Consider the partial differential equation:
$$\frac{\partial u}{\partial t}=\frac{\partial^2u}{\partial x^2} + a \frac{\partial u}{\partial x} + bu$$
for the function $u (x; t)$ where $a$ and $b$ are constants.
By using substitution of the form $u(x,t) = \exp(\alpha x+\beta t)v(x,t)$;
And suitable choice of constants alpha and beta, show that the PDE can be reduced to the heat equation
$$\frac{\partial v}{\partial t}=\frac{\partial^2v}{\partial x^2}.$$
you could compare the equations $$\beta v+ \frac{\partial v}{\partial t} \\=\alpha^2v+\frac{\partial^2 v}{\partial x^2}+2\alpha\frac{\partial v}{\partial x}+a\alpha v+a\frac{\partial v}{\partial x}+bv$$ and the old one and choose the constant that fits your request.