@Article{CristaldoVargFach:2015:EfPrEf,
author = "Cristaldo, Cesar F. C. and Vargas, Maycol Marcondes and Fachini
Filho, Fernando",
affiliation = "{Universidade Federal do Pampa (UNIPAMPA)} and {Instituto Nacional
de Pesquisas Espaciais (INPE)} and {Instituto Nacional de
Pesquisas Espaciais (INPE)}",
title = "Ferrofluid droplet vaporization under very large magnetic power:
effects of pressure and effective thermal conductivity of liquid",
journal = "Proceedings of the Combustion Institute",
year = "2015",
volume = "35",
number = "2",
pages = "1613--1620",
keywords = "Ferrofluid, Magnetic relaxation heating, Magnetic nanoparticle,
Droplet combustion.",
abstract = "The aim of current analysis is to quantify the influence of the
effective thermodynamic and transport coefficients and of the
transient process of mass and energy accumulation in the gas phase
(pressure effect) on the heating and vaporization of a single
ferrofluid droplet. Ferrofluids under external alternating
magnetic field heat up themselves due to the magnetic Brownian
relaxation mechanism. Under the condition of very large magnetic
power compared to the thermal power provided by heat transfer from
the gas phase, the magnetic heat source together with the heat
transfer from the gas phase impose a thermal boundary layer
adjacent to the droplet surface in the liquid side and the
temperature presents a maximum inside the droplet, not at the
surface. Since the transport coefficient increases significantly
with a dispersion of a small quantity of nanoparticles, the heat
transfer from the thermal boundary layer to the droplet core
increases. Then the temperature of that region increases faster
comparing to the case without nanoparticle dispersion. The
temperature inside the thermal boundary layer increases slower
because of the heat transfer to the droplet core as well as to the
droplet surface. Therefore, the boiling condition which is found
inside the thermal boundary layer is reached later when
considering effective thermal conductivity. The droplet
vaporization rate is augmented by the heat transfer from the
thermal boundary layer to the droplet surface. In addiction, the
strong dependence of the magnetic relaxation mechanism on
temperature imposes a dependence of the vaporization rate on the
initial condition of the problem.",
doi = "10.1016/j.proci.2014.06.009",
url = "http://dx.doi.org/10.1016/j.proci.2014.06.009",
issn = "1540-7489",
language = "en",
targetfile = "cristaldo_ferrofluid.pdf",
urlaccessdate = "27 abr. 2024"
}