Query 133

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course Mth 277

1/5 9

Question: Determine if the vector field F = (y- x^2)i + (2x + y^2)j is conservative, and if it is find a scalar potentialYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYY

Your solution:

Curl does not = 0. thus not conservative.

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Given Solution:

The vector field is conservative if, and only if, its curl is zero.

The curl of the field M i + N j + P k is (P_y - N_z) i + (M_z - P_x) j + (N_x - M_y) k.

For the current function there is no z dependence and P = 0, so the expression becomes just (N_x - M_y) k.

M_y = 1 and N_x = 2, so the field is not conservative.

If we did try to find the scalar potential function, we would try to find f(x, y) such that del f = F. If this was so then we would have f_x = M and f_y = N.

If f_x = (y - x^2), then integrating with respect to x we conclude that f = y x - x^3 / 3 + g(y), where g(y) is any function of y.

If f_y = (2 x + y^2), then integrating with respect to y we conclude that f = 2 x y + y^3 / 3 + h(x), where h(x) is any function of x.

We could let g(y) = y^3 / 3, and h(x) = - x^3 / 3. However the first integration yields y x, and the second yields 2 x y, both functions of x as well as y.

That is, any f function such that del f = F must contain the term x y as well as the term 2 x y. We can't accomplish this by adjusting either g(y) or h(x), and we conclude that no scalar potential function f exists for this F.

Had the original function been F(x, y) = (2 y - x^2) i + (2 x + y^2) j then :

Our integrals would have been 2 y x - x^3 / 3 + g(y) and 2 x y + y^3 / 3 + h(x). Letting g(y) = y^3 / 3 and h(x) = -x^3 / 3, our function would be the same using either the x or the y integral; either way we would get 2 x y - x^3 / 3 + y^3 / 3.

M_y would have been 2 and N_x would have been 2, so that our curl would have been (N_x - M_y) k = 0.

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Self-critique (if necessary):

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Question: Show that F = e^-y i - xe^-y j is conservative and find a scalar potential f for F. Evaluate the line integral Int[ F dot dR, C], where C is any smooth path connecting (0,0) and (1,1).

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Your solution:

done on paper, Had to look at Solution for the integration with respect to x part.

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Given Solution:

The curl of this function, which is of the form M i + N j + P k with M = e^-y, N = - x e^(-y) and P = 0, is easily found to be

(P_y - N_z) i + (M_z - P_x) j + (N_x - M_y) k = (N_x - M_y) k = ( -e^-y - (-e^(-y)) ) k = 0.

So the function is conservative and a scalar potential function exists.

We therefore integrate:

Integrating e^-y with respect to x we get x e^-y + g(y).

Integrating - x e^(-y) with respect to y we get x e^-y + h(x).

The general form of a scalar potential for our given vector field F is therefore f(x, y) = x e^-y + g(y) + h(x), where g(y) and h(x) are arbitrary functions of y and x, respectively.

The simplest such function is obtained by letting g(y) and h(x) both be zero, giving us

f(x, y) = x e^-y

We can easily verify that del f = F.

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Self-critique (if necessary):

ok

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Question:

Consider the integral Int[ 2x^2y dx + x^3 dy, C]. Evaluate it on each of the following curves C:

The semicircle x = sqrt(1-y) from -1 <= y <= 1.

The line segment from (0,-1) to (1,1) and then the line segment from (1,1) to (0,1).

The square with vertices (1,1), (-1,1), (-1,-1), (1,-1) traversed once clockwise.

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Your solution:

Well a semicircle I think would imply finding the curl of the function defined by the parameters -1 <= y <= 1.

So fill in x in the integral and solve from -1 to 1 for y values to get -3.078

for a line segment from (0,-1) to (1,1).

verify its on the curve. if x = sqrt(1-y), 0 does not = sqrt(1-(-1)) neither 1 = sqrt(1-1). not on curve.

as for the other points. the second point (0,1) is on the curve. (0,1)

so C should be evaluated on the left part of the curve

where x = sqrt(1-y). dx = -1/ 2sqrt(1-y)

fill in dx in the integral and evaluate y from -1 to 1.

integration is Int(-1 - 2/5(1-y)^5/2) dy from -1 to 1

answer is ( 28 sqrt(2) ) /5 -8. roughly -.08

for the square, it will be the closed interval transversed once. which means a total distance of 4 units.. So we can take our function, and our distance (4) and ""project"" the function F onto this line of 4 units, to find the work of this integral.

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The semicircle can be parameterized by

x = cos(t)

y = sin(t)

0 <= t <= pi

What is the resulting integral?

The line segment from (0, -1) to (1, 1) can be parmeterized by x = t, y = -1 + 2 t. This parameterization leads to int( 2 t^2 ( -1 + 2 t) * dt + t^3 * ( 2 dt) , t from 0 to 1).

What do you get?

How do you then parameterize the line segment from (1, 1) to (0, 1), and what integral results?

Us a similar approach for subsequent intervals.

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Given Solution:

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Self-critique (if necessary):

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Question: Verify that the integral Int[(xy cos (xy) + sin (xy))dx + (x^2 cos(xy)) dy, C] is independent of path and evaluate it where C is any path from (0, pi/18) to (1, pi/6).

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Your solution:

The function F is xy cos(xy) i + x^2cos(xy) j. Now getting the curl just take do the cross product rule where k=0 to get

(N_x - M_y) k = ( (2 x cos(xy) - x^2 y sin(x y)) - (x cos(x y) - x^2 y sin(x y) + x cos(x y) ) ) k = 0. scalar potential exist because that = 0. integrate with respect to x and get the constant function called g(y).

then integrate with respect to y adding the new constant we call h(x).

Worked on paper, function f(x,y) is -xcos(xy). If my integration is correct.

now evaluating the integral from our two points.

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Given Solution:

This integral is of the form F dot ds for F = (x y cos(x y) + sin(x y) ) i + x^2 cos(x y) j, of the form M i + N j.

We easily verify that curl F = (N_x - M_y) k = ( (2 x cos(xy) - x^2 y sin(x y)) - (x cos(x y) - x^2 y sin(x y) + x cos(x y) ) ) k = 0.

We conclude that a scalar potential function exists, and we integrate to find it:

Integrating x y cos(x y) + sin(x y) with respect to x we get cos( x y ) / y + x sin(x y) - cos(x y) / y = x sin(x y), to which we can add the arbitrary integration 'constant' g(y).

Integrating x^2 cos(x y) with respect to y we get x^2 ( sin(x y) / x) = x sin(x y) + h(x).

Our general scalar potential is therefore f(x, y) = x sin(x y) + g(y) + h(x), for arbitrary g(y) and h(x). The simplest scalar potential function is just f(x, y) = x sin(x y), and we will use this to evaluate our integral.

For conservative field F our fundamental theorem says that

integral ( F dot ds , between points (x0, y0) and (xf, yf) ) = f(xf, yf) - f(x0, y0)

Our current integral is conservative. Its path originates at (0, pi/18) and terminates at (1, pi/6), so

Int[(xy cos (xy) + sin (xy))dx + (x^2 cos(xy)) dy, C]

= f(1, pi/6) - f(0, pi/18)

= 1 sin(1 * pi / 6) - 0 sin(0 * pi/18)

= 1/2.

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Self-critique (if necessary):

Well my integral was incorrect, also, I dont see how you got your final integral. How do you know which x and y to substitute into your intial integral ?

Did you integrate this....Int[(xy cos (xy) + sin (xy))dx + (x^2 cos(xy)) dy, C]

then take that integration, and substitute the f(xy) from point to point ?"

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If f(x, y) is the scalar potential function then F = f_x `i + f_y `j, so that F dot `ds is M `i + N `j.

So M = f_x and N = f_y.

We have seen that

M = (x y cos(x y) + sin(x y) ) so

f_x = (x y cos(x y) + sin(x y) ) and we conclude that

f = int(( x y cos(x y) + sin(x y) ) dx)

For the moment let's replace y by a, just to make it look more like a constant. Then

f = int(( a x cos(a x) + sin(a x) ) dx).

Basic integration technique (integration by parts on x cos(a x) and straightforward substitution for sin(a x) leads us to the integral

f = x sin(a x) + constant.

Now remember that a just stands for y, which is regarded as constant for this integral, and since y is constant our integration constant can be any function of y. We conclude that

f = x sin(x y) + g(y).

N = x^2 cos(x y), which is equal to f_y, so that by analogous reasoning we get

f = int(x^2 cos(x y) dy) = x sin(x y) + h(x).

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It's not clear that you understand the process of parameterization in evaluating a line integral.

Check my other notes as well.

Let me know if you have questions.

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