Higher order differential equation, Slides of Mathematics

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Chapter-4
Higher order differential equation
Linear ordinary differential equation: A linear ordinary differential equation of order 𝑛 is an
equation of the form
𝑎0(𝑥)𝑑𝑛𝑦
𝑑𝑥𝑛+𝑎1(𝑥)𝑑𝑛−1𝑦
𝑑𝑥𝑛−1++𝑎𝑛−1(𝑥)𝑑𝑦
𝑑𝑥+𝑎𝑛(𝑥)𝑦=𝐹(𝑥)
Where 𝑎0(𝑥)0.
Homogeneous Differential Equation: A differential equation is said to be homogeneous if each
term of the equation contains at least a derivative or a dependent variable.
Homogeneous linear differential equation: A linear ordinary differential equation of order 𝑛 is an
equation of the form
𝑎0(𝑥)𝑑𝑛𝑦
𝑑𝑥𝑛+𝑎1(𝑥)𝑑𝑛−1𝑦
𝑑𝑥𝑛−1++𝑎𝑛−1(𝑥)𝑑𝑦
𝑑𝑥+𝑎𝑛(𝑥)𝑦=0
Where 𝑎0(𝑥)0.
Linearly independent: The 𝑛 functions 𝑓1,𝑓2,,𝑓𝑛 are called linearly independent if there exists
constants 𝑐1,𝑐2,,𝑐𝑛such that the linear combination 𝑐1𝑓1+𝑐2𝑓2++𝑐𝑛𝑓𝑛=0 implies that 𝑐1=
𝑐2==𝑐𝑛=0. If not all 𝑐𝑖 are zero then the functions 𝑓1,𝑓2,,𝑓𝑛 are called linearly dependent.
Wronskian: Let 𝑓1,𝑓2,,𝑓𝑛 be 𝑛 real functions each of which has (𝑛 1)𝑡ℎ derivative on a real
interval. The determinant
𝑊(𝑓1,𝑓2,,𝑓𝑛)=| 𝑓1𝑓2
𝑓1 𝑓2 𝑓𝑛
𝑓𝑛
𝑓1𝑛−1 𝑓2𝑛−1
𝑓𝑛𝑛−1|
in which primes denote derivatives, is called wronskian of these 𝑛 functions. If 𝑊(𝑓1,𝑓2,,𝑓𝑛)0
then the functions are linearly independent otherwise the functions are linearly dependent.
Theorem 1 (without proof): Every homogeneous linear differential equation of order 𝑛 has exactly
𝑛 number of independent solutions.
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Chapter- 4

Higher order differential equation

Linear ordinary differential equation: A linear ordinary differential equation of order 𝑛 is an

equation of the form

0

𝑛

𝑛

1

𝑛− 1

𝑛− 1

𝑛− 1

𝑛

Where 𝑎 0

Homogeneous Differential Equation: A differential equation is said to be homogeneous if each

term of the equation contains at least a derivative or a dependent variable.

Homogeneous linear differential equation: A linear ordinary differential equation of order 𝑛 is an

equation of the form

0

𝑛

𝑛

1

𝑛− 1

𝑛− 1

𝑛− 1

𝑛

Where 𝑎 0

Linearly independent : The 𝑛 functions 𝑓 1

2

𝑛

are called linearly independent if there exists

constants 𝑐 1

2

𝑛

such that the linear combination 𝑐

1

1

2

2

𝑛

𝑛

= 0 implies that 𝑐

1

2

𝑛

= 0. If not all 𝑐

𝑖

are zero then the functions 𝑓

1

2

𝑛

are called linearly dependent.

Wronskian : Let 𝑓 1

2

𝑛

be 𝑛 real functions each of which has (𝑛 − 1 )𝑡ℎ derivative on a real

interval. The determinant

1

2

𝑛

1

2

1

2

𝑛

𝑛

1

𝑛− 1

2

𝑛− 1

𝑛

𝑛− 1

in which primes denote derivatives, is called wronskian of these 𝑛 functions. If 𝑊(𝑓

1

2

𝑛

then the functions are linearly independent otherwise the functions are linearly dependent.

Theorem 1 (without proof) : Every homogeneous linear differential equation of order 𝑛 has exactly

𝑛 number of independent solutions.

Theorem 2 : If 𝑓

1

2

𝑛

are𝑛 number of independent solutions of the homogeneous linear

differential equation𝑎

0

𝑑

𝑛

𝑦

𝑑𝑥

𝑛

1

𝑑

𝑛− 1

𝑦

𝑑𝑥

𝑛− 1

𝑛− 1

𝑑𝑦

𝑑𝑥

𝑛

(𝑥)𝑦 = 0 then their linear

combination 𝑐 1

1

2

2

𝑛

𝑛

is also a solution of that differential equation.

Proof : If𝑓 1

2

𝑛

are independent solutions of homogeneous linear differential equation

0

𝑑

𝑛

𝑦

𝑑𝑥

𝑛

1

𝑑

𝑛− 1

𝑦

𝑑𝑥

𝑛− 1

𝑛− 1

𝑑𝑦

𝑑𝑥

𝑛

then we obtain

0

𝑑

𝑛

𝑓

1

𝑑𝑥

𝑛

1

𝑑

𝑛− 1

𝑓

1

𝑑𝑥

𝑛− 1

𝑛− 1

𝑑𝑓

1

𝑑𝑥

𝑛

1

0

𝑑

𝑛

𝑓 2

𝑑𝑥

𝑛

1

𝑑

𝑛− 1

𝑓 2

𝑑𝑥

𝑛− 1

𝑛− 1

𝑑𝑓 2

𝑑𝑥

𝑛

2

0

𝑑

𝑛

𝑓

𝑛

𝑑𝑥

𝑛

1

𝑑

𝑛− 1

𝑓

𝑛

𝑑𝑥

𝑛− 1

𝑛− 1

𝑑𝑓

𝑛

𝑑𝑥

𝑛

𝑛

= 0 (n+1)

Now if 𝑐 1

1

2

2

𝑛

𝑛

is a solution of equation (1) then it must satisfies the equation.

0

𝑛

1

1

2

2

𝑛

𝑛

𝑛

1

𝑛− 1

1

1

2

2

𝑛

𝑛

𝑛− 1

𝑛− 1

𝑑(𝑐

1

𝑓

1

+𝑐

2

𝑓

2

+⋯+𝑐

𝑛

𝑓

𝑛

)

𝑑𝑥

𝑛

1

1

2

2

𝑛

𝑛

1

0

𝑛

1

𝑛

1

𝑛− 1

1

𝑛− 1

𝑛− 1

1

𝑛

1

2

0

𝑛

2

𝑛

1

𝑛− 1

2

𝑛− 1

𝑛− 1

2

𝑛

2

𝑛

0

𝑛

𝑛

𝑛

1

𝑛− 1

𝑛

𝑛− 1

𝑛− 1

𝑛

𝑛

𝑛

Thus the linear combination 𝑐 1

1

2

2

𝑛

𝑛

is also a solution of equation (1) called the

general solution. (Proved)

Problem 1 : Consider the differential equation

′′

(a) Show that 𝑒

2 𝑥

and 𝑒

3 𝑥

are linearly independent solutions of this equation on the interval−∞ < 𝑥 <

(b) Write the general solution of the given equation.

Problem 2 : Consider the differential equation

′′

(a) Show that 𝑒

𝑥

and 𝑥𝑒

𝑥

are linearly independent solutions of this equation on the interval −∞ < 𝑥 <

(b) Write the general solution of the given equation.

(c) Find the solution that satisfies the conditions𝑦( 0 ) = 1 , 𝑦′( 0 ) = 4. Explain why this solution is

unique. Over what interval is it defined?

Solution : (a) Given that 𝑦

′′

Let 𝑦 = 𝑒

𝑥

then 𝑦′ = 𝑒

𝑥

and 𝑦′′ = 𝑒

𝑥

Substituting the values of 𝑦, 𝑦

, 𝑦′′ in 𝐿. 𝐻. 𝑆 of equation (1) we get

𝑥

𝑥

𝑥

Again let 𝑦 = 𝑥𝑒

𝑥

then 𝑦

𝑥

𝑥

and 𝑦

′′

𝑥

𝑥

𝑥

𝑥

𝑥

Substituting the values of 𝑦, 𝑦

, 𝑦′′ in 𝐿. 𝐻. 𝑆 of equation (1) we get

𝑥

𝑥

𝑥

𝑥

𝑥

Hence 𝑒

𝑥

and 𝑥𝑒

𝑥

are two solutions of equation (1).

Now 𝑊(𝑒

𝑥

𝑥

𝑥

𝑥

𝑥

𝑥

𝑥

2 𝑥

2 𝑥

2 𝑥

2 𝑥

≠ 0 for all 𝑥 in the interval

−∞ < 𝑥 < ∞. Thus 𝑒

𝑥

and 𝑥𝑒

𝑥

are linearly independent solutions of equation (1) on the interval

(b) The general solution of equation (1) is

1

𝑥

2

𝑥

(c) Here,

1

𝑥

2

𝑥

1

𝑥

2

𝑥

2

𝑥

Using initial conditions𝑦

= 4 in equation (2) and (3) we obtain

1

and

1

2

Solving equation (4) and (5) we get

1

2

Since the number of unknown constants and the number of equations from initial conditions are same

so the value of 𝑐

1

and 𝑐

2

are unique.

Thus the required solution is

𝑥

𝑥

Since 𝑐

1

and 𝑐

2

are unique so this solution is unique over the interval −∞ < 𝑥 < ∞.

Problem 3 : Consider the differential equation

2

′′

(a) Show that 𝑥and 𝑥

2

are linearly independent solutions of this equation on the interval 0 < 𝑥 < ∞.

(b) Write the general solution of the given equation.

(c) Find the solution that satisfies the conditions𝑦

= 2. Explain why this solution is

unique. Over what interval is it defined?

Solution : (a) Given that 𝑥

2

′′

Let 𝑦 = 𝑥 then 𝑦′ = 1 and 𝑦′′ = 0

Substituting the values of 𝑦, 𝑦

, 𝑦′′ in 𝐿. 𝐻. 𝑆 of equation (1) we get

Again let 𝑦 = 𝑥

2

then 𝑦′ = 2 𝑥 and 𝑦′′ = 2

Substituting the values of 𝑦, 𝑦

, 𝑦′′ in 𝐿. 𝐻. 𝑆 of equation (1) we get

2

2

Hence 𝑥and 𝑥

2

are two solutions of equation (1).

Now 𝑊

2

2

2

2

2

≠ 0 for all 𝑥on the interval

0 < 𝑥 < ∞. Thus 𝑥and 𝑥

2

are linearly independent solutions of equation (1) on the interval 0 < 𝑥 <

(b) The general solution of equation (1) is

1

2

2

(c) Here,

1

2

2

1

2

Using initial conditions𝑦( 1 ) = 3 , 𝑦′( 1 ) = 2 in equation (2) and (3) we obtain

1

2

and

Letting 𝑐 = 1 and recall 𝑤 = 𝑣′ we obtain

2

Again integrating we get

Thus the linearly independent solution is 𝑦 = 𝑣𝑥 = 𝑥 (𝑥 −

1

𝑥

2

Hence the general solution is

1

2

2

Problem 5 : Given that 𝑦 = 𝑥 + 1 is a solution of (𝑥 + 1 )

2

′′

  • 3 𝑦 = 0 find a linearly

independent solution by reducing the order.

Solution : Given (𝑥 + 1 )

2

′′

Let𝑦 = 𝑣(𝑥 + 1 ) then𝑦

= 𝑣 + (𝑥 + 1 )𝑣′ and 𝑦

′′

′′

′′

Substituting these values in equation (1) we get

2

′′

3

′′

2

′′

Letting 𝑤 = 𝑣′ we obtain the first – order homogeneous linear equation

Treating this as a separable equation, we obtain

By integrating we obtain

ln 𝑤 = ln(𝑥 + 1 ) + ln 𝑐

⇒ ln 𝑤 = ln(𝑥 + 1 ) + ln 𝑐

Letting 𝑐 = 1 and recall 𝑤 = 𝑣′ we obtain

Again integrating we get

2

Thus the linearly independent solution is 𝑦 = 𝑣(𝑥 + 1 ) = (𝑥 + 1 )

(𝑥+ 1 )

2

2

(𝑥+ 1 )

3

2

Hence the general solution is

1

2

3

Let 𝑦 = 𝑒

𝑚𝑥

be the trail solution of equation (1).

Then the auxiliary equation of equation (1) is

2

⇒ (m − 1 )(m − 2 ) = 0

Thus the required general solution is

1

𝑥

2

2 𝑥

Problem 7 : Solve the differential equation 𝑦

′′

Solution : Given the differential equation

′′

Let 𝑦 = 𝑒

𝑚𝑥

be the trail solution of equation (1).

Then the auxiliary equation of equation (1) is

2

⇒ (m − 2 )(m − 3 ) = 0

Thus the required general solution is

1

2 𝑥

2

3 𝑥

Problem 8 : Solve the differential equation 𝑦

′′′

′′

Solution : Given the differential equation

′′′

′′

Let 𝑦 = 𝑒

𝑚𝑥

be the trail solution of equation (1).

Then the auxiliary equation of equation (1) is

3

2

3

2

2

2

m − 1

m − 1

m − 1

m − 1

2

m − 1

Thus the required general solution is

1

𝑥

2

−𝑥

3

3 𝑥

Case II : Repeated real roots

Problem 9 : Solve the differential equation 𝑦

′′

Solution : Given the differential equation

′′

Let 𝑦 = 𝑒

𝑚𝑥

be the trail solution of equation (1).

Then the auxiliary equation of equation (1) is

2

m − 3

Then the two solutions are 𝑒

3 𝑥

and𝑒

3 𝑥

which are linearly dependent.

Thus their linear combination 𝑐

1

3 𝑥

2

3 𝑥

1

2

3 𝑥

0

3 𝑥

is not the general solution.

Since we already know the one solution is 𝑒

3 𝑥

, we let 𝑦 = 𝑣𝑒

3 𝑥

, then

3 𝑥

3 𝑥

′′

3 𝑥

′′

3 𝑥

3 𝑥

Substituting into equation (1) we get

3 𝑥

′′

3 𝑥

3 𝑥

3 𝑥

3 𝑥

3 𝑥

3 𝑥

′′

′′

Choosing 𝑐 = 1

Thus 𝑥𝑒

3 𝑥

is a linearly independent solution of equation (1)

Hence the general solution is

1

3 𝑥

2

3 𝑥

Problem 10 : Solve the differential equation 𝑦

′′

Solution : Given the differential equation

′′

Let 𝑦 = 𝑒

𝑚𝑥

be the trail solution of equation (1).

Then the auxiliary equation of equation (1) is

2

′′′

′′

Let 𝑦 = 𝑒

𝑚𝑥

be the trail solution of equation (1).

Then the auxiliary equation of equation (1) is

3

2

3

Thus the required general solution is

1

2 𝑥

2

2 𝑥

3

2

2 𝑥

1

2

3

2

2 𝑥

Problem 13 : Solve the differential equation 𝑦

𝑖𝑣

′′

Solution : Given the differential equation

𝑖𝑣

′′

Let 𝑦 = 𝑒

𝑚𝑥

be the trail solution of equation (1).

Then the auxiliary equation of equation (1) is

4

2

2

2

2

Thus the required general solution is

1

cos 2 𝑥 + 𝑐

2

sin 2 𝑥 + 𝑐

3

𝑥 cos 2 𝑥 + 𝑐

4

𝑥 sin 2 𝑥 = (𝑐

1

3

𝑥)cos 2 𝑥 + (𝑐

2

4

𝑥) sin 2 𝑥

Problem 14 : Solve the initial value problem

′′′

′′

′′

Solution : Given the differential equation

′′′

′′

Let 𝑦 = 𝑒

𝑚𝑥

be the trail solution of equation (1).

Then the auxiliary equation of equation (1) is

3

2

2

2

The general solution of equation (1) is

1

2 𝑥

2

cos 2 𝑥 + 𝑐

3

sin 2 𝑥) (2)

1

2 𝑥

2

sin 2 𝑥 + 2 𝑐

3

cos 2 𝑥) (3)

′′

1

2 𝑥

2

cos 2 𝑥 − 4 𝑐

3

sin 2 𝑥) (4)

Applying the initial conditions 𝑦( 0 ) = 2 , 𝑦

( 0 ) = 0 and𝑦

′′

( 0 ) = 0 in equations (2), (3) and (4) we

get

1

2

1

3

and 0 = 4 𝑐

1

2

Solving equations (5), (6) and (7) we get

1

2

= 1 and 𝑐

3

Thus the required solution is

2 𝑥

  • (cos 2 𝑥 − sin 2 𝑥)

Problem 15 : The roots of the auxiliary equation corresponding to a certain 11 th order homogeneous

linear differential equation with constant coefficients are

4 , 4 , 4 , 4 , 5 , 2 + 3 𝑖, 2 − 3 𝑖, 2 + 3 𝑖, 2 − 3 𝑖, 4 + 5 𝑖, 4 − 5 𝑖 write the general solution.

Solution : The general solution is

1

2

3

2

4

3

4 𝑥

5

5 𝑥

2 𝑥

6

7

cos 3 𝑥 +

8

9

sin 3 𝑥

4 𝑥

10

cos 5 𝑥 + 𝑐

11

sin 5 𝑥

Non homogeneous linear equation with constant coefficients :

𝑛

1

𝑛− 1

𝑛

)𝑦 = 𝐹(𝑥) where 𝐷 =

𝑑

𝑑𝑥

Problem 16 : Find the particular integral for 𝑭

𝒂𝒙

Solution : by successive differentiation we obtain

𝑎𝑥

𝑎𝑥

𝑎𝑥

𝑎𝑥

2

𝑎𝑥

2

𝑎𝑥

𝑛

𝑎𝑥

𝑛

𝑎𝑥

(n)

Multiplying equation (1), (2), …,(n) by 𝑎

𝑛

𝑛− 1

, ⋯ , 1 respectively and adding we get

𝑎𝑥

𝑎𝑥

The auxiliary equation of corresponding homogeneous equation of (1) is

2

2

∴ Complementary function, 𝑦 𝑐

1

2 𝑥

2

2 𝑥

Particular integral,

𝑝

2

2 𝑥

2 𝑥

2

2 𝑥

2

2 𝑥

Thus the required general solution is

𝑐

𝑝

1

2 𝑥

2

2 𝑥

2

2 𝑥

Problem 20 : Solve the equation (𝐷

3

2

𝑥

3 𝑥

Solution : Given that (𝐷

3

2

𝑥

3 𝑥

The auxiliary equation of corresponding homogeneous equation of (1) is

3

2

3

∴ Complementary function, 𝑦 𝑐

1

𝑥

2

𝑥

3

2

𝑥

Particular integral,

𝑝

3

2

𝑥

3

2

3 𝑥

2

𝑥

3 𝑥

2

𝑥

3 𝑥

3

𝑥

3 𝑥

3

𝑥

3 𝑥

Thus the required general solution is

𝑐

𝑝

1

𝑥

2

𝑥

3

2

𝑥

3

𝑥

3 𝑥

Particular integral for 𝑭(𝒙) = 𝒔𝒊𝒏 𝒂𝒙, 𝒄𝒐𝒔 𝒂𝒙

𝑝

2

sin 𝑎𝑥 , cos 𝑎𝑥 =

2

sin 𝑎𝑥 , cos 𝑎𝑥 ; 𝑓(𝑎

2

Problem 21 : Solve the equation (𝐷

2

𝑥

  • sin 2 𝑥

Solution : Given that

2

𝑥

  • sin 2 𝑥 (1)

The auxiliary equation of corresponding homogeneous equation of (1) is

2

∴ Complementary function,

𝑐

𝑥

2

(𝑐

1

cos

2

sin

Particular integral,

𝑝

2

𝑥

2

sin 2 𝑥

𝑥

2

sin 2 𝑥

𝑥

sin 2 𝑥 =

𝑥

sin 2 𝑥

𝑥

2

sin 2 𝑥 =

𝑥

2

sin 2 𝑥

𝑥

sin 2 𝑥 =

𝑥

2 cos 2 𝑥 + 3 sin 2 𝑥

Thus the required general solution is

𝑐

𝑝

𝑥

2

(𝑐

1

cos

2

sin

𝑥

2 cos 2 𝑥 + 3 sin 2 𝑥

Problem 22 : Solve the equation (𝐷

2

2

𝑦 = cos 3 𝑥

Solution : Given that (𝐷

2

2

𝑦 = cos 3 𝑥 (1)

The auxiliary equation of corresponding homogeneous equation of (1) is

2

2

2

∴ Complementary function,

𝑐

1

2

𝑥) cos 𝑥 + (𝑐

3

4

𝑥) sin 𝑥

Particular integral,

𝑝

2

2

cos 3 𝑥

𝑐

1

2

−𝑥

3

−𝑥

Particular integral,

𝑝

3

2

2 𝑥

3

2

2

3

2

2 𝑥

2

2

2

2 𝑥

− 2

2

− 2

2 𝑥

2

2

2

2 𝑥

2

2 𝑥

3

2

2

2 𝑥

3

2

Thus the required general solution is

𝑐

𝑝

1

2

−𝑥

3

−𝑥

2 𝑥

3

2

Particular integral for 𝑭

𝒂𝒙

𝑝

𝑎𝑥

𝑎𝑥

Problem 25 : Solve the equation (𝐷

2

3 𝑥

3 𝑥

Solution : Given that

2

3 𝑥

3 𝑥

The auxiliary equation of corresponding homogeneous equation of (1) is

2

∴ Complementary function,

𝑐

1

3 𝑥

2

− 3 𝑥

Particular integral,

𝑝

2

3 𝑥

2

3 𝑥

3 𝑥

3 𝑥

2

3 𝑥

3 𝑥

2

3 𝑥

3 𝑥

𝐷

6

3 𝑥

3 𝑥

𝐷

6

− 1

3 𝑥

3 𝑥

𝐷

6

3 𝑥

3 𝑥

3 𝑥

3 𝑥

2

3 𝑥

3 𝑥

2

Thus the required general solution is

𝑐

𝑝

1

3 𝑥

2

− 3 𝑥

3 𝑥

3 𝑥

2

Problem 26 : Solve the equation (𝐷

2

3 𝑥

sin 2 𝑥

Solution : Given that (𝐷

2

3 𝑥

sin 2 𝑥 (1)

The auxiliary equation of corresponding homogeneous equation of (1) is

2

∴ Complementary function,

𝑐

1

√ 11 𝑥

2

−√ 11 𝑥

Particular integral,

𝑝

2

3 𝑥

sin 2 𝑥 = 𝑒

3 𝑥

2

sin 2 𝑥

3 𝑥

2

sin 2 𝑥 = 𝑒

3 𝑥

2

sin 2 𝑥

3 𝑥

2

sin 2 𝑥 = 𝑒

3 𝑥

sin 2 𝑥

3 𝑥

sin 2 𝑥 = 𝑒

3 𝑥

2

sin 2 𝑥