Three different problem I got:
1.. $xu_x+2x^2u_y-u=x^2e^x$ and $u(x,x^2+x)=xe^x+x^2$
2.. $yu_{xx}+(x+y)u_{xy}+xu_{yy}=0, \quad x\neq y$
3.. $(y+xu)u_x+(x+yu)u_y=u^2-1$
Couldnt even start. Could you at least give me a hint? thanks.
edit1:
at 2. from $B^2-AC=\frac {(x-y)^2}4>0 $ so the equation is hyperbolic. so we can write its cononical forms. is it true?
edit2: for the first one :
by taking $\eta=x^2-y$ and $\xi=x$ I found $u(x,y)=xe^x+x(-x+1-e^{-x})$ for the second one :
I took $\xi=\frac{x^2-y^2}{2}$ and $\eta=x-y$ and found $u(x,y)=\frac {f^*(\frac{x^2-y^2}{2})}{x-y}+g(x-y)$
edit 3:----------------------
1-) $\frac ba=\frac {2x^2}{x}=2x=\frac {dy}{dx}$
$x^2-y=c$, $\eta =x^2-y$ and $\xi =x$
$u_x=w_{\xi}+w_{\eta}2x$ and $ u_y=-w_{\eta}$
$\xi(w_{\xi}+w_{\eta}2\xi)-2\xi ^2w_{\xi}-w=\xi^2e^\xi $
$w_{\xi}-\frac w \xi=e^\xi$ multiplying by $\frac 1\xi$
$\frac{d(w\frac 1\xi)}{d\xi}=e^\xi$
so we got $w=\xi e^\xi+g(\eta)$
$u(x,y)=xe^x+g(x^2-y)$
and $u(x,x^2+x)=xe^x+x^2 =xe^x+g(x^2-x^2-x)$
$g(-x)=x^2$, $g(x)=x^2$ so the $u(x,y)=xe^x+x^2$
//--------------------------------------------
3)$\frac {\frac{dx}{dt}}{y+ux}=\frac {\frac{dy}{dt}}{x+yu}=\frac {\frac{du}{dt}}{u^2-1}$
$\frac {\frac{dx}{dt}-\frac{dy}{dt}}{y+ux-x-yu}=\frac {\frac{du}{dt}}{u^2-1}$
$\frac {\frac{dx}{dt}-\frac{dy}{dt}}{(1-u)(y-x)}=\frac {\frac{du}{dt}}{u^2-1}$
$\frac {\frac{d(x-y)}{dt}}{y-x}=\frac {\frac{du}{dt}}{u+1}$
$ln(u+1)+ln(x-y)=c_1$------------------- (1) we got one independent solution we need another
$\frac {\frac{dx}{dt}+\frac{dy}{dt}}{y+ux+x+yu}=\frac {\frac{du}{dt}}{u^2-1}$
$\frac {\frac{dx}{dt}+\frac{dy}{dt}}{(1+u)(x+y)}=\frac {\frac{du}{dt}}{u^2-1}$
$\frac {\frac{d(x+y)}{dt}}{x+y}=\frac {\frac{du}{dt}}{u-1}$
$ln(u-1)-ln(x+y)=c_2$----------------------(2)
from (1) and (2) which form is $h(x,y,u)=c_1$ and $j(x,y,u)=c_2$
general solution would be in $j(x,y,u)=F(h(x,y,u))$ Where F is an arbitrary.
so $ln(u-1)-ln(x+y)=F(ln(u+1)+ln(x-y))$
Some hints:
First problem: 1st order linear PDE, use the method of characteristics and then apply the "boundary" condition. Edit: note that your solution doesn't satisfy nor the equation nor the "boundary condition". The characteristic equations are given by: $$ \frac{\mathrm{d} x}{x} = \frac{\mathrm{d} y}{2 x^2} = \frac{\mathrm{d} u}{u + x^2 e^x},$$ which from the first equality yields: $$ y - x^2 = \text{constant} \equiv \eta ,$$ which is the characteristic of the PDE. The remaining equation, which comes up from the equality of the first and third terms is a 1st order linear ODE for $u$ as a function of $x$: $$ \frac{\mathrm{d} u}{ \mathrm{d} x} = \frac{u}{x} + x e^x , $$ whose solution (use an integrating factor) is given by $u(x,y) = x \, ( e^x + C)$, being $C$ a constant of integration. Put $C = C(\eta(x,y))$ in order to get the complete solution.
Second problem: 2nd oder linear PDE, use the method of characteristics knowing that for $x - y \neq 0$ the equation is hyperbolic but parabolic when $x = y$ (I notice now that you are told $x \neq y$).
Cheers!