assignment 3

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course MTH 174

2/20/11 9:00 pm

If your solution to stated problem does not match the given solution, you should self-critique per instructions at

http://vhcc2.vhcc.edu/dsmith/geninfo/labrynth_created_fall_05/levl1_22/levl2_81/file3_259.htm

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Your solution, attempt at solution. If you are unable to attempt a solution, give a phrase-by-phrase interpretation of the problem along with a statement of what you do or do not understand about it. This response should be given, based on the work you did in completing the assignment, before you look at the given solution.

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Question: Section 6.5 Problem 3

6.5.3 (previously 6.5 #8) Galileo: time for unif accel object to traverse dist is same as if vel was ave of init and final; put into symbols and show why true

How can you symbolically represent the give statement?

How can we show that the statement is true?

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Your solution:

Velocity is equal to the sum of the initial velocity and the antiderivative of acceleration times time

V(t)= Vo + A(t) where A(t)= acceleration and Vo=initial velocity

The position of any object when velocity or acceleration is known can be figured out by the position function which is the antiderivative of the velocity function

P(t)= intergral of V(t)

Acceleration is the derivative of V(t)

A=V(t)'

If this were graphed velocity vs time we would see a linear line that is proportional to time and the area beneath the curve would be equal to the distance the object traveled during that given time interval

this can be figured out taking the inital time which could be ((t + (t+delta(t))*height)/2 this would give you the area under the line thus the distance traveled over a given time interval

confidence rating #$&*: 2

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Given Solution:

If acceleration is uniform, then it follows by straightforward integration of the constant a with respect to t that

v(t) = v_0 + a t,

where a is the acceleration and v_0 is the velocity at clock time t = 0.

It also follows that the position function, found by integrating the velocity function, can be expressed as

x(t) = x_0 + v_0 t + 1/2 a t^2.

From the velocity function we can get expressions for the initial and final velocity over an interval. If we average these and multiply by the duration of the interval we get a prediction fo the distance traveled by the object.

From the position function we can calculate the two positions and subtract to determine the actual change in position.

It will turn out that the two results are identical, confirming the statement:

Between clock time t = t_1 and t = t_2, the velocity will change from

v(t_1) = v_0 + a t_1

to

v(t_2) = v_0 + a t_2.

The average of these velocities is

ave of init and final vel = (v(t_1) + v(t_2) ) / 2

= ( v_0 + a t_1 + v_0 + a t_2) / 2

= v_0 + a ( t_1 + t_2 ) / 2.

The time interval is `dt = t_2 - t_1. Moving a velocity equal to the average of the two velocities the object would travel through a displacement of

`dx = (ave of velocities) * `dt

= ( v_0 + a ( t_1 + t_2 ) / 2 ) * ( t_2 - t_1)

= v_0 * (t_2 - t_1) + 1/2 a ( t_2^2 - t_1^2).

Now using the position function x(t) = x_0 + v_0 t + 1/2 a t^2:

The change in position between t_1 and t_2 is

x(t_2) - x(t_1) = (x_0 + v_0 t_2 + 1/2 a t_2^2) - (x_0 + v_0 t_1 + 1/2 a t_1^2)

= v_0 ( t_2 - t_1) + 1/2 a ( t_2^2 - t_1^2).

Our two expressions agree, proving the original statement true.

Alternative solution:

For uniform acceleration the velocity function can be expressed as

v0 + a t.

Integrating this function between clock times t1 and t2 we obtain the displacement s:

s = 1/2 a (t2^2 - t1^2) + v0 ( t2 - t1).

Dividing the integral (i.e., the displacement) by the length of the interval we get the average value of the function—i.e., the average velocity. The length of the interval is t2 - t1 so

displacement / interval =

Integral / interval =

(1/2 a (t2^2 - t1^2) + v0 ( t2 - t1)) / (t2 - t1) =

1/2 a ( t2 + t1) + v0.

The initial value of the velocity on the interval is v0 + a t1, the final velocity v0 + a t2, so the average of initial and final velocities is

Ave of init and final velocity =

(v0 + a t1 + v0 + a t2) / 2 =

v0 + 1/2 a ( t1 + t2).

This is identical to the expression obtained previously.

Thus the average of the initial and final velocities is equal to the average velocity on the interval, and the result is proven.

Still another solution:

If an object is dropped from rest and falls for time t it will reach velocity vf = a t. So the average of its initial and final velocities will be

Ave of init and final vel =(vf + v0) / 2 = (32 t + 0) / 2 = 16 t.

The distance fallen is known to be

s = 16 t^2.

But this is exactly the distance the object would travel in time t if its average velocity was 16 t. Thus the two quantities are identical.

A numerical example for a given s:

When s = 100, then, t is the positive solution to 100 = 16 t^2. This solution is t = 2.5.

The velocity function is v = a t. We have to find v when s = 100. When s = 100, we have t = 2.5, as just seen. So v = a t = 32 * 2.5 = 80, representing 80 ft/sec.

Now we know that s = 100, vf = 80 and v0=0. Substituting into t = s / [ (vf + v0)/2 ] we get t = 100 / [ (80 + 0) / 2 ] = 100 / 40 = 2.5.

This agrees with the t we got using s = .5 a t^2. **

Another argument:

The average value of any linear function over an interval is equal to the average of its initial and final values over the interval.

In a nutshell, because the v vs. t graph is linear, the average velocity is equal to the average of the initial and final velocities.

Since

time of fall = displacement / average velocity,

it follows that

time of fall = displacement / (ave of initial and final vel).

This latter expression is just the time that would be required to fall at a constant velocity which is equal to the average of initial and final velocities.

More rigorously:

The graph is linear, so the area beneath the graph is the area of a triangle.

The base of the triangle is the time of fall, and its altitude is the final velocity.

By a simple construction we know that the area of the triangle is equal to the area of a rectangle whose length is equal to the base of the triangle, and whose width is equal to half the altitude of the triangle.

It follows that the area of the triangle is equal to half the final velocity multiplied by the time interval.

Since the initial velocity is 0, the average of initial and final velocities is half the final velocity.

So the area of the triangle is the product of the time of fall and the average of initial and final velocities

area beneath graph = time of fall * ave of init and final vel

The area beneath the graph is equal to the integral of the velocity function over the time interval, which we know is equal to the displacement. So we have

displacement = time of fall * ave of init and final vel, so that

time of fall = displacement / ave of init and final vel.

This leads to the same conclusion as above.

The same argument, expressed more symbolically:

A graph of v vs. t graph is linear. Over any time interval t = t1 to t = t1 + `dt, displacement is represented by the area of the corresponding trapezoid, which is d = (v1 + v2) / 2 * `dt.

Solving for `dt we again obtain `dt = d / [ (v1+v2)/2 ].

Still another way of structuring the argument:

** Using s for the distance fallen we can translate Galileo's statement as follows:

t = s / [ (vf + v0)/2 ].

An object accelerating for time t, starting with initial velocity v0 at t = 0, has velocity function

v = v0 + a * t

and position function

s = .5 a t^2 + v0 t,

assuming that s = 0 at t = 0.

Both of these results are easily obtained, for the given initial condition that initial velocity is zero, by a straightforward integration of the acceleration function (to get the velocity function) then the velocity function (to get the position function).

For given displacement s we can solve the position equation for t. The equation is rearranged to the form of a standard quadratic:

.5 a t^2 + v0 t - s = 0, with solutions

t = (-v0 +- sqrt(v0^2 + 2 a s) ) / a ).

Substituting this into the velocity function we obtain the final velocity:

Final velocity

= v0 + a t = v0 + a * (-v0 +- sqrt(v0^2 + 2 a s) / a)

= +- sqrt(v0^2 + 2 a s) .

The average of the initial and final velocities is therefore

ave. of init and final vel = (initial vel + final vel) / 2 = (v0 +- sqrt(v0^2 + 2 a s)) / 2.

Traveling at this velocity for time t = (-v0 +- sqrt(v0^2 + 2 a s) ) / a ) the displacement will be

Displacement = average velocity * time of travel

= ( v0 +- sqrt(v0^2 + 2 a s)) (-v0 +- sqrt(v0^2 + 2 a s) ) / a ) / 2

The numerator is the product of the sum and the difference of two quantities and simplifies to 2 a s. The denominator is 2 a so the expression simplifies to just s.

This confirms that the distance traveled is the same as the distance that would be traveled at the average of the initial and final velocities.

Self-critique

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Question: **** query problem 7.1.18 integral of ` sqrt(cos(3t) ) * sin(3t)

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Your solution:

Int sqrt(cos(3t) * sin(3t) dt

let u=cos(3t)

then du=3-sin(3t) dt (we do have a sin(3t) in the problem but no (3-sin(3t) so we divide both sides by -3

-1/3du = sin(3t)

rewriting the problem we have (-1/3intergral (u^1/2 du)

taking the intergral we have (-(1/3)*(2/3)u^(3/2) after solving we have

-(2/9)*(cos(3t))^(3/2)+C

confidence rating #$&*: 3

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Given Solution:

** TYPICAL INCORRECT SOLUTION: (-2/3) (cos3t)^(3/2)

INSTRUCTOR COMMENT: The derivative of cos(3t) is -3 sin(3t), wo the derivative of -2/3 (cos(3t))^(-3/2) is 3 sqrt(cos(3t) sin(3t). This solution is not consistent with the Chain Rule.

To perform the integral use substitution. Very often the first substitution you want to try involves the inner function of a composite, and that is the case here. Cos(3t) is the inner function of the composite sqrt(cos(3t)), so we try using this as our substitution:

w = cos (3t) dw = -3 sin (3t)

so that sin(3t) = -dw / 3.

Thus our expression becomes

w^(1/2) * (-dw / 3).

The integral of -1/3 w^(3/2) with respect to w is -1/3 * (2/3) w^(3/2), treating w^(1/2) as a power function.

This simplifies to

-2/9 w^(3/2) or

-2/9 * (cos(3t))^(3/2).

The general antiderivative is

-2/9 * (cos(3t))^(3/2) + c,

where c is an arbitrary constant.**

DER

22:16:28

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Self-critique (if necessary):

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Question: Section 7.1 problem 6

7.1.6 (previously 7.1.21) antiderivative of x^2 e^(x^3+1)

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Your solution:

let u =(x^3+1) then du=3x^2 we have to divide both sides by 3 leaving us with (1/3)du = x^2 dx

rewriting the intergral = 1/3 intergral e^u du = (1/3)e^(x^3+1)+C

confidence rating #$&*: 3

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Given Solution:

Substituting for the inner function of the composite:

u = x^3 + 1 yields

du = 3 x^2 dx, so

x^2 dx = 1/3 du.

This makes the integrand 1/3 e^u du.

An antiderivative is then

antiderivative = 1/3 e^u, or 1/3 e^(x^3+1)

leading to the general indefinite integral

indefinite integral = 1/3 e^(x^3+1) + c

If we take the derivative of this function we do indeed obtain our original integrand.

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Self-critique (if necessary):

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Question: Section 7.1 Problem 9

7.1.9 (previously 7.1.35) Find an antiderivative of (t+1)^2 / t^2

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Your solution:

I tried this one several different ways before coming up with the correct answer

after seperating the numerator I have (t^2+2t +1)/t^2 then 1 + 2t^-1 + t^-2

after integrating each term seperately and adding them together I have t + 2 ln{x} + (-1/t) + C

confidence rating #$&*: 3

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Given Solution:

expand (t+1)^2 to get t^2+2t+1.

divide by t^2 to get 1 + 2t^-1 + t^-2.

Each term of this function is a power function. Integrate term-by-term and add the integration constant to get the general antiderivative

general antiderivative = t + 2ln(t) - t^-1 +C

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Question: Section 7.1 Problem 13

7.1.13 (previously 7.1.60). int(1/(t+7)^2, t, 1, 3) **** What did you get for the definite integral?

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Your solution:

let u = (t+7)

du = 1dt

rewriting the intergral we have int (1/u^2) bringing the exponent to the top we have 1*u^-2 taking the intergral of u^-2 we have -u^-1

substituting back for U we have -(-t - 7)^-1 pushing the exponent back to the bottom of the fraction getting 1/(-t -7)

evaluating the intergral from T(3) - T(1) = -1/10 - (-1/8) = 1/40

confidence rating #$&*: 3

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Given Solution:

This situation involves a composite of the power function 1 / z^2 and the linear function t + 7. The latter is the ‘inner’ function of the composite.

We therefore substitute u = t+7 to get du = dt; limits t = 1 and t = 3 become u = 8 and u = 10. So the integral becomes

integral( u^-2, u from 8 to 10).

The integrand is the power function u^-2, or 1 / u^2. Its simplest antiderivative can be expressed as -u^-1 or -1/u.

So the definite integral is

change in antiderivative =

-1/10 - (-1/8) =

1/8 - 1/10 =

1/40.

Amplified explanation

The given definite integral becomes the integral of 1 / u^2, integrated from u = 8 to u = 10. We can find our integral just in terms of the function u:

The definite integral is the change in the antiderivative function. The antiderivative function is - 1 / u, which between u = 8 and u = 10 changes from -1/8 to -1/10.

Subtracting -1/8 from -1/10 we get 1/40.

Alternatively, having found our antiderivative in terms of u, we could have substituted t + 7 for u and done the integral in terms of t:

Our antiderivative -1/u is equal to -1 / (t + 7).

Our original integral was form t = 1 to t = 3.

At t = 1 our antiderivative is -1/(1 + 7) = -1/8. At t = 3 our antiderivative is -1 / (3 + 7) = -1/10. Once more the change in the antiderivative is found to be 1/40.

Still another way of putting it:

If f(t) = 1 / (t + 7)^2, our antiderivative is F(t) = - 1 / (t + 7). Thus

integral ( f(t), t from 1 to 3) = F(3) - F(1) = -1/10 - (-1/8) = 1/40.

F(3) - F(1) is, of course, the change in the value of F(t) between t = 1 and t = 3; i.e., this is the change in the value of the antiderivative function.

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Question: Section 7.1 Problem 16

7.1.16 (previously 7.1.86). World population P(t) = 5.3 e^(0.014 t).

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Your solution:

I didn't see this problem in my text, the only problem was 7.1.108 it was about population but it was different

confidence rating #$&*: 0

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Given Solution:

What were the populations in 1990 and 2000?

What is the average population between during the 1990's and how did you find it?

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In 1990, t = 0 so the population is P(0) = 5.3 billion

In 2000, t = 0 so the population is P(10) = 6.1 billion

To find the average population we integrate the population function over the 10-year interval, then divide by the 10 years:

An antiderivative of 5.3 e^(0.014 t) is found by letting u equal the ‘inner function’ of the composite:

u = .014 t so

du = .014 dt and

dt = du / .014.

Thus the expression 5.3 e^(0.014 t) dt becomes 5.3 e^u * du / .014.

An antiderivative of e^u with respect to u is just e^u, so the antiderivative of the function is

5.3 e^u / .014 = 380 e^u, approximately. In terms of t this is

380 e^(.014 t).

At t = 0 this antiderivative would have value about 380.

At t = 0 your antiderivative would have value about 435.

The change in the value of the antiderivative is therefore about 435 - 380 = 55.

The change in the antiderivative is the definite integral of the function.

The average value of the function is equal to its definite integral divided by the time interval:

average value = 56.89 / 10 = 5.689.

This is quite close to, but a little less than the average of the initial and final populations.

It is less because the exponential function is concave upward, and the population curve therefore 'dips' below the straight line connecting the initial and final points.

However the curvature on this interval is not pronounced, and the function never 'dips' far below the straight line, so the average is close to the straight-line average you gave in your initial solution.

INCORRECT IF NOT UNREASONABLE ANSWER:

The average population seems as if it would be the average of the two, therefore

6.1 + 5.3/ 2 = 5.7 billion

INSTRUCTOR RESPONSE:

Review the definition of the average value of a function:

The average value of a function over an interval is equal to its integral over that interval, divided by the length of the interval.

Now if the function is linear, then the average of its initial and final values is equal to its average value (see the above given solution to the Galileo problem). However:

If the function is not linear, it is very unlikely that the average of its initial and final values is equal to its average value

If the function has nonzero positive or negative concavity on the entire interval it will never have an average value equal to the average of its initial and final values.

The exponential function is not linear, and is in fact concave upward on this interval, so averaging initial and final values on the interval won't work here.

You have to integrate the function and divide by the 10-year interval of integration.

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COMMON INTEGRATION ERRORS: integral( x^2 * e^(x^3+1) ) = integral( x^2) * integral (e^(x^3 + 1) ) = x^3 / 3 * e^(x^3 + 1)

INSTRUCTOR RESPONSE: You have essentially assumed that the integral of a product function is equal to the product of the integrals. The integral is of the form

integral (f * g)

with f(x) = x^2 and g(x) = e^(x^3 + 1).

However integral (f * g) is not the same as integral (f) * integral(g):

The derivative of our antiderivative function must equal the original integrand. That is, the derivative of integral(f * g) must be f * g.

However the derivative of integral (f) * integral(g) is expressed by the product rule as

(integral (f) * integral(g)) ' = ( integral (f) ) ' * integral(g) + integral (f) * (integral(g)) ' = f * integral(g) + g * integral(f).

This is much different than the original integrand f * g, so integral ( f * g) is not generally the same as integral(f) * integral(g).

Without going into the details, we'll also assert that

integral(f / g) is not the same as integral(f) / integral(g),

which you can if you wish verify for yourself by taking the derivative of integral(f) / integral(g), using the quotient rule. What you get is nothing like the original integrand f / g.

So for example integral( (t+1)^2 / t^2 ) is not the same as integral ( t + 1) / integral (t^2).

Note also that, while the integral of e^x with respect to x is e^x + c, the integral of (e^(x^3 + 1) ) with respect to x is NOT the same as e^(x^3 + 1) + c:

The derivative of e^(x^3 + 1) is 3 x^2 * e^(x^3 + 1), not e^(x^3 + 1).

So e^(x^3 + 1) is not an antiderivative of e^(x^3 + 1).

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