Sometimes by inspection one can guess the form of a particular solution. But this is not often the case. Most likely one have to solve the PDE thanks to the method of characteristics for example.
First equation :$$xu_x+yu_y= xy\sin(xy)\tag 1$$
The term on right side with $xy$ into it draw to look for a particular solution on the form
$$u=f(X)\quad\text{with}\quad X=xy$$
$u_x=yf'(X)\quad$ and $\quad u_y=xf'(X)$
$$xu_x+yu_y=2Xf'(X) =X\sin(X)$$
$$2f'(X)=\sin(X)$$
$$f(X)=-\frac12 \cos(X)$$
Doesn't mater the integration constant since we look for any one particular solution.
$$u=-\frac12 \cos(xy)\quad\text{is a particular solution}$$
The solution of the homogeneous PDE is $u=F\left(\frac{y}{x}\right)$ with arbitrary function $F$.
So, the general solution of the PDE $(1)$ is :
$$u(x,y)=F\left(\frac{y}{x}\right)-\frac12 \cos(xy)$$
Solving the PDE with the method of characteristics :
The Charpit-Lagrange system of characteristic ODEs is :
$$\frac{dx}{x}=\frac{dy}{y}=\frac{du}{xy\sin(xy)}$$
A first characteristic equation comes from solving $\frac{dx}{x}=\frac{dy}{y}$ :
$$\frac{y}{x}=c_1$$
A second characteristic equation comes from $\frac{dx}{x}=\frac{dy}{y}=\frac{ydx+xdy}{yx+xy}=\frac{d(xy)}{2xy}=\frac{du}{xy\sin(xy)}$
$$u+\frac12\cos(xy)=c_2$$
The general solution of the PDE expressed on implicit form $c_2=F(c_1)$ is :
$$u+\frac12\cos(xy)=F\left(\frac{y}{x}\right)$$
$$u(x,y)=F\left(\frac{y}{x}\right)-\frac12 \cos(xy)$$
Second equation :
$$2u_x+3u_y= 4x-9y^2\tag 2$$
By inspection. We try a particular solution with separated variables :
$$u=f(x)+g(y)$$
$u_x=f'(x)\quad$ and $\quad u_y=g'(y)$
$$2u_x+3u_y=2f'(x)+3g'(y)=4x-9y^2\quad\implies\quad f'(x)=2x\quad\text{and}\quad g'(y)=-3y^2$$
$$f(x)=x^2\quad\text{and}\quad g(y)=y^3$$
Doesn't mater the integration constant since we look for any one particular solution.
$$u=x^2-y^3\quad\text{is a particular solution}$$
The solution of the homogeneous PDE is $u=F\left(\frac{y}{3}-\frac{x}{2}\right)$ with arbitrary function $F$.
So, the general solution of the PDE $(2)$ is :
$$u(x,y)=F\left(\frac{y}{3}-\frac{x}{2}\right)+x^2-y^3$$
Solving the PDE with the method of characteristics :
The Charpit-Lagrange system of characteristic ODEs is :
$$\frac{dx}{2}=\frac{dy}{3}=\frac{du}{4x-9y^2}$$
A first characteristic equation comes from solving $\frac{dx}{2}=\frac{dy}{3}$ :
$$\frac{y}{3}-\frac{x}{2}=c_1$$
A second characteristic equation comes from $\frac{dx}{x}=\frac{dy}{y}=\frac{2xdx-3y^2dy}{2(2x)-3(3y^2)}=\frac{du}{4x-9y^2}$
$$u-x^2+y^3=c_2$$
The general solution of the PDE expressed on implicit form $c_2=F(c_1)$ is :
$$u-x^2+y^3=F\left(\frac{y}{3}-\frac{x}{2}\right)$$
$$u(x,y)=F\left(\frac{y}{3}-\frac{x}{2}\right)+x^2-y^3$$