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mass flux
The present paper reports careful experimental investigations of the flow past bodies of revolution in the presence on their surface of a transverse mass flux, especially at a low blowing intensity.
      
The method of matched asymptotic expansions is used to obtain an analytic solution of the problem of the concentration field and the diffusion mass flux to the surface of the cloud at small and large values of the Péclet number.
      
Effect of radial mass flux on the moment of the forces acting on a spherical particle rotating in a viscous nonisothermal gas
      
The mixing effect is taken into account by means of a concentrated mass flux in the section of discontinuity.
      
A new form of the heat-transfer, mass-transfer, and fluid-flow equations is proposed in which the transferred quantities are the heat flux, mass flux, and shear stress, respectively.
      
If this process is taken into account, there is an additional mass flux into the liquid and, consequently, the mass-transfer rate is higher.
      
The mass flux of very fine particles accounts for a few percent of the total dust mass flux from comet Halley.
      
The equation is complemented by conservation laws for the mass flux and the momentum flux through the deflagration front of finite thickness.
      
An expression for the mass flux is derived that is valid for Knudsen numbers much smaller than the reciprocal of the accommodation coefficients.
      
A new intermediate flow regime, for which the mass flux is given by an expression that differs from the classical (macroscopic) form, is found to exist.
      
The paper consists of the following main sections: the use of JEBAR as a correction of an error made by the authors of the method of mass flux; G.
      
In the southern part of the typhoon, the total cloud mass flux (Mc) is positive, whereas in the northern part of the typhoonMc is negative.
      
The main factors of the change of moist potential vorticity are the vertical and horizontal divergence of moist potential vorticity flux as well as the vertical transport caused by the cumulus mass flux.
      
The latter has a 60-km horizontal resolution and improved physical parameterization schemes including the mass flux cumulus parameterization scheme, the turbulent kinetic energy closure scheme (TKE) and an improved land process model (LPM).
      
Investigation of the system's control by transpiration mass flux, ablation amount and ablation velocity varying with time, time of the ablation's beginning and ending, etc., are presented.
      
The mass flux at the test section ranged from 15-220 kg/m2s.
      
The closed spherical gap problem is generalized into an open flow system by superimposing a mass flux in meridional direction.
      
Tests were performed for a mass flux of 100, 200, 400, and 600 kg/m2s, a heat flux of 5 to 20 kW/m2, and a saturation temperature of 40°C.
      
In this study, effect of heat flux, mass flux, vapor qualities, and hydraulic diameter on flow condensation were investigated and the experimental local condensation heat transfer coefficients and frictional pressure drop are shown.
      
Base flow characteristics are explained regarding the base configuration as well as the injection parameter which is defined as the mass flow rate of bleed jet non-dimensionalized by the product of the base area and freestream mass flux.
      
 

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