Difference between revisions of "Detailed Program Flow"

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=Implementation in C++=
 
  
The code is written in C++ for speed.  We attempt to use an somewhat object-based approach, but a good many of the member variables are declared as static global to allow their access across threads.
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The flowchart below shows a detailed view of the how the program works.
  
Here is a breakdown of the main classes and functions in the program.  There are numerous other functions but this is the core of the program:
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[[file:Overview_complex.png|800px|Figure 2: Comet program flow (detailed)]]
 
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* Main()
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** Spawns threads: <code>collisiondetectionthread</code> , <code>linkforcesthread</code>  and <code>applyforcesthread</code>  depending on the <code>USETHREAD_COLLISION</code> , <code>USETHREAD_LINKFORCES</code>  and <code>USETHREAD_APPLYFORCES</code>  parameters.
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** Parses the <code>comet_params.ini</code>  file to read parameters.  All of the parameters are implemented as globals (should fix at some point)
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** Creates the main <code>theactin</code>  and <code>nuc_object</code>  objects.
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** Runs through the main iteration loop, calling <code>theactin.iterate()</code>  and saving snapshots every so often.
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*  Actin class
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** There is only one actin object, <code>theactin</code> , which constitutes the network, i.e.~contains the nodes and the functions that deal with them.
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** The <code>iterate()</code>  function does one iteration pass, calling:
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***<code>nucleator_node_interactions()</code>  displaces any nodes out of the nucleator object along a normal to the nucleator surface
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***<code>nucleate()</code>  adds new harbinger nodes to the surface of the nucleator
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***<code>crosslinknewnodes()</code>  crosslinks harbingers once they are ready
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***<code>sortnodesbygridpoint()</code>  orders nodes by gridpoint. The {\it only} reason for this is for the division of labor when using threads: We do repulsion by gridpoint to save re-calculating nearby nodes if there are multiple nodes on one gridpoint, and we do not want to divide nodes on one gridpoint across multiple threads.
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***<code>collisiondetection()</code>  detects whether nodes are within <code>NODE_REPULSIVE_RANGE</code>  of one another and adds the repulsive force to <code>rep_force_vec[]</code> .
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***<code>linkforces()</code>  Calculates the forces between nodes due to links and puts into <code>link_force_vec[]</code> .  If a link goes above a certain threshold force, marks it as broken and removes next time (again to prevent thread problems---since a link is removed both ways and we can't guarantee that both nodes are being processed by same thread)
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***<code>applyforces()</code>  updates the positions of all the nodes.  Sums over the threads for <code>rep_force_vec[]</code> , <code>link_force_vec[]</code>  and <code>repulsion_displacement_vec[]</code> .
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***Numerous other functions for things like saving bmps, vrml etc.
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**Nucleator class
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*** There is only one nucleator object at the moment, <code>nuc_object</code> , which is closely linked to the actin object
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*** The nucleator is either a sphere, a capsule (i.e.~a sphere with a cylindrical segment stuck in the middle) or ellipsoid
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*** <code>addnodes()</code>  adds harbingers to the surface of the nucleator.  The probablility of addition of nodes is normalized by surface area and is symmetric if <code>ASYMMETRIC_NUCLEATION</code>  is zero, or asymmetric if 1 or 2 (stepped or linear bias)
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*** <code>definenucleatorgrid()</code>  sets a list of gridpoints to check in case of nodes entering the nucleator.  Called once at the beginning.
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*** <code>iswithinnucleator()</code>  returns true if the node is within the nucleator
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*** <code>collision()</code>  moves a node out of the nucleator along a normal vector
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**  Nodes class
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*** Nodes exist only as members of the actin object
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*** <code>nodegrid</code>  is a 3 dimensional C++ vector of node pointers.  Each nodegrid entry starts a circularly linked list of nodes representing the nodes within that gridpoint voxel.
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*** The actin class contains a vector of nodes.  Each node has an associated <code>nodenum</code> , <code>x</code>  <code>y</code>  and <code>z</code>  position, <code>nextnode</code>  and <code>prevnode</code>  node pointers for the nodegrid linked list, <code>rep_force_vec[]</code> , <code>link_force_vec[]</code>  and <code>repulsion_displacement_vec[]</code>  as described above, the grid position of the node, <code>harbinger</code>  and <code>polymer</code>  flags and a <code>listoflinks</code>  i.e. a vector of link object which attach this node to other nodes.
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*** <code>polymerize()</code>  Creates a node as a harbinger.  Adds its pointer to the gridpoint linked list.
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*** <code>depolymerize()</code>  Removes a node, deletes all links and removes from grid.
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*** <code>setgridcoords()</code>  Calculates new grid co-ordinates based on x,y,z position
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*** <code>addtogrid()</code>  adds the node to the current gridpoint
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*** <code>removefromgrid()</code>  removes node from the grid
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*** <code>updategrid()</code>  checks to see if node has moved gridpoints, and updates grid is needs to
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*** <code>removelink()</code>  removes the specified node from the list of links
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** Links class
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*** Links exist only as members of the node objects
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*** Each link has an associated <code>linkednodeptr</code>  which points to the target node that the link is to and a <code>broken</code>  flag which is read by <code>actin::linkforces()</code>  and tells it to delete the link if it broke.
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*** <code>orig_dist</code>  and <code>orig_distsqr</code>  store the original distance of the link (and the square of that in a misguided attempt to avoid taking square roots.)
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*** <code>breakcount</code>  stores the number of consecutive iterations the link force has been above <code>LINK_BREAKAGE_FORCE</code>  and is used to increase the probability of breakage
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*** <code>getlinkforces()</code>  returns the force acting on the link.  Also sets the <code>broken</code>  flag and increments <code>breakcount</code>  if appropriate
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Latest revision as of 17:57, 26 April 2009

The flowchart below shows a detailed view of the how the program works.

Figure 2: Comet program flow (detailed)