it's actually
(c + dz + ez^2)*T"(z) + a*T(z) + b = 0
T(z=0) = Ts
T'(z=Z) = 0
Don't let my explanation confuse you; forget the axial direction x for now; right now I'm solving a one dimensional ODE (radially only) with lots of constants, shown above.
I'm scared of the word "Bessel"...
Good questions.
I am investigating the properties of a sensor I am making, which involves the simultaneous interactions of convective heat transfer, joule heating, and potential theory. I am trying to build an analytic model that approximates all of these physics for simple geometries, namely a...
I simultaneously found the solution. The form is
T(x) = C1*cos(sqrt(a)*x) + C2*sin(sqrt(a)*x) - b/a
where C1 = Ts + b/a, C2 = C1*tan(sqrt(a)*L)
Your solution looks like it takes this form after some trig flexing.
Thanks!
pmsrw3, very close! Please see the following two plots:
The equation you gave models the homogenous boundary problem exactly, which is:
Txx + aT = -b, T(x=0) = Ts, T(x=L) = 0 (first plot)
What I need is the solution to the NON-homogenous boundary problem:
Txx + aT = -b, T(x=0) = Ts...
I've made a lot of simplifications to a Joule-heating problem I'm working on. I'm struggling to solve the following one-dimensional, one variable ODE:
Txx + aT = -b
with boundary conditions
T(x=0) = Ts (Dirichlet)
Tx(x=L) = 0 (Neumann)
I've learned that this is a non-homogeneous...