2017
DOI: 10.1016/j.jqsrt.2017.06.023
|View full text |Cite
|
Sign up to set email alerts
|

Radiative entropy generation in a gray absorbing, emitting, and scattering planar medium at radiative equilibrium

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

0
4
0

Year Published

2019
2019
2024
2024

Publication Types

Select...
6

Relationship

1
5

Authors

Journals

citations
Cited by 18 publications
(5 citation statements)
references
References 20 publications
0
4
0
Order By: Relevance
“…Hinojosa et al showed that for an open cavity with an isothermal heat source, the total dimensionless rate of entropy generation increases with increase in emissivity; that is a difference with isoflux heat source. Sadeghi and Safavinejad also showed that for a mixed boundary condition (constant heat flux and constant temperature at two planes) in a planar medium with radiative equilibrium, as the emissivity of wall increases, the entropy generation rate at wall decreases slightly.…”
Section: Resultsmentioning
confidence: 97%
“…Hinojosa et al showed that for an open cavity with an isothermal heat source, the total dimensionless rate of entropy generation increases with increase in emissivity; that is a difference with isoflux heat source. Sadeghi and Safavinejad also showed that for a mixed boundary condition (constant heat flux and constant temperature at two planes) in a planar medium with radiative equilibrium, as the emissivity of wall increases, the entropy generation rate at wall decreases slightly.…”
Section: Resultsmentioning
confidence: 97%
“…During their experiments in the 1930s, Hottel and his collaborators considered the emission of radiation from a hemispherical mass of gas toward a small surface element located in the center of the base of the hemisphere. It is evident that it is convenient to extend the emissivity data reported to masses of gases of other geometric configurations and this is carried out by introducing the concept of characteristic or mean beam length L , which represents the radius of an equivalent hemisphere 24–26 …”
Section: Methodsmentioning
confidence: 99%
“…It is evident that it is convenient to extend the emissivity data reported to masses of gases of other geometric configurations and this is carried out by introducing the concept of characteristic or mean beam length L, which represents the radius of an equivalent hemisphere. [24][25][26] The AS that allows obtaining the spectral emissivity of the participating gaseous medium is then a function of the product of the characteristic length of the beam L, the partial pressure of the participating component and the view factor between the leaving and reaching surfaces (see Figure 1), being described by the following mathematical relationship 27 :…”
Section: Characteristic Length or Average Length Of The Beammentioning
confidence: 99%
“…Therefore, emissivity is a complex function that involves the volume of the gas mixture, the partial pressure of each component of the mixture P x , the average temperature of the mixture, the product of the spectral absorption coefficient of the medium k λ , the view factor F 12 and L. 25,26 Due to its high complexity, the use of Equation ( 1) in engineering practice is null. Generally, for practical calculations, the generalization of approximate experimental values of L is preferred.…”
Section: Mean Beam Lengthmentioning
confidence: 99%