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MATHS I


Unit – 3


Series solution of differential equation


Working Rule

Step 1 Let be the solution of the given differential equation.

Step 2: Find etc.

Step 3: Substitute the expression of in the given differential equation.

Step 4: Calculate coefficient of various powers of x by equating coefficients to zero.

Step 5: Substitute the values of in the differential equation to get the required series solution.

Example. Solve in series the equation

Ans. 

Since x=0 is the ordinary point of the equation (1)

Then

Substituting in (1) we get

Equating to zero the coefficient of the various powers of x we obtain

Substituting these values in (2) we get

 

Solve.

Ans. Let,

Substituting the value of   in the given equation we get

Where the first summation extends over all values of K from 2 to

And the second from K =

Now equating the coefficient of equal to zero we have

For K =4

 

Solve.

Ans. Let

Substituting for in the given differential equation

Equating the coefficients of various powers of x to zero we get

 


Legendre’s equation is

And

 

Prove that

Ans. We know that

Put n=2

 

Prove that .

Ans. We know

+

 

Put x = 1 both sides we get

Equating the coefficient of on both sides we get

 

Prove that

Ans. We know

Differentiating with respect to z we get

Multiplying both sides by we get

Equating the coefficient of from both sides we get

 

Solve. Statement

Proof. Let is a solution of

is the solution of

Multiplying (1) by z and (2) by y and subtracting we get

Now integrative -1 to 1 we get

Now we have to prove that

 

We know that,

Squaring both sides we get

Integrating both sides between -1 to +1 we get

on both sides we get

here n = m

 

Prove that

Ans. The Recurrence formula is

Pn+1+nPn-1

Replacing n by (n+1) and (n-1) we have

Multiplying (1) and (2) and integrating in the limits -1 to 1 we get

 

(By orthogonality property)

 


Rodrigues' Formula: The Legendre Polynomials  can be expressed by Rodrigues' formula

 where 

Generating Function: The generating function of a Legendre Polynomial is

Orthogonality: Legendre Polynomials , form a complete orthogonal set on the interval . It can be shown that

By using this orthogonality, a piecewise continuous function  in  can be expressed in terms of Legendre Polynomials:

Where:

This orthogonal series expansion is also known as a Fourier-Legendre Series expansion or a Generalized Fourier Series expansion.

Even/Odd Functions: Whether a Legendre Polynomial is an even or odd function depends on its degree n.

Based on ,

• Pn(x) is an even function when n is even.

• Pn(x) is an odd function when n is odd.

In addition, fromPn'(x),

• Pn(x) is an even function when n is odd.

• Pn(x) is an odd function when n is even.

Recurrence Relation: A Legendre Polynomial at one point can be expressed by neighboring Legendre Polynomials at the same point.

• 

• 

• 

• 

• 

 


The Bessel equation is

 


The Bessel equation is

Bessel function of first kind

Bessel function of second kind

Recurrence Formula

1)     xJn'=nJn-xJn+1

2)    

3)    

4)    

5)    

6)    

 

Prove that (1)

Ans. We know

(b) Prove that

Ans. We know that

(3) Prove that

Ans. We know that

Jn(x)=

 

If n = 0

If n = 1

Note General solution of Bessel Equation

 

Text Book:

1) Calculus: Gorakh Prasad

2) Advance Engineering Mathematics – E. Kreyszig, John Wiley & Sons Inc.

 


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