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-
-Please answer the following:
-
-1.  Name of conference
-
-2.  Type of Presentation
-	Contributed:  Lecture form    
-			  Poster form     
-	Minisymposium:    
-
-3.  Equipment for Visual Support
-	Lecture Form/Minisymposium:
-		Overhead Projector    
-		2" x 2" Slide Projector (35mm)    
-	Poster Form:
-		Easel     Poster Board    
-		Other (specify)           
-
-More sophisticated equipment can be provided, but you may be
-required to pay the rental fee.  For details, indicate your 
-requirements below:
-
-
-4.  If you are a speaker in a minisymposium, who is the organizer?
-
-5.  What is the minisymposium title?
-
-6.  If more than one author, who will present the paper?
-
-% This is a macro file for creating a SIAM Conference abstract in
-% LaTeX.
-%
-% If you have any questions regarding these macros contact:
-%           Lillian Hunt
-%           SIAM
-%           3600 University City Center Center
-%           Philadelphia, PA 19104-2688
-%           USA
-%           (215) 382-9800      
-%           e-mail:meetings@siam.org
-
-
-\hsize=25.5pc
-\vsize=50pc
-\textheight 50pc
-\textwidth 25.5pc
-\parskip 0pt
-\parindent 0pt
-\pagestyle{plain}
-
-\def\title#1{\bf{#1}\vspace{6pt}}
-\def\abstract#1{\rm {#1}\vspace{6pt}}
-\def\author#1{\rm {#1}\vfill\eject}
-
-% end of style file
-
-% This is ltexconf.tex. Use this file as an example file for doing an SIAM
-% Conference abstract in LaTeX.
-   
-
-\documentstyle[ltexconf]{report} 
-\begin{document}
- 
-\title{Numerical Analysis of a 1-Dimensional
-Immersed-Boundary\\ Method}
- 
-\abstract{We present the numerical analysis of a simplified,
-one-dimensional version  
-of Peskin's immersed boundary method, which has been used to
-solve 
-the two- and three-dimensional Navier-Stokes equations in the 
-presence of immersed boundaries. We consider the heat
-equation  
- in a finite domain with a moving source term.  
-We denote the solution as $u(x,t)$ and the location of the
-source 
- term as $X(t)$.  The source term is a moving delta function  
-whose strength is a function of u at the location of the
-delta function. 
-The p.d.e. is coupled to an ordinary differential equation
-whose  
-solution gives the location of the source term. 
- The o.d.e. is $X'(t) = u(X(t),t)$, which can be interpreted as 
-saying the source term moves at the local velocity.   
-The accuracy the numerical method of solution depends on how
-the  
-delta function is discretized when the delta function is not
-at 
-a grid point and on how the solution, u, is represented 
- at locations between grid points. We present results showing 
-the effect of different choices of spreading the source to
-the grid and 
-of restricting the solution to the source location. 
-The problem we analyze is also similar to the Stefan problem
-and 
-the immersed-boundary method has features in common with
-particle-in-cell 
- methods.}
-\author{\underbar{Richard P. Beyer, Jr.}\\
-University of Washington, Seattle, WA\\
-Randall J. LeVeque\\
-University of Washington, Seattle, WA}
-
-\end{document}
-
-% end of example file.
-
-
-
-Please furnish complete addresses all co-authors.
-
-PLEASE INDICATE WHAT CONFERENCE ABSTRACT IS FOR.