Inverted Leidenfrost-like Effect during Condensation

Water droplets condensing on solidified phase change materials such as benzene and cyclohexane near their melting point show in-plane jumping and continuous ``crawling'' motion. The jumping drop motion has been tentatively explained as an outcome of melting and refreezing of the materials...

ver descrição completa

Detalhes bibliográficos
Autores: Beysens, D.A. (Daniel A.)|||/items/4aac4502-ec14-44e7-80cc-29857d0bb68a, Varanasi, K.K. (Kripa K.)|||/items/befba709-85ca-45e8-90bb-ebd20d602451, Gonzalez-Viñas, W. (Wenceslao)|||/items/51b6a297-7659-424d-acc7-efea981f638d, Medici, M.G. (Marie-Gabrielle)|||/items/e6136249-4bdf-4543-90b6-5574faf88c60, Rykaczewski, K. (Konrad)|||/items/e4841637-284e-4979-8161-165562270bda, Anand, S. (Sushant)|||/items/760730b0-a856-4397-9e8d-f9bb21b5ac86, Narhe, R.D. (Ramchandra D.)|||/items/50bb9ea8-1040-4d28-9bfe-788fb1603c31
Formato: artículo
Fecha de publicación:2015
País:España
Recursos:Universidad de Navarra
Repositorio:Dadun. Depósito Académico Digital de la Universidad de Navarra
Idioma:inglés
OAI Identifier:oai:dadun.unav.edu:10171/38356
Acesso em linha:https://hdl.handle.net/10171/38356
Access Level:acceso abierto
Palavra-chave:Condensation
Inverted Leidenfrost-like effect
Materias Investigacion::Física
Descrição
Resumo:Water droplets condensing on solidified phase change materials such as benzene and cyclohexane near their melting point show in-plane jumping and continuous ``crawling'' motion. The jumping drop motion has been tentatively explained as an outcome of melting and refreezing of the materials surface beneath the droplets and can be thus considered as an inverted Leidenfrost-like effect (in the classical case vapor is generated from a droplet on a hot substrate). We present here a detailed investigation of jumping movements using high-speed imaging and static crosssectional cryogenic focused ion beam scanning electron microscope imaging. Our results show that drop motion is induced by a thermocapillary (Marangoni) effect. The in-plane jumping motion can be delineated to occur in two stages. The first stage occurs on a millisecond time scale and comprises melting the substrate due to drop condensation. This results in droplet depinning, partial spreading, and thermocapillary movement until freezing of the cyclohexane film. The second stage occurs on a second time scale and comprises relaxation motion of the drop contact line (change in drop contact radius and contact angle) after substrate freezing. When the cyclohexane film cannot freeze, the droplet continuously glides on the surface, resulting in the crawling motion.