Publication: Faraday instability in a surface-frozen liquid
cris.virtual.author-gnd | 113167281X | |
cris.virtual.author-gnd | #PLACEHOLDER_PARENT_METADATA_VALUE# | |
cris.virtual.author-gnd | #PLACEHOLDER_PARENT_METADATA_VALUE# | |
cris.virtual.author-gnd | #PLACEHOLDER_PARENT_METADATA_VALUE# | |
cris.virtual.author-gnd | #PLACEHOLDER_PARENT_METADATA_VALUE# | |
cris.virtual.author-gnd | #PLACEHOLDER_PARENT_METADATA_VALUE# | |
cris.virtual.author-orcid | 0000-0002-2126-9100 | |
cris.virtual.author-orcid | #PLACEHOLDER_PARENT_METADATA_VALUE# | |
cris.virtual.author-orcid | #PLACEHOLDER_PARENT_METADATA_VALUE# | |
cris.virtual.author-orcid | #PLACEHOLDER_PARENT_METADATA_VALUE# | |
cris.virtual.author-orcid | #PLACEHOLDER_PARENT_METADATA_VALUE# | |
cris.virtual.author-orcid | #PLACEHOLDER_PARENT_METADATA_VALUE# | |
cris.virtual.department | Material- und Röntgenphysik M-2 | |
cris.virtual.department | #PLACEHOLDER_PARENT_METADATA_VALUE# | |
cris.virtual.department | #PLACEHOLDER_PARENT_METADATA_VALUE# | |
cris.virtual.department | #PLACEHOLDER_PARENT_METADATA_VALUE# | |
cris.virtual.department | #PLACEHOLDER_PARENT_METADATA_VALUE# | |
cris.virtual.department | #PLACEHOLDER_PARENT_METADATA_VALUE# | |
cris.virtualsource.author-gnd | 0ab4ea86-8d32-466d-b7e3-dbebb3d7f7de | |
cris.virtualsource.author-gnd | 9b804914-1aec-4211-8e9d-9206f13d2164 | |
cris.virtualsource.author-gnd | 7d361675-ab2a-4414-a78a-7c4114af43b7 | |
cris.virtualsource.author-gnd | 751d229c-cafd-4ee9-bc62-64bd104754b7 | |
cris.virtualsource.author-gnd | 700c20f2-6c16-4d84-bc91-483459b74095 | |
cris.virtualsource.author-gnd | b74945c1-1b70-4018-b52e-0c55408239a6 | |
cris.virtualsource.author-orcid | 0ab4ea86-8d32-466d-b7e3-dbebb3d7f7de | |
cris.virtualsource.author-orcid | 9b804914-1aec-4211-8e9d-9206f13d2164 | |
cris.virtualsource.author-orcid | 7d361675-ab2a-4414-a78a-7c4114af43b7 | |
cris.virtualsource.author-orcid | 751d229c-cafd-4ee9-bc62-64bd104754b7 | |
cris.virtualsource.author-orcid | 700c20f2-6c16-4d84-bc91-483459b74095 | |
cris.virtualsource.author-orcid | b74945c1-1b70-4018-b52e-0c55408239a6 | |
cris.virtualsource.department | 0ab4ea86-8d32-466d-b7e3-dbebb3d7f7de | |
cris.virtualsource.department | 9b804914-1aec-4211-8e9d-9206f13d2164 | |
cris.virtualsource.department | 7d361675-ab2a-4414-a78a-7c4114af43b7 | |
cris.virtualsource.department | 751d229c-cafd-4ee9-bc62-64bd104754b7 | |
cris.virtualsource.department | 700c20f2-6c16-4d84-bc91-483459b74095 | |
cris.virtualsource.department | b74945c1-1b70-4018-b52e-0c55408239a6 | |
datacite.resourceType | Other | en_US |
datacite.resourceTypeGeneral | Other | en_US |
dc.contributor.author | Huber, Patrick | |
dc.contributor.author | Soprunyuk, Viktor | |
dc.contributor.author | Embs, Jan P. | |
dc.contributor.author | Wagner, Christian | |
dc.contributor.author | Deutsch, Moshe | |
dc.contributor.author | Kumar, Satish | |
dc.date.accessioned | 2022-06-07T06:54:41Z | |
dc.date.available | 2022-06-07T06:54:41Z | |
dc.date.issued | 2005-04-08 | |
dc.description.abstract | Faraday surface instability measurements of the critical acceleration, ac, and wavenumber, kc, for standing surface waves on a tetracosanol (C₂4H₅0) melt exhibit abrupt changes at Ts=54degC above the bulk freezing temperature. The measured variations of ac and kc vs. temperature and driving frequency are accounted for quantitatively by a hydrodynamic model, revealing a change from a free-slip surface flow, generic for a free liquid surface (T>Ts), to a surface-pinned, no-slip flow, characteristic of a flow near a wetted solid wall (T < Ts). The change at Ts is traced to the onset of surface freezing, where the steep velocity gradient in the surface-pinned flow significantly increases the viscous dissipation near the surface. | en |
dc.identifier.arxiv | 0504056v1 | de_DE |
dc.identifier.citation | Physical Review Letters 94 (18): 184504 (2005-04-08) | de_DE |
dc.identifier.scopus | 2-s2.0-27144529986 | de_DE |
dc.identifier.uri | http://hdl.handle.net/11420/12825 | |
dc.language.iso | en | de_DE |
dc.publisher | American Physical Society | de_DE |
dc.relation.ispartof | Physical review letters | de_DE |
dc.relation.issn | 1079-7114 | de_DE |
dc.subject | Physics - Fluid Dynamics | de_DE |
dc.subject | Physics - Fluid Dynamics | de_DE |
dc.subject.ddc | 530: Physik | de_DE |
dc.title | Faraday instability in a surface-frozen liquid | de_DE |
dc.type | Journal Article | de_DE |
dc.type.casrai | Other | en_US |
dc.type.dini | Other | en_US |
dc.type.driver | Other | en_US |
dcterms.DCMIType | Other | en_US |
dspace.entity.type | Publication | |
local.status.inpress | false | de_DE |
local.type.legacy | Article | |
oaire.citation.articlenumber | 184504 | de_DE |
oaire.citation.issue | 18 | de_DE |
oaire.citation.volume | 94 | de_DE |
tuhh.abstract.english | Faraday surface instability measurements of the critical acceleration, ac, and wavenumber, kc, for standing surface waves on a tetracosanol (C₂4H₅0) melt exhibit abrupt changes at Ts=54degC above the bulk freezing temperature. The measured variations of ac and kc vs. temperature and driving frequency are accounted for quantitatively by a hydrodynamic model, revealing a change from a free-slip surface flow, generic for a free liquid surface (T>Ts), to a surface-pinned, no-slip flow, characteristic of a flow near a wetted solid wall (T < Ts). The change at Ts is traced to the onset of surface freezing, where the steep velocity gradient in the surface-pinned flow significantly increases the viscous dissipation near the surface. | de_DE |
tuhh.publisher.doi | 10.1103/PhysRevLett.94.184504 | |
tuhh.type.opus | Other | en_US |