Entry McQueen:2000:TDC from siggraph2000.bib

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BibTeX entry

@Article{McQueen:2000:TDC,
  author =       "David M. McQueen and Charles S. Peskin",
  title =        "A three-dimensional computer model of the human heart
                 for studying cardiac fluid dynamics",
  journal =      j-COMP-GRAPHICS,
  volume =       "34",
  number =       "1",
  pages =        "56--60",
  month =        feb,
  year =         "2000",
  CODEN =        "CGRADI, CPGPBZ",
  DOI =          "https://doi.org/10.1145/604446.604453",
  ISSN =         "0097-8930",
  bibdate =      "Wed Oct 7 09:18:19 MDT 2009",
  bibsource =    "http://www.math.utah.edu/pub/tex/bib/siggraph2000.bib",
  abstract =     "In all areas of computational fluid dynamics (CFD),
                 proper treatment of the boundary conditions is
                 essential to computing fluid behavior correctly. In
                 many engineering problems, CFD is simplified by a
                 priori knowledge of the motion of the boundary. The
                 well-known parabolic velocity profile in
                 fully-developed flow of an incompressible Newtonian
                 fluid in a pipe of circular cross-section is easily
                 computed because the boundary (the pipe wall) is known
                 to be in a fixed location. Even in more complex
                 settings, such as flow around a ship's propeller, the
                 motion of the boundary (the propeller) can be specified
                 in advance.

                 By contrast, in most biological fluid dynamics problems
                 the boundaries are not rigid and their motions are the
                 result of forces imposed on them by the motion of the
                 surrounding fluid. The motion of the fluid, of course,
                 cannot be known without knowledge of the boundary
                 motion. The motion of the boundary and the motion of
                 the fluid form a coupled system; both motions must be
                 computed simultaneously, which makes biological CFD
                 difficult.\par

                 A particular problem of interest is the flow of blood
                 in the chambers of the human heart. The heart is an
                 organ whose muscular contractions pump blood around the
                 body. Simplifying somewhat, the heart consists of two
                 main pumping chambers that contract simultaneously. One
                 chamber, the left ventricle, accepts oxygen-enriched
                 blood from the lungs and pumps it to the body. The
                 other chamber, the right ventricle, accepts
                 oxygen-depleted blood from the body and pumps it to the
                 lungs. The inlet and outlet of each ventricle are
                 guarded by valves whose opening and closing guarantee
                 one-directional flow around the circulatory system.
                 There are a total of four valves. The valves generally
                 consist of two or three leaflets - membranes made of
                 very flexible but inextensible material. Familiar
                 examples of materials with this property would be paper
                 or fabric which can be easily bent or twisted but which
                 are not easily stretched. One edge of each valve
                 leaflet is securely attached to the wall of the heart,
                 but the other edge is free of attachment and can move
                 with the flow. Structures analogous to a valve leaflet
                 are a shirt pocket, with one edge (three sides of a
                 rectangular patch pocket) securely stitched to the
                 shirt and one edge free of attachment, or a flag, one
                 edge attached to the flag pole, the other edge free to
                 wave in the wind. When flow is passing through the
                 valve in the forward direction, the valve's leaflets
                 are positioned out of the way, permitting flow. When
                 flow attempts to pass in the reverse direction, the
                 leaflets come together, their free edges pressing
                 against the free edges of their neighbors to occlude
                 the flow passage.\par

                 The motion of the leaflets is not caused by muscles in
                 the valve. The outflow valves are entirely passive
                 structures with no muscular tissue whatsoever. Even in
                 the case of the inflow valves, whose free edges are
                 connected to the heart muscle by a sparse network of
                 tendons, the opening and closing motions result from an
                 interaction with the surrounding fluid. The forward
                 motion of the fluid pushes the leaflets aside out of
                 the main flow stream, but the inextensibilty of the
                 leaflet material prevents free motion of the fluid near
                 the leaflet, affecting the entire flow field. Reverse
                 motion of the fluid causes the leaflets to move back
                 into the flow passage where contact between neighboring
                 leaflets and the inextensibilty of the leaflet material
                 halts the flow. The highly interactive nature of the
                 fluid and leaflet motions makes this an especially
                 interesting and challenging CFD
                 problem.\par

                 Commercially available software packages intended for
                 engineering CFD are not equipped to handle this type of
                 dynamic interaction between boundary and fluid. We have
                 developed a numerical method (the 'Immersed Boundary
                 Method') which simultaneously computes the motion of a
                 fluid and the motion of an elastic boundary immersed
                 in, and interacting with, that fluid. In the Immersed
                 Boundary Method, the fluid is represented by Eulerian
                 velocities and pressures that are stored on a regular
                 three-dimensional computational lattice. The scale of
                 the heart chambers is such that blood can be treated as
                 a Newtonian fluid. Fluid dynamics is computed by
                 numerical solution of the Navier--Stokes equations,
                 including a body force. The boundary is represented by
                 elastic structures that are free to move continuously
                 in the space sampled by the computational lattice. The
                 essence of the method is to replace the elastic
                 boundary by the forces that result from its
                 deformations. These forces are applied to the lattice
                 in the neighborhood of the elastic boundary with the
                 aid of a numerical approximation to the Dirac delta
                 function. The fluid moves under the action of this body
                 force. The numerical delta function is then used again,
                 to interpolate the newly computed lattice velocities to
                 the locations of the boundary, and then the boundary is
                 moved at the interpolated velocity to a new location
                 (the no-slip condition). The process of computing
                 forces, then fluid motion and then new boundary
                 location is repeated cyclically in a time-stepping
                 procedure with a suitably chosen time step. The only
                 requirements for the method are the physical properties
                 of the fluid, the (possibly time-dependent) elastic
                 properties of the boundary, and the initial geometry of
                 the boundary. A complete description of the Immersed
                 Boundary Method can be found in [1, 2].",
  acknowledgement = ack-nhfb,
  fjournal =     "Computer Graphics",
  journal-URL =  "http://portal.acm.org/browse_dl.cfm?idx=J166",
}

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