A Partial Differential Equation is a Differential Equation which has more than one independent variable: $u(x,y), u(t,x,y), …$
For instance:
\begin{equation} \pdv{U}{t} = \alpha \pdv[2]{U}{x} \end{equation}
Key Intuition
- PDEs may have no solutions (unlike Uniqueness and Existance for ODEs)
- yet, usually, there are too many solutions—so… how do you describe all solutions?
- usually, there are no explicit formulas
Laplacian of \(u(x,y)\)
Examples
Heat Equation
See Heat Equation
Wave Equation
see Wave Equation
Transport Equation
\begin{equation} \pdv{u}{t} = \pdv{u}{x} \end{equation}
generally any \(u = w(x+t)\) should solve this
Schrodinger Equation
We have some:
\begin{equation} u(x,t) \end{equation}
and its a complex-valued function:
\begin{equation} i \pdv{u}{t} = \pdv[2]{u}{x} \end{equation}
which results in a superposition in linear equations
Nonlinear Example
\begin{equation} \pdv{u}{t} = \pdv[2]{u}{x} + u(1-u) \end{equation}
this is a PDE variant of the logistic equation: this is non-linear
Monge-Ampere Equations
\begin{equation} u(x,y) \end{equation}
Hessian
\begin{equation} Hess(u) = \mqty(\pdv[2]{u}{x} & \frac{\partial^{2} u}{\partial x \partial y} \\ \frac{\partial^{2} u}{\partial x \partial y} & \pdv[2]{u}{y}) \end{equation}
If we take its determinant, we obtain:
\begin{equation} \pdv[2]{u}{x} \pdv[2]{u}{y} - \qty(\frac{\partial^{2} u}{\partial x \partial y})^{2} \end{equation}
Traveling Wave
For two-variable PDEs, it is called a Traveling Wave if solutions to \(u\) takes on the form:
\begin{equation} u(t,x) = w(x-ct) \end{equation}
for some constant \(c\), and where \(w(x)\) is a function which depends on only one of the two variables.
Bell Curves
See also Bell Curves