diff options
Diffstat (limited to 'Master/texmf-dist/source/latex/siam/ptexconf.all')
-rw-r--r-- | Master/texmf-dist/source/latex/siam/ptexconf.all | 102 |
1 files changed, 0 insertions, 102 deletions
diff --git a/Master/texmf-dist/source/latex/siam/ptexconf.all b/Master/texmf-dist/source/latex/siam/ptexconf.all deleted file mode 100644 index 06e2a7f38ae..00000000000 --- a/Master/texmf-dist/source/latex/siam/ptexconf.all +++ /dev/null @@ -1,102 +0,0 @@ - -Please answer the following: - -1. Name of conference -2. Type of Presentation - Contributed: Lecture form or Poster form - Minisymposium: - -3. Equipment for Visual Support - Lecture form/Minisymposium: Overhead Projector or - 2" x 2" Slide Projector (35mm) - - Poster form: Easel or Poster Board - -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 -% Plain Tex. -% -% 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 -\parskip=3pt -\parindent=0pt -\overfullrule=0pt -\nopagenumbers - -\def\title#1\\{\bf{#1}\vskip6pt} -\def\abstract#1\\{\rm {#1}} -\def\author#1\\{\vskip6pt\rm {#1}\vfill\eject} -\def\eol{\hfill\break} - -% end of style file - -% This is ptexconf.tex. Use this file as an example of a SIAM -% Conference abstract in plain TeX. - -\input ptexconf.sty - -\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.}\eol -University of Washington, Seattle, WA\eol -%\vskip3pt -Randall J. LeVeque\eol -University of Washington, Seattle, WA\\ -\bye - -% end of example file - - -Please furnish complete addresses for all co-authors. - - -PLEASE BE SURE TO INDICATE WHAT CONFERENCE THE ABSTRACT IS FOR.
\ No newline at end of file |