Implicit Functions:
Derivatives, Graphing, and Orthogonal Trajectories
Functions are often defined implicitly, G(x,y,c) = 0, where c is a parameter.� In the case that c can be solved for explicitly we have F(x,y) = c, which is the form we will be dealing with in this module.� For instance
can be rewritten as��
, an example we discuss later.
Implicit differentiation can be accomplished by differentiating the equation while treating y as a differentiable function of x� and applying the chain rule,.� If
�giving
, which can be readily solved for y�(x):
.� Our first example
will allow you to enter an implicit function, view its derivative and also
specify the number of contours to be graphed.
Orthogonal trajectories to a given family of curves is based
on the simple idea that perpendicular lines have slopes that are negative
reciprocals of each other.� Starting with
a family of curves one can implicitly differentiate, obtain the derivative,
take its negative reciprocal, and integrate, if possible, to obtain the
orthogonal family. One can easily verify this procedure by starting with �leading to the
orthogonal trajectory equation
.�
There is also a multivariable approach using the gradient
concept. The surface z = F(x,y)
contains the level curves F(x,y) = Const
and the gradient vector, �is perpendicular to
them.� Since (dx, dy) is tangent to these level curves we obtain the differential
equation of the level curves from the scalar product�
��with
, which can be viewed as an alternative formula for finding
implicit derivatives.� The differential
equation of the orthogonal trajectories is obtained by taking the negative
reciprocal of the right hand side, namely�
.� Written as
�this will be readily
integrable if it passes the exactness test which occurs if and only if F(x,y)
is a harmonic function; i.e., it satisfies
.� We also note that
the Cauchy-Riemann condition for analytic functions implies that the real and
imaginary part of an analytic function gives rise to orthogonal curves.� A particular application relates to
two-dimensional flow of an irrotational and incompressible fluid. A specific
example is the flow around an inside corner. If �
, the streamlines of the flow arise from the Im(f(z)) and the
velocity potential from Re(f(z)). In this case the application relates to the
curves in the first quadrant.
�