Question on deriving Bessel's equation

  • Thread starter Thread starter yungman
  • Start date Start date
  • Tags Tags
    deriving
yungman
Messages
5,741
Reaction score
294
\hbox { Bessel's equation of order p: }\;x^2y''+xy'+(x^2-p^2)y=0\;\hbox { and let}\;y=\sum_0^{\infty}C_nx^{n+r}
\Rightarrow\; \left[\sum_0^{\infty}C_k(k+r)(k+r-1)x^k+\sum_0^{\infty}C_k(k+r)x^k+\sum_2^{\infty} C_{k-2}x^k-p^2\sum_0^{\infty}C_kx^k\right]x^r\;=\;0
\Rightarrow\; x^r\left[(r^2-p^2)C_0+[(r+1)^2-p^2]C_1 x+\sum_2^{\infty}\left([(k+r)(k+r)-p^2]C_k+C_{k-2}\right)x^k\right]\;=\;0

According to the book, all the terms have to be zero for the equation to be zero.
(r^2-p^2)C_0=0\;\Rightarrow r=^+_-p
The book also say
[(r+1)^2-p^2]C_1=0\;\Rightarrow C_1=0\;\hbox { because from above, }\;r=^+_-p


My problem with this assumption ##C_1=0## is I can just as easy say ##(r+1)^2-p^2=0## and claim ##C_0=0##! This will change the whole equation of the Bessel's equation!

Why do I have to follow the book to let ##C_1=0## which result in all ##C_{2n+1}=0##? Is it just because it is simpler and more convenient this way?

Also, the book just said let ##C_0=\frac {1}{2^p\Gamma(1+p)}## without explaining why. Why?

I know it is for fitting the formula of:

J_p=\sum_0^{\infty} \frac{(-1)^k}{k! \Gamma(k+p+1)}\left(\frac {x}{2}\right)^{2k+p}

But can you just let ##C_0## to be anything?

Thanks
 
Last edited:
Physics news on Phys.org
yungman said:
\hbox { Bessel's equation of order p: }\;x^2y''+xy'+(x^2-p^2)y=0\;\hbox { and let}\;y=\sum_0^{\infty}C_nx^{n+r}
\Rightarrow\; \left[\sum_0^{\infty}C_k(k+r)(k+r-1)x^k+\sum_0^{\infty}C_k(k+r)x^k+\sum_2^{\infty} C_{k-2}x^k-p^2\sum_0^{\infty}C_kx^k\right]x^r\;=\;0
\Rightarrow\; x^r\left[(r^2-p^2)C_0+[(r+1)^2-p^2]C_1 x+\sum_2^{\infty}\left([(k+r)(k+r)-p^2]C_k+C_{k-2}\right)x^k\right]\;=\;0

According to the book, all the terms have to be zero for the equation to be zero.
(r^2-p^2)C_0=0\;\Rightarrow r=^+_-p
The book also say
[(r+1)^2-p^2]C_1=0\;\Rightarrow C_1=0\;\hbox { because from above, }\;r=^+_-p


My problem with this assumption ##C_1=0## is I can just as easy say ##(r+1)^2-p^2=0## and claim ##C_0=0##! This will change the whole equation of the Bessel's equation!

Why do I have to follow the book to let ##C_1=0## which result in all ##C_{2n+1}=0##? Is it just because it is simpler and more convenient this way?

You can make either choice. You will still find that the leading term in ##x^{k+r}## in the solution has degree ##p##. Choosing ##C_0\neq 0## makes ##r=p## and the sum over even powers ##k##, while choosing ##C_1\neq 0## makes ##r=p-1## and the sum over odd powers. In either case the series starts with ##x^p## and multiplies this by a polynomial in even powers. So the choice corresponds to shifting the definitions of ##k## and ##r## by ##\pm 1## in such a way that they cancel out in the complete solution.

Also, the book just said let ##C_0=\frac {1}{2^p\Gamma(1+p)}## without explaining why. Why?

I know it is for fitting the formula of:

J_p=\sum_0^{\infty} \frac{(-1)^k}{k! \Gamma(k+p+1)}\left(\frac {x}{2}\right)^{2k+p}

But can you just let ##C_0## to be anything?

Thanks

Yes, since the equation is linear, any multiple of a solution is still a solution. So we can choose any convenient normalization that we want when we define the Bessel functions.
 
Thanks for your answer.
 
Thread 'Direction Fields and Isoclines'
I sketched the isoclines for $$ m=-1,0,1,2 $$. Since both $$ \frac{dy}{dx} $$ and $$ D_{y} \frac{dy}{dx} $$ are continuous on the square region R defined by $$ -4\leq x \leq 4, -4 \leq y \leq 4 $$ the existence and uniqueness theorem guarantees that if we pick a point in the interior that lies on an isocline there will be a unique differentiable function (solution) passing through that point. I understand that a solution exists but I unsure how to actually sketch it. For example, consider a...
Back
Top