Differential equations describe many different physical systems, ranging form gravitation to fluid mechanics. They are difficult to study, they usually have individual equation, which needs to be analyzed as a separate problem.
A fundamental question for any PDE is the existence and uniqueness of a solution for given boundary conditions. For nonlinear equations these questions are in general hard to answer.
The equation describing the heat equation problem is
$$ k\frac{\partial^2 u}{\partial x^2} = \frac{\partial u}{\partial t},\hskip2em k\gt 0. $$So here is the equation describing the problem and the problem is defined also by its boundary and initial values or conditions. For example
Laplace's equation is useful for solving many physical problems such as electrostatic, gravitational or velocity in fluid mechanics. It can be also interpreted as a steady state temperature distribution. Laplace's equation in two and three dimensions is abbreviated as
$$ \begin{align} &\nabla^2 u = 0,\hskip2em &\text{where} \nonumber \\ &\nabla^2u = \frac{\partial^2 u}{\partial x^2} + \frac{\partial^2 u}{\partial y^2} \hskip2em &\text{(for 2D)}.\nonumber \end{align} $$