FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2894326963> ?p ?o ?g. }

• W2894326963 endingPage "318" @default.
• W2894326963 startingPage "311" @default.
• W2894326963 abstract "Faraday instability plays an important role to realize liquid atomization which has been widely applied in various fields. The spherical Faraday instability has different characteristics from the planar one. It is of great importance to understand the fundamental mechanisms of the surface deformation evolution and atomization of a spherical droplet induced by Faraday instability. In this paper, we first experimentally recorded the deformation and fragmentation process of a spherical droplet on a vertically vibrated plate with high speed camera. The results showed that the zonal, meridional and approximately circular standing waves in proper order exist on the surface of the spherical droplet with the increase of excitation amplitude. When Bo<3.0, the modes of low (zonal) and high (meridional) order m of the spherical harmonic occur more easily, and as Bo is increased, the order m becomes closer to the intermediate value of spherical mode number l. The mechanism of droplet atomization is that a spike forms first on the droplet surface due to the impingement of the liquid flowing from the neighboring trough portions, and then a neck appears because of the velocity difference between the head and bottom of the spike, and the velocity difference determines whether the head liquid can form a sub-droplet ejected from the surface of the parent droplet. The Mathieu equation was derived by a linear theoretical analysis with inviscid and incompressible assumptions for the spherical Faraday instability, in which the parameters have different definitions from its planar counterpart. In the instability diagram, the iso-curves of larger linear growth rate deviate further from the ordinate axis and finally disappear. It is also validated that Lang’s equation is applicable to the spherical Faraday instability in low frequency." @default.
• W2894326963 created "2018-10-05" @default.
• W2894326963 creator A5005151685 @default.
• W2894326963 creator A5030242775 @default.
• W2894326963 creator A5031587216 @default.
• W2894326963 creator A5049325188 @default.
• W2894326963 date "2019-01-01" @default.
• W2894326963 modified "2023-09-28" @default.
• W2894326963 title "Experimental investigation on the atomization of a spherical droplet induced by Faraday instability" @default.
• W2894326963 cites W1757848849 @default.
• W2894326963 cites W1964137444 @default.
• W2894326963 cites W1970743968 @default.
• W2894326963 cites W1974288028 @default.
• W2894326963 cites W1975599026 @default.
• W2894326963 cites W1978130032 @default.
• W2894326963 cites W1980404247 @default.
• W2894326963 cites W2007780624 @default.
• W2894326963 cites W2013553303 @default.
• W2894326963 cites W2037693448 @default.
• W2894326963 cites W2043060209 @default.
• W2894326963 cites W2043441339 @default.
• W2894326963 cites W2062518613 @default.
• W2894326963 cites W2068717224 @default.
• W2894326963 cites W2080922436 @default.
• W2894326963 cites W2083057893 @default.
• W2894326963 cites W2093288909 @default.
• W2894326963 cites W2094036076 @default.
• W2894326963 cites W2102120412 @default.
• W2894326963 cites W2110109357 @default.
• W2894326963 cites W2123080125 @default.
• W2894326963 cites W2125366494 @default.
• W2894326963 cites W2129483046 @default.
• W2894326963 cites W2131565292 @default.
• W2894326963 cites W2145681277 @default.
• W2894326963 cites W2147816319 @default.
• W2894326963 cites W2153704146 @default.
• W2894326963 cites W2522739248 @default.
• W2894326963 cites W2795593283 @default.
• W2894326963 cites W3104731704 @default.
• W2894326963 doi "https://doi.org/10.1016/j.expthermflusci.2018.09.016" @default.
• W2894326963 hasPublicationYear "2019" @default.
• W2894326963 type Work @default.
• W2894326963 sameAs 2894326963 @default.
• W2894326963 citedByCount "26" @default.
• W2894326963 countsByYear W28943269632018 @default.
• W2894326963 countsByYear W28943269632019 @default.
• W2894326963 countsByYear W28943269632020 @default.
• W2894326963 countsByYear W28943269632021 @default.
• W2894326963 countsByYear W28943269632022 @default.
• W2894326963 countsByYear W28943269632023 @default.
• W2894326963 crossrefType "journal-article" @default.
• W2894326963 hasAuthorship W2894326963A5005151685 @default.
• W2894326963 hasAuthorship W2894326963A5030242775 @default.
• W2894326963 hasAuthorship W2894326963A5031587216 @default.
• W2894326963 hasAuthorship W2894326963A5049325188 @default.
• W2894326963 hasConcept C108280814 @default.
• W2894326963 hasConcept C108948954 @default.
• W2894326963 hasConcept C115260700 @default.
• W2894326963 hasConcept C120665830 @default.
• W2894326963 hasConcept C121332964 @default.
• W2894326963 hasConcept C159985019 @default.
• W2894326963 hasConcept C192562407 @default.
• W2894326963 hasConcept C207821765 @default.
• W2894326963 hasConcept C2778439541 @default.
• W2894326963 hasConcept C2781052500 @default.
• W2894326963 hasConcept C3768446 @default.
• W2894326963 hasConcept C54355233 @default.
• W2894326963 hasConcept C57879066 @default.
• W2894326963 hasConcept C62520636 @default.
• W2894326963 hasConcept C74650414 @default.
• W2894326963 hasConcept C86252789 @default.
• W2894326963 hasConcept C86803240 @default.
• W2894326963 hasConceptScore W2894326963C108280814 @default.
• W2894326963 hasConceptScore W2894326963C108948954 @default.
• W2894326963 hasConceptScore W2894326963C115260700 @default.
• W2894326963 hasConceptScore W2894326963C120665830 @default.
• W2894326963 hasConceptScore W2894326963C121332964 @default.
• W2894326963 hasConceptScore W2894326963C159985019 @default.
• W2894326963 hasConceptScore W2894326963C192562407 @default.
• W2894326963 hasConceptScore W2894326963C207821765 @default.
• W2894326963 hasConceptScore W2894326963C2778439541 @default.
• W2894326963 hasConceptScore W2894326963C2781052500 @default.
• W2894326963 hasConceptScore W2894326963C3768446 @default.
• W2894326963 hasConceptScore W2894326963C54355233 @default.
• W2894326963 hasConceptScore W2894326963C57879066 @default.
• W2894326963 hasConceptScore W2894326963C62520636 @default.
• W2894326963 hasConceptScore W2894326963C74650414 @default.
• W2894326963 hasConceptScore W2894326963C86252789 @default.
• W2894326963 hasConceptScore W2894326963C86803240 @default.
• W2894326963 hasFunder F4320321001 @default.
• W2894326963 hasFunder F4320322919 @default.
• W2894326963 hasFunder F4320322927 @default.
• W2894326963 hasLocation W28943269631 @default.
• W2894326963 hasOpenAccess W2894326963 @default.
• W2894326963 hasPrimaryLocation W28943269631 @default.
• W2894326963 hasRelatedWork W1567197834 @default.
• W2894326963 hasRelatedWork W2030775989 @default.
• W2894326963 hasRelatedWork W2152640091 @default.

• next