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L p -trace-free generalized Korn inequalities for incompatible tensor fields in three space dimensions
For $1< p0$ such that \[ \lVert{ P }\rVert_{L^{p}(\Omega,\mathbb{R}^{3\times 3})}\leq c\,\left(\lVert{\operatorname{dev} \operatorname{sym} P }\rVert_{L^{p}(\Omega,\mathbb{R}^{3\times 3})} + \lVert{ \operatorname{dev} \operatorname{Curl} P }\rVert_{L^{p}(\Omega,\mathbb{R}^{3\times 3})}\right) \]...
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Published in: | Proceedings of the Royal Society of Edinburgh. Section A. Mathematics 2022-12, Vol.152 (6), p.1477-1508 |
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container_title | Proceedings of the Royal Society of Edinburgh. Section A. Mathematics |
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creator | Lewintan, Peter Neff, Patrizio |
description | For
$1< p0$
such that
\[ \lVert{ P }\rVert_{L^{p}(\Omega,\mathbb{R}^{3\times 3})}\leq c\,\left(\lVert{\operatorname{dev} \operatorname{sym} P }\rVert_{L^{p}(\Omega,\mathbb{R}^{3\times 3})} + \lVert{ \operatorname{dev} \operatorname{Curl} P }\rVert_{L^{p}(\Omega,\mathbb{R}^{3\times 3})}\right) \]
holds for all tensor fields
$P\in W^{1,p}_0(\operatorname {Curl}; \Omega ,\mathbb {R}^{3\times 3})$
, i.e., for all
$P\in W^{1,p} (\operatorname {Curl}; \Omega ,\mathbb {R}^{3\times 3})$
with vanishing tangential trace
$P\times \nu =0$
on
$\partial \Omega$
where
$\nu$
denotes the outward unit normal vector field to
$\partial \Omega$
and
$\operatorname {dev} P : = P -\frac 13 \operatorname {tr}(P) {\cdot } {\mathbb {1}}$
denotes the deviatoric (trace-free) part of
$P$
. We also show the norm equivalence
\begin{align*} &\lVert{ P }\rVert_{L^{p}(\Omega,\mathbb{R}^{3\times 3})}+\lVert{ \operatorname{Curl} P }\rVert_{L^{p}(\Omega,\mathbb{R}^{3\times 3})}\\ &\quad\leq c\,\left(\lVert{P}\rVert_{L^{p}(\Omega,\mathbb{R}^{3\times 3})} + \lVert{ \operatorname{dev} \operatorname{Curl} P }\rVert_{L^{p}(\Omega,\mathbb{R}^{3\times 3})}\right) \end{align*}
for tensor fields
$P\in W^{1,p}(\operatorname {Curl}; \Omega ,\mathbb {R}^{3\times 3})$
. These estimates also hold true for tensor fields with vanishing tangential trace only on a relatively open (non-empty) subset
$\Gamma \subseteq \partial \Omega$
of the boundary. |
doi_str_mv | 10.1017/prm.2021.62 |
format | article |
fullrecord | <record><control><sourceid>hal_cross</sourceid><recordid>TN_cdi_hal_primary_oai_HAL_hal_03234282v1</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>oai_HAL_hal_03234282v1</sourcerecordid><originalsourceid>FETCH-LOGICAL-c197t-f894ba9db7f26c5cea0321236fe3d79568aae765d05231edc775e27024be8bc03</originalsourceid><addsrcrecordid>eNo9kE1LxDAQhoMouK6e_AO5imTNR5O0x2VRVyx40XNI04kb6ZdJFfTXm6J4GuZ533kOg9AloxtGmb6ZYr_hlLON4kdoxQotiGa8OEYrKmhJOKPyFJ2l9EYpVaXUK-RrPGEyR-uA-AiAX2GAaLvwDS1-HOOAwwDvHxnMARL2Y8zAjf1k59B0gGcYUmY-QNemHOH5sFjSlIW4DX2Owzikc3TibZfg4m-u0cvd7fNuT-qn-4fdtiaOVXomvqyKxlZtoz1XTjqwVHDGhfIgWl1JVVoLWsmWSi4YtE5rCVxTXjRQNo6KNbr69R5sZ6YYehu_zGiD2W9rs7DsEwUv-SfL3evfrotjShH8_wGjZnln3nuzvNMoLn4AQqNpMw</addsrcrecordid><sourcetype>Open Access Repository</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>L p -trace-free generalized Korn inequalities for incompatible tensor fields in three space dimensions</title><source>Cambridge University Press</source><creator>Lewintan, Peter ; Neff, Patrizio</creator><creatorcontrib>Lewintan, Peter ; Neff, Patrizio</creatorcontrib><description>For
$1< p<\infty$
we prove an
$L^{p}$
-version of the generalized trace-free Korn inequality for incompatible tensor fields
$P$
in
$W^{1,p}_0(\operatorname {Curl}; \Omega ,\mathbb {R}^{3\times 3})$
. More precisely, let
$\Omega \subset \mathbb {R}^{3}$
be a bounded Lipschitz domain. Then there exists a constant
$c>0$
such that
\[ \lVert{ P }\rVert_{L^{p}(\Omega,\mathbb{R}^{3\times 3})}\leq c\,\left(\lVert{\operatorname{dev} \operatorname{sym} P }\rVert_{L^{p}(\Omega,\mathbb{R}^{3\times 3})} + \lVert{ \operatorname{dev} \operatorname{Curl} P }\rVert_{L^{p}(\Omega,\mathbb{R}^{3\times 3})}\right) \]
holds for all tensor fields
$P\in W^{1,p}_0(\operatorname {Curl}; \Omega ,\mathbb {R}^{3\times 3})$
, i.e., for all
$P\in W^{1,p} (\operatorname {Curl}; \Omega ,\mathbb {R}^{3\times 3})$
with vanishing tangential trace
$P\times \nu =0$
on
$\partial \Omega$
where
$\nu$
denotes the outward unit normal vector field to
$\partial \Omega$
and
$\operatorname {dev} P : = P -\frac 13 \operatorname {tr}(P) {\cdot } {\mathbb {1}}$
denotes the deviatoric (trace-free) part of
$P$
. We also show the norm equivalence
\begin{align*} &\lVert{ P }\rVert_{L^{p}(\Omega,\mathbb{R}^{3\times 3})}+\lVert{ \operatorname{Curl} P }\rVert_{L^{p}(\Omega,\mathbb{R}^{3\times 3})}\\ &\quad\leq c\,\left(\lVert{P}\rVert_{L^{p}(\Omega,\mathbb{R}^{3\times 3})} + \lVert{ \operatorname{dev} \operatorname{Curl} P }\rVert_{L^{p}(\Omega,\mathbb{R}^{3\times 3})}\right) \end{align*}
for tensor fields
$P\in W^{1,p}(\operatorname {Curl}; \Omega ,\mathbb {R}^{3\times 3})$
. These estimates also hold true for tensor fields with vanishing tangential trace only on a relatively open (non-empty) subset
$\Gamma \subseteq \partial \Omega$
of the boundary.</description><identifier>ISSN: 0308-2105</identifier><identifier>EISSN: 1473-7124</identifier><identifier>DOI: 10.1017/prm.2021.62</identifier><language>eng</language><publisher>Royal Society of Edinburgh</publisher><subject>Analysis of PDEs ; Mathematics</subject><ispartof>Proceedings of the Royal Society of Edinburgh. Section A. Mathematics, 2022-12, Vol.152 (6), p.1477-1508</ispartof><rights>Distributed under a Creative Commons Attribution 4.0 International License</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c197t-f894ba9db7f26c5cea0321236fe3d79568aae765d05231edc775e27024be8bc03</citedby><cites>FETCH-LOGICAL-c197t-f894ba9db7f26c5cea0321236fe3d79568aae765d05231edc775e27024be8bc03</cites><orcidid>0000-0002-1615-8879 ; 0000-0002-7188-4806</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,776,780,881,27903,27904</link.rule.ids><backlink>$$Uhttps://hal.science/hal-03234282$$DView record in HAL$$Hfree_for_read</backlink></links><search><creatorcontrib>Lewintan, Peter</creatorcontrib><creatorcontrib>Neff, Patrizio</creatorcontrib><title>L p -trace-free generalized Korn inequalities for incompatible tensor fields in three space dimensions</title><title>Proceedings of the Royal Society of Edinburgh. Section A. Mathematics</title><description>For
$1< p<\infty$
we prove an
$L^{p}$
-version of the generalized trace-free Korn inequality for incompatible tensor fields
$P$
in
$W^{1,p}_0(\operatorname {Curl}; \Omega ,\mathbb {R}^{3\times 3})$
. More precisely, let
$\Omega \subset \mathbb {R}^{3}$
be a bounded Lipschitz domain. Then there exists a constant
$c>0$
such that
\[ \lVert{ P }\rVert_{L^{p}(\Omega,\mathbb{R}^{3\times 3})}\leq c\,\left(\lVert{\operatorname{dev} \operatorname{sym} P }\rVert_{L^{p}(\Omega,\mathbb{R}^{3\times 3})} + \lVert{ \operatorname{dev} \operatorname{Curl} P }\rVert_{L^{p}(\Omega,\mathbb{R}^{3\times 3})}\right) \]
holds for all tensor fields
$P\in W^{1,p}_0(\operatorname {Curl}; \Omega ,\mathbb {R}^{3\times 3})$
, i.e., for all
$P\in W^{1,p} (\operatorname {Curl}; \Omega ,\mathbb {R}^{3\times 3})$
with vanishing tangential trace
$P\times \nu =0$
on
$\partial \Omega$
where
$\nu$
denotes the outward unit normal vector field to
$\partial \Omega$
and
$\operatorname {dev} P : = P -\frac 13 \operatorname {tr}(P) {\cdot } {\mathbb {1}}$
denotes the deviatoric (trace-free) part of
$P$
. We also show the norm equivalence
\begin{align*} &\lVert{ P }\rVert_{L^{p}(\Omega,\mathbb{R}^{3\times 3})}+\lVert{ \operatorname{Curl} P }\rVert_{L^{p}(\Omega,\mathbb{R}^{3\times 3})}\\ &\quad\leq c\,\left(\lVert{P}\rVert_{L^{p}(\Omega,\mathbb{R}^{3\times 3})} + \lVert{ \operatorname{dev} \operatorname{Curl} P }\rVert_{L^{p}(\Omega,\mathbb{R}^{3\times 3})}\right) \end{align*}
for tensor fields
$P\in W^{1,p}(\operatorname {Curl}; \Omega ,\mathbb {R}^{3\times 3})$
. These estimates also hold true for tensor fields with vanishing tangential trace only on a relatively open (non-empty) subset
$\Gamma \subseteq \partial \Omega$
of the boundary.</description><subject>Analysis of PDEs</subject><subject>Mathematics</subject><issn>0308-2105</issn><issn>1473-7124</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><recordid>eNo9kE1LxDAQhoMouK6e_AO5imTNR5O0x2VRVyx40XNI04kb6ZdJFfTXm6J4GuZ533kOg9AloxtGmb6ZYr_hlLON4kdoxQotiGa8OEYrKmhJOKPyFJ2l9EYpVaXUK-RrPGEyR-uA-AiAX2GAaLvwDS1-HOOAwwDvHxnMARL2Y8zAjf1k59B0gGcYUmY-QNemHOH5sFjSlIW4DX2Owzikc3TibZfg4m-u0cvd7fNuT-qn-4fdtiaOVXomvqyKxlZtoz1XTjqwVHDGhfIgWl1JVVoLWsmWSi4YtE5rCVxTXjRQNo6KNbr69R5sZ6YYehu_zGiD2W9rs7DsEwUv-SfL3evfrotjShH8_wGjZnln3nuzvNMoLn4AQqNpMw</recordid><startdate>20221201</startdate><enddate>20221201</enddate><creator>Lewintan, Peter</creator><creator>Neff, Patrizio</creator><general>Royal Society of Edinburgh</general><scope>AAYXX</scope><scope>CITATION</scope><scope>1XC</scope><orcidid>https://orcid.org/0000-0002-1615-8879</orcidid><orcidid>https://orcid.org/0000-0002-7188-4806</orcidid></search><sort><creationdate>20221201</creationdate><title>L p -trace-free generalized Korn inequalities for incompatible tensor fields in three space dimensions</title><author>Lewintan, Peter ; Neff, Patrizio</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c197t-f894ba9db7f26c5cea0321236fe3d79568aae765d05231edc775e27024be8bc03</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><topic>Analysis of PDEs</topic><topic>Mathematics</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Lewintan, Peter</creatorcontrib><creatorcontrib>Neff, Patrizio</creatorcontrib><collection>CrossRef</collection><collection>Hyper Article en Ligne (HAL)</collection><jtitle>Proceedings of the Royal Society of Edinburgh. Section A. Mathematics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Lewintan, Peter</au><au>Neff, Patrizio</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>L p -trace-free generalized Korn inequalities for incompatible tensor fields in three space dimensions</atitle><jtitle>Proceedings of the Royal Society of Edinburgh. Section A. Mathematics</jtitle><date>2022-12-01</date><risdate>2022</risdate><volume>152</volume><issue>6</issue><spage>1477</spage><epage>1508</epage><pages>1477-1508</pages><issn>0308-2105</issn><eissn>1473-7124</eissn><abstract>For
$1< p<\infty$
we prove an
$L^{p}$
-version of the generalized trace-free Korn inequality for incompatible tensor fields
$P$
in
$W^{1,p}_0(\operatorname {Curl}; \Omega ,\mathbb {R}^{3\times 3})$
. More precisely, let
$\Omega \subset \mathbb {R}^{3}$
be a bounded Lipschitz domain. Then there exists a constant
$c>0$
such that
\[ \lVert{ P }\rVert_{L^{p}(\Omega,\mathbb{R}^{3\times 3})}\leq c\,\left(\lVert{\operatorname{dev} \operatorname{sym} P }\rVert_{L^{p}(\Omega,\mathbb{R}^{3\times 3})} + \lVert{ \operatorname{dev} \operatorname{Curl} P }\rVert_{L^{p}(\Omega,\mathbb{R}^{3\times 3})}\right) \]
holds for all tensor fields
$P\in W^{1,p}_0(\operatorname {Curl}; \Omega ,\mathbb {R}^{3\times 3})$
, i.e., for all
$P\in W^{1,p} (\operatorname {Curl}; \Omega ,\mathbb {R}^{3\times 3})$
with vanishing tangential trace
$P\times \nu =0$
on
$\partial \Omega$
where
$\nu$
denotes the outward unit normal vector field to
$\partial \Omega$
and
$\operatorname {dev} P : = P -\frac 13 \operatorname {tr}(P) {\cdot } {\mathbb {1}}$
denotes the deviatoric (trace-free) part of
$P$
. We also show the norm equivalence
\begin{align*} &\lVert{ P }\rVert_{L^{p}(\Omega,\mathbb{R}^{3\times 3})}+\lVert{ \operatorname{Curl} P }\rVert_{L^{p}(\Omega,\mathbb{R}^{3\times 3})}\\ &\quad\leq c\,\left(\lVert{P}\rVert_{L^{p}(\Omega,\mathbb{R}^{3\times 3})} + \lVert{ \operatorname{dev} \operatorname{Curl} P }\rVert_{L^{p}(\Omega,\mathbb{R}^{3\times 3})}\right) \end{align*}
for tensor fields
$P\in W^{1,p}(\operatorname {Curl}; \Omega ,\mathbb {R}^{3\times 3})$
. These estimates also hold true for tensor fields with vanishing tangential trace only on a relatively open (non-empty) subset
$\Gamma \subseteq \partial \Omega$
of the boundary.</abstract><pub>Royal Society of Edinburgh</pub><doi>10.1017/prm.2021.62</doi><tpages>32</tpages><orcidid>https://orcid.org/0000-0002-1615-8879</orcidid><orcidid>https://orcid.org/0000-0002-7188-4806</orcidid><oa>free_for_read</oa></addata></record> |
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ispartof | Proceedings of the Royal Society of Edinburgh. Section A. Mathematics, 2022-12, Vol.152 (6), p.1477-1508 |
issn | 0308-2105 1473-7124 |
language | eng |
recordid | cdi_hal_primary_oai_HAL_hal_03234282v1 |
source | Cambridge University Press |
subjects | Analysis of PDEs Mathematics |
title | L p -trace-free generalized Korn inequalities for incompatible tensor fields in three space dimensions |
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