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The fat-free mass, body cell mass, phase angle, and capacitance were also determined.
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The effects of bulk phase mass transfer resistances, interfacial sorption kinetics, and finite phase volumes are included.
During the first 1 2 days, an increase in the mass (swelling phase) then a gradual decrease (desorption phase) is observed.
The duration time depends on the mass of phase change materials and also depends on phase change materials itself which have different melting temperatures.
Approximately 30 g of tripalmitin was melted at 70°C and mixed with 1.5 ml of 10 m m DiIC12(3) (Molecular probes D-383; Invitrogen, Carlsbad, CA, USA) ethanol solution to form a uniform molten mass (lipid phase).
Another scenario exists in which material is lost from the inner binary; in stead of a stable mass transfer phase, mass is expelled through a CE-phase.
After about 3 Myr, the primary star fills its Roche lobe and initiates a mass transfer phase (Figure 8).
In this last scenario, the triple undergoes the MIEK mechanism, despite and because of the mass transfer phase.
The effects of thermal mass and phase change material on building cooling/heating loads and peak loads are discussed.
The modification of the Roche lobe affects the evolution of the mass transfer phase, e.g. the duration and the mass loss rate.
For simplicity, we make the common assumption that any circularized system entering RLOF, is and will remain synchronized during the mass transfer phase.
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