Assume that $U(\rho,z)$ and $V(\rho,z)$ functions are given.
We have the system of equations for these functions in the form
$$
\frac{\partial^2 U}{\partial\rho^2}+\frac{1}{\rho}\frac{\partial U}{\partial\rho}+\frac{\partial^2 U}{\partial z^2} = 0 \ ,
$$
and
$$
\frac{\partial V}{\partial\rho} = \rho\left[\left(\frac{\partial U}{\partial\rho}\right)^2+\left(\frac{\partial U}{\partial z}\right)^2 \right]\ ,
\qquad \frac{\partial V}{\partial z} = 2\rho\frac{\partial U}{\partial\rho}\frac{\partial U}{\partial z}\ ,
$$
Can we use separation of the variable in the first equation?
How about in the second and the third equations?
How can solve these system of differential equation?
76 Views Asked by Bumbble Comm https://math.techqa.club/user/bumbble-comm/detail AtThere are 2 best solutions below
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Snifkes, Thank you very much for your solution. Actually, I have solved this problem in the prolate coordinates, $$ \rho=\sqrt{(x^2-1)(1-y^2)} \ , z=xy $$ and we get $$ \left[\left(x^2-1\right)U_x\right]_x + \left[\left(1-y^2\right)U_y\right]_y=0 \ , $$ $$ V_x = \frac{1-y^2}{x^2-y^2}\left[x(x^2-1)U_x^2-x(1-y^2)U_y^2 -2y(x^2-1)U_xU_y\right] \ , $$ $$ V_y = \frac{x^2-1}{x^2-y^2}\left[y(x^2-1)U_x^2-y(1-y^2)U_y^2 +2x(1-y^2)U_xU_y\right] \ , $$
Solution of the first equation is $$ U(x,y)=\sum_{n=0}^{\infty}(a_n P_n(x)+b_n Q_n(x))(c_n P_n(x)+d_n Q_n(x)) $$ But my question was different: You are making separation of variable in the function $U(\rho,z)$, finally it depend on $\lambda$ which is separation constant and you need to sum over lambda like: $U= \sum_{\lambda} R_{\lambda}(\rho)Z_{\lambda}(z)$ - which is correct, but other two equations are not linear. As far as I know it is impossible to use summation over with separation constant for non linear equations. What do you think about it?
I will start the solution problem over here to show you exactly what I mean. The super-position principle, as you mentioned exists in linear systems. Hence, for the first part:
$ \frac{\partial^2 U}{\partial \rho^2}+\frac{ 1}{ \rho}\frac{\partial U}{\partial \rho}+\frac{\partial^2 U}{\partial z^2} = 0 $
with $U = R(\rho)Z(z)$
we get:
$ R''+(1/\rho) R' = -\lambda^2 R$
$ R = a_1 Y_0(\lambda \rho) + a_2 J_0(\lambda \rho) $
Here, $J_0$ and $Y_0$ are Bessel functions of the first and second kind, respectively.
$ Z'' = -\lambda^2 Z$
$ Z = b_1 \sin(\lambda z)+b_2 \cos(\lambda z)$
Next, as I tried to mention, $V$ depends only on $U$. There is no need of anything like the superposition principle:
$ \frac{\partial V}{\partial z} = 2\rho R'Z'(RZ)$
$ V = 2\rho R'R\big(\int Z'Z\partial z\big) +f(\rho) = \rho R'RZ^2 +f(\rho)$
$ \frac{\partial V}{\partial \rho} = \rho R''RZ^2 + R'RZ^2 + \rho (R')^2 Z^2 +f'(\rho)$
We also have: $ \frac{\partial V}{\partial \rho} = \rho ((R')^2Z^2+R^2(Z')^2)$
Then you can use the quantities $a_1,a_2,b_1,b_2,\lambda$ and $f(\rho)$ to make sense of the equality:
$\rho R''RZ^2 + R'RZ^2 + \rho (R')^2 Z^2 +f'(\rho) = \rho ((R')^2Z^2+R^2(Z')^2)$
$\rho (-R'/\rho -\lambda^2 R)RZ^2 + R'RZ^2 + \rho (R')^2 Z^2 +f'(\rho) = \rho ((R')^2Z^2+R^2(Z')^2)$
$ f'(\rho) = \rho R^2(\lambda^2 Z^2+(Z')^2)$
Probably you should check again, but I believe that $ (\lambda^2 Z^2+(Z')^2) $ is always constant (i.e. it does not depend on $z$). Therefore, you will get:
$ f'(\rho) = \rho R^2(\text{some constant in }b_1,b_2,\lambda)$
and you can solve for $V$