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Convergence and Divergence of Series: Geometric and Harmonic Series, Study notes of Signals and Systems

An in-depth analysis of series, their partial sums, and the conditions for convergence and divergence. It covers geometric series, telescopic series, and the harmonic series, with proofs and examples. Students of mathematics, particularly those studying calculus or advanced algebra, will find this document useful for understanding the concepts of series and their properties.

What you will learn

  • How do you find the sum of a geometric series?
  • Why does the harmonic series diverge?
  • What is the definition of a convergent series?

Typology: Study notes

2021/2022

Uploaded on 09/27/2022

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4.2. SERIES 87
4.2. Series
Aseries is an infinite sum:
X
n=1
an=a1+a2+a3+···+an+···
In order to define the value of this sum we start be defining its
sequence of partial sums
sn=
n
X
i=1
ai=a1+a2+···+an.
Then, if limn→∞ sn=sexists the series is called convergent and its
sum is that limit:
X
n=1
an=s= lim
n→∞ sn.
Otherwise the series is called divergent.
For instance, consider the following series:
1
2+1
22+1
23+···+1
2n+···=
X
n=1
1
2n.
Its partial sums are:
sn=
n
X
i=1
1
2i=1
2+1
22+···+1
2n= 1 1
2n.
Hence its sum is
X
n=1
1
2n= lim
n→∞
n
X
i=1
1
2i= lim
n→∞ µ11
2n= 1 + 0 = 1 .
4.2.1. Geometric Series. A series verifying an+1 =ran, where r
is a constant, is called geometric series. If the first term is a6= 0 then
the series is
a+ar +ar2+···+arn+···=
X
n=0
arn.
The partial sums are now:
sn=
n
X
i=0
ari.
pf3
pf4

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4.2. Series

A series is an infinite sum: ∑^ ∞

n=

an = a 1 + a 2 + a 3 + · · · + an + · · ·

In order to define the value of this sum we start be defining its sequence of partial sums

sn =

∑^ n

i=

ai = a 1 + a 2 + · · · + an.

Then, if limn→∞ sn = s exists the series is called convergent and its sum is that limit: ∑∞

n=

an = s = lim n→∞ sn.

Otherwise the series is called divergent.

For instance, consider the following series: 1 2

2 n^

∑^ ∞

n=

2 n^

Its partial sums are:

sn =

∑^ n

i=

2 i^

2 n^

2 n^

Hence its sum is ∑^ ∞

n=

2 n^

= lim n→∞

∑^ n

i=

2 i^

= lim n→∞

2 n

4.2.1. Geometric Series. A series verifying an+1 = ran, where r is a constant, is called geometric series. If the first term is a 6 = 0 then the series is

a + ar + ar^2 + · · · + arn^ + · · · =

∑^ ∞

n=

arn^.

The partial sums are now:

sn =

∑^ n

i=

ari^.

The nth partial sum can be found in the following way:

sn = a + ar + ar^2 + · · · + arn rsn = ar + ar^2 + · · · + arn^ + arn+

hence

sn − rsn = a + 0 + 0 + · · · + 0 − arn+1^ ,

so:

sn =

a(1 − rn+1) 1 − r

If |r| < 1 we can rewrite the result like this:

sn =

a 1 − r

a 1 − r

rn+1^ ,

and then get the limit as n → ∞:

s = lim n→∞

sn =

a 1 − r

a 1 − r

lim n→∞

rn+ ︸ ︷︷ ︸ ↓ 0

a 1 − r

So for |r| < 1 the series is convergent and

∑^ ∞

n=

arn^ =

a 1 − r

For |r| ≥ 1 the series is divergent.

4.2.2. Telescopic Series. A telescopic series is a series whose terms can be rewritten so that most of them cancel out.

Example: Find

∑^ ∞

n=

n(n + 1)

Answer : Note that

n(n + 1)

n

n + 1

. So the nth partial sum

is

sn =

∑^ ∞

i=

i

i + 1

n

n + 1 = 1 −

n + 1

Example: Show that

∑^ ∞

n=

sin n diverges.

Answer : All we need to show is that sin n does not tend to 0. If for some value of n, sin n ≈ 0, then n ≈ kπ for some integer k, but then

sin (n + 1) = sin n cos 1 + cos n sin 1 ≈ sin kπ cos 1 + cos kπ sin 1 = 0 ± sin 1 = ± 0. 84 · · · 6 = 0

So if a term sin n is close to zero, the next term sin (n + 1) will be far from zero, so it is impossible for sin n to get permanently closer and closer to 0.

4.2.6. Operations with Series. If

n=1 an^ and^

n=1 bn^ are con- vergent series and c is a constant then the following series are also convergent and:

∑^ ∞

n=

can = c

∑^ ∞

n=

an

∑^ ∞

n=

(an + bn) =

∑^ ∞

n=

an +

∑^ ∞

n=

bn

∑^ ∞

n=

(an − bn) =

∑^ ∞

n=

an −

∑^ ∞

n=

bn