
Higher_Mathematics_Part_3
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This series is convergent by d’Alembert’s test if | x | lim |
an+1 |
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< 1. Then |
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an+1 |
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n→∞ |
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lim |
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n→∞ |
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Then the radius of convergence is
R = lim |
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an |
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a |
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n→∞ |
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n+1 |
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By analogy we may use Cauchy’s test and receive
1 |
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R = |
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lim n | a |
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n→∞ |
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Remark. If lim an+1 = 0 then R = ∞.
n→∞ an
(2.4)
(2.5)
2.6.Properties of Power Series
1.Power series (2.2) absolutely and uniformly converges on any segment [−a; a] which lies completely within (−R; R).
2.On every interval completely within the interval of convergence the sum of power series is a continuous function.
3.(Differentiation of power series) We can differentiate a power series term-
by-term within the interval of convergence. If a power series |
S (x) = a0 + |
+ a1x + a2 x2 + ... + an xn + ... has an interval of convergence (−R; R) |
therefore the |
series γ (x) = a1 + 2a2 x + 3a3 x2 + ... + nan xn−1 + ... obtained by termwise differenti-
ation of series |
a + a x + a x2 |
+ ...+ a xn + ... has the same interval of convergence |
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(−R; R) and |
0 |
1 |
2 |
n |
γ (x) = S′ (x) |
within this interval. That is, within the interval of |
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convergence |
the |
derivative of the sum of the power series a0 + a1 x + |
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+ a2 x2 + ... + an xn + ... |
is equal to the sum of the series obtained by termwise |
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differentiation. |
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41 |
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If
∞
S(x) = ∑an xn ,
n=1
then
∞
S′(x) = ∑nan xn−1.
n=1
Theorem If a power series converges in an interval (−R; R), its sum is a
function which has derivatives of any order within the interval of convergence. Each of these derivatives is a sum of the series resulting from term-by-term differentiation of the given series at appropriate number of time. The interval of convergence of each series obtained by differentiation is the same
interval (−R; R).
4. (Integration of power series) If the limits of integration α and β lie within the interval of convergence of a power series then the integral of the sum of the series is equal to the sum of integrals of the terms of series. This series has the
same interval of convergence (−R; R).
∞ |
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If S(x) = ∑an xn then |
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n=1 |
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β |
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β |
∞ |
n |
∞ |
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β |
n |
dx. |
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∫ S(x) dx = ∫ |
∑an x |
dx = ∑ |
∫ an x |
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α |
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α n=1 |
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n=1 α |
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∞ |
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If the segment of integration is [0; x] (−R; R) |
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and S(x) = ∑an xn then |
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n=1 |
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x |
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∞ |
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∞ x |
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∞ |
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xn+1 |
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∫ S(x) dx = ∫ ∑an x |
dx = ∑ ∫ an x |
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dx = ∑an |
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0 |
0 n=1 |
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n=1 0 |
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n=1 |
n + 1 |
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∞ |
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5. We can add, subtract and multiply power series ∑an xn and ∑bn xn |
with |
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radii of convergence R1 |
and |
R2 respectively. |
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n=0 |
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n=0 |
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2.7. Taylor’s Series |
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Suppose a function |
f (x) |
is defined at some neighborhood of a point x0 |
and |
has derivatives of all orders. Can we write this function as a power series in powers of x − x0 ? That is,
f (x) = a |
+ a (x − x ) + a (x − x )2 |
+ ... + a (x − x )n + ... . |
(2.6) |
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0 |
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Let’s find the coefficients of the given series. To do it let’s differentiate a series (2.6) with respect to х:
42
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f (x) = a |
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+ a (x − x ) + a (x − x )2 |
+ ... + a (x − x )n + ... |
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0 |
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f ′(x) = a + |
2a (x − x ) + 3a (x − x )2 |
+ |
...+ na (x − x )n−1 + ... |
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n−2 |
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2a3 (x − x0 ) + 4 3a4 (x − x0 ) |
... + n(n −1)an (x − x0 ) |
+ ... |
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f |
(x) = 2 1a2 + 3 |
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f |
′′′ |
+ 4 3 2a4 (x − x0 ) + ... + n(n − 1)(n − |
2)an (x − x0 ) |
n−3 |
+ ... |
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(x) = 3 2 1a3 |
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. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .
If we substitute x = x0 we get
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a0 = f (x0 ), a1 = |
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f |
′(x ) |
, a2 |
= |
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f ′′(x ) |
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an = |
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f (n) (x ) |
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, …, |
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, … . |
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1! |
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2! |
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n! |
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Therefore a formula (2.6) will be |
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f (x) = f (x |
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f ′(x0 ) |
(x − x |
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f ′′(x0 ) |
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(x − x |
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+ |
f (n) (x ) |
(x − x )n + ... . |
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(2.7) |
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n! |
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Definition. A series |
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f |
′(x ) |
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f ′′(x ) |
(x − x )2 + ... + |
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f (n) (x ) |
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f (x ) + |
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(x − x ) |
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is called a Taylor’s series of a function |
f (x) . |
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If a function f (x) has at a point |
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and its neighborhood all derivatives up |
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to the |
( |
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− th |
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then |
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any |
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this neighborhood |
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Taylor’s formula is true |
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f (x) = f (x0 ) + |
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(x − x0 ) + |
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f ′′(x0 ) |
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+ |
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f |
(n) (x ) |
(x − x )n |
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+ R |
(x) , |
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f (n+1) (c) |
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where |
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R (x) = |
(x − x )n+1 |
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a |
remainder |
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Lagrange’s |
form, |
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c = x0 + θ(x − x0 ), 0 < θ < 1. |
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Taylor’s series (2.8) converges to the function |
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Theorem 1 |
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(x0 − R; x0 + R) |
if and only if a function |
f (x) has derivatives of |
all orders and remaining member of Taylor’s formula tends to zero if n → ∞ for all x from this interval:
lim Rn (x) = 0 , x (x0 − R; x0 + R).
n→∞
43
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Theorem 2 |
If a function |
f (x) has derivatives of all orders in an interval |
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(x0 − R; x0 + R) and there is a number M > 0 such as |
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f (n) (x) |
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x (x0 − R; x0 + R) , n =1, 2, ..., |
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then a function f (x) can be expanded into Taylor’s series. This series converges to the given function.
Definition. If x0 = 0 then series (2.8) is called a Maclaurin’s series. It looks like
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f |
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f |
(n) |
(0) |
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f (x) = f (0) + |
f (0) |
x + |
(0) |
x2 |
+ ... + |
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xn + ... |
(2.9) |
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1! |
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2! |
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2.8. An Expansion of Elementary Functions
into Maclaurin’s Series
To expand a function f (x) into the Maclaurin’s series, it is needed:
1) to calculate values of derivatives f ′(x), f ′′(x), ..., f (n) (x) , ... at point x = 0 ;
2)to write down a series (2.8) and find the interval of its convergence;
3)to define an interval in which remaining member of Maclaurin’s formula
Rn (x) → 0 if n → 0.
Let’s write expansions of some elementary functions into Maclaurin’s series (Table 2.2):
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Table 2.2 |
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Maclaurin’s series of a function |
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f (x) |
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Domain of convergence |
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−∞ < x < ∞ |
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e = 1 + 1! + 2! + 3! + …+ |
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n! + … |
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sin x = x − |
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+ |
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x2n+1 |
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cos x = 1 |
− |
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+ |
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−∞ < x < ∞ |
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4! |
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ln(1+ x) = x − 2 + 3 − …+ (−1) |
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arctg x = x − 3 |
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End of table 2.2
Maclaurin’s series of a function f (x)
(1 + x)m = 1 + |
m |
x + |
m(m − 1) |
x2 + |
m(m − 1)(m − 2) |
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+ |
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+…+ |
m(m − 1)(m − 2) |
(m − (n − 1)) |
xn + … |
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Domain of convergence
−1 ≤ x ≤ 1, if m ≥ 0;
−1 < x ≤ 1,
if m ( − 1; 0);
−1 < x < 1, if m ≤ −1.
−1 < x < 1
−1 < x < 1
2.9. Some Applications of Power Series
The power series are used for the approximate calculation of values of functions, definite integrals, solutions of differential equations which satisfy initial conditions, and others like.
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2.9.1. Approximate Calculation of Values of Functions |
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Suppose we want to calculate the value of function |
f (x) at |
x = x0 . |
If a |
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function f (x) |
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can be expanded in a power series in an interval |
(−R; R) |
and |
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x0 (−R; R) then a value f (x0 ) |
equals the sum of this series at a point |
x = x0 . |
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Approximate |
value equals the |
partial sum Sn (x0 ) . |
An absolute |
error |
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f (x0 ) − Sn (x0 ) |
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= |
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r(x0 ) |
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can be found estimating the remainder of a series rn (x0 ) . |
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Thus for alternating series (series of Leibniz’ Type) the following estimation is true:
r(x0 ) = un+1 (x0 ) − un+2 (x0 ) + … < un+1 (x0 ) .
In the case of series with positive terms we can use the following estimation:
r(x0 ) = un+1 (x0 ) + un+2 (x0 ) + … ≤ un+1 (x0 ) + un+2 (x0 ) + … .
∞
If there exists a series ∑ an with positive terms such as
n=1
un+1 (x0 ) ≤ a1, un+2 (x0 ) ≤ a2 , …,
45
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then
∞
r(x0 ) ≤ ∑ an .
n=1
2.9.2. Approximate Calculation of Definite Integrals
b
Let it is needed to calculate a definite integral ∫ f (x)dx. Suppose an antide-
a
rivative F(x) is not expressed through elementary functions or it is difficult to find it. In this case we make the following actions:
1)set an accuracy of calculation ε > 0 ;
2)expand an integrand f (x) into the power series ( into Maclaurin’s series);
3)use property about term-by-term integration of power series if interval of integration [a; b] belongs to the interval of convergence (−R; R) .
Determination of the error of calculations is the same as for the calculation of values of functions.
2.9.3. Approximate Solution of Differential Equations
Suppose the solution of a differential equation is not expressed through elementary functions or integration of equation is complicated. Then we apply approximate solution of a differential equation using the Taylor’s series.
Suppose it is needed to solve the Cauchy’s problem, that is, to find partial solution of equation
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y′ = |
f (x, y), |
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(2.10) |
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which satisfies an initial condition |
y(x0 ) = y0 . |
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We find the solution of equation as the Taylor’s series |
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y = y(x ) + |
y |
′(x ) |
(x − x ) + |
y′′(x ) |
(x − x )2 + ... + |
y(n) (x ) |
(x − x )n |
+ ... |
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where y(x0 ) = y0 |
is |
the initial condition, and other coefficients |
y′(x0 ), |
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y′′(x ), ..., y(n) (x ),... |
are the subjects to determination. Putting in differential |
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0 |
0 |
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x = x0 , |
y = y0 , we will define a coefficient |
y′(x0 ). That |
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equation (2.10) values |
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is y′(x0 ) = f (x0 , |
y0 ). To find a coefficient y′′(x0 ) we differentiate both parts of |
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equation with respect to x : ( y′)′ = ( f (x, y))′ . We get |
y′′ = f1 (x, y, |
y′) . Putting |
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in right part of this equation |
x = x0 , |
y = y0 , y′ = y′(x0 ) we’ll obtain the value |
y′′(x0 ). Continuing the process of differentiation and substituting in right part of the received equations the known values, we’ll obtain coefficients y′′′(x0 ),
46
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y(4) (x0 ) . Taylor’s series with obtained coefficients is the solution of equation
(2.10) for those values x at which it is convergent. The partial sum of this series is the approximate solution of the Cauchy’s problem.
Remark. 1. Considered method is applicable for the solution of differential equations of any order.
2. We do not examine a question concerning the error of approximate solution of differential equation.
Micromodule 2
EXAMPLES OF PROBLEM SOLUTIONS
Find the domain of convergence of functional series.
∞ |
1 |
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Example 1. ∑ |
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n=1 nx |
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∞ |
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Solution. Generalized harmonic series ∑ |
is convergent for |
p > 1. |
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p |
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n=1 n |
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Then the given |
series converges if x2 + x −1 > 1. That is |
x2 + x − 2 > 0. |
Therefore, the domain of convergence of this series is x (−∞; − 2) (1; ∞).
∞ n
Example 2. ∑ .
n=1 2nx
Solution. The given series is defined for all real x and the terms of this series are positive. Let’s use d’Alembert’s test:
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l(x) = lim |
n + 1 |
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2nx |
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1 |
lim |
n + 1 |
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n→∞ 2(n+1) x |
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2x n→∞ |
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A series is convergent if l(x) < 1. Then |
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x > 0. |
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x = 0. |
∑ |
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Therefore, the domain of convergence of the given series is an interval (0; ∞) .
∞ |
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Example 3. ∑ |
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n=1 |
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Solution. The given series is defined for all real x except one point x = −1. Let’s consider the following cases:
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1) |
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x =1. Then |
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un = |
1 |
doesn’t tend to zero. Therefore the given series is |
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2 |
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divergent if x = 1 ; |
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2) |
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−1 < x < 1. Then |
lim xn = 0, |
lim |
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≠ 0. |
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Therefore |
the given |
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series is divergent; |
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n→∞ |
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3) |
x (−∞; − 1) (1; ∞) . Let’s prove the series to be convergent. |
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∞ |
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The series ∑ |
1 |
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x such as |
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n=1 x |
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xn |
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n→∞ |
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We use comparison test of convergence. Then the given series is convergent for x > 1 .
Therefore, the domain of convergence of the given series is (−∞;−1) (1;∞). Investigate the functional series for uniform convergence.
∞ sin nx
Example 4. ∑ .
n=1 n3
Solution. The given series is defined for all real x (−∞; ∞). It is plus-and- minus functional series. Let’s prove this series to be absolutely and uniformly
∞ 1
convergent for all real x. We use Weierstrass’ test. Numerical series ∑
n=1 n3
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convergent |
and it |
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dominating series for the series ∑ |
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n = 1, 2, |
for all x (−∞; ∞) . Therefore the given series is |
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absolutely and uniformly convergent by Weierstrass’ test. |
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∞ (−1)n+1
Example 5. ∑ . n=1 n + | x |
Solution. The given series is defined for all real x. It is plus-and-minus functional series. It is an alternating functional series. We’ll estimate a
remainder |
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n+1 |
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≤ |
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x (−∞; ∞). Let’s ε > 0. It is needed to specify a number N = N(ε), |
dependent |
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on ε and |
not dependent |
on x, |
that |
for all n > N and for all |
x D the |
following inequality is true
rn (x) < ε.
48
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For the given series |
an |
inequality |
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rn (x) |
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< ε is true for all real x and |
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n > N(ε), where |
N(ε) = |
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a series converges uniformly for all |
x (−∞; ∞) . However this convergence is |
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not absolute because ∑ |
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x | |
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n=1 |
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n=1 n + | x | |
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harmonic series). Consequently, an initial series converges conditionally, but not absolutely.
Find the domain of convergence of power series.
∞ |
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n |
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Example 6. ∑ |
(−1)n+1 |
(x − 5) |
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n |
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n=1 |
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n 3 |
Solution. The given series is a power series. We evaluate the radius of convergence using formula (2.4). We receive
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a |
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(−1)n+1 |
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n+1 |
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(−1)n+ 2 |
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n 3n |
(n + 1) |
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R = lim |
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= 3 lim |
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The interval |
of |
convergence is: |
−3 < x − 5 < 3, 2 < x < 8. |
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Therefore, the |
given series is absolutely convergent within the interval (2; 8).
Let’s investigate the behaviour of the series in the end points of interval. Suppose x = 2. Then this series is divergent:
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Suppose x = 8. |
Then |
∑ (−1)n+1 |
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This series is conditio- |
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nally convergent. |
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Therefore, the domain of convergence of the given series is (2; 8] . |
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Example 7. ∑ n!(x + 2)n . |
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Solution. By formula (2.4) we receive |
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49 |
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The radius of convergence equals zero. Then this power series is convergent at one point x = −2.
∞ |
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Example 8. ∑ |
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x |
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2n + 1 |
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n=1 |
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Solution. Let’s denote x2 = t. We obtain a power series |
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∞ |
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∑ |
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(2.11) |
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n=1 |
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The radius of convergence of this series is calculated by the formula (2.5):
R = |
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= lim |
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lim |
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Therefore, the series (2.11) converges for t (−2; 2). We have to investigate
this series at the end points of interval of convergence. If t = 2, we’ll obtain a numerical series
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n=1 |
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lim |
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the series (2.11) is |
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convergent. By analogy for |
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the series (2.11) is convergent too. Conse- |
quently, the series (2.11) is convergent within interval t (−2; 2). Let’s define the domain of convergence of initial series:
x2 (−2; 2), | x |< 2, − 2 < x < 2.
∞ 2 2
Example 9. ∑ 5n xn .
n=1
Solution. A series is incomplete, that is why application of formulas (2.4), (2.5) is impossible. We use Cauchy’s test and get
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∞, if |
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Consequently, a series converges within interval |
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of the indicated interval a series is divergent.
50
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