I have a finite square well like the one on the picture below:
I have done some calculations on it and got a transcendental equation for even solutions which is like this:
$$ \boxed{\dfrac{\mathcal{K}}{\mathcal{L}} = \tan \left(\mathcal{L \dfrac{d}{2}}\right)} $$
where:
\begin{align} &\mathcal{K}\equiv \sqrt{\frac{2m (W - W_p)}{\hbar^2}} &&\mathcal{L} \equiv \sqrt{\frac{2mW}{\hbar^2}} \end{align}
I have been looking in Griffith's book where he says that transcendental equation can be solved graphically so i did try to write it down so i could draw it (i inserted $\mathcal K$ and $\mathcal L$):
$$ \sqrt{1 - \dfrac{W_p}{W}} = \tan\left( \frac{\sqrt{2mW}}{\hbar} \frac{d}{2} \right) $$
I noticed that i don't even know what am i looking for. Is it the total energy $W$? If so i must know potential $W_p$ outside the well, width $d$, and a mass of a particle $m$. But still how could i graphically solve this?
EDIT:
I set all the constants to be $W_p=d=m=\hbar=1$ and ploted a graph for an even solutions:
I allso plotted a graph for the odd solutions which for which transcendental equation is ($\mathcal K$ and $\mathcal L$ stay the same as before):
$$ \boxed{-\dfrac{\mathcal{L}}{\mathcal{k}} = \tan \left(\mathcal{L \dfrac{d}{2}}\right)} $$
$$ -\sqrt{\frac{1}{1 - W_p/W}} = \tan\left( \frac{\sqrt{2mW}}{\hbar} \frac{d}{2} \right) $$
Could anyone please confirm that i got the right graph for transcendental equation?