Any help to solve this second-order inhomogeneous partial differential equation
$ \frac{1}{f(y)}~ \frac{d^2 f(y)}{dy^2} - b ~\frac{1}{k(t)}~ \frac{d^2 k(t)}{dt^2} - b B ~\frac{1}{k(t)}~ \frac{d k(t)}{dt } =0 $
Where b and B are constants.
Here is my trail:
I'm using the separation of variables method in Griffith’s book of electrodynamics, so I have assumed
$ \frac{1}{f(y)}~ \frac{d^2 f(y)}{dy^2} = c_1, ~~~~~ (1) $
$ b ~\frac{1}{k(t)}~ \frac{d^2 k(t)}{dt^2} + b B ~\frac{1}{k(t)}~ \frac{d k(t)}{dt } = c_2 ~~~~~ (2) $
With: $ ~~~~ c_1- c_2 = 0 $
Then (1) and (2) become
$ \frac{d^2 f(y)}{dy^2} = n^2 f(y) $
$ \frac{d^2 k(t)}{dt^2} + B \frac{d k(t)}{dt } = n^2 \frac{k(t)}{b}~~~~~~~ <-- ~ \text{is this correct?} $
The solution of (1) is:
$ f(y) = A e^{ny} + D e^{-ny} $
While (2) I have solved as in:
https://www.mathsisfun.com/calculus/differential-equations-second-order.html
And found that:
$ k= E e^{\frac{1}{2} (- B + \sqrt{B^2+ 4 \frac{n^2}{b} } ) t} + G e^{-\frac{1}{2} (B + \sqrt{B^2+ 4 \frac{n^2}{b} } ) t} $
From the initial conditions: $f(0)= 0$ and $k(t) =0$, one can find that : $E+ G= 0$ and $A+D =0$, but anyhow, I will choose $G=D =0.$
Please let me know if these results are right or not.