Transcript Document

Chapter 1: Infinite Series I. Background

• An infinite series is an expression of the form:

n

   1

a n

 

1

a

2

a

3

a n

 ...

where there is some rule for how the a’s are related to each other.

Ch. 1- Infinite Series>Background

ex:

2) 1 2 4 1 8 ...

2

x

3

2  ...

Ch. 1- Infinite Series>Background •

Why do physicists care about infinite series?

1) Loads of physics problems involve infinite series.

ex:

Dropped ball- how far does it travel?

d h h

2

h

4

h

8 ...

ex:

Swinging pendulum- how long until it stops swinging? (or will it ever stop?) T stop  4

s

 4

s

3  4

s

6  ...

*picture?*

Ch. 1- Infinite Series>Convergence and Divergence 2) Complicated math expressions can be approximated by series and then solved more easily.

ex:

e x

 

(1

x

3 

3

x

4

6

...)

dx

II. Convergence and Divergence

• How do we know if a series has a finite sum? (eg. will the pendulum ever stop?)

defn:

Mathematics terminology- The series converges if it has a finite sum; otherwise, the series diverges.

defn:

We define the sum of a series (if it has one) to be:

S n

k n

  1

a k a

a n S

lim

x



S n

terms of the series.

ex:

n

   1 1

n

1 2 1 3 1 4 ...

doesn’t converge. It approaches zero too slowly. (Proof in hw)

Ch. 1- Infinite Series>Convergence and Divergence>Geometric Series

A. Geometric series

• Each term is multiplied by a fixed number to get the next term.

a

ar

ar

2

ar

3

...

ex:

1) 1 + 3 + 9 + 27 + ... 2) 2 – 5 + 18 – 54 + ... • We can show that only for a geometric series, the sum of the first

n

terms is

S n

a

(1 

r n

) 1 

r

Proof:

S n ar

ar

2 

S r n S n

ar

S r n

ar

2 

ar ar n

3

ar

3 

S n

(1

r a

(1 

r n

) 

S n

a

(1 

r n

) (1 

r

)

ar n ar n

 1 (geometric series only)

Ch. 1- Infinite Series>Convergence and Divergence>Geometric Series The sum of the geometric series is then:

S

x

lim 

S n

x

lim 

a

(1 

r n

) (1 

r

) n if r >1, then r gets infinitely big as n   , so S     , so

S

a

1-

r

(for |r|<1, geometric series only)

ex:

0 .

555 5

5 10

5 100

5 1000

...

a

ar

2 

ar

3 

...

where

a

5 10

, r

1 10

ex:

0.583333…

Ch. 1- Infinite Series>Convergence and Divergence>Alternating Series

B. Alternating Series:

Series whose terms are alternately positive and negative.

ex:

1 ) 1  2  3  4  5 

...

2 )  1  1 2  1 4  1 8 

...

• Test for converging for alternating series: An alternating series converges if the absolute value of the terms decreases steadily to zero. and

n

1

a n

lim

n

 

a n

 0

ex:

n

   1

a n

  1  1 2  1 4  1 8  ...

Ch. 1- Infinite Series>Convergence and Divergence>More General Results>Preliminary Test

C. More general results:

There are loads of other types of series besides geometric and alternating. So, how do we find whether a general series converges? This is a hard problem. Here are some simple tests (tons more exist). We’ll look at 3 tests:

1) Preliminary Test:

If the terms of an infinite series do not tend to zero (

a n

 0 ) , then the series diverges.

n

lim   Note: this test does not tell you whether the series converges. It only weeds out wickedly divergent series.

ex:

1 ) 1 3  2 3  3 3  4 3  ...

2 ) 1 3  1 6  1 12  1 24  ...

Ch. 1- Infinite Series>Convergence and Divergence>More General Results>Preliminary Test The next tests are for convergence of series of positive terms, or for absolute convergence of a series with either all positive or some negative terms.

defn:

Say we have a series (series #1) with some negative terms. Then say we make a new series (series #2) by taking the absolute value of each term in the original series. If series #2 converges, then we say series #1 converges absolutely.

ex:

n

   1

a n

 

1

let  

n

 1

b n

1

1 2

1 2

1 4

1 4 1 8

...

1 8

...

If ∑b n converges, then ∑a n converges absolutely.

Thm: If a series converges absolutely, then it converges. (eg, if ∑b n converges, then ∑a n converges in above example.)

Ch. 1- Infinite Series>Convergence and Divergence>More General Results>Comparison Test

2) Comparison Test: ex:

a) Compare your series a 1 +a 2 +a 3 +… to a series known to converge m

a n

m n

1 +m 2 +m 3 +….

a 1 +a 2 +a 3 +… is absolutely convergent.

b) Compare your series a 1 +a 2 +a 3 +… to a series known to diverge d

a n

d

1 +d 2 +d 3 +….

If for all n from some point on, then the series

n

a 1 +a 2 +a 3 +… is divergent.

n

   1 1

n

2  1  1 4  1 9  1 16  1 25  ...

does this converge?

Ch. 1- Infinite Series>Convergence and Divergence>More General Results>Ratio Test

3) Ratio Test:

For this test, we compare a n+1 in the limit of large n: to a n : Ratio test: If p < 1, the series converges.

If p = 1, use a different test. If p > 1, the series diverges.

ex:

n

   1

2

n n

2

ex:

Harmonic Series

n

   1 1

n

III. Power Series defn:

A power series is of the form:

n

   1

a n

(

x

a

)

n

a

0 

a

1 (

x

a

) 

a

2 (

x

a

) 2  ...

where the coefficients a n are constants.

Note: Commonly, we see power series with a=0:

n

   1

a n

(

x

)

n

a

0 

a

1

x

a

2

x

2  ...

ex:

1 )

x

x

2 

x

3  ...

2 ) 1  1 2 3 ) 1 3

x

x

1 6  1 4

x

2 

x

2  1 8 1 9

x

3  ...

x

3  ...

Ch. 1- Infinite Series>Power Series

Ch. 1- Infinite Series>Power Series>Convergence

A. Convergence

of a power series depends on the values of x. m

ex:

1 3

x

 1 6

x

2  1 9

x

3  ...

 3 1

n x n

 ...

Ch. 1- Infinite Series>Power Series>Convergence We must consider the endpoints ±1 separately: (because these points fail the ratio test) ??? keep the following ????

if x = -1: converges by alternating series test.

if x = 1: (harmonic series), so it diverges at x=1.

Thus, our power series converges for 1≤ x <1 and diverges otherwise.

Ch. 1- Infinite Series>Power Series>Expanding Functions

B. Expanding functions as power series:

From the previous section, we know that the sum of a power series depends on x:

S

(

x

) 

n

   0

a n

(

x

a

)

n

So, S(x) is a function of x!

Useful trick: Try to expand a given function f(x) as a power series (Taylor series.) (We often do this when the original function is too complex to use easily.)

ex:

f(x) = e x

Ch. 1- Infinite Series>Power Series>Expanding Functions

More generally:

How do we find the Taylor Series expansion of a general function f(x):

f

(

x

) 

a

0 

a

1 (

x

a

) 

a

2 (

x

a

) 2 

a

3 (

x

a

) 3  ...

(This approximates f(x) near the point x=a.) Here’s how:

f

(

x

) 

a

0 

a

1 (

x

a

) 

a

2 (

x

a

) 2 

a

3 (

x

a

) 3 

a

4 (

x

a

) 4  ...

f

' (

x

) 

e x

a

1  2

a

2 (

x

a

)  3

a

3 (

x

a

) 2  4

a

4 (

x

a

) 3  ...

f

'' (

x

) 

e x

 2

a

2  6

a

3 (

x

a

)  12

a

4 (

x

a

) 2  ...

f

' '' (

x f n

(

x

) ) 

e x

 6

a

3  24

a

4 (

x

a

)  ...

n

!

a n

 (

n

 1 )!

a n

 1 (

x

a

) 1  (

n

 2 )!

a n

 2 (

x

a

) 2  ...

Evaluating each of these at x=a:

f f f f f

(

x

' (

x

 

a

)

a

)  

a

0

a

1  

a

0

a

1 '' (

x

a

)  2

a

2   

a

2 ' '' (

x

a

)  6

a

3 

a

3

f f

(

a

)   ' (

a

) 1 2 1 6

f f

' '' (

a

) '' (

a

)

n

(

x

a

) 

n

!

a n

a n

 1

n

!

f n

(

a

) So, our Taylor series expansion of f(x) about the point x=a is:

f

(

x

) 

a

0 

a

1 (

x

a

) 

a

2 (

x

a

) 2 

a

3 (

x

a

) 3 

a

4 (

x

a

) 4  ...

f(x)  f(a)  f' (a)(x  a)  1 2!

f'' (a)(x  a) 2  1 3!

f''' (a)(x  a) 3  ...

 1 n!

f n (a)(x  a) n  ...

defn:

a MacLaurin Series is a Taylor Series with a=0. Ch. 1- Infinite Series>Power Series>Expanding Functions

ex:

f(x) = sin(x) ex: Electric field of a dipole

Ch. 1- Infinite Series>Power Series>Expanding Functions And, you can do all sorts of math with these series to get other series… (see section 13 for examples) ex: (x 2 +3) sin(x) (find the MacLaurin Series expansion.) ex: sin(x 2 )