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Dust distribution

Heat transfer in the furnace is mainly by radiation, from the incandescent particles in the flame and from hot radiating gases such as carbon dioxide and water vapor. The detailed theoretical prediction of overall radiation exchange is complicated by a number of factors such as carbon particle and dust distributions, and temperature variations in three-dimensional mixing. This is overcome by the use of simplified mathematical models or empirical relationships in various fields of application. [Pg.347]

Absolute Values of Isokinetic Sampling Efficiency for Various Cotton Dust Distributions... [Pg.68]

Ginoux P. Prospero J. and Torres O. (2002). Long-term simulation of dust distribution with the GOCART model Correlation with the North Atlantic Oscillation. In J.A. Lee and T.M. Zobeck (eds.), Proceedings of ICAR5/GCTE-SEN Joint Conference. International Center for Arid and Semiarid Lands Studies, Texas Tech. University, Lubbock, Texas, pp. 241-245. [Pg.527]

A Comparison of Mean Values of the Protein Bearing and Total Dust Distribution Parameters Between Elevator and Ambient Air... [Pg.305]

To choose better model from model one and three, this article make dust trajectories numerical simulation by the method of single-phase coupling, stu-ding the move track of different size of dust under rated operating conditions. The direction of incident velocity plumb imported face of velocity, incidence velocity is same as inlet velocity, solid mass flow rate is zero, in order to observed trajectory, set source of jet is single-size dust, distributing... [Pg.540]

Dust explosions most often occur in containers with dust distributed in the atmosphere. They can also occur when some activity suddenly creates a cloud of airborne dust in the presence of an ignition source. Similar to gas and vapor explosions, dust explosions show effects related to the L/D ratio of the container. [Pg.248]

A model, frequently referred to as dusty-gas model [1-3], can be used to describe multi-component diffusion in porous media. This model is based on the Stefan-Maxwell approach for diluted gases which is an approximation of Boltzmann s equation. The pore walls are considered as consisting of giant molecules ( dust ) distributed in space. These dust molecules are treated as the n+l-th pseudo-species in a n-component gaseous mixture. The dust particles are kept fixed in space, and are treated like a gas component in the Stefan-Maxwell equations. This model analyzes the transport problem by distinguishing three separate components 1) diffusion, 2) viscous flow and 3) structure of the porous medium. [Pg.147]

The possibility of observing the outburst of Supernovae at the remote Galaxy regions, invisible within optical band because of interstellar extinction using thermal IR-radiation of interstellar dust heated by Supernova outburst is discussed in this paper. The investigation of this phenomenon by means of cooled IR-telescopes will allow the Supernova outburst parameters to be determined and the characteristics of the interstellar dust distribution to be studied. The similar effects can be detected in the vicinities of the well-known remnants of Supernovae, in particular, near Tycho Brahe and Cassiopeia A Supernovae. [Pg.41]

Polycyclic aromatic hydrocarbons (PAHs) Hydrocarbons in complex chains and agglomerated rings thought to be responsible for the diffuse emission Unes observed in dust nebulae in the near-infrared. These molecules form the lowest-mass end of the dust distribution and are responsible for ubiquitous diffuse emission in the 1- to 25-fxm galactic background radiation. [Pg.2]

A full description of the data and models of the dust distribution in galaxies can be found in a paper that has been submitted to the Astronomical Journal. [Pg.150]

An alternative to the spherically symmetric optically thin shell of large grains considered above is an anisotropic distribution of optically thick dust condensations. Anisotropy has exciting implications for relating dust distributions to general questions of outflows and of planetary formation in young steUax objects. However, optically thick disks of the kind usually considered in standard disk models are expected to radiate more mid-infrared radiation than we observe from the core component of LkHa 101. [Pg.314]


See other pages where Dust distribution is mentioned: [Pg.397]    [Pg.1611]    [Pg.57]    [Pg.242]    [Pg.51]    [Pg.304]    [Pg.306]    [Pg.77]    [Pg.85]    [Pg.92]    [Pg.397]    [Pg.1433]    [Pg.1925]    [Pg.360]    [Pg.397]    [Pg.289]    [Pg.92]    [Pg.1915]    [Pg.1615]    [Pg.212]    [Pg.541]    [Pg.728]    [Pg.132]    [Pg.132]    [Pg.201]    [Pg.324]    [Pg.539]   
See also in sourсe #XX -- [ Pg.85 ]

See also in sourсe #XX -- [ Pg.132 ]




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Distribution of dust

Dust grains particle size distribution

Interstellar dust particle size distribution

Surface dust size distribution

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