Homogeneous differential equation explained

A differential equation can be homogeneous in either of two respects.

A first order differential equation is said to be homogeneous if it may be written

f(x,y)dy=g(x,y)dx,

where and are homogeneous functions of the same degree of and .[1] In this case, the change of variable leads to an equation of the form
dx
x

=h(u)du,

which is easy to solve by integration of the two members.

Otherwise, a differential equation is homogeneous if it is a homogeneous function of the unknown function and its derivatives. In the case of linear differential equations, this means that there are no constant terms. The solutions of any linear ordinary differential equation of any order may be deduced by integration from the solution of the homogeneous equation obtained by removing the constant term.

History

The term homogeneous was first applied to differential equations by Johann Bernoulli in section 9 of his 1726 article De integraionibus aequationum differentialium (On the integration of differential equations).[2]

Homogeneous first-order differential equations

A first-order ordinary differential equation in the form:

M(x,y)dx+N(x,y)dy=0

is a homogeneous type if both functions and are homogeneous functions of the same degree . That is, multiplying each variable by a parameter, we find

M(λx,λy)=λnM(x,y)andN(λx,λy)=λnN(x,y).

Thus,

M(λx,λy)
N(λx,λy)

=

M(x,y)
N(x,y)

.

Solution method

In the quotient \frac = \frac, we can let to simplify this quotient to a function of the single variable :

M(x,y)
N(x,y)

=

M(tx,ty)
N(tx,ty)

=

M(1,y/x)
N(1,y/x)

=f(y/x).

That is
dy
dx

=-f(y/x).

Introduce the change of variables ; differentiate using the product rule:

dy=
dx
d(ux)
dx

=x

du
dx

+u

dx
dx

=x

du
dx

+u.

This transforms the original differential equation into the separable form

xdu
dx

=-f(u)-u,

or
1xdx
du
=
-1
f(u)+u

,

which can now be integrated directly: equals the antiderivative of the right-hand side (see ordinary differential equation).

Special case

A first order differential equation of the form (are all constants)

\left(ax+by+c\right)dx+\left(ex+fy+g\right)dy=0

where can be transformed into a homogeneous type by a linear transformation of both variables (and are constants):

t=x+\alpha;  z=y+\beta.

Homogeneous linear differential equations

See also: Linear differential equation. A linear differential equation is homogeneous if it is a homogeneous linear equation in the unknown function and its derivatives. It follows that, if is a solution, so is, for any (non-zero) constant . In order for this condition to hold, each nonzero term of the linear differential equation must depend on the unknown function or any derivative of it. A linear differential equation that fails this condition is called inhomogeneous.

A linear differential equation can be represented as a linear operator acting on where is usually the independent variable and is the dependent variable. Therefore, the general form of a linear homogeneous differential equation is

L(y)=0

where is a differential operator, a sum of derivatives (defining the "0th derivative" as the original, non-differentiated function), each multiplied by a function of :

L=

n
\sum
i=0
f
i(x)di
dxi

,

where may be constants, but not all may be zero.

For example, the following linear differential equation is homogeneous:

\sin(x)

d2y
dx2

+4

dy
dx

+y=0,

whereas the following two are inhomogeneous:

2x2

d2y
dx2

+4x

dy
dx

+y=\cos(x);

2x2

d2y
dx2

-3x

dy
dx

+y=2.

The existence of a constant term is a sufficient condition for an equation to be inhomogeneous, as in the above example.

See also

References

External links

Notes and References

  1. Book: Dennis G. Zill. A First Course in Differential Equations with Modeling Applications. 15 March 2012. Cengage Learning. 978-1-285-40110-2.
  2. June 1726 . De integraionibus aequationum differentialium . Commentarii Academiae Scientiarum Imperialis Petropolitanae . 1. 167–184.