First order homogenous D.E
In first order H.D.E all the terms are of the same dimension
Consider the table about dimensions
Term | X | x2 | 1/x | xn | 3 | y | yn | x2/y | x2y |
Dimension | 1 | 2 | -1 | n | O | 1 | N | 1 | 3 |
|
dy/dx | dy2/dx2 | xdy/dx | yx | |||||
0 | 1 | 2 |
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O shows there is no effect on the term
Which of the following equation are first order homogeneous
a) x2 = y2
b) xy = x2 + y2
c) x2
= 1 + xy
d) (x2
=
e) (x2 – y2) = 2xy
f) (1 + y2) = x
Solution of 1st order Homogeneous differential equation
1st order homogeneous d.e can be written in the form = Q
Where both P and Q are function of and have same dimension.
Suppose p and Q hence the dimension
Then divide by xn and use the substitution
Y = vx = v =
i.e
Example 1.
Solve =
Solution
Since all terms are of degree 2, i.e the equation is homogeneous
Let y = vx
= v +
And
=
= (
)
=
V + =
=
– v
=
=
=
=
dx
= lnx + c
But v =
2 = ln x + c
= lnx + c
Y2 = 2x2 (lnx + c)
Example 2
Solve xy = x2 + y2
Solution
All terms are of the order 2
xy = x2 + y2……
Let y = vx
= v +
From the equation…
=
+
But y = vx
= =
+
= x2
=
V + =
=
=
=
=
= lnx + A
But v =
2 = lnx + A
Y2 = 2x2 (lnx + A)
Example 3
Solve the following
(x2 + xy) = xy – y2
Solution
Let y = vx
= v +
And
=
=
v + =
=
-v
=
=
=
[(
dv +
dv)] =
–½ ( + ln v) = lnx + c
= ln (x2 V) + 2c
But v =
= ln (x2
) + 2c
– 2c = ln (x2.
)
Let ln A = -2c
+ ln A = ln xy
Xy = Aex/y
EXERCISE
Solve the differential equation
1. x2 = y (x + y)
2. (x2 + y2) = xy
First order exact differential equation
We know that
Now consider
+ y = ex
Integrating both side w.r.t.x
= xy = e2 + c
Y = (ex + c)
Y = (ex + C)
2. Find the general solution of the following exact differential equation.
i)exy + ex = 2
ii) cos x – ysin x = x2
Solution
i) Given
(exy) = 2
Integrating both sides with respect to x
(exy) dx =
ii) Given
cosx – y sin x = x2
(y cos x) = x2
Integrating both side with respect to x
= (exy) dx =
Y cos x = + c
3ycosx = x3 + 3C
3ycosx = x3 + 4
3.
+ lny = x + 1
Soln
Given
+ lny = x + 1
Integrating both sides w.r.t x
(x ln y) dx =
Xln y = ½ x2 + x + C
2xlny + x2 + 2x + 2c
2x lny + x2 + x + A
Integrating factors
Consider first order differential equation of the form
+ py =Q
Where p and Q are functions of x
Multiplying by integrating factor F both sides will make an exact equation
i.e F + Fpy + FQ…….i
=
+
+
…..ii
Comparing (i) (ii)
+ Fpy =
+
Fpy =
= Fp
dF =
by separating of variables
F = is the required integrating factor
Examples
1. Solve + y = x3
Solution
+ y = x3
+
= x2
Compare with + py = Q
P =
Then =
dx
= ln x
If F = eln x
F = eln x
(xy) = x2 x
(xy) =
Xy = x4 + C
2. Solve
(x + 1) + y + (x + 1)2
Soln
(x + 1) + y + (x + 1)2
= +
= x + 1
= +
, y = x + 1
P =
F = esp
= eln (x + 1)
= x + 1
Y (x + 1) =
=
= x3 + x2 + x + c
= + c
Y = +
3. Solve (1 – x2) – xy = 1
Solution –
y =
P =
=
dx
= ½ ln (1 – )
F = e ln (1 – ½
= (1 – x2) ½
Y =
dx
= dx
Y =
4. tanx + y = ex tan x
Solution
+
, y = ex
P = = cot x
=
= ln
F = eln
=
Y =
dx
Integrating by parts the R.H.S
= = ex
–
dx
= ex sin x – (ex cos x +
dx
= ex
– ex
–
dx
2 sin x dx = e x (
–
)
=
(
)
Y sin x = (
) + c
Bernoulli’s equation
This is a first order D.E of the form
+ p (x) y = Q (x) y n
p (x) and Q (x) are functions of x or constant
Steps
+ p (x) y = Q (x) yn……i
Divide both sides by yn gives
Y-n + p (x) y1 – n = Q (x)…… (ii)
Let z = y1-n
(1 – n) y-n
Multiplying (ii) by (1 – n) both sides gives
(1 – n) y-n
+ (1 – n) p (x) y (1 – n) = (1 – n) Q (x)
+ (1 – n) p (x) y (1 – n) = (1 – n) Q (x)
+ p1 (x) y (1 – n) = Q1 (x)
p1 (x) and Q1 (x) are functions of x or constant
But z = y (1 -n)
= + p1 (x) z = Q1 (x)……..ii
iii) is linear the use of integrating factor can be used
Example 1
Solve +
= xy2
Solution
Dividing both sides by gives
Let Z =
Multiply (ii) by -1 gives
But Z =
=
=
=
Then Z.F=
= -1
=
But Z =
Example 2
Solve
Solution
1st Expressing the equation in the form
–
–
Let Z =
But Z =
=
=
Then
But Z =
Example 3
Solve
Solution
Expressing the equation in the form
Then dividing by
let Z =
Multiply (ii) by -2 gives
But Z =
Then,
But Z =
Exercise
Solve the following first order D.es
1.
2.