Lie group structure of incompressible deformations?











up vote
0
down vote

favorite












In the context of incompressible elasticity, I failed at finding
a Lie group structure, which respects the incopressibility.



Question:



Let $mathcal B, mathcal S$ be Riemannian manifolds and $overline{mathcal B}$ is compact.



Does the smooth manifold of incompressible deformations
$$
mathcal{C} := { varphi: mathcal{B} to mathcal S mid varphi in mathrm{Diff}(mathcal B, mathcal S) ~text{with}~ mathrm{det}(mathrm{D} varphi) = 1}
$$

admit a Lie group structure?
(Here, $mathcal B$ is the reference configuration of the body (fixed in time) and $mathcal S$ is the space in which the body is placed, i.e. $varphi(X)$ is the current position of the material point $X$.)



Is a Lie structure only possible, if for example $mathcal S subseteq mathbb{R}^d$ or if $mathcal S$ is a Lie group?



Recommendations for related literature or a short 'No, there is no Lie group' are very welcome!



My problem:



A reasonable candidate for the Lie group operation is the composition of maps.
But if $mathcal B neq mathcal S$, it is tricky to define $varphi_2 circ varphi_1$ for $varphi_i in mathrm{Diff}(mathcal B, mathcal S)$.



Fluid dynamics:



In fluid dynamics, there seem to exists a Lie group, since typically the Eulerian perspective is used. If $Omega$ denotes the domain of the fluid,
then the displacement of fluid particles is a map $phi in mathrm{Diff}(Omega, Omega)$, which is a Lie group with the composition of two maps as group operation.



But I was not able to transfer this to the setting above.










share|cite|improve this question















This question has an open bounty worth +50
reputation from Steffen Plunder ending in 3 days.


This question has not received enough attention.












  • 1




    Well, for a 2d manifold, the group is just that of Poisson brackets, namely $SU(infty)$, as you are probably aware from 2d hydrodynamics. In fact, as you can tell from Liouville's theorem in classical mechanics, classical phase-space flows in all dimensions are incompressible. In odd-dimensional manifolds, Nambu brackets are utilized, and the group structure is more moot.
    – Cosmas Zachos
    2 days ago






  • 1




    A modern book on symplectomorphism groups, 2018. For the standard theory, see JMP 1990.
    – Cosmas Zachos
    2 days ago















up vote
0
down vote

favorite












In the context of incompressible elasticity, I failed at finding
a Lie group structure, which respects the incopressibility.



Question:



Let $mathcal B, mathcal S$ be Riemannian manifolds and $overline{mathcal B}$ is compact.



Does the smooth manifold of incompressible deformations
$$
mathcal{C} := { varphi: mathcal{B} to mathcal S mid varphi in mathrm{Diff}(mathcal B, mathcal S) ~text{with}~ mathrm{det}(mathrm{D} varphi) = 1}
$$

admit a Lie group structure?
(Here, $mathcal B$ is the reference configuration of the body (fixed in time) and $mathcal S$ is the space in which the body is placed, i.e. $varphi(X)$ is the current position of the material point $X$.)



Is a Lie structure only possible, if for example $mathcal S subseteq mathbb{R}^d$ or if $mathcal S$ is a Lie group?



Recommendations for related literature or a short 'No, there is no Lie group' are very welcome!



My problem:



A reasonable candidate for the Lie group operation is the composition of maps.
But if $mathcal B neq mathcal S$, it is tricky to define $varphi_2 circ varphi_1$ for $varphi_i in mathrm{Diff}(mathcal B, mathcal S)$.



Fluid dynamics:



In fluid dynamics, there seem to exists a Lie group, since typically the Eulerian perspective is used. If $Omega$ denotes the domain of the fluid,
then the displacement of fluid particles is a map $phi in mathrm{Diff}(Omega, Omega)$, which is a Lie group with the composition of two maps as group operation.



But I was not able to transfer this to the setting above.










share|cite|improve this question















This question has an open bounty worth +50
reputation from Steffen Plunder ending in 3 days.


This question has not received enough attention.












  • 1




    Well, for a 2d manifold, the group is just that of Poisson brackets, namely $SU(infty)$, as you are probably aware from 2d hydrodynamics. In fact, as you can tell from Liouville's theorem in classical mechanics, classical phase-space flows in all dimensions are incompressible. In odd-dimensional manifolds, Nambu brackets are utilized, and the group structure is more moot.
    – Cosmas Zachos
    2 days ago






  • 1




    A modern book on symplectomorphism groups, 2018. For the standard theory, see JMP 1990.
    – Cosmas Zachos
    2 days ago













up vote
0
down vote

favorite









up vote
0
down vote

favorite











In the context of incompressible elasticity, I failed at finding
a Lie group structure, which respects the incopressibility.



Question:



Let $mathcal B, mathcal S$ be Riemannian manifolds and $overline{mathcal B}$ is compact.



Does the smooth manifold of incompressible deformations
$$
mathcal{C} := { varphi: mathcal{B} to mathcal S mid varphi in mathrm{Diff}(mathcal B, mathcal S) ~text{with}~ mathrm{det}(mathrm{D} varphi) = 1}
$$

admit a Lie group structure?
(Here, $mathcal B$ is the reference configuration of the body (fixed in time) and $mathcal S$ is the space in which the body is placed, i.e. $varphi(X)$ is the current position of the material point $X$.)



Is a Lie structure only possible, if for example $mathcal S subseteq mathbb{R}^d$ or if $mathcal S$ is a Lie group?



Recommendations for related literature or a short 'No, there is no Lie group' are very welcome!



My problem:



A reasonable candidate for the Lie group operation is the composition of maps.
But if $mathcal B neq mathcal S$, it is tricky to define $varphi_2 circ varphi_1$ for $varphi_i in mathrm{Diff}(mathcal B, mathcal S)$.



Fluid dynamics:



In fluid dynamics, there seem to exists a Lie group, since typically the Eulerian perspective is used. If $Omega$ denotes the domain of the fluid,
then the displacement of fluid particles is a map $phi in mathrm{Diff}(Omega, Omega)$, which is a Lie group with the composition of two maps as group operation.



But I was not able to transfer this to the setting above.










share|cite|improve this question













In the context of incompressible elasticity, I failed at finding
a Lie group structure, which respects the incopressibility.



Question:



Let $mathcal B, mathcal S$ be Riemannian manifolds and $overline{mathcal B}$ is compact.



Does the smooth manifold of incompressible deformations
$$
mathcal{C} := { varphi: mathcal{B} to mathcal S mid varphi in mathrm{Diff}(mathcal B, mathcal S) ~text{with}~ mathrm{det}(mathrm{D} varphi) = 1}
$$

admit a Lie group structure?
(Here, $mathcal B$ is the reference configuration of the body (fixed in time) and $mathcal S$ is the space in which the body is placed, i.e. $varphi(X)$ is the current position of the material point $X$.)



Is a Lie structure only possible, if for example $mathcal S subseteq mathbb{R}^d$ or if $mathcal S$ is a Lie group?



Recommendations for related literature or a short 'No, there is no Lie group' are very welcome!



My problem:



A reasonable candidate for the Lie group operation is the composition of maps.
But if $mathcal B neq mathcal S$, it is tricky to define $varphi_2 circ varphi_1$ for $varphi_i in mathrm{Diff}(mathcal B, mathcal S)$.



Fluid dynamics:



In fluid dynamics, there seem to exists a Lie group, since typically the Eulerian perspective is used. If $Omega$ denotes the domain of the fluid,
then the displacement of fluid particles is a map $phi in mathrm{Diff}(Omega, Omega)$, which is a Lie group with the composition of two maps as group operation.



But I was not able to transfer this to the setting above.







lie-groups mathematical-physics classical-mechanics






share|cite|improve this question













share|cite|improve this question











share|cite|improve this question




share|cite|improve this question










asked Nov 17 at 10:35









Steffen Plunder

473211




473211






This question has an open bounty worth +50
reputation from Steffen Plunder ending in 3 days.


This question has not received enough attention.








This question has an open bounty worth +50
reputation from Steffen Plunder ending in 3 days.


This question has not received enough attention.










  • 1




    Well, for a 2d manifold, the group is just that of Poisson brackets, namely $SU(infty)$, as you are probably aware from 2d hydrodynamics. In fact, as you can tell from Liouville's theorem in classical mechanics, classical phase-space flows in all dimensions are incompressible. In odd-dimensional manifolds, Nambu brackets are utilized, and the group structure is more moot.
    – Cosmas Zachos
    2 days ago






  • 1




    A modern book on symplectomorphism groups, 2018. For the standard theory, see JMP 1990.
    – Cosmas Zachos
    2 days ago














  • 1




    Well, for a 2d manifold, the group is just that of Poisson brackets, namely $SU(infty)$, as you are probably aware from 2d hydrodynamics. In fact, as you can tell from Liouville's theorem in classical mechanics, classical phase-space flows in all dimensions are incompressible. In odd-dimensional manifolds, Nambu brackets are utilized, and the group structure is more moot.
    – Cosmas Zachos
    2 days ago






  • 1




    A modern book on symplectomorphism groups, 2018. For the standard theory, see JMP 1990.
    – Cosmas Zachos
    2 days ago








1




1




Well, for a 2d manifold, the group is just that of Poisson brackets, namely $SU(infty)$, as you are probably aware from 2d hydrodynamics. In fact, as you can tell from Liouville's theorem in classical mechanics, classical phase-space flows in all dimensions are incompressible. In odd-dimensional manifolds, Nambu brackets are utilized, and the group structure is more moot.
– Cosmas Zachos
2 days ago




Well, for a 2d manifold, the group is just that of Poisson brackets, namely $SU(infty)$, as you are probably aware from 2d hydrodynamics. In fact, as you can tell from Liouville's theorem in classical mechanics, classical phase-space flows in all dimensions are incompressible. In odd-dimensional manifolds, Nambu brackets are utilized, and the group structure is more moot.
– Cosmas Zachos
2 days ago




1




1




A modern book on symplectomorphism groups, 2018. For the standard theory, see JMP 1990.
– Cosmas Zachos
2 days ago




A modern book on symplectomorphism groups, 2018. For the standard theory, see JMP 1990.
– Cosmas Zachos
2 days ago















active

oldest

votes











Your Answer





StackExchange.ifUsing("editor", function () {
return StackExchange.using("mathjaxEditing", function () {
StackExchange.MarkdownEditor.creationCallbacks.add(function (editor, postfix) {
StackExchange.mathjaxEditing.prepareWmdForMathJax(editor, postfix, [["$", "$"], ["\\(","\\)"]]);
});
});
}, "mathjax-editing");

StackExchange.ready(function() {
var channelOptions = {
tags: "".split(" "),
id: "69"
};
initTagRenderer("".split(" "), "".split(" "), channelOptions);

StackExchange.using("externalEditor", function() {
// Have to fire editor after snippets, if snippets enabled
if (StackExchange.settings.snippets.snippetsEnabled) {
StackExchange.using("snippets", function() {
createEditor();
});
}
else {
createEditor();
}
});

function createEditor() {
StackExchange.prepareEditor({
heartbeatType: 'answer',
convertImagesToLinks: true,
noModals: true,
showLowRepImageUploadWarning: true,
reputationToPostImages: 10,
bindNavPrevention: true,
postfix: "",
imageUploader: {
brandingHtml: "Powered by u003ca class="icon-imgur-white" href="https://imgur.com/"u003eu003c/au003e",
contentPolicyHtml: "User contributions licensed under u003ca href="https://creativecommons.org/licenses/by-sa/3.0/"u003ecc by-sa 3.0 with attribution requiredu003c/au003e u003ca href="https://stackoverflow.com/legal/content-policy"u003e(content policy)u003c/au003e",
allowUrls: true
},
noCode: true, onDemand: true,
discardSelector: ".discard-answer"
,immediatelyShowMarkdownHelp:true
});


}
});














 

draft saved


draft discarded


















StackExchange.ready(
function () {
StackExchange.openid.initPostLogin('.new-post-login', 'https%3a%2f%2fmath.stackexchange.com%2fquestions%2f3002184%2flie-group-structure-of-incompressible-deformations%23new-answer', 'question_page');
}
);

Post as a guest















Required, but never shown






























active

oldest

votes













active

oldest

votes









active

oldest

votes






active

oldest

votes
















 

draft saved


draft discarded



















































 


draft saved


draft discarded














StackExchange.ready(
function () {
StackExchange.openid.initPostLogin('.new-post-login', 'https%3a%2f%2fmath.stackexchange.com%2fquestions%2f3002184%2flie-group-structure-of-incompressible-deformations%23new-answer', 'question_page');
}
);

Post as a guest















Required, but never shown





















































Required, but never shown














Required, but never shown












Required, but never shown







Required, but never shown

































Required, but never shown














Required, but never shown












Required, but never shown







Required, but never shown







Popular posts from this blog

Quarter-circle Tiles

build a pushdown automaton that recognizes the reverse language of a given pushdown automaton?

Mont Emei