assignment 14

course Mth 174

֌jЪ۔}Zassignment #014

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Physics II

11-15-2006

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23:42:42

query problem 10.1.23 (3d edition 10.1.20) (was 9.1.12) g continuous derivatives, g(5) = 3, g'(5) = -2, g''(5) = 1, g'''(5) = -3

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23:46:40

what are the degree 2 and degree 3 Taylor polynomials?

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degree 2 = 3-2(x-5)+.5(x-5)^2

degree 3 = 3-2(x-5)+.5(x-5)^2+.5(x-5)^3

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23:47:42

What is each polynomial give you for g(4.9)?

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degree 2 = 3.205

degree 3 = 3.2055

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23:49:21

What would g(4.9) be based on a straight-line approximation using graph point (5,3) and the slope -2? How do the Taylor polynomials modify this tangent-line estimate?

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Using the standard form y-y1=m(x-x1) we obtain the equation

y-3=-2(x-5), which simplifies to

y =-2x+13

Evaluating at x = 4.9 we obtain

Y =-2(4.9)+13

=-9.8+13

=3.2.

This is identical, as must be the case, with the first-degree Taylor polynomial y = 3-2(x-5), which simplifies to y = -2 x + 13.

This is close to both the second- and third-degree approximations, but not as accurate as either. The third-degree approximation is the most accurate.

The second-degree polynomial adds .05 to the linear approximation, while the third-degree polynomial adds another .005 to the second-degree approximation.

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23:49:30

query problem 10.1.35 (3d edition 10.1.33) (was 9.1.36) estimate the integral of sin(t) / t from t=0 to t=1

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23:49:34

what is your degree 3 approximation?

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23:49:37

what is your degree 5 approximation?

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23:49:40

What is your Taylor polynomial?

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degree 3 = x - x^3/3! degree 5 = x-x^3/3!+x^5/5!

These are the polynomials for sin(x). To get the polynomials for sin(t) / t you would have to substitute t for x, then divide by t. The to answer the question given in the problem, you would have to integrate the resulting polynomial over the given interval.

The degree 3 approximation of sin(t) is sin(t) = t - t^3 / 6, approx.

So sin(t) / t = 1 - t^2 / 6, approx.

The degree 5 approximations are sin(t) = t - t^3 - 6 + t^5 / 120 approx., and sin(t) / t = 1 - t^2 / 6 + t^4 / 120

Antiderivatives would be

integral( sin(t) / t) = t - t^3 / 18 approx. and

integral( sin(t) / t) = t - t^3 / 18 + t^5 / 600, approx.

The definite integrals would be found using the Fund Thm. You would get

1 - 1/18 = .945 approx. and

1 - 1/18 + 1/600 = .947 approx.

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23:49:44

Explain in your own words why a trapezoidal approximation will not work here.

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GOOD STUDENT RESPONSE:

I think that a trapezoid approximation won`t work well because of the shape of the graph of the sin t. Also, it definently won`t work for our initial expression from the book, because the fn is undefined at t=0. The altitudes of each line go from being too small to too large and so on. Perhaps that is the reason, but I am not completely certain.

INSTRUCTOR RESPONSE: The biggest problem is the undefined value at t = 0, which you recognize in your answer. Very good.

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23:49:54

Query problem 10.2.25 (3d edition 10.2.21) (was 9.2.12) Taylor series for ln(1+2x)

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23:49:57

show how you obtained the series by taking derivatives

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ln(1 + 2x) is a composite function. Its successive derivatives are a little more complicated than the derivatives of most simple function, but are not difficult to compute, and form a pattern.

ln(1 + 2x) = f(g(x)) for f(z) = ln(z) and g(x) = 1 + 2x.

f ' (z) = 1 / z, and g ' (x) = 2. So the derivative of ln(1 + 2x) is

f ' (x) = (ln(1 + 2x) ) ' = g ' (x) * f ' ( g(x) ) = 2 * (1 / g(x) ) = 2 / ( 1 + 2x).

Then

f ''(x) = (2 / ( 1 + 2x) )' = -1 * 2 * 2 / (1 + 2x)^2 = -4 / (1 + 2x)^2.

f '''(x) = ( -4 / (1 + 2x)^2 ) ' = -2 * 2 * (-4) = 16 / (1 + 2x)^3

etc.. The numerator of every term is equal to the negative of the power in the

denominator, multiplied by 2 (for the derivative of 2 + 2x), multiplied by the previous numerator. A general expression would be

f [n] (x) = (-1)^(n-1) * (n - 1)! * 2^n / ( 1 + 2x) ^ n.

The (n - 1)! accumulates from multiplying by the power of the denominator at each step, the 2^n from the factor 2 at each step, the (-1)^n from the fact that the denominator at each step is negative.

Evaluating each derivative at x = 0 gives

f(0) = ln(1) = 0

f ' (1) = 2 / (1 + 2 * 0) = 2

f ''(1) = -4 / (1 + 2 * 0)^2 = -4

f '''(1) = 16 / (1 + 2 * 0)^2 = 16

f[n](0) = (-1)^n * (n - 1)! * 2^n / ( 1 + 2 * 0) ^ n = (-1)^n * (n-1)! * 2^n / 1^n = (-1)^n (n-1)! * 2^n.

The corresponding Taylor series coefficients are

f(0) / 0! = 0

f'(0) / 1! = 2

f''0) / 2! = -4/2 = -2

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f[n](0) = (-1)^n (n-1)! * 2^n / n! = (-1)^n * 2^n / n

(this latter since (n-1)! / n! = 1 / n -- everything except the n in the denominator cancels).

So the Taylor series is

f(x) = 0 + 2 * (x-0) - 2 ( x - 0)^2 + 8/3 ( x - 0)^3 - ... + (-1)(^n) * 2^n /n * ( x - 0 ) ^ n

= 0 + 2 x - 2 x^2 + 8/3 x^3 - ... + (-1)(^n) * 2^n /n * x^n + ...

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23:50:04

how does this series compare to that for ln(1+x) and how could you have obtained the above result from the series for ln(1+x)?

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RESPONSE -->

The derivatives of g(x) = ln(x) are

g'(x) = 1/x

g''(x) = -1/x^2

g'''(x) = -2 / x^3

g''''(x) = 6 / x^4

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g[n](x) = (-1)^n * (n-1)! / x^n

yielding the Taylor series about n = 1:

ln(x) = (x - 1) - (x - 1)^2 / 2 + (x-1)^3 / 3 - (x - 1)^4 / 4 ... + (-1)^(n-1) (x-1)^n / n + ...

To get ln(1 + x), we can just substitute 1 + 2x for x in the above. It follows that

ln(1 + 2x) = (1 + x - 1) - (1 + x - 1)^2 / 2 + (1 + x - 1)^3 / 3 - (1 + x - 1)^4 / 4 ... + (-1)^(n-1)(1 + x-1)^n / n + ...

= x x^2 / 2 + x^3 / 3 x^4 / 4 + + (-1)^(n-1) x^n / n.

The function ln(1 + 2x) is obtained by just substituting 2x into the previous:

ln(1 + 2x) = 2x - (2x)^2 / 2 + (2x)^3 / 3 - (2x)^4 / 4 ... + (-1)^(n-1) ( 2x )^n / n + ...

or writing out the terms more explicitly

ln(1 + 2x) = 2 x 2^2 x^2 / 2 + 2^3 x^3 / 3 2^4 x^4 / 4 + + (-1)^(n-1) x^n / n +

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23:50:08

What is your expected interval of convergence?

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23:50:12

Query Add comments on any surprises or insights you experienced as a result of this assignment.

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See my notes. It would be a very good idea for you to insert detailed self-critiques on most of these questions (denoted by *&*& so I can easily identify your self-critiques) and send me the resulting document.