I’ve been attempting to find a solution to the following differential equation but to no avail $$2q^{2}h\frac{d^{2} C}{d q^{2}}-h(1+2(v+1)q)\frac{d C}{d q}=\ln (C) - \ln{(h\exp({2h(v+1)}))}$$
Subject to the boundary condition $$C(0)=\frac{\exp(2h(1+v))-1}{2(v+1)}$$
Is it possible to find a closed form solution for this equation?
Does anyone know a reference to a paper discussing ODEs of the form $f’’(x)+f’(x)+\ln(f(x))=0$ ?
Thanks, J
This is not an answer, but I hope this might be useful.
I consider the asymptotic case $q \gg 1$, which greatly simplifies the equation. In fact, I have obtained a canonical form of the general Abel equation, which is a well known nonlinear ODE.
I don't use the (single?) boundary condition so far, but it may hint at another way to solve the problem.
$\mathbf{1)}$ We write the equation in a simplified form by introducing a function:
$$f(C)=\frac{1}{2h} \ln \left( \frac{C}{h} \right)-(v+1)$$
Dividing the equation by $2h$ we obtain:
$$q^2 C''-\left( \frac{1}{2}+(v+1)q \right)C'-f(C)=0 \tag{1}$$
Now, as I said, we consider the case $q \gg 1$ which allows us to get rid of $\frac{1}{2}$ inside the bracket. The simplified equation reads:
$\mathbf{2)}$ Now we will consider the inverse function $q(C)$ instead, such that:
$$C'=\frac{1}{q'}, \qquad C''=-\frac{q''}{q'^3}$$
After substitution the equation reads:
$\mathbf{3)}$ Now we will introduce a new function:
$$q(C)=e^{s(C)}, \qquad q'=s'e^{s}, \qquad q''=(s''+s'^2)e^{s}$$
After substitution and simplifications the equation becomes:
Introducing another function:
$$s'=p$$
We can write:
$\mathbf{4)}$ Introducing another function:
$$p=\frac{1}{w}, \qquad p'=-\frac{w'}{w^2}$$
We obtain the equation:
And after changing the variable:
$$x=(v+2) C, \qquad g(x)=\frac{f(C)}{v+2}$$
We finally have the canonical form of Abel equation linked at the top of the post:
Where:
$$g(x)=\frac{1}{2h(v+2)} \ln \left( \frac{x}{h(v+2)} \right)-\frac{v+1}{v+2}$$
Or we can rewrite it as:
$$g(x)= a \ln x-b$$
Unfortunately, I haven't found the solution to this equation neither in the linked file, nor in Mathematica.
Quite another idea (still not sure what it leads to):
$$4h q C''+2h q^2 C'''-2h(v+1) C'-h(1+2(v+1) q) C''-\frac{C'}{C}=0$$
Simplifying, we obtain:
If I have any more ideas, I will update this post.