Stokes' Theorem - Limits of Integration

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The discussion centers on evaluating the integral of the curl of a vector function using Stokes' Theorem over a triangular area defined by points (1,1), (2,2), and (2,1). The vector function is given, and the curl is calculated to be -12x²y² in the z-direction. The main issue arises with determining the correct limits of integration for the double integral over the triangular region, with suggestions provided for integrating first with respect to y or x. Despite attempts to reconcile the results from the surface integral and the path integral, discrepancies remain, leading to confusion about the limits and the correctness of the calculations. The conversation emphasizes the importance of accurately defining integration limits to ensure consistency between the two methods.
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Stokes' Theorem - Limits of Integration - Urgent! Please give a hand :)

Homework Statement



Assume the vector function

\vec{A} = \hat{a}_x \left( 3x^2 y^3 \right) + \hat{a}_y \left( -x^3 y^2 \right)

Evaluate

\int \left( \nabla \times \vec{A} \right) \cdot d\vec{s}

over the triangular area (see figure attached).

Homework Equations



Above.

The Attempt at a Solution



Step 1.

\nabla \times \vec{A} &amp; = \begin{vmatrix} \displaystyle \hat{a}_x &amp; \displaystyle \hat{a}_y &amp; \displaystyle \hat{a}_z \vspace{0.25cm} \\ \displaystyle \frac{\partial}{\partial x} &amp; \displaystyle \frac{\partial}{\partial y} &amp; \displaystyle \frac{\partial}{\partial z} \vspace{0.25cm} \\ \displaystyle A_x &amp; \displaystyle A_y &amp; \displaystyle 0 \end{vmatrix} \\<br /> &amp; = \begin{vmatrix} \displaystyle \frac{\partial}{\partial y} &amp; \displaystyle \frac{\partial}{\partial z} \\ \displaystyle A_y &amp; \displaystyle 0 \end{vmatrix} \hat{a}_x - \begin{vmatrix} \displaystyle \frac{\partial}{\partial x} &amp; \displaystyle \frac{\partial}{\partial z} \\ \displaystyle A_x &amp; \displaystyle 0 \end{vmatrix} \hat{a}_y + \begin{vmatrix} \displaystyle \frac{\partial}{\partial x} &amp; \displaystyle \frac{\partial}{\partial y} \\ \displaystyle A_x &amp; \displaystyle A_y \end{vmatrix} \hat{a}_z \\<br /> &amp; = \cancelto{0}{-\frac{\partial A_y}{\partial z} \, \hat{a}_x} + \cancelto{0}{\frac{\partial A_x}{\partial z} \, \hat{a}_y} + \left( \frac{\partial A_y}{\partial x} - \frac{\partial A_x}{\partial y} \right) \, \hat{a}_z

Step 2

\frac{\partial A_y}{\partial x} = \frac{\partial}{\partial x} \left( -x^3 y^2 \right) = -y^2 \frac{d}{dx} \left( x^3 \right) = -3x^2 y^2

Step 3
- \frac{\partial A_x}{\partial y} = - \frac{\partial}{\partial y} \left( 3x^2 y^3 \right) = -3x^2 \frac{d}{dy} \left( y^3 \right) = -9x^2y^2

Step 4
\nabla \times \vec{A} &amp; = \left( \frac{\partial A_y}{\partial x} - \frac{\partial A_x}{\partial y} \right) \, \hat{a}_z \\<br /> &amp; = \left(-12x^2 y^2 \right) \, \hat{a}_z

Step 5

\int \int \left(-12x^2 y^2 \right) \, \hat{a}_z \cdot \left( dx dy\right) \hat{a}_zNot sure about the limits of integration - THIS IS "THE" PROBLEM. Maybe it's trivial and I just can't see it right now. I do expect to get one of the limits as a variable.

I actually did the other way around (via Stokes' Theorem) P1 (1,1) to P2 (2,2) to P3 (2,1) to P1 and got

\oint _S \vec{A} \cdot d\vec{\ell} = 7y^3 - 7x^3

I'm pretty sure this one is right, so I keep trying to make my other method work but without success so far. Any help is highly appreciated.

THANKS, FOLKS!
 

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thiago_j said:

Homework Statement



Assume the vector function

\vec{A} = \hat{a}_x \left( 3x^2 y^3 \right) + \hat{a}_y \left( -x^3 y^2 \right)

Evaluate

\int \left( \nabla \times \vec{A} \right) \cdot d\vec{s}

over the triangular area (see figure attached).

Homework Equations



Above.

The Attempt at a Solution



Step 1.

\nabla \times \vec{A} &amp; = \begin{vmatrix} \displaystyle \hat{a}_x &amp; \displaystyle \hat{a}_y &amp; \displaystyle \hat{a}_z \vspace{0.25cm} \\ \displaystyle \frac{\partial}{\partial x} &amp; \displaystyle \frac{\partial}{\partial y} &amp; \displaystyle \frac{\partial}{\partial z} \vspace{0.25cm} \\ \displaystyle A_x &amp; \displaystyle A_y &amp; \displaystyle 0 \end{vmatrix} \\<br /> &amp; = \begin{vmatrix} \displaystyle \frac{\partial}{\partial y} &amp; \displaystyle \frac{\partial}{\partial z} \\ \displaystyle A_y &amp; \displaystyle 0 \end{vmatrix} \hat{a}_x - \begin{vmatrix} \displaystyle \frac{\partial}{\partial x} &amp; \displaystyle \frac{\partial}{\partial z} \\ \displaystyle A_x &amp; \displaystyle 0 \end{vmatrix} \hat{a}_y + \begin{vmatrix} \displaystyle \frac{\partial}{\partial x} &amp; \displaystyle \frac{\partial}{\partial y} \\ \displaystyle A_x &amp; \displaystyle A_y \end{vmatrix} \hat{a}_z \\<br /> &amp; = \cancelto{0}{-\frac{\partial A_y}{\partial z} \, \hat{a}_x} + \cancelto{0}{\frac{\partial A_x}{\partial z} \, \hat{a}_y} + \left( \frac{\partial A_y}{\partial x} - \frac{\partial A_x}{\partial y} \right) \, \hat{a}_z

Step 2

\frac{\partial A_y}{\partial x} = \frac{\partial}{\partial x} \left( -x^3 y^2 \right) = -y^2 \frac{d}{dx} \left( x^3 \right) = -3x^2 y^2

Step 3
- \frac{\partial A_x}{\partial y} = - \frac{\partial}{\partial y} \left( 3x^2 y^3 \right) = -3x^2 \frac{d}{dy} \left( y^3 \right) = -9x^2y^2

Step 4
\nabla \times \vec{A} &amp; = \left( \frac{\partial A_y}{\partial x} - \frac{\partial A_x}{\partial y} \right) \, \hat{a}_z \\<br /> &amp; = \left(-12x^2 y^2 \right) \, \hat{a}_z

Step 5

\int \int \left(-12x^2 y^2 \right) \, \hat{a}_z \cdot \left( dx dy\right) \hat{a}_z


Not sure about the limits of integration - THIS IS "THE" PROBLEM. Maybe it's trivial and I just can't see it right now. I do expect to get one of the limits as a variable.
Surely, you learned how to handle this long before you got to Stoke's theorem! The region is a triangle with vertices at (1,1), (2,1), and (2,2). If you choose to integrate with respect to y first, so that the outer integral is with respect to x, then x must cover the entire figure: x must go from 1 to 2. Now, for each x, y must go from the lower edge, y= 1 to the upper edge which is the line y= x. Your integral is
\int_{x=1}^2 \int_{y=1}^x f(x,y)dydx

If, instead, you want to integrate with respect to x first so that the outer integral is with respect to y, then, again to cover the entire triangle, y must go from 1 to 2 and, for each y, x must go from the line x= y on the left to the line x= 2 on the right. Your integral is
\int_{y= 1}^2 \int_{x=y}^2 f(x,y)dxdy

I actually did the other way around (via Stokes' Theorem) P1 (1,1) to P2 (2,2) to P3 (2,1) to P1 and got

\oint _S \vec{A} \cdot d\vec{\ell} = 7y^3 - 7x^3

I'm pretty sure this one is right, so I keep trying to make my other method work but without success so far. Any help is highly appreciated.

THANKS, FOLKS!
 
HallsofIvy, thanks for your comments.

I actually tried those limits before, which sound reasonable to me - by the way. The problem is that I do get

\int _1 ^2 \int _y ^2 \left(-12x^2 y^2 \right) dx dy = -\frac{98}{3} \neq \oint _S \vec{A} \cdot d\vec{\ell} = 7y^3 - 7x^3

Hence, one of the sides is not correct. I double checked the work on the circulation and I can't see a mistake. Here's what I've got:

Path of integration:

P_1 (1,1) \to P_2 (2,2) \to P_3 (2,1) \to P_1 (1,1)

Step 1:

\oint _S \vec{A} \cdot d\vec{\ell} &amp; = \int _{P_1 P_2} \vec{A} \cdot d\vec{\ell} + \int _{P_2 P_3} \vec{A} \cdot d\vec{\ell} + \int _{P_3 P_4} \vec{A} \cdot d\vec{\ell}Step 2:

\int _{P_1 P_2} \vec{A} \cdot d\vec{\ell} &amp; = \int _1 ^2 A_x \: dx + \int _1 ^2 A_y \: dy \\<br /> &amp; = \int _1 ^2 \left( 3x^2 y^3 \right) \, dx + \int _1 ^2 \left( -x^3 y^2 \right) \, dy \\<br /> &amp; = 3y^3 \int _1 ^2 x^2 \: dx - x^3 \int _1 ^2 y^2 \: dy \\<br /> &amp; = 3y^3 \left. \frac{x^3}{3} \right| _1 ^2 - x^3 \left. \frac{y^3}{3} \right| _1 ^2 = 7y^3 - \frac{7}{3}x^3 \\

Step 3:

\int _{P_2 P_3} \vec{A} \cdot d\vec{\ell} &amp; = \int _2 ^2 A_x \: dx + \int _2 ^1 A_y \: dy \\<br /> &amp; = -\int _1 ^2 \left( -x^3 y^2 \right) \, dy \\<br /> &amp; = x^3 \int _1 ^2 y^2 \: dy \\<br /> &amp; = x^3 \left. \frac{y^3}{3} \right| _1 ^2 = \frac{7}{3}x^3 \\

Step 4:

\int _{P_3 P_2} \vec{A} \cdot d\vec{\ell} &amp; = \int _2 ^1 A_x \: dx + \int _1 ^1 A_y \: dy \\<br /> &amp; = -\int _1 ^2 \left( 3x^2 y^3 \right) \, dx \\<br /> &amp; = -3y^3 \int _1 ^2 x^2 \: dx \\<br /> &amp; = -3y^3 \left. \frac{x^3}{3} \right| _1 ^2 = - 7x^3\\

Step 5:

\oint _S \vec{A} \cdot d\vec{\ell} = 7y^3 - 7x^3

Thanks again.
 
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You said you could do the path integral around the boundary! You do understand that the path integral should be a number, not a function of x and y?
:rolleyes:
I get 98/3 both ways- integrating over the surface and integrating around the boundary. (NOT -98/3: Since the path is clockwise around the surface, the normal is -\hat{a}_z, not \hat{a}_z: "right hand rule".)

I divided the boundary into three parts:
I: The line from (2,1) to (1,1). Take x= t with t going from 2 to 1, y= 1. Then dx= dt, dy= 0 so the integral becomes
\int_2^1 3t^2 dt= t^3 \right|_2^1= 1- 8= -7[/itex]<br /> <br /> II: The line from (2,2) to (2,1). Take x= 2, y= t with t going from 2 to 1. Then dx= 0, dy= dt so the integral becomes<br /> -8\int_2^1 t^2 dt= -\frac{8}{3}t^2\right|_2^1= \frac{8}{3}(1- 8)= -\frac{56}{3}<br /> <br /> III: The line from (1,1) to (2,2). Take x= t, y= t with t going from 1 to 2. Then dx= dy= dt so the integral becomes<br /> \int_1^2 (3t^5- t^5)dt= 2\int_1^2 t^5 dt= \frac{1}{3}t^6\right|_1^2= \frac{1}{3} (64- 1)= \frac{63}{3}<br /> <br /> So the complete integral is <br /> - 7+ \frac{56}{3}+ \frac{63}{3}= \frac{-21+ 56+ 63}{3}= \frac{98}{3}
 
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Question: A clock's minute hand has length 4 and its hour hand has length 3. What is the distance between the tips at the moment when it is increasing most rapidly?(Putnam Exam Question) Answer: Making assumption that both the hands moves at constant angular velocities, the answer is ## \sqrt{7} .## But don't you think this assumption is somewhat doubtful and wrong?

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