T., S.M.I., P.J.E.R., W.X., and M.J.R. performed research and analyzed data. M.T., S.M.I., A.O., D.K., and L.S.I. wrote the paper.
Acknowledgments
L.S.I., M.T., S.M.I., P.J.E.R., and W.X. acknowledge support from the Medical Research Council of the UK (including Grant G1002329), and L.S.I. acknowledges support from the Medical Research Foundation.
Footnotes
This is an open access article under the CC BY license (http://creativecommons.org/licenses/by/3.0/).
Contributor Information
David Klenerman, Email: dk10012@cam.ac.uk.
Laura S. Itzhaki, Email: lsi10@cam.ac.uk.
Supplemental Information
References
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