Generalisation of the Poincaré Lemma
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Let $Omega subset mathbb{R}^3$ be an open but not simply connected domain and let $v : colon Omega to mathbb{R}^3$ be a continuously differentiable vector field. Assume that $textrm{curl} , v = 0$ in $Omega$. As $Omega$ is not simply connected, we cannot conclude that there is a function $varphi in C^2(Omega, mathbb{R})$ such that $v = nabla varphi$.
However, if we additionally assume that for all smooth loops $gamma : colon [0, 1] to Omega$ the line integral
begin{equation}
int_{gamma} v(r) cdot textrm{d}r = 0, qquad (1)
end{equation}
then we find $varphi in C^2(Omega, mathbb{R})$ such that $ v = nabla varphi$.
My question is now:
Let $Omega subset mathbb{R}^3$ be an open but not simply connected domain and given a vector field $ v in L^2(Omega, mathbb{R}^3)$ with $textrm{curl} , v = 0$ in $Omega$. Is there a similar condition like $(1)$ that ensures the existence of a function $varphi in H^1(Omega)$ such that $v = nabla varphi$?
Thanks in advance!
real-analysis differential-geometry reference-request
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up vote
3
down vote
favorite
Let $Omega subset mathbb{R}^3$ be an open but not simply connected domain and let $v : colon Omega to mathbb{R}^3$ be a continuously differentiable vector field. Assume that $textrm{curl} , v = 0$ in $Omega$. As $Omega$ is not simply connected, we cannot conclude that there is a function $varphi in C^2(Omega, mathbb{R})$ such that $v = nabla varphi$.
However, if we additionally assume that for all smooth loops $gamma : colon [0, 1] to Omega$ the line integral
begin{equation}
int_{gamma} v(r) cdot textrm{d}r = 0, qquad (1)
end{equation}
then we find $varphi in C^2(Omega, mathbb{R})$ such that $ v = nabla varphi$.
My question is now:
Let $Omega subset mathbb{R}^3$ be an open but not simply connected domain and given a vector field $ v in L^2(Omega, mathbb{R}^3)$ with $textrm{curl} , v = 0$ in $Omega$. Is there a similar condition like $(1)$ that ensures the existence of a function $varphi in H^1(Omega)$ such that $v = nabla varphi$?
Thanks in advance!
real-analysis differential-geometry reference-request
add a comment |
up vote
3
down vote
favorite
up vote
3
down vote
favorite
Let $Omega subset mathbb{R}^3$ be an open but not simply connected domain and let $v : colon Omega to mathbb{R}^3$ be a continuously differentiable vector field. Assume that $textrm{curl} , v = 0$ in $Omega$. As $Omega$ is not simply connected, we cannot conclude that there is a function $varphi in C^2(Omega, mathbb{R})$ such that $v = nabla varphi$.
However, if we additionally assume that for all smooth loops $gamma : colon [0, 1] to Omega$ the line integral
begin{equation}
int_{gamma} v(r) cdot textrm{d}r = 0, qquad (1)
end{equation}
then we find $varphi in C^2(Omega, mathbb{R})$ such that $ v = nabla varphi$.
My question is now:
Let $Omega subset mathbb{R}^3$ be an open but not simply connected domain and given a vector field $ v in L^2(Omega, mathbb{R}^3)$ with $textrm{curl} , v = 0$ in $Omega$. Is there a similar condition like $(1)$ that ensures the existence of a function $varphi in H^1(Omega)$ such that $v = nabla varphi$?
Thanks in advance!
real-analysis differential-geometry reference-request
Let $Omega subset mathbb{R}^3$ be an open but not simply connected domain and let $v : colon Omega to mathbb{R}^3$ be a continuously differentiable vector field. Assume that $textrm{curl} , v = 0$ in $Omega$. As $Omega$ is not simply connected, we cannot conclude that there is a function $varphi in C^2(Omega, mathbb{R})$ such that $v = nabla varphi$.
However, if we additionally assume that for all smooth loops $gamma : colon [0, 1] to Omega$ the line integral
begin{equation}
int_{gamma} v(r) cdot textrm{d}r = 0, qquad (1)
end{equation}
then we find $varphi in C^2(Omega, mathbb{R})$ such that $ v = nabla varphi$.
My question is now:
Let $Omega subset mathbb{R}^3$ be an open but not simply connected domain and given a vector field $ v in L^2(Omega, mathbb{R}^3)$ with $textrm{curl} , v = 0$ in $Omega$. Is there a similar condition like $(1)$ that ensures the existence of a function $varphi in H^1(Omega)$ such that $v = nabla varphi$?
Thanks in advance!
real-analysis differential-geometry reference-request
real-analysis differential-geometry reference-request
edited Jul 7 '16 at 13:28
Henning Makholm
235k16299534
235k16299534
asked Jul 7 '16 at 13:19
Mike
509210
509210
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1 Answer
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The general condition is that if for all divergence free compactly supported smooth vector fields, that is $f in mathcal{D}(Omega,mathbb{R}^3)$ with $div(f)=0$, $v in L^2(Omega,mathbb{R}^3)$ satisfies,
begin{equation}
int_Omega v.f dx = 0
end{equation}
then there will exist $phi in H^1(Omega) $ such that $v=nabla phi$. This condition on $v$ will imply $curl (v)=0$ but not the other way around. This is in fact quite a general result and would work for $v$ in more general Sobolev spaces or in the space of distributions (each component of $v$ is a distribution).
add a comment |
1 Answer
1
active
oldest
votes
1 Answer
1
active
oldest
votes
active
oldest
votes
active
oldest
votes
up vote
0
down vote
The general condition is that if for all divergence free compactly supported smooth vector fields, that is $f in mathcal{D}(Omega,mathbb{R}^3)$ with $div(f)=0$, $v in L^2(Omega,mathbb{R}^3)$ satisfies,
begin{equation}
int_Omega v.f dx = 0
end{equation}
then there will exist $phi in H^1(Omega) $ such that $v=nabla phi$. This condition on $v$ will imply $curl (v)=0$ but not the other way around. This is in fact quite a general result and would work for $v$ in more general Sobolev spaces or in the space of distributions (each component of $v$ is a distribution).
add a comment |
up vote
0
down vote
The general condition is that if for all divergence free compactly supported smooth vector fields, that is $f in mathcal{D}(Omega,mathbb{R}^3)$ with $div(f)=0$, $v in L^2(Omega,mathbb{R}^3)$ satisfies,
begin{equation}
int_Omega v.f dx = 0
end{equation}
then there will exist $phi in H^1(Omega) $ such that $v=nabla phi$. This condition on $v$ will imply $curl (v)=0$ but not the other way around. This is in fact quite a general result and would work for $v$ in more general Sobolev spaces or in the space of distributions (each component of $v$ is a distribution).
add a comment |
up vote
0
down vote
up vote
0
down vote
The general condition is that if for all divergence free compactly supported smooth vector fields, that is $f in mathcal{D}(Omega,mathbb{R}^3)$ with $div(f)=0$, $v in L^2(Omega,mathbb{R}^3)$ satisfies,
begin{equation}
int_Omega v.f dx = 0
end{equation}
then there will exist $phi in H^1(Omega) $ such that $v=nabla phi$. This condition on $v$ will imply $curl (v)=0$ but not the other way around. This is in fact quite a general result and would work for $v$ in more general Sobolev spaces or in the space of distributions (each component of $v$ is a distribution).
The general condition is that if for all divergence free compactly supported smooth vector fields, that is $f in mathcal{D}(Omega,mathbb{R}^3)$ with $div(f)=0$, $v in L^2(Omega,mathbb{R}^3)$ satisfies,
begin{equation}
int_Omega v.f dx = 0
end{equation}
then there will exist $phi in H^1(Omega) $ such that $v=nabla phi$. This condition on $v$ will imply $curl (v)=0$ but not the other way around. This is in fact quite a general result and would work for $v$ in more general Sobolev spaces or in the space of distributions (each component of $v$ is a distribution).
answered Nov 13 at 13:30
Animesh Pandey
11
11
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