Derivation of curl in two dimension
$begingroup$
Let $f(x,y) = u(x,y) e_x + v(x,y) e_y$ be a vector valued function on $mathbb{R}^2$. I'm not sure how the formula is determined.
I take this definition of curl:
The curl at point $P$ is the (directed) anglular velocity a "infinitesemal" disc would rotate with, when it's center is aligned with $P$
From this, it's easy to see (by eg: treating it as torque) for a curve $gamma$ with enclosed area $A$, the torque experined by it is $frac{1}{|A|} oint_{gamma} f cdot dS $ where the integral is taken along the surface of the curve.
Now, we need to prove that $displaystyle lim_{|A| rightarrow 0} frac{1}{|A|} oint_{gamma} f cdot dS = frac{partial u}{partial x} - frac{partial v}{partial y}$ for any curve $gamma$, but how do you do that ?
I'm stuck even for the very simple case when $gamma$ is a circle, and I'm finding it very counterintuive why would the limit even be the same and not depending on the shape of $gamma$.
calculus multivariable-calculus curl
$endgroup$
add a comment |
$begingroup$
Let $f(x,y) = u(x,y) e_x + v(x,y) e_y$ be a vector valued function on $mathbb{R}^2$. I'm not sure how the formula is determined.
I take this definition of curl:
The curl at point $P$ is the (directed) anglular velocity a "infinitesemal" disc would rotate with, when it's center is aligned with $P$
From this, it's easy to see (by eg: treating it as torque) for a curve $gamma$ with enclosed area $A$, the torque experined by it is $frac{1}{|A|} oint_{gamma} f cdot dS $ where the integral is taken along the surface of the curve.
Now, we need to prove that $displaystyle lim_{|A| rightarrow 0} frac{1}{|A|} oint_{gamma} f cdot dS = frac{partial u}{partial x} - frac{partial v}{partial y}$ for any curve $gamma$, but how do you do that ?
I'm stuck even for the very simple case when $gamma$ is a circle, and I'm finding it very counterintuive why would the limit even be the same and not depending on the shape of $gamma$.
calculus multivariable-calculus curl
$endgroup$
add a comment |
$begingroup$
Let $f(x,y) = u(x,y) e_x + v(x,y) e_y$ be a vector valued function on $mathbb{R}^2$. I'm not sure how the formula is determined.
I take this definition of curl:
The curl at point $P$ is the (directed) anglular velocity a "infinitesemal" disc would rotate with, when it's center is aligned with $P$
From this, it's easy to see (by eg: treating it as torque) for a curve $gamma$ with enclosed area $A$, the torque experined by it is $frac{1}{|A|} oint_{gamma} f cdot dS $ where the integral is taken along the surface of the curve.
Now, we need to prove that $displaystyle lim_{|A| rightarrow 0} frac{1}{|A|} oint_{gamma} f cdot dS = frac{partial u}{partial x} - frac{partial v}{partial y}$ for any curve $gamma$, but how do you do that ?
I'm stuck even for the very simple case when $gamma$ is a circle, and I'm finding it very counterintuive why would the limit even be the same and not depending on the shape of $gamma$.
calculus multivariable-calculus curl
$endgroup$
Let $f(x,y) = u(x,y) e_x + v(x,y) e_y$ be a vector valued function on $mathbb{R}^2$. I'm not sure how the formula is determined.
I take this definition of curl:
The curl at point $P$ is the (directed) anglular velocity a "infinitesemal" disc would rotate with, when it's center is aligned with $P$
From this, it's easy to see (by eg: treating it as torque) for a curve $gamma$ with enclosed area $A$, the torque experined by it is $frac{1}{|A|} oint_{gamma} f cdot dS $ where the integral is taken along the surface of the curve.
Now, we need to prove that $displaystyle lim_{|A| rightarrow 0} frac{1}{|A|} oint_{gamma} f cdot dS = frac{partial u}{partial x} - frac{partial v}{partial y}$ for any curve $gamma$, but how do you do that ?
I'm stuck even for the very simple case when $gamma$ is a circle, and I'm finding it very counterintuive why would the limit even be the same and not depending on the shape of $gamma$.
calculus multivariable-calculus curl
calculus multivariable-calculus curl
asked Jan 7 at 13:50
alxchenalxchen
644421
644421
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