Consider a family of
exponential curves (y = Aex), where A is an arbitrary constant for
different values of A, we get different members of the family. Differentiating
the relation (y = Aex) w.r.t.x, we get dy/dx = Aex
Eliminating the arbitrary
constant between y = Aex and dy/dx = Aex, we get
dy/dx = y. This is the differential equation of the family of curves
represented by y = Aex
Thus, by eliminating one
arbitrary constant, a differential equation of first order is obtained.
Now consider the family of
curves given by y = A cos 2x + B sin 2x ... (1)
Where A and B are
arbitrary consists.
Differentiating (1) w.r.t,
x we get dy/ dx = - 2Asin 2x + 2Bcos 2x ... (2)
Differentiating (2) w.r.t.
x we get d²y/ dx² = - 4Acos ax - 4Bsin 2x ... (3)
Eliminating A and B from
equations (1) and (2) (3), we get
d²y/ dx² = - 4y ⇒ d²y/ dx² + 4y = 0
Here we note that by
eliminating two arbitrary consists, a differential equation of second order is
obtained.
Step
I: write the given equation involving
independent variable x (say), dependent variable y (say) and the arbitrary
constants.
Step
II: obtained the numbers of a
arbitrary constants in step in step I. let there be n arbitrary consists.
Step
III: differentiate the relation in step
in times with respect to x.
Step
IV: eliminate arbitrary constants with
the help of n equations involving differential coefficient obtained in step III
and an equation in step I.
The equation so obtained
is the desired differential equation.
Example: Show that the differential
equation that represented all parabolas having their axis symmetry coincident
with the axis of x is yy₂ + y₁² = 0.
Solution: The equation that represents a
family of parabolas having their axis of symmetry coincident with the axis of x
is y² = 4a(x - h) ... (1)
This equation contains two
arbitrary constants, so we shall differentiate twice to obtain second order
differential equation.
Differentiating (1) w.r.t
x we get
2y dy/dx = 4a ⇒ y dy/ dx = 2a ... (2)
Differentiating (2) w.r.t,
x we get
y d²y/ dx² + (dy/ dx)² = 0 ⇒ yy₂ + y₁² = 0
Which is the required
differential equation.
Example: Find the differential
equation of all non-horizontal lines in a plane.
Solution: The equation of the family of all
non-horizontal line in a plane is given by
Ax + by = 1 ... (1)
Where a, b are arbitrary
constants such that (a ≠ 0)
Differentiating (1)
w.r.t, x we get
a dx/dy + b = 0
Differentiating this w.r.t
y we get
ad²x/ dy² = 0
⇒ d²x/
dy² = 0
Hence, the differential
equation of all non-horizontal lines in a plane is d²x/ dy² = 0.
Example: Find the differential equation of
all non- vertical lines in a plane.
Solution: The general equation of all
non-vertical lines in a plane is (ax + by = 1) where (b ≠ 0).
Now,
ax + by = 1
a + b dy/dx =
0 [differentiating
w.r.t.x]
b d²y/ dx =
0 [differentiating
w.r.t.x]
d²y/ dx² = 0 [∵ b ≠ 0]
Hence, the differential
equation is d²y/ dx² = 0
Solution
of a differential equation: The solution of a differential
equation is a relation between the variable involved which satisfies the
differential equation. Such a relation and the derivates obtained therefore
when substituted in the differential equation, makes left hand right hand sides
identically equal.
General
solution: The solution which
contains as many as arbitrary constants as the order of the differential
equations is called the general solution of the differential equation.
For example, y = Acos x +
Bsin x is the general solutions one arbitrary constant.
Particular
solution: Solution obtained by
giving particular values to the arbitrary constant in the general solution of a
differential equation is called a particular solution.
Example: Show that xy = aex +
be- x + x² is a solution of the differential equation x
d²y/ dx² + 2 dy/dx - xy + x² - 2 = 0
Solution: We are given that xy =
aex + be- x + x² ... (1)
Differentiating w.r.t.x,
we get x dy/ dx + y = aex - be- x + 2x
Differentiating again
w.r.t.x, we get xd²y/ dx² + dy/dx + dy/dx = aex + be-
x + 2
xd²y/ dx² + 2dy/dx = aex +
be- x + 2 ... (2)
Now x d²y/ dx² + 2dy/dx -
xy + x2 - 2
= [aex + be- x + 2] - [aex + be- x + x²] + x² - 2
= 0 [using (1) and (2)]
Thus, (xy = aex + be- x + x²) is a solution of the given differential equation.