Query104

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course Mth 277

935pm 11/13/2011

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

.

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.

At the end of this document, after the qa problems (which provide you with questions and solutions), there is a series of Questions, Problems and Exercises.

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Question:

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Your solution:

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Given Solution:

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Self-critique (if necessary):

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Question: Find T(t) and N(t) when R(t) = (e^-2t cost)i + (e^-2t sint )j + e^-2t.

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Your solution:

I am going to assume that e^-2t is the k component.

R(t) = (e^-2t cost)i + (e^-2t sint )j + e^-2tk

R'(t) = 2*e^-2t*sin(t) i - 2e^-2t*cos(t) j - 2e^-2t k

T= R' / ||R'||

= [2*e^-2t*sin(t) i - 2e^-2t*cos(t) j - 2e^-2t k] / || (4e^-4t)*sin^2(t) + (4e^-4t)*cos^2(t) + (4e^-4t) ||

= [2*e^-2t*sin(t) i - 2e^-2t*cos(t) j - 2e^-2t k] / sqrt(8e^-4t)

= [4*e^-4t*sin^2(t) i + 4e^-2t*cos^2(t) j + 4e^-4t k] / (8e^-4t)

= [0.5*sin^2(t) i + 0.5*cos^2(t) j + 0.5 k]

N = T' / ||T'||

= sin(t)cos(t) i - sin(t)cos(t) j / || [sin^2(t)cos^2(t) + sin^2(t)cos^2(t)] ||

= 1/sqrt(2) i - 1/sqrt(2) j

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Given Solution:

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Question: Find the curvature of the plane curve y = sin (-3x) at x = pi/2.

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Your solution:

y= sin (-3x)

y' = -3cos(-3x)

y"" = -sin(-3x)

K = y"" / [1+(y')^2]^(3/2)

= -9sin(-3x) / [1 + 9cos^2(-3x)]^(3/2)

= -9sin(-3 * pi/2) / [1 + 9cos^2(-3pi/2)]^(3/2)

= -9 / [1 + 9/2 + 9/2cos(-3pi)]^(3/2)]

= -9 / (11/2 - 9/2)^(3/2)

= -9sqrt(2) / 4

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Given Solution:

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Question: Let C be the curve given by R(t) = (1-cos t)i + (t-sin t)j + (4sin(t/2))k

Find the unit tangent vector T(t) to C

Find dT/ds and the curvature k(t)

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Your solution:

R(t) = (1-cos t)i + (t-sin t)j + (4sin(t/2))k

R'(t) = sin(t)i + (1 - cos(t)) j + 2cos(t/2) k

||R'|| = sqrt[sin^2(t) + (cos^2(t) -2cos(t) + 1) + 4cos^2(t/2)]

= sqrt(1+ 1 - 2cos(t) + 2 + 2cos(t))

= sqrt(4) = 2

T = R'(t) / ||R'||

= [sin(t)i + (1 - sin(t)) j + 2cos(t/2) k] / 2

= [sin(t) / 2] i + [(1-cos(t)) / 2] j + [cos(t/2)] k

dT/ds = K = ||T'||/||R'||

T' = cos(t)/2 i + sin(t)/2 j - sin(t/2) / 2 k

||T'|| = sqrt[cos^2(t)/4 + sin^2(t)/4 + sin^2(t/2)/4]

= sqrt(1/4 + sin^2(t/2)/4)

K = sqrt(1/4 + sin^2(t/2)/4) / 2

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Given Solution:

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Self-critique (if necessary):

Couldn't figure out how to break down the equation [1/4 + sin^2(t/2)/4} any further

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Question: Find the maximum curvature for the curve y = e^3x.

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Your solution:

y = 3^3x

y' = 3e^3x

(y')^2 = 9e^6x

y"" = 9e^3x

K = y"" / [1 + (y')^2]^(3/2)

K = (9e^3x) / [1 + 9e^6x]^(3/2)

= (9e^3x) * [1 + 9e^6x]^(-3/2)

k'= (9e^3x)*(54e^6x)*(-2/5)*(1+9e^6x)^(-5/2) + (1+9e^6x)^(-3/2)*27e^3x

0 = (972e^9x) / -5*(1+9e^6x)^(5/2) + (27e^3x) / (1+9e^6x)^(3/2)

(972e^9x) / [5*(1+9e^6x)] = 27e^3x

972*e^9x = (135e^3x)*(1+9e^6x)

7.2*e^6x = 1 + 9e^6x

I tried to work the solution out, but I can't find x. I tried to do the limit as x->-infinity and found x = 0

So either there is no maximum(which doesn't make since) since an exponential function has a curve. The only time you would find where there is no maximum is when you have an absolute value function or possibly a linear function

So I take x = 0 and plug back into K and I get K = 9/[10sqrt(10)] =approx. .285 units

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Given Solution:

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Self-critique (if necessary):

@&

If you put your expression for k ' into a form with a common denominator you get a numerator which must equal zero.

If you factor everything you can out of the numerator you are left with the expression

1 - 18 e^(6 x) = 0

so that

e^(6 x) = 1/18

which has solution

x = -ln(18) / 6,

approximately x = -.48.

A graph of y = e^(3 x) remains close to the x axis until x gets close to 0, when it begins curving dramatically upward and by the time x = 1 is nearly vertical.

For example when x = -1, e^(3 x) is about -1/16 and very nearly horizontal (slope is about -1/50). By the time x = 0 the graph has slope 3.

So max curvature near x = -1/2 seems about right.

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Question:

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Your solution:

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Given Solution:

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Question: If T and N are the unit tangent and normal vectors on the trajectory of a moving body, we can define B = T X N to be the unit binormal vector.

A coordinate system with three planes can be made at each point with these vectors since they are mutually orthogonal.

Show that T is orthogonal to dB/ds (Hint: Differentiate B dot T)

Show that B is orthogonal to dB/ds (Hint: Differentiate B dot B)

Show that dB/ds = -(tau)N for some constant tau. (We call the constant tau the torsion of the trajectory)

**Prove the Frenet-Serret formulas: (dT/ds = kN, dN/ds = -kT + tauB, dB/ds = -tauN). Where k is the curvature and tau = tau(s) is a scalar function.

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Your solution:

I don't understand how you want me to show you how they are orthoganl, but I believe that I can explain it in words.

B = T X N

T = R'/||R'||

N = T'/||T'||

B = R'/||R'|| X T'/||T'||

When you do the right-hand rule, B is your thumb.

So the vector R is coming from the x-y axis from point (x_0,y_0) along some curve. At the point where R(t) meets the curve, there is a tangent line at that point. The dirivative of that tangent is normal to the tangent line. Similar to a position vector from (x_0,y_0), a velocity vector is tangent to the curve.

So the unit tangent vector is the derivitive of the position vector divided by the maginitude. thats why they call it a unit vector, it shows direction. The Normal unit vector is perpendicular to the Tangent unit vector, similar to the way an acceleration vector is to a velocity vector, when there is constant acceleration like the video of the planet around the sun.

So, now we have a normal vector that is perpendicular to the tangent vector which is perpendicular to the position vector. So since B= T X N, then it can be easily assumed that B dot T and B dot B are orthoganl and equal zero.

If the normal vector is perpendicular to the tangent which is perpendicular to the position, that makes the normal vecotr opposite the position vecotr and dB/ds = -(tau)N is understood to be true.

(dT/ds = kN

k is curvature or the reciprocal of the radius. So kN is N/r which is the rate of change of the tangent unit vector with respect to position. Once again, normal is perpendicular to tangent.

dN/ds = -kT + tauB,

The rate of change of the Normal vector with respect to position is equal to the negative value of curvature + tau * B vector.

The normal vector is orthoganl to B and goes back towards the center of the curve. The more that normal vector changes, the greater the angle of tau multiplies the B vector. B vector is your thumb on the right hand rule.

dB/ds = -tauN

And as far as the last equation is the B vector(right hand thumb) changes with respect to position eqauls the negative normal vector times the angle between those two vectors.

I'm not certain at all I got the answer to this question right, I just wanted to be sure that I gave a good answer to my understanding of this chapter. Its all interlinked, through phyics and normal vectors, accelerations and gravity, radians and calculus. I am connecting the dots and the picture is still hazy, but becoming much clearer.

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Given Solution:

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@&

You've expressed some good insights and given a pretty good plausibility argument.

The rigorous solutions are most easily found by following the hints.

Here's a solution to the first question:

The derivative of B dot T is dB/ds dot T + B dot dT/ds.

dT/ds is in the normal direction so it perpendicular to B. Thus the derivative of B dot T is dB/ds dot T.

B dot T is always zero, so dB/ds dot T is always zero.

Thus dB/ds is perpendicular to T.

These proofs won't actually appear on the test, but the insights you have given in your solution will be valuable on other problems.

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