Solving Heat equation using pdepe does not give credible results

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Hello,
I am using pdepe to solve an heat equation, (the end goal being to simulate a fiber splicer and get the power input necessary). To create the interaction fiber to air (air heated by the graphite filament) I considered the following equation for my fiber (m=1, cylinder) :
function[c,f,s]=pdefun(x,t,u,DuDx)
ro=123.218;
C=281;
lambda=1.7;
alpha=ro*C/lambda;
c=alpha;
f=DuDx;
s=0;
end
And the boundary conditions to get heat from air to the fiber are :
function[pl,ql,pr,qr]=bcfun(xl,ul,xr,ur,t)
h=25;
R=2;
k=5;
Ts=300;%%fiber
Tf=350;%%air
pl=0;
ql=1;
pr=(h/k)*(Ts-Tf);
qr=1;
end
The initial conditions of the fiber being
function u0=icfun(x)
u0=300;
end
My problem is that when used at my fiber dimensions (270µm of diameter), I get a fiber temperature rising above the air temperature. I guess I forgot a term leading to stabilization of my sytem?
m=1;
xmesh=linspace(0,270E-6,270);
tspan=linspace(0,2,50);
sol=pdepe(m,@pdefun,@icfun,@bcfun,xmesh,tspan);
u=sol(:,:,1);
figure();
surf(xmesh,tspan,u);
The lack of visible variations on the x axe is only because of the size of my fiber (when I change xmesh I get the expected x variations).
I also get the same problem when I add a pvol term (s~=0 for pdepe model equation). Leading to absurdly low amount of power needed for the filament to generate high temperature (Code below).
%% m=0 because I chose to unroll it
function[c,f,s]=pdefunfilament(x,t,u,DuDx)%%equation for the filament
global PowerFil
ro=2.3E3;
C=720;
lambda=120;
alpha=ro*C/lambda;
c=alpha;
f=DuDx;
s=PowerFil/9E-9;%%(R*I^2)/dtau (dtau volume)
end
function u0=icfunfilament(x)%%initial conditions
u0=300;
end
function[pl,ql,pr,qr]=bcfunfilament(xl,ul,xr,ur,t)%%boundary conditions
pl=0;
ql=1;
pr=0;
qr=1;
end
For this kind of code I get results like this :
Does anyone has an idea of where my pdepe model did go wrong?
  2 个评论
Walter Roberson
Walter Roberson 2022-11-2
编辑:Walter Roberson 2022-11-2
Pure black output from surf() typically means that edges are dense enough that they have taken over the display (since they are constant screen width no matter what magnification being used.)
m=1;
xmesh=linspace(0,270E-6,270);
tspan=linspace(0,2,50);
sol=pdepe(m,@pdefun,@icfun,@bcfun,xmesh,tspan);
u=sol(:,:,1);
figure();
surf(xmesh,tspan,u, 'edgecolor', 'none');
colorbar()
min(u(:)), max(u(:))
ans = 300
ans = 481.8633
function[c,f,s]=pdefun(x,t,u,DuDx)
ro=123.218;
C=281;
lambda=1.7;
alpha=ro*C/lambda;
c=alpha;
f=DuDx;
s=0;
end
function[pl,ql,pr,qr]=bcfun(xl,ul,xr,ur,t)
h=25;
R=2;
k=5;
Ts=300;%%fiber
Tf=350;%%air
pl=0;
ql=1;
pr=(h/k)*(Ts-Tf);
qr=1;
end
function u0=icfun(x)
u0=300;
end
Hugo
Hugo 2022-11-2
编辑:Hugo 2022-11-2
Thank you for your answer,
I get the part for the black surf, what I don't get is why I obtain temperature values above the temperature of the air which is heating the fiber by conducto-convection. That is impossible when considering thermodynamic.
Even if the time span I gave my algorithm is too wide in front of the system size, the temperatures should reach stable values after a certain time. Here they should never go beyond 350 K (because there is no other flux involved).

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采纳的回答

Torsten
Torsten 2022-11-2
编辑:Torsten 2022-11-2
m=1;
xmesh=linspace(0,270E-6,270);
tspan=linspace(0,2,50);
sol=pdepe(m,@pdefun,@icfun,@bcfun,xmesh,tspan);
u=sol(:,:,1);
figure();
surf(xmesh,tspan,u, 'edgecolor', 'none');
function[c,f,s]=pdefun(x,t,u,DuDx)
rho = 123.218;
cp = 281;
lambda = 1.7;
c = rho*cp;
f = lambda*DuDx;
s = 0;
end
function [pl,ql,pr,qr] = bcfun(xl,ul,xr,ur,t)
alpha = 5;
Tf = 350;%%air
pl = 0;
ql = 1;
pr = alpha*(ur-Tf);
qr = 1;
end
function u0=icfun(x)
u0 = 300;
end
  4 个评论
Hugo
Hugo 2022-11-3
Yes sorry about that k==lambda in my case, I picked up formulas from different books and forgot to change the name of my variables.
Torsten
Torsten 2022-11-3
But you defined k = 5 and lambda = 1.7 ...
But you know now about the boundary condition setup.

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