2015
DOI: 10.1016/j.icheatmasstransfer.2015.08.020
|View full text |Cite
|
Sign up to set email alerts
|

The characteristic variational multiscale method for time dependent conduction–convection problems

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

2
10
0

Year Published

2016
2016
2024
2024

Publication Types

Select...
9

Relationship

4
5

Authors

Journals

citations
Cited by 16 publications
(12 citation statements)
references
References 16 publications
2
10
0
Order By: Relevance
“…We present the isotherms, streamlines and isobars in Figure 11 with increasing Ra = 1, 10 4 and 10 5 . We can see that, for cases Ra = 1,10 4 , the isotherms, streamlines and isobars computed by our method simulate the temperature field, fluid field, and pressure field very well, which also conforms with the numerical results presented by Su et al (2014) and Wu et al (2015). Notes: (a) The decoupled characteristic stabilized FEM with P 1 -P 1 -P 1 triples; (b) the decoupled characteristic stabilized FEM with P 1 -P 0 -P 1 triples; (c) the standard characteristic FEM with P 1 b-P 1 -P 1 triples; (d) P 1 -P 1 -P 1 triples without addition of a stabilization term Stabilized finite element method Furthermore, our method still exhibited good stability behavior even with higher Rayleigh number Ra = 10 5 .…”
Section: Methodssupporting
confidence: 87%
“…We present the isotherms, streamlines and isobars in Figure 11 with increasing Ra = 1, 10 4 and 10 5 . We can see that, for cases Ra = 1,10 4 , the isotherms, streamlines and isobars computed by our method simulate the temperature field, fluid field, and pressure field very well, which also conforms with the numerical results presented by Su et al (2014) and Wu et al (2015). Notes: (a) The decoupled characteristic stabilized FEM with P 1 -P 1 -P 1 triples; (b) the decoupled characteristic stabilized FEM with P 1 -P 0 -P 1 triples; (c) the standard characteristic FEM with P 1 b-P 1 -P 1 triples; (d) P 1 -P 1 -P 1 triples without addition of a stabilization term Stabilized finite element method Furthermore, our method still exhibited good stability behavior even with higher Rayleigh number Ra = 10 5 .…”
Section: Methodssupporting
confidence: 87%
“…The characteristic methods are proven to be efficient in many physical problems, especially for convection-dominated problems (Qian et al , 2014). Wu et al (2015a) formulated the characteristic variational multiscale (C-VMS) finite element method (FEM) for time dependent conduction-convection problem. In this paper, we use the char- acteristic method combining variational multiscale strategy to overcome the stability issue due to the nonlinear inertial term and the hyperbolic term for conventional FEMs.…”
Section: Introductionmentioning
confidence: 99%
“…The coarse scale is then projected into an appropriate subspace while the fine scale is directly stabilized against highly localized affects such as those seen in turbulence modeling. This method has been further developed in later work and applied to problems involving incompressible flows [21,22,23] and convection-diffusion [24,25,26].…”
Section: Multiple Concurrent Methods Have Been Developed For Couplingmentioning
confidence: 99%