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Alpha-shapes

Part of the problem with defining the shape of a protein is that we start with nothing but a point set, and the "shape" of a set of discontinuous points is poorly defined. The problem is, what do we mean by shape? As you saw above, the shape of a molecule depends on what is being used to measure it. To handle this ambiguity, we will introduce a method of shape calculation based on a parameter, α, which will determine the radius of a spherical probe that will define the surface. The method defines a class of shapes, called α-shapes for any given point set. It allows fast, accurate, and efficient calculations of volume and surface area.

α-shapes are a generalization of the convex hull . Consider a point set S. Define an α-ball as a sphere of radius α. An α-ball is empty if it contains no points in S. For any α between zero and infinity, the α-hull of S is the complement of the union of all empty α-balls.

  • For α of infinity, the α-shape is the convex hull of S.
  • For α smaller than the 1/2 smallest distance between two points in S, the α-shape is S itself.
  • For any α in between, one can think of the α-hull as the largest polygon (polyhedron) or set thereof whose vertices are in the point set and whose edges are of length less than 2α. The presence of an edge indicates that a probe of radius α cannot pass between the edge endpoints.

Two-dimensional α-shapes

Some α-shapes are shown for a point set and various values of α. On the left, α is 0 or slightly more, such that an α-ball can fit between any two points in the set. The α-shape is therefore the original point set. On the right, α is infinity, so an α-ball can be approximated locally by a line. α on this scale yields the convex hull of the point set. The middle image shows the α-shape for α equal to the radius of the ball shown. This yields two disjoint boundaries, one of which has a significant indentation. Voids , or empty pockets completely enclosed by the α-shape, are also possible, for instance if the α-shape is ring-like (in 2D) or forms a hollow shell (in 3D).

Computing the alpha-shape: delaunay triangulation

A triangulation of a three-dimensional point set S is any decomposition of S into non-intersecting tetrahedra (triangles for two-dimensional point sets). The Delaunay triangulation of S is the unique triangulation of S satisfying the additional requirement that no sphere circumscribing a tetrahedron in the triangulation contains any point in S. Although it is incidental to α-shapes, it is worth noting that the Delaunay triangulation maximizes the average of the smallest angle over all triangles. In other words, it favors relatively even-sided triangles over sharp and stretched ones.

Two-dimensional delaunay triangulation

The Delaunay triangulation of the four points given is shown on the right. Note that the circumscribing circles on the left each contain one point of S, whereas the circles on the right do not. The transition from the triangulation on the left to that on the right is called an edge flip, and is the basic operation of constructing a two-dimensional Delaunay triangulation. Face flipping is the analogous procedure for five points in three dimensions.
The Delaunay triangulation of a point set is usually calculated by an incremental flip algorithm as follows:
  • The points of S are sorted on one coordinate (x, y, or z). This step is not strictly necessary but makes the algorithm run faster than if the points were in arbitrary order.
  • Each point is added in sorted order. Upon adding a point:
    • The point is connected to previously added points that are "visible" to it, that is, to points to which it can be connected by a line segment without passing through a face of a tetrahedron.
    • Any new tetrhedra formed are checked and flipped if necessary.
    • Any tetrahedra adjacent to flipped tetrahedra are checked and flipped. This continues until further flipping is unnecessary, which is guaranteed to occur
This algorithm runs in worst case O(n^2) time, but expected O(n^(3/2)) time. Without the sort in the first step, the expected case would be O(n log n) . A full description and analysis of Delaunay triangulation algorithms is given in [1] , chapter 9.

Questions & Answers

A golfer on a fairway is 70 m away from the green, which sits below the level of the fairway by 20 m. If the golfer hits the ball at an angle of 40° with an initial speed of 20 m/s, how close to the green does she come?
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2. A sled plus passenger with total mass 50 kg is pulled 20 m across the snow (0.20) at constant velocity by a force directed 25° above the horizontal. Calculate (a) the work of the applied force, (b) the work of friction, and (c) the total work.
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Nevermind i just realied that the graph is the phons output for a person with normal hearing and not just the phons output of the sound waves power, I should read the entire thing next time
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Follow up question, does anyone know where I can find a graph that accuretly depicts the actual relative "power" output of sound over its frequency instead of just humans hearing
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A string is 3.00 m long with a mass of 5.00 g. The string is held taut with a tension of 500.00 N applied to the string. A pulse is sent down the string. How long does it take the pulse to travel the 3.00 m of the string?
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Source:  OpenStax, Geometric methods in structural computational biology. OpenStax CNX. Jun 11, 2007 Download for free at http://cnx.org/content/col10344/1.6
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