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To sketch the graph of xJ12(x)for x from 0 to π.

Short Answer

Expert verified

The graph of the function xJ12(x)is given below:

Step by step solution

01

 Step 1: Concept of Bessel’s Equation:

The solution of Bessel's equation is,x2y"+xy'+(x2-n2)y=0 .

Jn(x)=k=0(-1)k(k+1)(n+k+1)(x2)2k+n

02

Calculation of the function xJ12(x) for x :

Given function Jp(x)for p=12and x from 0 to π.

role="math" localid="1659269941142" Jp(x)=n=0(-1)n(n+1)(n+1+p)(x2)2n+p

For, p=12in above function.

Jp(x)=n=0(-1)n(n+1)(n+1+p)(x2)2n+pxJ12(x)=n=0-1n(n!)n+12!x22n+12+12(n+1)=n!xJ12(x)=112!x2-132!x23+12!152!x25-13!172!x27+14!192!x2=15!2-1112!x211+16!-1132!x213-17!-1152!x215+......

03

Draw the graph of the function xJ12(x) :

The graph of the function xJ12(x) is given below:

From the above graph, we can observe that there are three zeros of xJ12(x)fromx=0to π.

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Most popular questions from this chapter


Use the recursion relation (5.8a) and the values of P0(x)and P1(x) to find localid="1664340078504" P2(x)P3(x),P4(x),P5(x), and P6(x). [After you have found P3(x), use it to find P4(x) and so on for the higher order polynomials.]

To show the following equation shown in the problem

2ddxJa(x)=Ja-1(x).

Prove the least squares approximation property of Legendre polynomials [see (9.5) and (9.6)] as follows. Let f(x) be the given function to be approximated. Let the functions pl(x)be the normalized Legendre polynomials, that is, pl(x) = √(2l+1)/2 Pl(x) , so that

-11[pl(x)"]"2dx=1.

Show thatLegendre series for f(x)as far as the p2(x)term is

f(x)=c0p0(x)+c1p1(x) +c3p3(x) with c1 =∫-11f(x)pl(x) dx

Write the quadratic polynomial satisfying the least squares condition as b0p0(x)+b1p1(x)+b0p0(x)by Problem 5.14 any quadratic polynomial can be written in this form). The problem is to find b0, b1, b2so that I=∫-11[f2(x)+(b0-c0)2+(b1-c1)2+(b2-c2)2 -c02 -c12 -c22] dx

Now determine the values of the b's to make I as small as possible. (Hint: The smallest value the square of a real number can have is zero.) Generalize the proof to polynomials of degree n.

The equation for the associated Legendre functions (and for Legendre functions when m=0) usually arises in the form (see, for example, Chapter 13, Section 7) 1/sinθ d/dθ (sinθ dy/dθ)+[l (l+1)-m2/sin2θ] y=0.

Make the change of variable x=cosθ, and obtain (10.1):

(1-x2) y"-2xy'+[l (l+1) -m2/1-x2] y=0

Multiply(5.8e)by {P1}(x)and integrate from -1 to 1. To evaluate the middle term, integrate by parts.

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