?? ex5bvp.m
字號(hào):
function ex5bvp
%EX5BVP Example 5 of the BVP tutorial.
% Falkner-Skan BVPs are discussed in T. Cebeci and H.B. Keller,
% Shooting and parallel shooting methods for solving the Falkner-Skan
% boundary-layer equation, J. Comp. Phy., 7 (1971) 289-300. This is
% the positive wall shear case for which the parameter beta is known
% and the problem is to be solved for a range of the parameter. This
% is the hardest case of the table in the paper.
%
% The problem is posed on [0 infinity). As in the paper cited, the
% boundary condition at infinity is imposed at a finite point, here
% called 'infinity'. It is best to start with a relatively small value
% and increase it until consistent results are obtained. A value of 6
% appears to be satisfactory. Starting with a "large" value is tempting,
% but not a good tactic because the code will fail with the crude guess
% and default tolerances used here.
% 'infinity' is a variable to facilitate experimentation.
infinity = 6;
% The constant guess for the solution satisfies the boundary conditions.
solinit = bvpinit(linspace(0,infinity,5),[0 0 1]);
options = bvpset('stats','on');
sol = bvp4c(@ex5ode,@ex5bc,solinit,options);
eta = sol.x;
f = sol.y;
fprintf('\n');
fprintf('Cebeci & Keller report f''''(0) = 0.92768.\n')
fprintf('Value computed here is f''''(0) = %7.5f.\n',f(3,1))
figure
plot(eta,f(2,:));
axis([0 infinity 0 1.4]);
title('Falkner-Skan equation, positive wall shear, \beta = 0.5.')
xlabel('\eta')
ylabel('df/d\eta')
% --------------------------------------------------------------------------
function dfdeta = ex5ode(eta,f)
%EX5ODE ODE function for Example 5 of the BVP tutorial.
beta = 0.5;
dfdeta = [ f(2)
f(3)
-f(1)*f(3) - beta*(1 - f(2)^2) ];
% --------------------------------------------------------------------------
function res = ex5bc(f0,finf)
%EX5BC Boundary conditions for Example 5 of the BVP tutorial.
res = [f0(1)
f0(2)
finf(2) - 1];
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