Graduate → Differential Equations → Partial Differential Equations ↓
Method of Characteristics
The method of characteristics is a powerful technique used to solve certain types of partial differential equations (PDEs), particularly those that are first-order and linear or quasi-linear in nature. It simplifies the PDE into a set of ordinary differential equations (ODEs), which are often much easier to solve. This method is fundamental in fields such as fluid dynamics, wave propagation, and traffic flow analysis. The essence of the method is to transform the PDE into a system of ODEs with characteristic curves, which we solve to find a solution to the original equation.
To begin exploring the method of characteristics, let us first consider a basic first-order PDE in two variables, x and t:
a(x, t) u_x + b(x, t) u_t = c(x, t, u)
a(x, t) u_x + b(x, t) u_t = c(x, t, u)
This equation contains the partial derivatives of an unknown function u(x, t)
with respect to x
and t
. The idea is to find paths, called characteristics, along which the PDE reduces to a simpler form. These paths are the solutions of a system of ODEs derived from the PDE. Let's dig deeper.
Derivatives of characteristic curves
Looking at the PDE:
a(x, t) u_x + b(x, t) u_t = c(x, t, u)
a(x, t) u_x + b(x, t) u_t = c(x, t, u)
We assume that we can parameterize the variables and the unknown function (x, t, u)
with so-called characteristic curves. That is, we look for a parameter s
such that:
x = x(s), t = t(s), u = u(s)
x = x(s), t = t(s), u = u(s)
This parameterization allows the PDE to be transformed into an ODE. The partial derivatives are transformed as follows:
u_x = (du/ds) / (dx/ds), u_t = (du/ds) / (dt/ds)
u_x = (du/ds) / (dx/ds), u_t = (du/ds) / (dt/ds)
Substitute these expressions into our PDE:
a(x, t) (du/ds) / (dx/ds) + b(x, t) (du/ds) / (dt/ds) = c(x, t, u)
a(x, t) (du/ds) / (dx/ds) + b(x, t) (du/ds) / (dt/ds) = c(x, t, u)
To make the equation valid for any du/ds
other than zero, we must equate the terms relating the change in x
and t
with s
:
a(x, t) / (dx/ds) + b(x, t) / (dt/ds) = 0
a(x, t) / (dx/ds) + b(x, t) / (dt/ds) = 0
Rewriting achieves:
dx/ds = a(x, t) dt/ds = b(x, t) du/ds = c(x, t, u)
dx/ds = a(x, t) dt/ds = b(x, t) du/ds = c(x, t, u)
These are the characteristic equations. Solving these ODEs gives the characteristic of the PDE, which gives a path in the x-t plane along which the PDE becomes an ODE that can be easily solved.
Solving PDEs using characteristics
Consider the simple wave equation:
u_t + cu_x = 0
u_t + cu_x = 0
Here, c
is a constant indicating the wave speed. The characteristic equations are as follows:
dx/ds = c => x = cs + x_0 dt/ds = 1 => t = s + t_0 du/ds = 0 => u = constant
dx/ds = c => x = cs + x_0 dt/ds = 1 => t = s + t_0 du/ds = 0 => u = constant
These result in the following relationships:
x(t) = ct + C_1 u(x(t), t) = f(C_1)
x(t) = ct + C_1 u(x(t), t) = f(C_1)
Since C_1
is constant along a characteristic curve, it completes the solution, which shows that u(x, t) = f(x - ct)
is a combination of two traveling waves. Calculate these with initial or boundary conditions to find specific solutions.
A practical example
Let's take a more complex problem:
u_t + xu_x = x^2
u_t + xu_x = x^2
Here, we identify specific equations:
dx/ds = x => x = C_1 e^s dt/ds = 1 => t = s + C_2 du/ds = x^2 => integrate to find u
dx/ds = x => x = C_1 e^s dt/ds = 1 => t = s + C_2 du/ds = x^2 => integrate to find u
dx/ds = x
:
∫(1/x) dx = ∫ ds => ln(x) = s + ln(C_1) => x = C_1 e^s
∫(1/x) dx = ∫ ds => ln(x) = s + ln(C_1) => x = C_1 e^s
Similarly, t = s + C_2
, and upon integration du/ds = x^2
:
u = ∫(C_1^2 e^{2s}) ds = (C_1^2 / 2)e^{2s} + C_3
u = ∫(C_1^2 e^{2s}) ds = (C_1^2 / 2)e^{2s} + C_3
Express these relations with marginal conditions to conclude the solution. These applications highlight the effectiveness of the method in simplifying complex PDEs.
It shows how the analytical and graphical approaches of the method of characteristics beautifully combine to produce solution curves for systems developed in the realm of physics and engineering. This method is essential for solving and understanding deep non-trivial scenarios in wave dynamics and conservation laws.
Complex matters and conservation laws
In more advanced studies, properties are essential in solving conservation laws, especially in shock analysis and simple waves in fluid dynamics. Here is how this method addresses shock waves:
u_t + f(u)_x = 0
u_t + f(u)_x = 0
Using conservation laws under specific boundary conditions yields different downstream and upstream characteristic solutions, creating shocks where the characteristics converge, which represent changes in the gas dynamics such as density changes.
Different fields apply extensions of this method - the attribute mesh method, the attribute method with source words, etc. Each brings unique problem-solving approaches and efficiency to its domain.
Conclusion
The method of features is more than just a technique - it is a deep insight into how solutions evolve in a PDE context, simplifying complex phenomena into a manageable series of steps. Whether simple or multidimensional problems, this method aligns with other analytical techniques to provide clarity and insight.