Second order nonhomogeneous, Slides of Physics

Second order homogeneous equations

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Chapter One first order differential equation - Homogenous
4
2.2. Homogenous method
A function 𝑓( 𝑥,𝑦) is said to be homogeneous of degree n if the equation
𝑓( 𝑧𝑥,𝑧𝑦)= 𝑧𝑛 𝑓( 𝑥, 𝑦)
Holds for all 𝑥, 𝑦 , and 𝑧 (for which both sides are defined).
Example 1: 𝑓( 𝑥, 𝑦) = 𝑥 2+ 𝑦2 is homogeneous of degree 2
Example 2: 𝑓( 𝑥, 𝑦) = 𝑥 8 3𝑥2 𝑦6 is homogeneous of degree 4
Example 3: 𝑓( 𝑥,𝑦) = 𝑥 3sin𝑦
𝑥 + 𝑥 2𝑦 ln𝑥 is homogeneous of degree 3
Example 4: 𝑓( 𝑥,𝑦) = 𝑦
𝑥 𝑒 𝑥+ tanh 𝑦
𝑥 is homogeneous of degree 0
The method for solving homogeneous equations follows from this fact:
The substitution y = x u dy = xdu + udx
Or x = y u dx = ydu + udy
Transforms a homogeneous equation into a separable one
Example 1: Solve
( 𝐱𝟐 𝐲𝟐 ) 𝐝𝐱 + 𝐱𝐲 𝐝𝐲 = 𝟎
Solution
This equation is homogeneous. Thus to solve it, make the substitutions
y = x u 𝑎𝑛𝑑 dy = x du + u dx:
( x2 y2 ) dx + xy dy = 0
[ x2 (xu)2] dx + x(xu) (x du + u dx) = 0
[ x2 x2 u2] dx + (x3u du + x2 u2 dx) = 0
x2 dx x2 u2 dx + x3u du + x2 u2 dx = 0
x2 dx + x3u du = 0 𝑑𝑖𝑣𝑖𝑑𝑖𝑛𝑔 𝑏𝑦 x2 𝑇𝑒𝑛 dx + xu du = 0
This final equation is now separable. Proceeding with the solution,
dx
x = u du
dx
x = u du 1
2 u2= lnx + lnC or u2=2lnC
x
Put u = y
x Then [y
x]2=2lnC
x or y2= 2 x2 lnC
x
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2.2. Homogenous method

A function 𝑓( 𝑥, 𝑦) is said to be homogeneous of degree n if the equation

𝑛

Holds for all 𝑥, 𝑦 , and 𝑧 (for which both sides are defined).

Example 1: 𝑓( 𝑥, 𝑦) = 𝑥

2

2

is homogeneous of degree 2

Example 2: 𝑓( 𝑥, 𝑦) =

8

2

6

is homogeneous of degree 4

Example 3 : 𝑓( 𝑥, 𝑦) = 𝑥

3

sin

𝑦

𝑥

2

𝑦 ln 𝑥 is homogeneous of degree 3

Example 4 : 𝑓( 𝑥, 𝑦) =

𝑦

𝑥

𝑥

  • tanh

𝑦

𝑥

is homogeneous of degree 0

The method for solving homogeneous equations follows from this fact:

The substitution y = x u dy = xdu + udx

Or x = y u dx = ydu + udy

Transforms a homogeneous equation into a separable one

Example 1 : Solve

𝟐

  • 𝐲

𝟐

Solution

This equation is homogeneous. Thus to solve it, make the substitutions

y = x u 𝑎𝑛𝑑 dy = x du + u dx:

( x

2

  • y

2

) dx + xy dy = 0

[

x

2

xu

2

]

dx + x(xu) (x du + u dx) = 0

[

x

2

  • x

2

u

2

]

dx + (x

3

u du + x

2

u

2

dx) = 0

x

2

dx – x

2

u

2

dx + x

3

u du + x

2

u

2

dx = 0

x

2

dx + x

3

u du = 0 𝑑𝑖𝑣𝑖𝑑𝑖𝑛𝑔 𝑏𝑦 x

2

𝑇ℎ𝑒𝑛 dx + xu du = 0

This final equation is now separable. Proceeding with the solution,

dx

x

= − u du

dx

x

u du →

1

2

u

2

= − ln x + ln C or u

2

= 2 ln

C

x

Put u =

y

x

Then [

y

x

]

2

= 2 ln

C

x

or y

2

= 2 x

2

ln

C

x

Example 2: Solve

𝟏

Solution

The differential equation is homogeneous. With degree equal 1

The substitutions y = xv and dy = x dv + v dx

x + 2 𝑥𝑣

dx +

xv − x

x dv + v dx

2 x dx + 4 𝑥𝑣 dx + x

2

v dv − x

2

dv + x v

2

dx − 𝑥v dx = 0

2 x + 3 𝑥𝑣 + x v

2

dx +

x

2

v − x

2

dv = 0

( 2 x + 3 𝑥𝑣 + x v

2

) dx + (x

2

v − x

2

) dv = 0

𝑥 ( 2 + 3 𝑣 + v

2

) dx + x

2

(v − 1 ) dv = 0 divided by 𝑥

( 2 + 3 𝑣 + v

2

) dx + x (v − 1 ) dv = 0

The equation is now separable. Separating the variables and integrating gives

v − 1

2 + 3𝑣 + v

2

dv = −

x

dx

Or

− 2

v + 1

dv +

3

v + 2

dv = −

1

x

dx

By integration ∫

− 2

v + 1

dv + ∫

3

v + 2

dv = ∫ −

1

x

dx

− 2 ln(v + 1 ) + 3 ln( v + 2 ) = − ln x + ln C

Or ln[(v + 1 )

− 2

(v + 2 )

3

] = ln

C

x

Or (v + 1 )

− 2

(v + 2 )

3

C

x

Or (

y

x

− 2

y

x

3

C

x

Put 𝑦 = 0 at 𝑥 = 1 then (

0

1

− 2

0

1

3

C

1

→ C = 8

The particular solution (

y

x

− 2

y

x

3

8

x

This can be simplified to [ 2 𝑥 + 𝑦]

3

= 8 [𝑥 + 𝑦]

2

v − 1

2 + 3 𝑣 + v

2

𝐴

𝑣+ 1

𝐵

𝑣+ 2

Av+ 2 A+Bv+B

(v+ 1 )(v+ 2 )

By solve equation together then

𝐴 = − 2 and 𝐵 = 3

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