The mathematical formulations of many problems in science and engineering reduce to study of first-order PDEs. The use of first-order PDEs was seen in gas flow problems, traffic flow problems, phenomenon of shock waves, the motion of wave fronts and quantum mechanics etc.. It is therefore essential to study the theory of first-order PDEs and the nature their solutions to analyze the related real-world problems.

We shall study first-order linear, quasi-linear and nonlinear PDEs and methods of solving these equations. An important method of characteristics is explained for these equations in which solving PDE reduces to solving an ODE system along a characteristics curve. Further, the Charpit’s method and the Jacobi’s method for nonlinear first-order PDEs are discussed.

A first order PDE in two independent variables and the dependent variable can be written in the form

For convenience, we set

Equation can be modified as

The equations of this type arise in many applications in geometry and physics. For

example, let us consider the following geometrical problem.

__Problem 1:__ Find all functions such that the tangent plane to the graph at any arbitrary point passes through the origin characterized by the PDE .

__Solution:__ The equation of the tangent plane to the graph at is

This plane passes through the origin and hence, we must have

For this equation to hold for all in the domain of must satisfy

which is a first-order PDE.

We classify the equation depending on the special forms of the function .

1) If equation is of the form

then it is called **linear first-order PDE**. Note that the function is linear in and with all coefficients depending on the independent variables and only.

2) If equation is of the form

then it is called **semi-linear** because it is linear in the leading (highest-order) terms . However, it need not be linear in . Note that the coefficients of are functions of the independent variables only.

3) If equation is of the form

then it is called **quasi-linear PDE**. Here the function is linear in the derivatives with the coefficients depending on the independent variables and as well as on the unknown .

Note: Linear and Semi-linear equations are special cases of Quasi-linear equations.

Any equation that does not fit into one of these forms is called **N****on-linear.**

Few examples are listed below

- (linear)
- (semilinear)
- (linear)
- (quasilinear)
- (nonlinear)

Recall the initial value problem for a first-order ODE which ask for a solution of the

equation that takes a given value at a given point of . The IVP for first-order PDE ask for a solution of which has given values on a curve in . The conditions to be satisfied in the case of IVP for first-order PDE are formulated in the classic problem of Cauchy which may be stated as follows:

Let be a given curve in described parametrically by the equations

;

where are in . Let be a given function in . The IVP or Cauchy’s problem for first-order PDE

is to find a function with the following properties:

- and its partial derivatives with respect to x and y are continuous in a region

Ω of containing the curve - is a solution of in Ω, i.e., in Ω
- On the curve ,

__Problem 2:__ Determine the solution the following IVP:

, ,

where is a given function and is a constant.

__Solution:__

To apply the method of characteristics, parameterize the initial curve as follows:

The family of characteristics curves are determined by solving the ODEs

The solution of the system is and .

Using initial conditions,

, .

we find that , , and hence

and .

To modify equation in the parametric form of the solution, we have and . Therefore, we find that .

Since , we obtain . Thus, the

parametric form of the solution of the problem is given by

, , .

To express and as and , we have . We now write the solution in the explicit form as .

Clearly, if is differentiable, the solution satisfies given PDE as well as the initial condition.

NOTE:

This problem characterizes unidirectional wave motion with velocity . If we consider the initial function to represent a waveform, the solution shows that a point for which constant, will always occupy the same position on the wave form. If , the entire initial wave form moves to the right without changing its shape with speed (if , the direction of motion is reversed).