Maths encyclopedia and lessons  
Search

Mathematics Encyclopedia and Lessons

 
     
 

Lessons

Popular
Subjects

algebra
arithmetic
calculus
equations
geometry
differential equations
trigonometry
number theory
probability theory
more
 

References

applied mathematics
mathematical games
mathematicians
more
 
 

Frobenius method

In mathematics, the Frobenius method describes a way to find an infinite series solution for a second-order ordinary differential equation of the form

z^2u''+p(z)zu'+q(z)u=0\!\;

We can divide through by z2 to obtain a differential equation of the form

u''+{p(z) \over z}u'+{q(z) \over z}u=0

which we can solve with regular power series methods if p(z)/z or q(z)/z are analytic at z = 0, but of course these functions are not. The Frobenius method enables us to create a power series solution to such a differential equation.

Explanation

The Frobenius method tells us that we can seek a power series solution of the form

u(z)=\sum_{k=0}^{\infty} A_kz^{k+r}

Differentiating:

u'(z)=\sum_{k=0}^{\infty} (k+r)A_kz^{k+r-1}
u''(z)=\sum_{k=0}^{\infty} (k+r-1)(k+r)A_kz^{k+r-2}

Substituting:

z^2\sum_{k=0}^{\infty} (k+r-1)(k+r)A_kz^{k+r-2}+zp(z)\sum_{k=0}^{\infty} (k+r)A_kz^{k+r-1}+q(z)\sum_{k=0}^{\infty} A_kz^{k+r}
=\sum_{k=0}^{\infty} (k+r-1)(k+r)A_kz^{k+r}+p(z)\sum_{k=0}^{\infty} (k+r)A_kz^{k+r}+q(z)\sum_{k=0}^{\infty} A_kz^{k+r}
=\sum_{k=0}^{\infty} (k+r-1)(k+r)A_kz^{k+r}+p(z)(k+r)A_kz^{k+r}+q(z)A_kz^{k+r}
=\sum_{k=0}^{\infty} ((k+r-1)(k+r)+p(z)(k+r)+q(z))A_kz^{k+r}
=(r(r-1)+p(0)r+q(0))A_0z^r+\sum_{k=1}^{\infty} ((k+r-1)(k+r)+p(z)(k+r)+q(z))A_kz^{k+r}

The expression r(r-1)+p(0)r+q(0)=I(r) is known as the indicial polynomial, which is quadratic in r.

Using this, the general expression of the coefficient of zk+r is

I(k+r)A_k+\sum_{j=0}^{k-1}((j+r)p(k-j)+q(k-j))A_j

These coefficients must be zero, since they are to be solutions of the differential equation, so

I(k+r)A_k+\sum_{j=0}^{k-1}((j+r)p(k-j)+q(k-j))A_j=0
\sum_{j=0}^{k-1}((j+r)p(k-j)+q(k-j))A_j=-I(k+r)A_k
{1\over-I(k+r)}\sum_{j=0}^{k-1}((j+r)p(k-j)+q(k-j))A_j=A_k

The series solution with Ak above,

U_{r}(z)=\sum_{k=0}^{\infty}A_kz^{k+r}

satisfies

z^2U_{r}(z)''+p(z)zU_{r}(z)'+q(z)U_{r}(z)=I(r)z^{r}\!\;

If we choose one of the roots to the indicial polynomial for r in Ur(z), we gain a solution to the differential equation. If the difference between the roots is not an integer, we get another, linearly independent solution in the other root.

Example

Let us solve

z^2f''-zf'+(1-z)f=0\,

Divide throughout by z2 to give

f''-{z\over z^2}f'+{1-z\over z^2}f=f''+{1\over z}f'+{1-z \over z^2}f=f''+{1\over z}f'+({1\over z^2}-{1\over z})f=0

which has the requisite singularity at z=0.

Use the series solution

f   = \sum_{k=0}^\infty A_kz^{k+r}
f'  = \sum_{k=0}^\infty (k+r)A_kz^{k+r-1}
f'' = \sum_{k=0}^\infty (k+r)(k+r-1)A_kz^{k+r-2}

Now, substituting

\sum_{k=0}^\infty (k+r)(k+r-1)A_kz^{k+r-2}-{1\over z}\sum_{k=0}^\infty (k+r)A_kz^{k+r-1}+({1\over z^2}-{1\over z})\sum_{k=0}^\infty A_kz^{k+r}
= \sum_{k=0}^\infty (k+r)(k+r-1)A_kz^{k+r-2}-{1\over z}\sum_{k=0}^\infty (k+r)A_kz^{k+r-1}+{1\over z^2}\sum_{k=0}^\infty A_kz^{k+r}-{1\over z}\sum_{k=0}^\infty A_kz^{k+r}
= \sum_{k=0}^\infty (k+r)(k+r-1)A_kz^{k+r-2}-\sum_{k=0}^\infty (k+r)A_kz^{k+r-2}+\sum_{k=0}^\infty A_kz^{k+r-2}+\sum_{k=0}^\infty A_kz^{k+r-1}

We need to shift the final sum.

= \sum_{k=0}^\infty (k+r)(k+r-1)A_kz^{k+r-2}-\sum_{k=0}^\infty (k+r)A_kz^{k+r-2}+\sum_{k=0}^\infty A_kz^{k+r-2}+\sum_{k-1=0}^\infty A_{k-1}z^{k+r-2}
= \sum_{k=0}^\infty (k+r)(k+r-1)A_kz^{k+r-2}-\sum_{k=0}^\infty (k+r)A_kz^{k+r-2}+\sum_{k=0}^\infty A_kz^{k+r-2}+\sum_{k=1}^\infty A_{k-1}z^{k+r-2}

We can take one element out of the sums that start with k=0 to obtain the sums starting at the same index.

= ((r)(r-1)A_0z^{r-2})+\sum_{k=1}^\infty (k+r)(k+r-1)A_kz^{k+r-2}-((r)A_0z^{r-2})+\sum_{k=1}^\infty (k+r)A_kz^{k+r-2}
+(A_0z^{r-2})+\sum_{k=1}^\infty A_kz^{k+r-2}+\sum_{k=1}^\infty A_{k-1}z^{k+r-2}
= (r(r-1)-r+1)A_0z^{r-2}+\,
\sum_{k=1}^\infty \left(  ((k+r)(k+r-1)+(k+r)+1)A_k + A_{k-1}  \right)z^{k+r-2}

We obtain one linearly independent solution by solving the indicial polynomial r(r-1)-r+1 = r2-2r+1 =0 which gives a double root of 1. Using this root, we set the coefficient of zk+r-2 to be zero (for it to be a solution), which gives us the recurrence

((k+1)(k)+(k+1)+1)A_k + A_{k-1}  =(k^2+2k+2)A_k+A_{k-1}=0\,
A_k = {-A_{k-1}\over k^2+2k+2}

Given some initial conditions, we can either solve the recurrence entirely or obtain a solution in power series form.

External links

The Frobenius method can be generalized to orders of ordinary differential equation greater than two, see

01-04-2007 01:18:14
The contents of this article are licensed from Wikipedia.org
under the GNU Free Documentation License. How to see transparent copy