Assignment 12

course Mth 174

Please explain problem 9.2.29.

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Physics II

07-24-2009

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13:18:06

Query problem 9.2.8 (3d editin 9.1.6) (was 9.4.6) first term and ratio for y^2 + y^3 + y^4 + ...

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RESPONSE -->

Not a geometric series since a=y, not a constant.

** The common ratio is

y^3 / y^2 = y^4 / y^3 = y.

If we factor out y^2 we get

y^2 ( 1 + y + y^2 + … ),

which is in the standard form a ( 1 + r + r^2 + …) with a = y^2 and r = y.

For | y | < 1 this series would converge to sum

y^2 * Sum ( 1 + y + y^2 + . . . =

y^2 * 1 / (1 - y). **

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13:18:31

either explain why the series is not geometric or give its first term and common ratio

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The series is not geometric because there is no constant value for a.

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13:29:59

how do you get the common ratio?

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RESPONSE -->

divide the second term by the first term = y^3/y^2 = y

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14:03:37

what do you get when you factor out y^2? How does this help you determine the first term?

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1+y+y^2+y^3+...

It shows that the first term is indeed an easily identifiable constant.

good

Additional information: The sum of this series.

The sum of a geometric series can be expressed in a number of different ways.

Your text says that a + a x + a x^2 + ... sums to a / (1 - x). If you use this form then the series must start with constant number a.

An alternative statement is evey more restrictive:

1 + x + x^2 + ... = 1 / (1 - x).

Of course this is the same as the preceding form, just dividing through by the non-zero constant a.

You could express this series as

y^2 ( 1 + y + y^2 + ...), in which case you would use a = y^2 and get the result

a / (1 - y) = y^2 / (1 - y).

Alternatively you could just say that since the expression 1 + y + y^2 + ... is 1 / 1 - y, then y^2 ( 1 + y + y^2 + ...) = y^2 / (1 - y).

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14:05:32

Query problem 9.2.29 (3d edition 9.1.24) (was 9.4.24) bouncing ball 3/4 ht ratio

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14:09:58

how do you verify that the ball stops bouncing after 1/4 `sqrt(10) + 1/2 `sqrt(10) `sqrt(3/2) (1 / (1-`sqrt(3/4)) sec?

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RESPONSE -->

the series that the bounces create approaches 0 at about 11 seconds, showing that the ball stops bouncing at that time.

** If the ball starts from height h, it falls to the floor then bounces up to 3/4 of its original height then back down, covering distance 3/2 h on its first complete bounce. Then it bounces to 3/4 of that height, covering in the round trip a distance of 3/4 ( 3/2 h). Then it bounces to 3/4 of that height, covering in the round trip a distance of 3/4 [ 3/4 ( 3/2 h) ] = (3/4)^2 * (3/2 h). On the next bounce the round trip will be 3/4 of this, or (3/4)^3 * (3/2 h). All the bounces give us a distance of (3/4) * (3/2 h) + (3/4)^2 * (3/2 h) + (3/4)^3 * (3/2 h) + ... = [ 3/4 ( 3/2 h) ] * ( 1 + 3/4 + (3/4)^2 + ... ) = [9/8 h] * ( 1 + 3/4 + (3/4)^2 + ... ) = (9/8 h) ( 1 / ( 1 - 3/4) ) = 9/2 h. There is also the initial drop h, so the total distance is 11/2 h. But this isn't the question. The question is how long it takes the ball to stop.

The time to fall distance y is ( 2 * y / g ) ^ .5, where g is the acceleration of gravity. This is also the time required to bounce up to height h. The distances of fall for the complete round-trip bounces are 3/4 h, (3/4)^2 h, (3/4)^3 h, etc.. So the times of fall are ( 2 * 3/4 h / g ) ^ .5, ( 2 * (3/4)^2 h / g ) ^ .5, ( 2 * (3/4)^3 h / g ) ^ .5, ( 2 * (3/4)^4 h / g ) ^ .5, etc.. The times for the ‘complete’ round-trip bounces will be double these times; the total time of fall will also include the time sqrt( 2 h / g) for the first drop.

We can factor the ( 3/4 ) ^ .5 out of each expression, getting times of fall (3/4)^.5 * ( 2 * h / g ) ^ .5 = `sqrt(3)/2 * ( 2 * h / g ) ^ .5, ( sqrt(3)/2 ) ^ 2 * ( 2 * h / g ) ^ .5, ( sqrt(3)/2 ) ^ 3 * ( 2 * h / g ) ^ .5, etc..

Adding these terms up, multiplying by 2 since the ball has to go up and down on each bounce, and factoring out the (2 * h / g ) ^ .5 we get 2 * (2 * h / g ) ^ .5 * [ ( sqrt(3)/2 ) + ( sqrt(3)/2 ) ^ 2 + ( sqrt(3)/2 ) ^ 3 + ( sqrt(3)/2 ) ^ 4 + ... ] .

The expression in brackets is a geometric series with r = ( sqrt(3)/2 ), so the sum of the series is 1 / ( 1 - ( sqrt(3)/2 ) )

h and g are given by the problem so 2 * (2 * h / g ) ^ .5 is just a number, easily calculated for any given h and g.

We also add on the time to fall to the floor after the drop, obtaining total time sqrt(2 h / g) + 2 * (2 h / g)^.5 (1 / (1 – sqrt(3)/2) ). Rationalizing the last fraction and factoring out sqrt(2 h / g) we have

sqrt(2 h / g) * ( 1 + 2 * (4 + 2 sqrt(3) ) = sqrt(2 h / g ) ( 9 + 4 sqrt( 3) ).**

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16:14:32

What geometric series gives the time and how does this geometric series yield the above result?

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16:14:43

How far does the ball travel on the nth bounce?

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16:15:47

How long does it takes a ball to complete the nth bounce?

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(1/4sqrt10)^n

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18:35:15

Query 9.2.21 (was p 481 #6) convergence of 1 + 1/5 + 1/9 + 1/13 + ...

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18:52:30

with what integral need you compare the sequence and did it converged or diverge?

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Int.(1/(1-x),0,inf)dx It converged.

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18:19:29

Explain in terms of a graph how you set up rectangles to represent the series, and how you oriented these rectangles with respect to the graph of your function in order to prove your result.

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&#Good responses. See my notes and let me know if you have questions. &#