Using the gradient operator
we may rewrite equation (1) as

This equation says that the directional derivative in the
(1, c) direction (in the
t, x-plane) is zero. So our solution
u(x, t) must be constant in this direction. In the
t, x-plane, the
(1, c) direction is along lines parallel to
x = ct, which are called the
characteristics of equation (1).

Now, fix a point on the x-axis, say (x0, 0). The line through this point parallel to x = ct
is given by x = x0 + ct. Since our solution is constant along this line, we must have
But from the initial data,

where f is known. So, for any (x, t),

Joan Remski, "The Transport Equation and Directional Derivatives - Solution of the Transport Equation," Convergence (August 2004)