Solve $$\begin{cases} u_{t}-u_{xx}=\frac{1}{2}xt \ \ &\text{for} \ \ 0\lt x\lt \pi, t\gt0\\ u(0,t)=u(\pi,t)=0 \ \ \\ u(x,0) = \sin x \ \ \\ \end{cases}$$
How to transform it to the normal case?
Solve $$\begin{cases} u_{t}-u_{xx}=\frac{1}{2}xt \ \ &\text{for} \ \ 0\lt x\lt \pi, t\gt0\\ u(0,t)=u(\pi,t)=0 \ \ \\ u(x,0) = \sin x \ \ \\ \end{cases}$$
How to transform it to the normal case?
Try to find a solution of the form
$$ u(x,t) = \sum_n T_n(t)X_n(x) $$
where
\begin{cases} X'' = -\lambda^2 X \\ X(0) = X(\pi) = 0 \end{cases}
You'll get
$$ u(x,t) = \sum_{n=1}^\infty T_n(t)\sin(nx) $$
and the PDE becomes
$$ \sum_{n=1}^\infty\big[T_n'(t) + n^2T_n(t)\big]\sin(nx) = \frac12 tx $$
Decompose the RHS into the corresponding Fourier series
$$ \frac12 tx = \sum_{n=1}^\infty a_n(t) \sin(nx) $$
You'll get a family of IVPs
\begin{cases} T_n''(t) + n^2 T_n(t) = a_n(t) \\ T_1(0) = 1 \\ T_{n>1}(0) = 0 \end{cases}