- Open Access
CAVER: a new tool to explore routes from protein clefts, pockets and cavities
© Petřek et al; licensee BioMed Central Ltd. 2006
- Received: 24 February 2006
- Accepted: 22 June 2006
- Published: 22 June 2006
The main aim of this study was to develop and implement an algorithm for the rapid, accurate and automated identification of paths leading from buried protein clefts, pockets and cavities in dynamic and static protein structures to the outside solvent.
The algorithm to perform a skeleton search was based on a reciprocal distance function grid that was developed and implemented for the CAVER program. The program identifies and visualizes routes from the interior of the protein to the bulk solvent. CAVER was primarily developed for proteins, but the algorithm is sufficiently robust to allow the analysis of any molecular system, including nucleic acids or inorganic material. Calculations can be performed using discrete structures from crystallographic analysis and NMR experiments as well as with trajectories from molecular dynamics simulations. The fully functional program is available as a stand-alone version and as plug-in for the molecular modeling program PyMol. Additionally, selected functions are accessible in an online version.
The algorithm developed automatically finds the path from a starting point located within the interior of a protein. The algorithm is sufficiently rapid and robust to enable routine analysis of molecular dynamics trajectories containing thousands of snapshots. The algorithm is based on reciprocal metrics and provides an easy method to find a centerline, i.e. the spine, of complicated objects such as a protein tunnel. It can also be applied to many other molecules. CAVER is freely available from the web site http://loschmidt.chemi.muni.cz/caver/.
- Molecular Dynamic Simulation
- Convex Hull
- Access Route
- Molecular Dynamic Trajectory
- Source Vertex
The shape of a protein is complicated by its many clefts, pockets, protrusions, channels and cavities. Protein concavities offer a unique microenvironment for biological functions, such as ligand binding or enzymatic catalysis. Protein shape is of great interest to medicinal chemists working in the drug discovery industry and looking for inhibitors, enzymologists interested in identifying substrate molecules based on the well known "lock and key" mechanism and protein chemists studying protein-protein or protein-DNA interactions. The identification of protein pockets and cavities has been the focus of several studies [1–4] and various algorithms have been developed for the calculation of protein volume and surface area. A large number of enzymes possess buried active sites that are connected to the external solvent environment by access routes (tunnels or channels). A catalytic step must always be preceded by the formation of an enzyme-substrate complex, which may require passage of the substrate through these routes. The size and shape of the access routes may become an important determinant of enzyme substrate specificity . Changes in the diameter of the access tunnels during the dynamic movement of a protein play an important biological role, such as that described for acetylcholinesterase . Two narrow active site gorges are positioned deep inside the protein core and movement of the residues making up the gorge walls is necessary to allow ligands access to the active site. A method based on molecular surface was used for the calculation of the gorge diameter in acetylcholinesterase. The diameter was defined as the maximum probe size that produces a continuous molecular surface between an active site and a solvent. Calculation of one diameter in this approach requires the generation of several molecular surfaces using a series of probes of increasing size . A more effective method is implemented in the CAST program, which utilizes the alpha shape theory. CAST computation of pockets and their openings does not require direct human interaction. The required inputs are atomic coordinates, van der Waals radii, and the radius of the probe sphere . The program VOIDOO, a component of O package utilizes a grid-based algorithm for detection, delineation, and measurement of protein cavities and solvent accessible pockets. The VOIDOO algorithm suffers from crude grid spacing and the "can-of-worms" phenomenon . The central problem in the analysis of tunnels in protein structures is the identification of the centerline, i.e. spine, of a 3D object. Algorithms dealing with centerlines have been applied to medical procedures, for example in virtual colonoscopy and bronchoscopy [8–11].
The aim of this study was to develop a rapid and accurate algorithm for the identification of routes from buried active sites to the external solvent in static protein structures. We aimed to produce an algorithm that could also be applied to molecular dynamic trajectories. Further, the algorithm was intended to allow changes in the radius of a channel gorge with time to be monitored and the most probable access routes to be identified. Several other requirements were taken into consideration during development of the algorithm and its implementation: (i) speed, thus enabling rapid analysis of an entire trajectory from a molecular dynamic simulation, i.e. thousands of snapshots, in a few hours; (ii) easy identification of a starting point for the calculation; (iii) that the algorithm functions independently of the probe radius; (iv) storage of paths in PDB format; and (v) intuitive visualization.
Attention is paid to nodes that lie on a boundary of the modeled convex hull. These nodes are potential end-stops of the grid search algorithm because each boundary node can be treated as a putative outfall of the channel. The mathematical object, which is called a vertex-weighted graph, is constructed and the algorithm applied to identify the shortest low-cost path. Each possible path from the active site to the exterior is evaluated as a positive value. This value represents the relative cost to navigate each path in what could be described as a "highway-toll". Long and complicated paths are more "expensive", while the short direct paths are "cheaper" (Fig. 2). More formally, the cost function C(P) is defined (Eq. 1) for the given path P as the sum of node-price-function values calculated for all nodes forming the path P. Let N(P) be the set of all points form the path P, then the C(P) is expressed as
This cost function depends on the number of nodes in each sum and, as such, this function is not suitable for the purposes of comparison. A normalized cost function is defined (Eq. 2) to avoid cost function dependence on a summand number:
where N is the number of the summand. Next, the single node cost function c(x) must fulfill two requirements. First, it must provide a positive value for each node and a low-value for nodes that are surrounded by empty space. Second, it must identify preferred nodes that are surrounded by sufficient empty space to allow a hypothetical substrate to pass through a channel without risk of collision. These low-weighted nodes are preferentially selected by the search-algorithm. In our case, the cost function c(x) for a single node was chosen (Eq. 3)
where function rmax (x) is equal to the maximal radius of a hypothetical ball that can be inserted into node x just touching the protein surface. The small constant ε is here only for technical purposes to get rid of a singularity of the function in points where rmax (x) equals zero.
The method was implemented in the CAVER program (Additional file 1 and web page http://loschmidt.chemi.muni.cz/caver/. The program uses the publicly-licensed software qhull  that quickly (in O(N log N) time) computes a convex hull for a given set of N points in three dimensions. The result of qhull was used to eliminate nodes located outside the convex hull. All points were investigated regardless of whether they lay inside or outside the convex hull. This can be achieved by traversing all facets of the convex hull and testing whether a point lies in the same halfspace as another convex hull point. This process takes O(NK) time, where N is the number of points inside the convex hull, and K is the number of facets forming the convex hull.
Based on graph theory, several methods for the shortest path problem have been described. The most widely used algorithms are Dijkstra's , Bellman-Ford's [14, 15], A* search algorithm, and the Floyd-Warshall algorithm . In our case, a positively vertex-weighted graph is plotted on a three dimensional grid, where the source vertex is known while the destination vertex is not. We used a modified form of the Dijkstra's algorithm.
The Dijkstra's algorithm effectively solves the problem of the shortest path from a single source vertex to the destination one. It was originally designed for edge-weighted graphs but its vertex-weighted variation is easy to implement. The algorithm can be used even if the destination vertex is unknown. In the main loop of the algorithm, the shortest path to the closest available vertex (measured from the source vertex) is determined. Then, estimates of the shortest path for all the adjacent vertices are updated. This means searching can be terminated if the nearest available vertex is the boundary vertex indicating that the shortest path has been identified. To speed up the algorithm, a modification related to the cost function was implemented. The single node cost function is evaluated as part of the main loop of the Dijkstra's algorithm. The cost function is evaluated only at nodes where it is required.
The identified path can be easily visualized since the program writes a PDB file containing the coordinates of the path nodes accompanied by the maximum probe radius that touches the vdW protein surface (Fig. 3). A user-friendly GUI was implemented in the graphic program PyMol .
An algorithm to perform a skeleton search on a defined grid was developed and implemented in the CAVER program as described in the Methods section. The algorithm developed automatically finds the easiest path from the starting point, typically located inside the molecule, to the exterior of the molecule. The identified path resembles a tunnel that connects protein clefts, pockets or cavities with the surrounding bulk solvent. The tunnel characteristics, e.g. length, mean radius and gorge radius are determined and can be further analyzed. In molecular dynamics trajectories it is possible to analyze time fluctuations of tunnel characteristics and construct a dynamic picture of tunnel behavior.
The tunnel gorge radius rgorge is one of the most important tunnel characteristics because the tunnel gorge can form a bottleneck for substrate access or product release to and from the active site of a protein. The radius rgorge as estimated by the algorithm is always underestimated in finite grids. The maximal error "max" of an rgorge estimation is expressed by the equation (Eq. 4):
where d is equal to the length of the grid cell edge. The probability of εmax realization is equal to zero and this error is overestimated, therefore the mean error should be defined. The mean error of rgorge determination is equal to (Eq. 5):
and its variance and deviation equal to (Eq. 6)
The rgorge estimation should be corrected by adding 0.48d to the rgorge. The corrected rgorge estimate has a mean error value με = 0 and the variance of error is var(ε) = 0.019d2. In the case of a globular protein (50 × 50 × 50 Å3) the εmax (rgorge) costs 0.43 Å for a grid with d = 0.5 Å, however, the mean ε(rgorge) equals 0.24 Å, and σε = 0.07 Å. The results of the tests (depicted in Fig. 4) focus on the convergence of the identified paths with d decreasing from 1.0 to 0.3 Å.
Performance of the method is given as the tunnel volume i.e. number of vertexes searched rather than the number of atoms. In the case of haloalkane dehalogenases (the active site volume ~200Å3) the typical calculation of one tunnel takes about 10–12 sec. but in the case of cytochrome P450 2C9 or 3A4 (which has larger active sites ~500–600Å3) the calculation takes about 20–25 sec. In case of very large cavities (e.g. RNA) calculation may take several minutes at low resolution (d = 1–2Å). The program performance was tested on Pentium IV 3.2 GHz machine with 2 GB RAM running on Windows XP Professional operating system.
Analysis of X-ray structures
Characteristics of tunnels. Characteristics of the four most accessible paths connecting the active sites of DhlA, DhaA and LinB with the bulk solvent.
0.89 ± 0.04
34.2 ± 2.6
16.1 ± 0.4
0.86 ± 0.05
34.8 ± 4.7
15.1 ± 0.4
0.71 ± 0.08
46.2 ± 6.1
15.6 ± 0.3
0.70 ± 0.11
51.6 ± 12.1
16.6 ± 1.5
1.47 ± 0.16
14.3 ± 7.7
13.8 ± 0.6
1.28 ± 1.02
24.0 ± 9.4
15.0 ± 4.3
1.00 ± 0.16
29.0 ± 10.7
15.5 ± 3.9
0.97 ± 0.35
32.0 ± 16.4
14.8 ± 2.4
1.41 ± 0.11
16.3 ± 1.6
14.2 ± 0.7
1.11 ± 0.15
22.6 ± 6.8
14.1 ± 0.6
0.97 ± 0.08
31.7 ± 4.7
15.1 ± 0.4
0.83 ± 0.06
35.4 ± 5.8
14.7 ± 0.7
The three crystal structures available for the DhaA enzyme (1BN6, 1BN7 and 1CQW) were analyzed for the presence of access routes. CAVER detected one clearly preferred route, which corresponded to the upper tunnel. The gorge of this tunnel is made up of W141, F144, A145, F159, V172 and C176 (numbered according to dhaA sequence). The additional paths were located in the slot (Fig. 6B). The slots of the three structures studied showed a slightly different spatial position and variable size with respect to the mean gorge radius, mainly due to repositioning of the side-chain R133. The cost function of these routes was almost twice that of the upper tunnel (Table 1), but still comparable with the main tunnel and the slot of DhlA, which are known to be involved in substrate binding and product release. Exchange of solvent molecules between the active site and the slot was observed during a 1ns molecular dynamic simulation .
Analysis of eleven available LinB crystal structures (1CV2, 1D07, 1K5P, 1K6E, 1MJ5, 1K63, 1IZ8, 1IZ7, 1G5F, 1G4H and 1G42) identified the lower tunnel as the most accessible access route in nine of them (underlined). The gorge of this tunnel is made up of P144, D147, L177 and A247. The upper tunnel was identified as the most accessible route in two out of the nine structures. The gorge of the upper tunnel is formed by D147, F151, V173 and L177. Systematic searches of the four tunnels in the structures revealed the slot as another possible access route (Fig. 6C). The cost function of this route is, however, twice that of the lower tunnel (Table 1). Its gorge is formed by D142, P144, L248, G251 and M253. Previous molecular dynamics simulations  demonstrated that all three access routes can be used in the exchange of water molecules between the active site and the bulk solvent. The existence of alternative export routes explains the activity of LinB mutants that carry a large amino acid residue at position L177 . L177 is located inside the lower tunnel and its substitution may result in closure of this tunnel.
Analysis of molecular dynamics trajectories
As in the previous case, the molecular dynamics simulation of the DhaA enzyme was analyzed using the CAVER program. Two main clusters were identified by CAVER, one having two subclusters (Fig. 7B) of gorges resulting in three different paths,. The most populated access gorges (64%) were located in the upper tunnel and the two remaining gorge clusters were positioned in the slot. The two subclusters in the slot (Fig. 7B) have populations equal to 26% (cluster 2) and 10% (cluster 3), respectively. Analysis of the LinB molecular dynamics trajectory identifies the main tunnel as the most accessible route to the active site (Fig. 7C).
A new algorithm for the identification of tunnels in large molecular systems was developed and implemented in the CAVER program, which is available within the public domain. The algorithm automatically explores a grid, which is constructed over the molecule and stripped to its convex hull. Nodes are evaluated using a cost function, which determines the amount of free space around the node. The grid search algorithm is used to find the lowest-cost centerline path between a given starting point and the surface of the molecule. The user needs only to provide the molecular geometry, atomic van der Waals radii and the designated starting point, to enable the analysis of any molecular system be it protein, nucleic acid or inorganic material. The algorithm is sufficiently rapid and robust for the routine analysis of molecular dynamics trajectories that contain thousands of snapshots. The program is also available as a plug-in for PyMol and, additionally a Web-based version of the program offers analysis of static protein structures online.
The authors express their thanks to Petr Kulhánek (NCBR, Brno, Czech Republic) for his valuable suggestions. This work was supported by the Czech Ministry of Education and the Grant Agency of the Czech Republic (MSM6198959216, MSM0021622413, LC512 and 305/06/P139). J.D. is funded by an EMBO/HMMI Young Investigator grant.
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