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Bending-Twisting Motions and Main Interactions in Nucleoplasmin Nuclear Import

  • Marcos Tadeu Geraldo ,

    mtgeraldo@gmail.com

    Affiliation Laboratório de Bioinformática e Biofísica Computacional, Departamento de Física e Biofísica, Instituto de Biociências de Botucatu, UNESP – Universidade Estadual Paulista, Botucatu, SP, 18618-970, Brazil

    ORCID http://orcid.org/0000-0001-8250-2159

  • Agnes Alessandra Sekijima Takeda,

    Affiliations Laboratório de Bioinformática e Biofísica Computacional, Departamento de Física e Biofísica, Instituto de Biociências de Botucatu, UNESP – Universidade Estadual Paulista, Botucatu, SP, 18618-970, Brazil, Instituto de Biotecnologia (IBTEC), UNESP – Universidade Estadual Paulista, Botucatu, SP, 18607-440, Brazil

  • Antônio Sérgio Kimus Braz,

    Affiliation Laboratório de Biologia Computacional e Bioinformática, Centro de Ciências Naturais e Humanas, UFABC – Universidade Federal do ABC, Santo André, SP, 09210-170, Brazil

  • Ney Lemke

    Affiliation Laboratório de Bioinformática e Biofísica Computacional, Departamento de Física e Biofísica, Instituto de Biociências de Botucatu, UNESP – Universidade Estadual Paulista, Botucatu, SP, 18618-970, Brazil

Bending-Twisting Motions and Main Interactions in Nucleoplasmin Nuclear Import

  • Marcos Tadeu Geraldo, 
  • Agnes Alessandra Sekijima Takeda, 
  • Antônio Sérgio Kimus Braz, 
  • Ney Lemke
PLOS
x

Abstract

Alpha solenoid proteins play a key role in regulating the classical nuclear import pathway, recognizing a target protein and transporting it into the nucleus. Importin-α (Impα) is the solenoid responsible for cargo protein recognition, and it has been extensively studied by X-ray crystallography to understand the binding specificity. To comprehend the main motions of Impα and to extend the information about the critical interactions during carrier-cargo recognition, we surveyed different conformational states based on molecular dynamics (MD) and normal mode (NM) analyses. Our model of study was a crystallographic structure of Impα complexed with the classical nuclear localization sequence (cNLS) from nucleoplasmin (Npl), which was submitted to multiple 100 ns of MD simulations. Representative conformations were selected for calculating the 87 lowest frequencies NMs of vibration, and a displacement approach was applied along each NM. Based on geometric criteria, using the radius of curvature and inter-repeat angles as the reference metrics, the main motions of Impα were described. Moreover, we determined the salt bridges, hydrogen bonds and hydrophobic interactions in the Impα-NplNLS interface. Our results show the bending and twisting motions participating in the recognition of nuclear proteins, allowing the accommodation and adjustment of a classical bipartite NLS sequence. The essential contacts for the nuclear import were also described and were mostly in agreement with previous studies, suggesting that the residues in the cNLS linker region establish important contacts with Impα adjusting the cNLS backbone. The MD simulations combined with NM analysis can be applied to the Impα-NLS system to help understand interactions between Impα and cNLSs and the analysis of non-classic NLSs.

Introduction

Solenoid proteins are molecules composed of structural motifs that are arranged in tandem, creating a superhelical architecture. This modular characteristic provides the establishment of folding and binding contacts that contrasts the globular proteins, allowing higher flexibility and the arrangement of cooperative protein-protein interactions due to the formation of diversified interfaces [14].

A remarkable characteristic in nuclear protein import regulation is the contribution of solenoid proteins to recognizing a target protein and transporting it into the nucleus [5]. One of the most studied pathways is the classical nuclear import pathway, which requires the interaction between the solenoid Importin-α (Impα) and Importin-β (Impβ) proteins, followed by the assembly of the cargo protein to Impα [610]. This trimeric complex is translocated through the nuclear pore complex (NPC), and the cargo protein is delivered into the cell nucleus mediated by Ran-GTP-dependent steps of protein-protein interactions [11, 12]. The dissociation of the cargo protein from Impα is catalyzed by nucleoporins (e.g., NUP50) [13], and Impα binds to its export factor CAS complexed with RanGTP [14]. A final step is the recycling of both Impα and Impβ back to the cytoplasm.

Impα is composed of ten tandem repeats of armadillo motifs (ARM) oriented in an elongated and curved-twisted shape [6, 10, 15]. Each motif is formed by a superhelical architecture of three α-helices [6, 15, 16]. From the curved orientation, convex and concave surfaces can be identified; in particular, the inner concave surface harbors conserved residues that mediate the cargo protein binding [6, 17].

Cargo protein transport depends on the recognition of a specific sequence signal by Impα called the nuclear localization sequence (NLS). For classical NLSs (cNLSs), the binding pattern to Impα is primarily mediated by one or two clusters of positively charged residues, the monopartite or bipartite cNLSs, respectively [1822]. The clusters of bipartite cNLSs are separated by 10–12 variant residues, denominated as the linker region.

The inner concave surface of Impα is adapted to receive either monopartite or bipartite cNLSs, and its specific binding sites can be identified as the major and minor sites. Structural and biophysical studies have related important positions of Impα to the NLS binding: positions P2–P5 from the major site (ARMs 2–4; binding to both monopartite and bipartite cNLSs) and P1’-P2’ from the minor site (ARMs 6–8; binding preferentially to bipartite cNLSs) [21, 23]. Moreover, the region between major and minor sites (ARMs 4–6) provides interactions and is also considered fundamental in cNLS recognition [21, 2430].

Few studies have reported the flexibility and structural integrity of Impβ [2, 31]; however, the application of computational simulation approaches is underexplored for understanding the wide structural motions and the interaction basis of nuclear import mediated by Impα binding. Therefore, two main questions arose: (i) Are there motions related to NLS recognition? (ii) What is the dynamical behavior of the interactions on the complex interface? Motivated by these questions, we combined molecular dynamics simulations (MD) and normal mode (NM) analysis. As our cNLS model of study, we used the crystallographic structure of nucleoplasmin NLS (NplNLS) complexed with Impα because experimental works involving Npl [17, 24, 32] are available and could be used to support and contrast with our simulation results. Npl is the first protein to be described as a molecular chaperone involved in chromatin reprogramming [33], and it is characterized as containing a bipartite cNLS (Npl:151GSAVKRPAATKKAGQAKKKKLD172; residues in bold indicate the positions in contact with Impα minor and major binding sites, respectively). We determined that bending and twisting-like major movements of Impα may influence the NLS binding. In addition, we confirmed the importance of contacts in the major and minor sites, along with contacts flanking these sites, including the linker region, for the establishment of carrier-cargo recognition.

Materials and Methods

Model of study: Classical bipartite NLS

All simulation analyses were conducted using the crystallographic structure of NplNLS complexed to mouse Impα isoform 2 (Impα -NplNLS; PDB ID: 3UL1) [17]. The missing atoms from residues G152 and S342 of NplNLS (152GSAVKRPAATKKAGQAKKKKLD172) and Impα (ImpαΔIBB, residues 72–497), respectively, were modeled with MODELLER v9.11 software [34]. The N-terminal Impβ-binding (IBB, residues 1 to 71) domain from Impα was kept truncated because it competes in the binding in the NLS region. The choice criteria for determining the best model were guided by the correct stereochemistry and the occurring interactions in the complex interface, using Molprobity [35] and PISA [36] servers, respectively. An additional modeling for Impα was conducted removing the peptide (Apo Impα) to compare the motions and flexibility of Impα in the presence and absence of the cNLS.

MD simulations

The topology and parameter files were generated on the program GROMACS v4.5.3 [37], employing the force field Charmm36 [38] without a protonation requirement because the PROKPA webserver (http://propka.org) analysis indicated no protonation changes. A cubic box of 56,568 explicit TIP3P water molecules [39, 40] was generated, ensuring at least 10 ångströms (Å) from the protein system to each edge of the box. Counter ions were added for system-charge neutralization by replacing water molecules. The system was submitted to a gradual energy minimization composed of four steps: (i) 500 steps of energy minimization by the steepest descent method, limiting the protein and peptide movement to accommodate the solvent molecules; (ii) 50,000 steps of energy minimization by the steepest descent method, limiting the movement of the protein and peptide’s main chains; (iii) 50,000 steps of unrestricted energy minimization by the steepest descent method; and (iv) 50,000 steps of unrestricted energy minimization by the conjugated gradients (CG) method.

Equilibration and unrestrained MDs were performed in periodic boundary conditions. The leapfrog integrator was used for integrating Newton’s equations of motion. The linear constraint solver (LINCS) method [37, 41] was used to freeze bonds involving hydrogen atoms, allowing an integration step of 2 femtoseconds (fs). The cutoff distance for short-range electrostatic and van der Waals interactions was 10 Å. The Particle Mesh Ewald method (PME) [42] was used to treat long-range electrostatics.

The system was equilibrated in two steps, both applying a position restraining force on the heavy atoms of the protein. The first stage involved the adoption of NVT conditions (constant number of particles, volume and temperature), heating the system to the target temperature of 300 kelvin (K) and simulating in this condition by 100 picoseconds (ps) with a velocity-rescaling (V-rescale) thermostat [43]. The second stage involved 100 ps of equilibration by the adoption of NPT conditions (constant number of particles, pressure and temperature), with pressure coupling using the Parrinello-Rahman barostat [44] and keeping the pressure relatively constant, close to the value of 1 bar. After the equilibration procedures, the restraints were removed, and the system was submitted to three MD simulations of 100 nanoseconds (ns) each, with structure sampling every 10 ps.

To ensure the conformational sampling of the system, a clustering technique proposed by Lyman and Zuckerman [45] was applied. In this approach, the steps below were applied to generate a collection of reference structures of the simulations {Si}: (1) A cutoff root-mean square deviation (RMSD) d was defined. (2) Each simulation was merged into a single trajectory file. (3) One structure from the trajectory file was sampled randomly and denominated as the reference structure. (4) All structures were compared to the sampled reference structure, and the ones with an RMSD less than d were removed from the trajectory file. (5) Steps 1, 2, 3 and 4 were repeated until all structures were removed, thus generating a collection of reference structures {Si}. (6) Based on the collection {Si}, each frame from the trajectory file was clustered with the nearest reference structure, and the frequency of structures of each cluster was then calculated. An estimation of convergence is assessed when each reference structure is equivalently represented in each simulation. The parameter for the calculation of d was the global RMSD of carbon-α (Cα) atoms. The choice of d (= 2.5 Å) was constrained to a feasible number of reference structures for the subsequent analysis of NMs.

NM analysis

Each reference structure obtained from MD simulations was minimized in the GROMACS program with explicit solvent using the same methodology described above. All NM analyses were carried out in the CHARMM v.36b1 program [46]. The topology and parameter files required for CHARMM were generated with the CHARMM-GUI server (www.charmm-gui.org) employing an additional energy minimization. The CG algorithm was applied with harmonic constraints that were progressively decreased from 250 to 5 kcal/mol-1Å-2, with 100 steps of minimization at each decrease. Then, the constraints were removed, and 10,000 steps of CG were carried out. Afterwards, the adopted basis Newton Raphson (ABNR) algorithm was applied with no constraints for 300,000 steps.

The final minimized structure was used for the calculation of the 87 lowest frequency NMs, using the VIBRAN module of CHARMM for each reference structure. An NM-displacement method using the VMOD facility of CHARMM was applied, generating structures along each NM based on short MD simulations at a low temperature (30 K), followed by energy minimization. Based on the values of mass-weighted root mean square (MRMS), the maximum displacement range was set to 3 Å for each direction of the NM with a 0.1 Å projection step, totaling 61 structures per NM. For each MRMS step, a harmonic force constant over the Cα atoms was applied (increasing from 1,000 until 10,000 kcal/mol-1Å-2), and a short MD simulation was carried out for 1 ps for each constant value, totaling 10 ps of simulation. Keeping the restraints, 1,000 steps of CG energy minimization were employed to generate the final structure. In addition, for each projection step, a value of the total restraint energy, according to the miscellaneous mean field potential (MMFP) facility of CHARMM, was used as a criterion for discarding unfavorable conformations.

Data Analysis

PCA over MD simulations.

Principal component analysis (PCA) from MD simulations was performed using the quasi-routine of the module VIBRAN of CHARMM to obtain the covariance matrix of Cα atomic displacements from the trajectories and identify the most relevant structural variations. The calculation was performed according to the description of Floquet et al. [47], and the resulting principal components (PCs) were used to compare the motions observed in NMs.

Collectivity.

The measurement of the involvement of atoms in a particular protein motion (referred to as degree of collectivity) for a given NM was calculated according to Bruschweiler [48] and Tama and Sanejouand [49], using an in-house CHARMM script. The degree of collectivity is comprised between 0 and 1. Values close to 1 indicate maximum collectivity.

Geometric analysis of Impα.

The wide motions from Impα were described in terms of geometrical measurements. For bending characterized motions, three vertices (represented by Impα residues R117, A313 and K486) were manually selected: two vertices in distal tips and one vertex at the middle point of the protein. The plane formed by these three vertices corresponded to the plane of the observed bending motion (Fig 1). Then, the radius of curvature (R) was calculated: (1) d is the distance from the distal vertices to the middle vertex, and m is half the distance between the two distal vertices.

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Fig 1. Scheme of geometrical methods adopted for the description of the Impα motions.

(A) Display of the selected vertices and the determined distances (2m and d) for the calculation of the radius of curvature. (B) The vectors generated to H3 for each ARM repeat.

https://doi.org/10.1371/journal.pone.0157162.g001

For twisting characterized motions, the angle between α-helices 3 (H3) from neighboring ARM repeats were calculated using an available script for PyMol (http://www.pymolwiki.org/index.php/AngleBetweenHelices). For each pair of helices, vectors were defined along the Cα atoms, and the torsion angles between these vectors were determined.

This geometric analysis was also applied to X-ray-solved structures of Impα complexed with different types of bipartite NLSs. These structures were retrieved by the basic local alignment search tool allocated at Prody software [50] using the Impα -NplNLS model as the query. Only structures with 100% of sequence identity to Impα were selected to be compared to the simulation data.

Maps of cross-correlations.

The initial comparison of residue-residue contacts from the MD and NM results was initially performed by the generation of maps of cross-correlation to evaluate the associated movements between NplNLS and Impα. The calculation of correlations corresponded to the ensemble of the trajectories of all MD simulations into one final pseudo-trajectory. Similarly, an ensemble of all structures from NM-displacements into one pseudo-trajectory was conducted. The cross-correlation calculations were performed in the Wordom software [51].

Interactions evaluation.

The occurrence of specific interactions in the Impα-NplNLS interface was evaluated. The determination of salt bridges and hydrogen bonds were performed using the VMD software [52]. The criteria for considering the occurrence of these interactions were the donor-acceptor distance for salt bridges and hydrogen bonds ⩽3.5 Å and the donor-hydrogen-acceptor angle deviation for hydrogen bonds ⩽60 degrees. The determination of hydrophobic contacts was based initially on the LIGPLOT program, using the crystallographic and in silico model of Impα -NplNLS to generate a list of possible interactions. Later, based on this list, the distances of the closest carbon atom from the hydrophobic side chains of each residue-pair were calculated for the MD and NM ensemble pseudo-trajectories to calculate the percentage of the occurrence of each hydrophobic contact. The criterion adopted was distances ⩽4 Å.

Complementary analysis.

The backbone RMSD and the Cα root-mean-square fluctuations (RMSF) of MD and NM-displacements were calculated in the Wordom software [51]. The structural alignment of NplNLS peptides was performed in the Crystallographic Object-Oriented Toolkit (Coot) software [53]. All graphics from the calculations above were performed using the R software [54], and the structural analysis, visualization and generation were performed in the Pymol software [55].

Results

Selection of Impα -NplNLS model

A stereochemical analysis allowed for the selection of the best complex model, taking into account the geometry and maintenance of the main interactions in the peptide-protein interface. The best-selected model showed a Ramachandran plot for Impα with 96.7% and 3.3% of the residues in favored and allowed regions, respectively, without residues in the outlier region, whereas NplNLS had 100% of the residues in favored regions.

An overall evaluation of the Impα -NplNLS model indicated the NplNLS harboring in both major and minor binding sites of Impα, with the main residues inside the binding pockets (Fig 2). Furthermore, we were able to evidence the previously stated interactions in the interface of this complex [17, 24]; the only major exception was the absence of ImpαD325 in contact with NplK155 in the minor site (S1 Fig).

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Fig 2. The starting structure of Impα-NplNLS for MD simulations.

(A) The Impα as a cartoon diagram colored based on each ARM repeat as a rainbow spectrum from N-terminal (blue) to C-terminal (red) and the NplNLS as a cyan cartoon diagram positioned in an antiparallel configuration compared to Impα. (B) The surface representation of Impα with the NplNLS as a cyan stick diagram, indicating both major (blue) and minor (orange) binding sites. (C) The major site zoom indicating positions P2–P5 and (D) the minor site zoom in P1’ and P2’. In both sites, the positively charged side chains are positioned in the main pockets of the Impα binding core.

https://doi.org/10.1371/journal.pone.0157162.g002

Standard MD combined with NM-displacement method

The trajectories obtained from the three Impα-NplNLS MD simulations were clustered into three reference structures (67,730 ps, 207,080 ps and 274,970 ps), each one exhibiting a similar frame-frequency among simulations, indicating a likely convergence of the MDs (S2 Fig). Reference structure 207,080ps was the most representative in the simulations (approximately 80% of the trajectories clustered with this structure) and was more similar to the X-ray-solved NplNLS structure based on the backbone RMSD values (S1 Table) obtained from the structural alignment of the NLSs (S3 Fig). In this alignment, important positions from major and minor sites were occupied by the expected residues, with similar side chain conformations, represented by NplK167, NplK168 and NplK170 in positions P2, P3 and P5, respectively, and NplK155 and NplR156 in P1’ and P2’, respectively. Reference structures 67,730 ps and 274,970 ps showed a greater structural variance of side chains in the major site than in the minor site.

The subsequent step was the NM-displacement method applied to the three MD reference structures. We observed flexible and favorable motions in the early NMs (modes 7–20) of Impα-NplNLS, represented by lower values of restriction energy along the whole displacement range, compared to the remaining modes (blue areas in the S4 Fig). Similar patterns were also observed for Apo Impα; however, the favorable motions were extended up to NM29 (S5 Fig), indicating that more conformations could be acquired favorably compared to the Impα bound to NplNLS.

The distribution of backbone RMSD showed that standard MD in combination with the NM-displacement method increased the conformational exploration, reaching values over 5 Å, particularly to reference structures 207,080 ps and 274,970 ps, whereas MD alone reached only approximately 2.5 Å (S6 Fig). Moreover, greater Cα fluctuations were observed in the NM-displacement technique, based on the RMSF values (S7 and S8 Figs). The comparison between the RMSF values for Impα-NplNLS and Apo Impα showed small differences, primarily limited to the region of the major site (within the range of residue 100 to 200), where Apo Impα was more flexible (S9 Fig).

Collective motions of Impα

The description of the motions obtained from MD and NM calculations combined the results from a qualitative vector-based analysis and a quantitative geometrical analysis. The first NMs showed wide and collective types of motions of the ARM repeats of Impα, primarily along modes 7–17 (S10 Fig). A qualitative analysis of vectors from modes 7 and 9 clearly showed a motion pattern, described by a bend and a twist (Fig 3 and S1 and S3 Movies), respectively.

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Fig 3. Main motions observed from NM analysis of Impα -NplNLS.

Impα (cartoon model) is shown as a rainbow spectrum from N-terminal (blue) to C-terminal (red), and NplNLS (cyan cartoon model) is positioned in an antiparallel configuration compared to Impα. The vector arrows for NM7–9 are shown with the correspondent description of the motion that they described. NM7 is shown in a front view, whereas NM8 and NM9 are shown in an upper view (90° rotation in the X-axis).

https://doi.org/10.1371/journal.pone.0157162.g003

The bend motions in NM7/PC1 were characterized by the opening and closing of Impα in the concave surface, along the NLS binding pockets. The quantitative analysis using geometric measurements determined the radius of curvature in opened and closed configurations of Impα (Fig 4A, S12 Fig and S1 Movie) and showed different amplitudes for the bending motion, in which Apo Impα had higher amplitudes than the Impα-NplNLS complex.

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Fig 4. Geometric analysis of the bending and twisting motions of Impα.

(A) The bending motion was quantitatively characterized by the radius of curvature along NM7 (solid line) and PC1 (dashed line) for Impα -NplNLS and along NM7 for Apo Impα (dotted line), whereas (B) the twisting motion was quantitatively characterized by the average values for the angles between helices along NM9 (solid line) and PC3 (dashed line) for Impα -NplNLS and along NM9 for Apo Impα (dotted line).

https://doi.org/10.1371/journal.pone.0157162.g004

The twist pattern for the Impα structures along NM9/PC3 (Fig 3, S12 Fig and S3 Movie) oscillated from maximum and minimum values of torsion over the entire protein (Fig 4B). A general observation of the angles for the Impα-NplNLS complex and Apo Impα showed similarities among the structures. A more detailed analysis, considering the inter-repeat angles (Fig 5), detected oscillation between the ARMs in the Impα-NplNLS complex, primarily between ARMs 5–6. Movements with smaller amplitudes were observed for most pairs of ARMs in Apo Impα, except the oscillation observed between ARMs 6–7.

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Fig 5. Angle between helices of Impα.

The angles between neighboring H3 pairs from the motions described as lateral-bending/twisting (along PC2 and NM8) and twisting (along PC3 and NM9) for Impα -NplNLS and Apo Impα. The ARM groups considered for each angle calculation are depicted with different color assignments.

https://doi.org/10.1371/journal.pone.0157162.g005

Bending and twisting movements were also evaluated for the crystal structures of Impα in the presence of different types of bipartite cNLSs. A comparison of geometries indicated a small difference among them in the order of tenths of ångströms (S5 Table). The qualitative vector analysis of Impα-NplNLS NM8/PC2 indicated a combination of two motions, characterized by a “lateral” bending tendency (based on a 90° X-axis rotation of Impα in relation to the bending orientation in NM7/PC1) in ARMs 1–6, mixed with a twist in ARMs 7–10 (Fig 3, S12 Fig and S2 Movie). The amplitude of the inter-repeat angle variation was slightly distinct between NM8 and PC2; however, in both cases, we could verify motions that almost reached both sites, including their intermediate region (Fig 5). The complexity of these mixed motions increased in the following modes (S11 and S13 Figs). The same analysis for Apo Impα NM8 showed the reduction of movement amplitude for most ARMs.

Main contacts in Impα-NplNLS interface

In general, the cross-correlations results from MD and NM analyses were similar (Fig 6). Well-bounded areas of positive correlations could be identified, highlighting the NplNLS range of residues in contact with Impα major and minor sites and the linker region. However, for standard MD, the correlations were more scattered in the linker.

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Fig 6. Heatmap of cross-correlations between Impα and NplNLS.

(A) Trajectories from standard MD simulations (300 ns ensemble) and (B) NM-displacement (ensemble from references structures 67,730 ps, 207,080 ps and 274,970 ps) were used for the calculation of correlations. A color bar indicates the degree of correlation from anti-correlated (negative values) to correlated (positive values) residues. The X and Y axes, respectively, show the position of each ARM repeat in relation to the Impα sequence and the NplNLS residues in contact with the protein binding sites.

https://doi.org/10.1371/journal.pone.0157162.g006

Subsequent analysis showed that most correlations could be related to specific interactions in the interface of Impα-NplNLS. Compared to our simulation data, the starting structure exhibited more contacts of hydrogen bonds and hydrophobic interactions (S1 Fig). Throughout the simulations, some of those initial contacts were lost, and MD and NM showed mostly common results (Fig 7). In particular, we observed salt bridges (ImpαE396, ImpαD280, ImpαD192 and ImpαD270) that were established along the NplNLS, specifically in P2’, P2 and the linker region. Hydrophobic contacts mediated by tryptophans (ImpαW399, ImpαW357, ImpαW273, ImpαW231, ImpαW184 and ImpαW142) occurred mostly in major and minor sites, specifically in P2’, P3 and P5. As expected, a great number of hydrogen bonds were established along the NplNLS, such as ImpαS360, ImpαN361, ImpαG323, ImpαV321, ImpαR315, ImpαY277, ImpαR238, ImpαA148, ImpαG150 and ImpαN188.

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Fig 7. Schematic representation of the interactions observed in the Impα-NplNLS interface.

(A) The major (P2–P5) and minor (P1’-P2’) sites and the linker region are indicated in the sequence of the NplNLS. (B) The standard MD (300 ns ensemble) and (C) NM-displacement (ensemble from reference structures 67,730 ps, 207,080 ps and 274,970 ps) interaction scheme is shown with salt bridges (red) and hydrogen bonds (green) as dashed-lines, and hydrophobic contacts are shown as arcs with radiating spokes. The important tryptophan residues that mediate the hydrophobic contacts are depicted in the scheme as black sticks. The main chain of the NplNLS is represented as a gray horizontal line with its respective amino acid sequences, together with side chains shown as perpendicular lines. Only interactions that had an occupancy rate ≥50% of the analyzed trajectories are indicated in the scheme.

https://doi.org/10.1371/journal.pone.0157162.g007

Most of the aforementioned interactions occurred with side chains of the charged residues of the NplNLS. Moreover, we highlighted residues ImpαD192, ImpαE396, ImpαW184, ImpαW231, ImpαW357, ImpαW399 and ImpαY277 that were observed in more than 90% of the analyzed trajectory frames from MD and NM ensembles (S2, S3 and S4 Tables).

Discussion

Bending and twisting motions may be directly related to Impα function

Both bending and twisting motions are good candidates to adapt the Impα to the cNLS, because their motion pattern promotes conformational changes in the NLS binding pockets. The combination of these motion patterns appeared to be similarly recurring in other modes, such as NM8. The vectors from other high-collectivity modes, such as NM10–13 and NM17–18, also exhibited these two main motions but in smaller portions of the protein, and they were also associated with undefined types of motions. This finding was expected because modes with higher frequency are normally associated with localized vibrations [56]. Studies involving the protein Impβ– a solenoid protein similar to Impα [1, 31, 57]– suggested the importance of bending and twisting motions to generate the flexibility of Impβ, allowing it to bind to different types of proteins [31, 58]. In our Impα computational analysis, the described movements could be equally important to adapt to different sizes of cargo proteins and NLSs, enhancing the contacts over the NLS binding site. Although no significant changes were observed by the geometric analysis from the Impα crystallographic structures bound to different types of bipartite NLSs, we must consider that the presence of only a peptide (approximately 20 amino acid length) submitted to similar crystallization conditions may not be sufficient to induce large conformational changes in this system. Therefore, the role of Impα motions is likely critical for the cNLS accommodation, considering the entire protein that contains it.

The MD/NM approaches complementarily showed the flexibility of Impα by the analysis of NM7–9 and PC1–3. The bending observed in NM7/PC1 may be directly related to the accessibility to the binding sites and the release of NLSs. This movement was observed in both Impα-NplNLS and Apo Impα, with small differences in their amplitude, resembling “open” and “close” movements. Bending motions have been reported in globular proteins to identify movements of domains along with opened and closed states [59, 60]. The bending analysis for Impα was possible because its small curvature [1] allowed for the establishment of a plane comprising two distal (N- and C-termini) atoms and a central atom. Solenoid Impβ required a more complex analysis, determining angles between vectors projected onto a reference plane in each motif to evaluate the curvature changes [31]. Specifically, the concerted bending motion of Impα NM7 could operate as an opening-closing gateway, allowing the NLS entrance and adjusting the amplitude of this motion in relation to the cargo protein size. The absence of a ligand may imply in a wider curvature favoring the access to the inner concave surface of Impα, allowing the IBB domain or cargo protein binding. Pumroy et al. [61] compared the flexibility of three human Impα isoforms (α-1, α-3 and α-7) considering their bound and unbound states and applying MD simulations. Based on the protein end-to-end distance measurements, the authors observed an increase in the flexibility of Apo Impα isoforms, in accordance with our bending characterization that showed a higher radius of curvature for Apo Impα.

According to Kobe et al. [1], the “twist” takes into account the rotations of the neighboring repeats relative to each other along the backbone direction, and ARM repeat proteins have large twist movements, allowing the accommodation of extended and flexible peptides. The twist observed in the NM9/PC3 of Impα-NplNLS showed similarities to each other, confirming the observations of Hayward et al. [62], which compared NM/PC for lysozyme protein. Although Impα-NplNLS and Apo Impα had similar average values (Fig 4B), the differences were found only in individual analyses of the neighboring ARM repeats. The angle variation between ARM6 and ARM7 in NM9 of Apo Impα (Fig 5) is remarkable, and a similar result was already observed for Apo Impα-3 [61]. The lack of a ligand (IBB domain or NLS) interacting with the Apo Impα concave portion may lead to a higher twist in the middle of Apo Impα due to the lack of interactions that stabilize and provide binding specificity. The increment of the angle amplitude in this region was contrasted by lower values for the remaining protein regions compared to Impα-NplNLS. Therefore, Impα-NplNLS may require conformational changes for the NLS adjustment to the binding pockets of the Impα inner surface, which explains the greater variation in the ARM’s angles in contrast to Apo Impα, which would not require such adjustments. This same explanation applies to the amplitude variations also found in NM8 for the bound/unbound states of Impα.

Experiments and MD simulation with Neurospora crassa Impα emphasize the instability of an N-terminally truncated Impα in the absence of an NplNLS peptide, indicating the occupancy of the NLS binding sites as a requirement for Impα crystallization [63]. In addition, Falces et al. [64] also showed, performing circular dichroism assays with Impα-1ΔIBB from Xenopus laevis, the stabilization of the protein upon association with Npl, thus reinforcing the aforementioned observations. The establishment of polar contacts settles the NLS backbone, whereas hydrophobic and electrostatic interactions with positively charged NLS residues allow the specificity [16, 21]. The greater structural flexibility of Apo Impα was only observed by the geometrical analysis for the NM7 bending. Despite the non-association of the NM8/NM9 twisting motions to a greater overall flexibility of Impα, the NLS absence allowed for a greater motion amplitude of other NMs, such as modes 21–27, comparing the restriction energies of Impα-NplNLS (S4 Fig) and Apo Impα (S5 Fig), indicating that the higher flexibility of Apo Impα appeared to be distributed over these modes. In addition, considering the Cα fluctuations of Impα in its bound and unbound states (S9 Fig), we observed a higher flexibility in the major site of Apo Impα. This result was also observed for Apo Impα-3 [61], and the authors predicted a weaker binding for NLSs that relies primarily on the major site. However, this statement does not seem to apply to our case because Impα-2 has been crystallized with different types of NLSs, including those with preference to the major site; e.g., simian virus 40 (SV40) NLS [24]. Moreover, the binding stability of Impα-2 to some of those NLSs was also observed with ligand binding assays [17, 65, 66]. In summary, the NLS binding stabilizes Impα, apparently restricting the motion range represented by some higher-frequency NMs; however, it may also allow localized adjustments between the ARM repeats to improve the overall affinity to the bound NLS.

The role of the linker residues in cNLS recognition

The cross-correlation calculations performed for both MD simulations (Fig 6A) and displacement along NMs (Fig 6B) showed positive correlations from residues of both major and minor sites of Impα. Further analysis showed that the majority of positive correlations observed could be explained by the correspondence of salt bridges, hydrogen bonds and hydrophobic interactions. We could determine that positions P2 and P5 from the major site and P1’ and P2’ of the minor binding site have high levels of contact with the NplNLS, based on the occupancy values of some interactions in those regions. These data confirm the maintenance of the main contacts between Impα and NplNLS, showing that our simulation results are in agreement with the experimental data [17, 24].

A classical bipartite NLS sequence interacts simultaneously with major and minor binding sites of Impα and depends on a linker region containing a minimum of 10 residues between P2’ and P2 positions to act as a cNLS [5, 30]. The linker region in the NplNLS appears to play a key role in the process of cNLS recognition. The cross-correlation maps clearly indicated an involvement of this region in the promotion of contacts with Impα. A detailed analysis of the interactions showed the occurrence of salt bridges, hydrogen bonds and hydrophobic contacts along the NplNLS. The involvement of ImpαR238, ImpαR315, ImpαW273 and ImpαY277 was already observed in Impα-NplNLS crystal structures [17, 24]. However, the computational approach indicated other interactions previously reported in single structures; ImpαK353 and ImpαN350 were reported with the NLS from FEN-1 [30] and ImpαD280 from SV40 NLS bound to the Impα from a filamentous fungus [67]. Moreover, new possible contacts were detected; e.g., residues ImpαN446, ImpαR101 and ImpαR102 interacted in the N- and C-terminal regions of the NLS.

Our simulation analyses suggest that the linker contacts are important to settle the cNLS, and help to accommodate the cNLS side chains into the grooves of major and minor binding sites. The linker region, in addition to the N- and C-terminals of an NLS, may also compensate for interactions for the establishment of an activation pattern of the other NLS region [22], which indicates that the linker contacts may occur in different NLSs and can be maintained after the docking of the bipartite NLS in both major and minor binding sites, depending on the residues composing the linker, such as proline and acidic amino acids [5, 22]. In summary, the recurrent presence of residues outside the major and minor sites strongly reinforces their importance for the proper binding of the NLS, which corroborates other studies involving other NLSs [21, 2529] and further encourages us to understand in greater detail their roles and effects during the nuclear import process.

NM analysis with classic MD simulations

MD simulations and NM analysis have been used for macromolecules as a complementary analysis to the experimental data to describe their main motions and relate to a specific function [59, 60, 68, 69]. The approach used for the Impα-cNLS complex combines NMs robustness—to evaluate wider protein movements—with the reference structures from the MD and indicates the benefits of this association in protein-peptide analysis.

The data sampling from MD simulations, despite the time constraints and convergence difficulties associated with this technique [70, 71], were balanced among the selected reference structures. Considering the time of the simulations, there is a likely stability of the studied system. Although we have not performed classical MD of Apo Impα, Takeda et al. [63] reinforce the instability of an N-terminally truncated Impα in the absence of an NLS peptide. One way of computationally evaluating the N-terminally truncated Impα would be applying long MDs to observe the effects of high protein flexibility. However, with a simple NM calculation, we could observe in general, based on the restraint energy profile, RMSF values and geometrical analysis, the higher flexibility of Impα in the absence of the NLS.

The MD data with the Impα-NplNLS complex not only supported the maintenance of the protein-peptide complex but also showed some of the major movements and interactions occurring at the complex interface. NMs promoted an analytical method to access the dynamics of the system, allowing the possibility of the recognition of new interactions and dribbling the convergence and conformational restrictions from standard MD. The main motions described here in NMs were also obtained in the PC analysis, in agreement with the comparison between the lowest NMs and the first PCs obtained from MD simulations in the lysozyme model [62] and a subunit of the GroEl chaperone [69]. The highlighted movements are of high occurrence in the protein’s lifetime and are likely to be functionally important. Moreover, the low computational cost of NM is once more an attractive feature for application in biological systems.

Conclusions

Computational approaches of MD and NM analysis were combined to evaluate the main of motions of Impα and its interaction to a cNLS peptide. The bending motion may be involved in the NLS entrance and the accommodation of cargo protein depending on its size, whereas the twist motions may be involved in the NLS recognition and accommodation into the Impα binding sites. The combination of these movements could allow local adjustments between the ARM repeats, which could improve the overall affinity to the cNLS. The absence of an NLS was also evaluated and may imply in a wider curvature of Apo Impα, allowing for the IBB domain or cargo protein binding. Moreover, a higher twist in the middle of Apo Impα was detected possibly due to the lack of interactions that stabilize and provide binding specificity, which could explain the challenges in crystallizing N-terminally truncated Apo Impα.

The evaluation of salt bridges, hydrogen bonds and hydrophobic interactions corroborates the fundamental interactions between Impα and NplNLS and gives additional support for interactions outside the classical binding pockets that are important during this process. The linker contacts in cNLS assist the adjustment of the peptide backbone, which helps the interactions between cNLS side chains and residues from major and minor binding grooves. In conclusion, MD simulations combined to NM analysis supported the maintenance of the Impα-NplNLS complex exploring the conformational space and accessing the dynamics of the system with a lower computational cost. This approach may help to understand the affinities between Impα and cNLS peptides and non-classic NLSs.

Supporting Information

S1 Movie. Movie of NM7.

Impα is shown in a cartoon diagram, and it is colored according to each ARM repeat, from the N-terminal (blue) to the C-terminal (red) ends of the protein. The NplNLS is represented in a cyan cartoon diagram positioned in an antiparallel configuration compared to Impα.

https://doi.org/10.1371/journal.pone.0157162.s001

(MP4)

S2 Movie. Movie of NM8.

Impα is shown in a cartoon diagram, and it is colored according to each ARM repeat, from the N-terminal (blue) to the C-terminal (red) ends of the protein. The NplNLS is represented in a cyan cartoon diagram positioned in an antiparallel configuration compared to Impα.

https://doi.org/10.1371/journal.pone.0157162.s002

(MP4)

S3 Movie. Movie of NM9.

Impα is shown in a cartoon diagram, and it is colored according to each ARM repeat, from the N-terminal (blue) to the C-terminal (red) ends of the protein. The NplNLS is represented in a cyan cartoon diagram positioned in an antiparallel configuration compared to Impα.

https://doi.org/10.1371/journal.pone.0157162.s003

(MP4)

S1 Fig. Interactions from the starting structure.

Scheme of interactions of the starting structure for MD simulations. The representation is similar to the description of Fig 7.

https://doi.org/10.1371/journal.pone.0157162.s004

(PDF)

S2 Fig. Convergence analysis.

Bar plot indicating the frequency of structures clustered within each reference (67,730 ps, 207,080 ps and 274,970 ps) from the MD simulations.

https://doi.org/10.1371/journal.pone.0157162.s005

(PDF)

S3 Fig. Structural alignment of NplNLS.

Structural representation of the NplNLSs from reference structures 67,730 ps (orange), 207,080 ps (green) and 274,970 ps (blue) aligned with the NplNLS from X-ray (red). (A) Stick diagram of the main chain, with major and minor sites indicated. (B-C) Stick diagram including side chains and the residues from each site.

https://doi.org/10.1371/journal.pone.0157162.s006

(PDF)

S4 Fig. Heatmap of the total restraint energy values from Impα -NplNLS.

The values are from the structures generated from the NM-displacement of the most representative reference structure (207,080 ps) according to the convergence analysis. The X-axis is the displacement range, represented as values of mass-weighted root mean square (MRMS), and the Y-axis is the NM numbers. Lower values of energy (blue tons) indicate favorable conformations.

https://doi.org/10.1371/journal.pone.0157162.s007

(PDF)

S5 Fig. Heatmap of the total restraint energy values from Apo Impα.

The values are from the structures generated from the NM-displacement. The X-axis is the displacement range, represented as values of MRMS, and the Y-axis is the NM numbers. Lower values of energy (blue tons) indicate favorable conformations.

https://doi.org/10.1371/journal.pone.0157162.s008

(PDF)

S6 Fig. Conformational exploration.

Box-plot of the RMSD distribution from the trajectories of standard MD (MD-1, MD-2 and MD-3) and NM-displacement (67,730 ps, 207,080 ps and 274,970 ps).

https://doi.org/10.1371/journal.pone.0157162.s009

(PDF)

S7 Fig. Residue fluctuations of Impα -NplNLS.

Residue fluctuations based on Cα RMSF of Impα from the ensemble trajectories of standard MD (red) and NM-displacement (cyan).

https://doi.org/10.1371/journal.pone.0157162.s010

(PDF)

S8 Fig. Residue fluctuations of NplNLS.

Residue fluctuations based on Cα RMSF of NplNLS from the ensemble trajectories of standard MD (red) and NM-displacement (cyan).

https://doi.org/10.1371/journal.pone.0157162.s011

(PDF)

S9 Fig. Residue fluctuations of apo ImpαΔIBB.

Residue fluctuations based on Cα RMSF of Impα from the trajectories of the NM-displacement of Impα -NplNLS (from reference structure 207,080 ps; cyan) and Apo ImpαΔIBB (black).

https://doi.org/10.1371/journal.pone.0157162.s012

(PDF)

S10 Fig. Collectivity from Impα -NplNLS.

The collectivity values are plotted for each NM, and a smoothed line is fitted (blue line), representing the data tendency. The shaded area is the confidence interval around the smoothed line calculated with the ggplot package (http://ggplot2.org/) in R.

https://doi.org/10.1371/journal.pone.0157162.s013

(PDF)

S11 Fig. Main motions observed in NMs10–13, NM17 and NM18.

The vector arrows indicating the motions are shown. The Impα is displayed in a cartoon diagram, with each ARM colored from blue to red, corresponding to N to C-terminals. The NplNLS (cyan) is in a cartoon representation and is positioned in an antiparallel configuration compared to Impα.

https://doi.org/10.1371/journal.pone.0157162.s014

(PDF)

S12 Fig. Main motions observed in PCs1–3 from standard MD.

The vector arrows indicating the motions are shown. The Impα is displayed in a Cα representation, with each ARM colored from blue to red, corresponding to N to C-terminals. The NplNLS (cyan) is in Cα representation and is positioned in an antiparallel configuration compared to Impα.

https://doi.org/10.1371/journal.pone.0157162.s015

(PDF)

S13 Fig. Angles between helices of Impα -NplNLS for NMs10–13, NM17 and NM18.

The ARM groups considered for each angle calculation are depicted with different color assignments, similar to Fig 5.

https://doi.org/10.1371/journal.pone.0157162.s016

(PDF)

S1 Table. Backbone RMSD values from structural alignment.

The reference structures are aligned with the Impα -NplNLS crystallographic structure (PDB ID 3UL1).

https://doi.org/10.1371/journal.pone.0157162.s017

(PDF)

S2 Table. Salt bridges occupancies.

The occupancies of salt bridges between NplNLS and Impα in standard MD and NM-displacement. Interactions that were above 50% of occupancy are highlighted in gray.

https://doi.org/10.1371/journal.pone.0157162.s018

(PDF)

S3 Table. Hydrogen bonds occupancies.

The occupancies of hydrogen bonds between NplNLS (blue) and Impα (green) in standard MD and NM-displacement. Interactions that were above 50% of occupancy are highlighted in gray.

https://doi.org/10.1371/journal.pone.0157162.s019

(PDF)

S4 Table. Hydrophobic contacts occupancies.

The occupancies of hydrophobic contacts between NplNLS and Impα in standard MD and NM-displacement. Interactions that were above 50% of occupancy are highlighted in gray.

https://doi.org/10.1371/journal.pone.0157162.s020

(PDF)

S5 Table. Radius of curvature and average angles for the crystallographic structures.

PDB IDs: 1pjm, 1pjn, 3tpm, 3ukw, 3ukx, 3uky, 3ukz, 3ul1 and 3uvu.

https://doi.org/10.1371/journal.pone.0157162.s021

(PDF)

Acknowledgments

This study was supported by Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP) [grant numbers 2012/19447-2; 2014/21976-9] and Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq) [grant number 142110/2012-4]. We are grateful to Prof. Dr. Cesar Martins for providing computational access for running part of the simulations.

Author Contributions

Conceived and designed the experiments: MTG AAST ASKB NL. Performed the experiments: MTG. Analyzed the data: MTG AAST ASKB NL. Wrote the paper: MTG AAST.

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