34 taylor's remainder theorem ii

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Taylor's Remainder Theorem II

Transcript of 34 taylor's remainder theorem ii

Page 1: 34 taylor's remainder theorem ii

Taylor's Remainder Theorem II

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Taylor's Remainder Theorem II

We state the general form of the Taylor's remainder formula.

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Taylor's Remainder Theorem II

We state the general form of the Taylor's remainder formula.

Taylor's Remainder Theorem (General Form): Let f(x) be an infinitely differentiable function over some open interval that contains [a, b]

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Taylor's Remainder Theorem II

We state the general form of the Taylor's remainder formula.

Taylor's Remainder Theorem (General Form): Let f(x) be an infinitely differentiable function over some open interval that contains [a, b]

a( )[ ]

b

f(x) is infinitely differentiable in here

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Taylor's Remainder Theorem II

We state the general form of the Taylor's remainder formula.

Taylor's Remainder Theorem (General Form): Let f(x) be an infinitely differentiable function over some open interval that contains [a, b] and

pn(x) =

be the n'th Taylor-poly expanded around at a.

a( )[ ]

b

f(x) is infinitely differentiable in here

Σk=0

n (x – a)k

k! f(k)(a)

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Taylor's Remainder Theorem II

We state the general form of the Taylor's remainder formula.

Taylor's Remainder Theorem (General Form): Let f(x) be an infinitely differentiable function over some open interval that contains [a, b] and

pn(x) =

be the n'th Taylor-poly expanded around at a.

Then there exists a "c" between a and b such that

f(b) = pn(b) + (b – a)n+1(n + 1)! f(n+1)(c)

a( )[ ]

bc

f(x) is infinitely differentiable in here

Σk=0

n (x – a)k

k! f(k)(a)

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or in full detail,

f '(a)(b – a)f(2)(a)

+ 2!= f(a) + (b – a)2f(b) ..f(n)(a)

n! (b – a)n+

Taylor's Remainder Theorem II

+ Rn(b)

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or in full detail,

where Rn(b) = (b – a)n+1

(n + 1)! f(n+1)(c)

is the Lagrange form of the Taylor-remainder.

f '(a)(b – a)f(2)(a)

+ 2!= f(a) + (b – a)2f(b) ..f(n)(a)

n! (b – a)n+

Taylor's Remainder Theorem II

+ Rn(b)

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or in full detail,

where Rn(b) = (b – a)n+1

(n + 1)! f(n+1)(c)

is the Lagrange form of the Taylor-remainder.

f '(a)(b – a)f(2)(a)

+ 2!= f(a) + (b – a)2f(b) ..f(n)(a)

n! (b – a)n+

Again, we note the following

Taylor's Remainder Theorem II

+ Rn(b)

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or in full detail,

where Rn(b) = (b – a)n+1

(n + 1)! f(n+1)(c)

is the Lagrange form of the Taylor-remainder.

f '(a)(b – a)f(2)(a)

+ 2!= f(a) + (b – a)2f(b) ..f(n)(a)

n! (b – a)n+

Again, we note the following

* the theorem also works for the interval [b, a]

Taylor's Remainder Theorem II

+ Rn(b)

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or in full detail,

where Rn(b) = (b – a)n+1

(n + 1)! f(n+1)(c)

is the Lagrange form of the Taylor-remainder.

f '(a)(b – a)f(2)(a)

+ 2!= f(a) + (b – a)2f(b) ..f(n)(a)

n! (b – a)n+

Again, we note the following

* the theorem also works for the interval [b, a]

* the value c changes if the value of b or n changes

Taylor's Remainder Theorem II

+ Rn(b)

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or in full detail,

where Rn(b) = (b – a)n+1

(n + 1)! f(n+1)(c)

is the Lagrange form of the Taylor-remainder.

f '(a)(b – a)f(2)(a)

+ 2!= f(a) + (b – a)2f(b) ..f(n)(a)

n! (b – a)n+

Again, we note the following

* the theorem also works for the interval [b, a]

* the value c can't be easily determined, we just know there is at least one c that fits the description

* the value c changes if the value of b or n changes

Taylor's Remainder Theorem II

+ Rn(b)

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Example: A. Find the Taylor-series of f(x) = sin(x) at x = .π

2

Taylor's Remainder Theorem II

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Example: A. Find the Taylor-series of f(x) = sin(x) at x = .π

2sin(x)

cos(x)

-sin(x)

-cos(x)

Taylor's Remainder Theorem II

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Example: A. Find the Taylor-series of f(x) = sin(x) at x = .π

2sin(x)

cos(x)

-sin(x)

-cos(x)

At x = π2 , we get the sequence of coefficients

1, 0, -1, 0, 1, 0, -1, …

Taylor's Remainder Theorem II

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Example: A. Find the Taylor-series of f(x) = sin(x) at x = .π

2sin(x)

cos(x)

-sin(x)

-cos(x)

At x = π2 , we get the sequence of coefficients

1, 0, -1, 0, 1, 0, -1, … So the Taylor expansions is

= 1P(x)

Taylor's Remainder Theorem II

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Example: A. Find the Taylor-series of f(x) = sin(x) at x = .π

2sin(x)

cos(x)

-sin(x)

-cos(x)

At x = π2 , we get the sequence of coefficients

1, 0, -1, 0, 1, 0, -1, … So the Taylor expansions is

– = 1P(x)(x – π/2)2

2!

Taylor's Remainder Theorem II

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Example: A. Find the Taylor-series of f(x) = sin(x) at x = .π

2sin(x)

cos(x)

-sin(x)

-cos(x)

At x = π2 , we get the sequence of coefficients

1, 0, -1, 0, 1, 0, -1, … So the Taylor expansions is

– = 1P(x)(x – π/2)2

2!

1(x – π/2)4

+ 4!

Taylor's Remainder Theorem II

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Example: A. Find the Taylor-series of f(x) = sin(x) at x = .π

2sin(x)

cos(x)

-sin(x)

-cos(x)

At x = π2 , we get the sequence of coefficients

1, 0, -1, 0, 1, 0, -1, … So the Taylor expansions is

– = 1P(x)(x – π/2)2

2!

1(x – π/2)4

+ 4!–

1(x – π/2)6

6!..1(x – π/2)8

+ 8!

Taylor's Remainder Theorem II

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Example: A. Find the Taylor-series of f(x) = sin(x) at x = .π

2sin(x)

cos(x)

-sin(x)

-cos(x)

At x = π2 , we get the sequence of coefficients

1, 0, -1, 0, 1, 0, -1, … So the Taylor expansions is

– = 1P(x)(x – π/2)2

2!

1(x – π/2)4

+ 4!–

1(x – π/2)6

6!..

or P(x) = Σ(-1)n(x – π/2)2n

(2n)!n=0

n =∞

1(x – π/2)8

+ 8!

Taylor's Remainder Theorem II

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Example:

B. Describe the Taylor remainder Rn(b) and show that f(b) = P(b) for all values b. (a = ) π/2

Taylor's Remainder Theorem II

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Example:

B. Describe the Taylor remainder Rn(b) and show that f(b) = P(b) for all values b. (a = )

The remainder Rn(b) = (b – a)n+1

(n + 1)! f(n+1)(c)

π/2

Taylor's Remainder Theorem II

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Example:

B. Describe the Taylor remainder Rn(b) and show that f(b) = P(b) for all values b. (a = )

The remainder Rn(b) = (b – a)n+1

(n + 1)! f(n+1)(c)

=

π/2

(b – )n+1

(n + 1)! f(n+1)(c) π

2

Taylor's Remainder Theorem II

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Example:

B. Describe the Taylor remainder Rn(b) and show that f(b) = P(b) for all values b. (a = )

The remainder Rn(b) = (b – a)n+1

(n + 1)! f(n+1)(c)

=

π/2

(b – )n+1

(n + 1)! f(n+1)(c) π

2

where f(n+1) may be ±sin(x) or ±cos(x) and for some c that is between a and b.

Taylor's Remainder Theorem II

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Example:

B. Describe the Taylor remainder Rn(b) and show that f(b) = P(b) for all values b. (a = )

The remainder Rn(b) = (b – a)n+1

(n + 1)! f(n+1)(c)

=

π/2

(b – )n+1

(n + 1)! f(n+1)(c) π

2

where f(n+1) may be ±sin(x) or ±cos(x) and for some c that is between a and b.

Since |f(n+1)(c)| < 1,

Taylor's Remainder Theorem II

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Example:

B. Describe the Taylor remainder Rn(b) and show that f(b) = P(b) for all values b. (a = )

The remainder Rn(b) = (b – a)n+1

(n + 1)! f(n+1)(c)

=

π/2

(b – )n+1

(n + 1)! f(n+1)(c) π

2

where f(n+1) may be ±sin(x) or ±cos(x) and for some c that is between a and b.

Since |f(n+1)(c)| < 1, we've (b – )n+1

(n + 1)! f(n+1)(c) π

2 <(n + 1)!

(b – )n+1π2

Taylor's Remainder Theorem II

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Example:

B. Describe the Taylor remainder Rn(b) and show that f(b) = P(b) for all values b. (a = )

The remainder Rn(b) = (b – a)n+1

(n + 1)! f(n+1)(c)

=

π/2

(b – )n+1

(n + 1)! f(n+1)(c) π

2

where f(n+1) may be ±sin(x) or ±cos(x) and for some c that is between a and b.

Since |f(n+1)(c)| < 1, we've (b – )n+1

(n + 1)! f(n+1)(c) π

2 <(n + 1)!

(b – )n+1π2

Again, as n we've (n + 1)!

(b – )n+1π2 0∞,

Taylor's Remainder Theorem II

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Example:

B. Describe the Taylor remainder Rn(b) and show that f(b) = P(b) for all values b. (a = )

The remainder Rn(b) = (b – a)n+1

(n + 1)! f(n+1)(c)

=

π/2

(b – )n+1

(n + 1)! f(n+1)(c) π

2

where f(n+1) may be ±sin(x) or ±cos(x) and for some c that is between a and b.

Since |f(n+1)(c)| < 1, we've (b – )n+1

(n + 1)! f(n+1)(c) π

2 <(n + 1)!

(b – )n+1π2

Again, as n we've (n + 1)!

(b – )n+1π2 0∞,

Hence Rn(b) 0 and that f(b) = P(b) for all b.

Taylor's Remainder Theorem II

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Differentiation and Integration of Power Series

The Taylor series of f(x) is the only power series that could be the same as f(x).

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Σk=0

Differentiation and Integration of Power Series

Let f(x) = ck(x – a)k for all x in an open interval

(a – R, a + R) for some R, then the series ck(x – a)k

is the Taylor series P(x) of f(x).

Σk=0

Theorem (Uniqueness theorem for Taylor series) :

The Taylor series of f(x) is the only power series that could be the same as f(x).