2. Classification of Linear Second Order
Partial Differential Equations
When we model the realistic phenomena, we always
have nonlinear partial differential equations that are
not, in principle, solvable.
For the solution of these equations numerically, we use
finite difference methods and test these schemes for
the standard PDEs.
We develop finite difference schemes to parabolic,
hyperbolic and elliptic equations.
3. It is well known that the differential equations that can be solved by explicit
analytical formulae are very few. Therefore accurate numerical approximation
schemes are essential for extracting quantitative information as well as
qualitative understanding of the various behaviours of their solutions.
The process includes:
Replacing differential equations by suitable
finite differences
Applying boundary conditions
Converting into system of equations
Solutions of the algebraic equations
Analysis of the solution numerically.
4. The general second order linear PDE has the following form:
where the coefficients and the free term are in general functions
of the independent variables but do not depend on the unknown
function .
The classification of second order equations depends
on the form of the leading part of the equations consisting of the
second order terms.
The type of the above equation depends on the sign of the
quantity which is called the discriminant of .
5. The classification of second order linear
PDEs is given by the following.
Elliptic equation if
Parabolic equation if
Hyperbolic equation if
7. The simplest examples of the above
equations are the following:
Elliptic equation : (Two dimensional Laplace equation)
Parabolic equation : (One dimensional heat equation)
Hyperbolic equation : (One dimensional wave equation)
8. HEAT EQUATION
The heat equation is an important partial differential
equation which describes the distribution of heat (or
variation in temperature) in a given region over time.
9. WAVE EQUATION
The wave equation is one of the most important equations
in mechanics. It describes not only the movement of strings
and wires, but also the movement of fluid surfaces, e.g.,
water waves.
10. LAPLACE EQUATION
The Laplace equations are used to describe the steady-state
conduction heat transfer without any heat sources or sinks.
Laplace equations can be used to determine the potential at any
point between two surfaces when the potential of both surfaces is
known.
Now let us have a look at the different forms of Laplace equation
examples in Physics.
, the Laplace equation electrostatics defined for electric
potential .
If then, the Laplace equation in gravitational field.
is the velocity of the steady flow.