Series Solution of Linear Ordinary Differential Equations · Power series method about an ordinary...
Transcript of Series Solution of Linear Ordinary Differential Equations · Power series method about an ordinary...
Series Solution of Linear Ordinary DifferentialEquations
Department of MathematicsIIT Guwahati
SU/KSK MA-102 (2018)
Aim: To study methods for determining series expansions forsolutions to linear ODE with variable coefficients.
In particular, we shall obtain
• the form of the series expansion,
• a recurrence relation for determining the coefficients, and
• the interval of convergence of the expansion.
SU/KSK MA-102 (2018)
Review of power series
A series of the form
∞∑n=0
an(x− x0)n = a0 + a1(x− x0) + a2(x− x0)
2 + · · · , (1)
is called a power series about the point x0. Here, x is avariable and an’s are constants.
The series (1) converges at x = c if∑∞
n=0 an(c− x0)n
converges. That is, the limit of partial sums
limN→∞
N∑n=0
an(c− x0)n <∞.
If this limit does not exist, the power series is said to divergeat x = c.
SU/KSK MA-102 (2018)
Note that∑∞
n=0 an(x− x0)n converges at x = x0 as
∞∑n=0
an(x0 − x0)n = a0.
Q. What about convergence for other values of x?
Theorem: (Radius of convergence)For each power series of the form (1), there is a number R(0 ≤ R ≤ ∞), called the radius of convergence of the powerseries, such that the series converges absolutely for|x− x0| < R and diverge for |x− x0| > R.
If the series (1) converges for all values of x, then R =∞.When the series (1) converges only at x0, then R = 0.
SU/KSK MA-102 (2018)
Theorem: (Ratio test) If
limn→∞
∣∣∣∣an+1
an
∣∣∣∣ = L,
where 0 ≤ L ≤ ∞, then the radius of convergence (R) of thepower series
∑∞n=0 an(x− x0)
n is
R =
1L
if 0 < L <∞,∞ if L = 0,0 if L =∞.
Remark. If the ratio∣∣∣an+1
an
∣∣∣ does not have a limit, then
methods other than the ratio test (e.g. root test) must beused to determine R.
SU/KSK MA-102 (2018)
Example: Find R for the series∑∞
n=0(−2)nn+1
(x− 3)n.
Note that an = (−2)nn+1
. We have
limn→∞
∣∣∣∣an+1
an
∣∣∣∣ = limn→∞
∣∣∣∣(−2)n+1(n + 1)
(−2)n(n + 2)
∣∣∣∣ = limn→∞
2(n + 1)
(n + 2)= 2 = L.
Thus, R = 1/2. The series converges absolutely for|x− 3| < 1
2and diverge for |x− 3| > 1
2.
Next, what happens when |x− 3| = 1/2?
At x = 5/2, the series becomes the harmonic series∑∞
n=01
n+1,
and hence diverges. When x = 7/2, the series becomes analternating harmonic series, which converges.
Thus, the power series converges for each x ∈ (5/2, 7/2].
SU/KSK MA-102 (2018)
Given two power series
f(x) =∞∑n=0
an(x− x0)n, g(x) =
∞∑n=0
bn(x− x0)n,
with nonzero radii of convergence. Then
f(x) + g(x) =∞∑n=0
(an + bn)(x− x0)n
has common interval of convergence.The formula for the product is
f(x)g(x) =∞∑n=0
cn(x− x0)n, where cn :=
n∑k=0
akbn−k. (2)
This power series in (2) is called the Cauchy product and willconverge for all x in the common interval of convergence forthe power series of f and g.
SU/KSK MA-102 (2018)
Differentiation and integration of power series
Theorem: If f(x) =∑∞
n=0 an(x− x0)n has a positive radius of
convergence R, then f is differentiable in the interval|x− x0| < R and termwise differentiation gives the powerseries for the derivative:
f ′(x) =∞∑n=1
nan(x− x0)n−1 for |x− x0| < R.
Furthermore, termwise integration gives the power series forthe integral of f :∫
f(x)dx =∞∑n=0
ann + 1
(x− x0)n+1 + C for |x− x0| < R.
SU/KSK MA-102 (2018)
Example: A power series for
1
1− x= 1 + x + x2 + x3 + · · ·+ · · · .
Since ddx{1/(1− x)} = 1
(1−x)2 , we obtain a power series for
1
(1− x)2= 1 + 2x + 3x2 + 4x3 + · · ·+ nxn−1 + · · · .
A power series for
1
1 + x2= 1− x2 + x4 − x6 + · · ·+ (−1)nx2n + · · · .
Since tan−1 x =∫ x
01
1+t2dt, integrate the series for 1
1+x2
termwise to obtain
tan−1 x = x− 1
3x3 +
1
5x5 − 1
7x7 + · · ·+ (−1)nx2n+1
2n + 1+ · · · .
SU/KSK MA-102 (2018)
Shifting the summation index
The index of a summation in a power series is a dummy indexand hence
∞∑n=0
an(x− x0)n =
∞∑k=0
ak(x− x0)k =
∞∑i=0
ai(x− x0)i.
Shifting the index of summation is particularly important whenone has to combine two different power series.
Example:
∞∑n=2
n(n− 1)anxn−2 =
∞∑k=0
(k + 2)(k + 1)ak+2xk.
x3
∞∑n=0
n2(n− 2)anxn =
∞∑n=3
(n− 3)2(n− 5)an−3xn.
SU/KSK MA-102 (2018)
Adding two power series
Problem: Write Σ∞n=12ncnxn−1 + Σ∞n=06cnx
n+1 as one series.In order to add the series, we require that both summationindices start with the same number and that the powers of xin each series be “in phase”;that is, if one series starts with amultiple of x1 say, then we want the other series also to startwith the same power of x. By writing
Σ∞n=12ncnxn−1 + Σ∞n=06cnx
n+1
= 2.1.c1x0 + Σ∞n=22ncnx
n−1 + Σ∞n=06cnxn+1
we have both the series Σ∞n=22ncnxn−1 and Σ∞n=06cnx
n+1 ofthe right hand side of the above equation start with x1.
SU/KSK MA-102 (2018)
To get the same summation index, we are inspired by the exponents of x.We let k = n− 1 in the first series and let k = n+ 1 in the second series.Thus the right hand side of the above equation becomes
2c1 + Σ∞k=12(k + 1)ck+1xk + Σ∞k=16ck−1x
k
= 2c1 + Σ∞k=1[2(k + 1)ck+1 + 6ck−1]xk
which is the required form (as a single series) of the sum of the two givenseries.
SU/KSK MA-102 (2018)
Definition: (Analytic function)A function f is said to be analytic at x0 if it has a power seriesrepresentation
∑∞n=0 an(x− x0)
n in an neighborhood aboutx0, and has a positive radius of convergence.
Example: Some analytic functions and their representations:
ex =∞∑n=0
xn
n!.
sinx =∞∑n=0
(−1)n
(2n + 1)!x2n+1.
lnx =∞∑n=1
(−1)n−1
n(x− 1)n, x > 0.
SU/KSK MA-102 (2018)
Power series solutions to linear ODEs
Consider linear ODE of the form:
a2(x)y′′(x) + a1(x)y′(x) + a0(x)y(x) = 0, a2(x) 6= 0. (∗)
Writing in the standard form
y′′(x) + p(x)y′(x) + q(x)y(x) = 0,
where p(x) := a1(x)/a2(x) and q(x) := a0(x)/a2(x).
Definition: A point x0 is called an ordinary point of (∗) if bothp(x) = a1(x)/a2(x) and q(x) = a0(x)/a2(x) are analytic atx0. If x0 is not an ordinary point, it is called a singular pointof (∗).
SU/KSK MA-102 (2018)
Fact from Analysis: If p(x) and q(x) are polynomilas in x having no
common factors, then p(x)q(x) is analytic at all points where q(x) 6= 0. And
at the points where q(x) = 0, the function p(x)q(x) is not analytic.
SU/KSK MA-102 (2018)
Example: The differential equation xy′′ + (Sin x)y = 0 has anordinary point at x = 0 because
Sin x
x= 1− x2
3!+
x4
5!− · · · .
The singular points of the equation (x2− 1)y′′+ 2xy′+ 6y = 0are 1 and −1. All other points are ordinary points.The equation (x2 + 1)y′′ + xy′ − y = 0 has two singular pointsgiven by i,−i. All other finite values of x (real or complex),are ordinary points.
SU/KSK MA-102 (2018)
Power series method about an ordinary point
Consider the equation
2y′′ + xy′ + y = 0. (∗∗)
Let’s find a power series solution about x = 0. Seek a powerseries solution of the form
y(x) =∞∑n=0
anxn,
and then attempt to determine the coefficients an’s.Differentiate termwise to obtain
y′(x) =∞∑n=1
nanxn−1, y′′(x) =
∞∑n=2
n(n− 1)anxn−2.
SU/KSK MA-102 (2018)
Substituting these power series in (∗∗), we find that
∞∑n=2
2n(n− 1)anxn−2 +
∞∑n=1
nanxn +
∞∑n=0
anxn = 0.
By shifting the indices, we rewrite the above equation as
∞∑k=0
2(k + 2)(k + 1)ak+2xk +
∞∑k=1
kakxk +
∞∑k=0
akxk = 0.
Combining the like powers of x in the three summation toobtain
4a2 + a0 +∞∑k=1
[2(k + 2)(k + 1)ak+2 + kak + ak]xk = 0.
SU/KSK MA-102 (2018)
Equating the coefficients of this power series equal to zeroyields
4a2 + a0 = 0
2(k + 2)(k + 1)ak+2 + (k + 1)ak = 0, k ≥ 1.
This leads to the recurrence relation
ak+2 =−1
2(k + 2)ak, k ≥ 1.
Thus,
a2 =−1
22a0, a3 =
−1
2 · 3a1
a4 =−1
2 · 4a2 =
1
22 · 2 · 4a0, a5 =
−1
2 · 5a3 =
1
22 · 3 · 5a1
· · · · · ·
SU/KSK MA-102 (2018)
With a0 and a1 as arbitrary constants, we find that
a2n =(−1)n
22nn!a0, n ≥ 1,
and
a2n+1 =(−1)n
2n[1 · 3 · 5 · · · (2n + 1)]a1, n ≥ 1.
From this, we have two linearly independent solutions as
y1(x) =∞∑n=0
(−1)n
22nn!x2n,
y2(x) =∞∑n=0
(−1)n
2n[1 · 3 · 5 · · · (2n + 1)]x2n+1.
SU/KSK MA-102 (2018)
Hence the general solution is
y(x) = a0y1(x) + a1y2(x).
Remark. Suppose we are given the value of y(0) and y′(0),then a0 = y(0) and a1 = y′(0). These two coefficients leads toa unique power series solution for the IVP.
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SU/KSK MA-102 (2018)