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Journal Articles
Accepted Manuscript
Article Type: Research-Article
J. Heat Mass Transfer.
Paper No: HT-22-1655
Published Online: March 21, 2023
Journal Articles
Accepted Manuscript
Article Type: Research-Article
J. Heat Mass Transfer.
Paper No: HT-22-1138
Published Online: March 21, 2023
Journal Articles
Article Type: Research-Article
J. Heat Mass Transfer. May 2023, 145(5): 052003.
Paper No: HT-22-1643
Published Online: March 20, 2023
Journal Articles
Article Type: Research-Article
J. Heat Mass Transfer. August 2023, 145(8): 083901.
Paper No: HT-22-1636
Published Online: March 20, 2023
Journal Articles
Article Type: Research-Article
J. Heat Mass Transfer. July 2023, 145(7): 072701.
Paper No: HT-22-1500
Published Online: March 20, 2023
Journal Articles
Article Type: Research-Article
J. Heat Mass Transfer. May 2023, 145(5): 052004.
Paper No: HT-22-1693
Published Online: March 20, 2023
Journal Articles
Article Type: Research-Article
J. Heat Mass Transfer. July 2023, 145(7): 072301.
Paper No: HT-22-1148
Published Online: March 20, 2023
Includes: Supplementary data
Image
in New Insights in Turbulent Heat Transfer With Oil and Hybrid Nano-Oils, Subject to Discrete Heating, for Parabolic Trough Absorbers
> ASME Journal of Heat and Mass Transfer
Published Online: March 20, 2023
Fig. 1 Schematic of the 3D, straight, long, horizontal tube with boundary conditions for computational fluid dynamics analyses More
Image
in New Insights in Turbulent Heat Transfer With Oil and Hybrid Nano-Oils, Subject to Discrete Heating, for Parabolic Trough Absorbers
> ASME Journal of Heat and Mass Transfer
Published Online: March 20, 2023
Fig. 2 Generated structured mesh for 3D computational fluid dynamics analyses More
Image
in New Insights in Turbulent Heat Transfer With Oil and Hybrid Nano-Oils, Subject to Discrete Heating, for Parabolic Trough Absorbers
> ASME Journal of Heat and Mass Transfer
Published Online: March 20, 2023
Fig. 3 Grid independence test using the time-averaged axially varying ( a ) fluid temperature at the centerline and ( b )the inner wall temperature for 2 ≤ z (in m) < 4 More
Image
in New Insights in Turbulent Heat Transfer With Oil and Hybrid Nano-Oils, Subject to Discrete Heating, for Parabolic Trough Absorbers
> ASME Journal of Heat and Mass Transfer
Published Online: March 20, 2023
Fig. 4 Comparison between ( a ) CFD-analyzed and wall-law for U + with coarse, medium, and fine meshes at z = 1.9 m and Re = 20,000, and ( b ) CFD-analyzed overall, surface-area-averaged, Nusselt number ( Nu CFD ), and the Gnielinski correlation ( Nu Gnielinski ) for TVP1 with 5000 ≤ ... More
Image
in New Insights in Turbulent Heat Transfer With Oil and Hybrid Nano-Oils, Subject to Discrete Heating, for Parabolic Trough Absorbers
> ASME Journal of Heat and Mass Transfer
Published Online: March 20, 2023
Fig. 5 RANS-based axial velocity contour at the different axial locations for TVP1 with Re = 5000, without and with gravity effect ( g = 0 and 9.81 m/s 2 ), and different heat flux ratios ( q r = 1 and 50) More
Image
in New Insights in Turbulent Heat Transfer With Oil and Hybrid Nano-Oils, Subject to Discrete Heating, for Parabolic Trough Absorbers
> ASME Journal of Heat and Mass Transfer
Published Online: March 20, 2023
Fig. 6 RANS-based axial velocity contour at the different axial locations for TVP1 with Re = 20,000, without and with gravity effect ( g = 0 and 9.81 m/s 2 ), and different heat flux ratios ( q r = 1 and 50) More
Image
in New Insights in Turbulent Heat Transfer With Oil and Hybrid Nano-Oils, Subject to Discrete Heating, for Parabolic Trough Absorbers
> ASME Journal of Heat and Mass Transfer
Published Online: March 20, 2023
Fig. 7 ( a )–( h ) RANS-based axial velocity for simulations without gravity effect and with gravity effect, different Reynolds number Re = 5000 and 20,000, and different heat flux ratios q r = 1 and 50 More
Image
in New Insights in Turbulent Heat Transfer With Oil and Hybrid Nano-Oils, Subject to Discrete Heating, for Parabolic Trough Absorbers
> ASME Journal of Heat and Mass Transfer
Published Online: March 20, 2023
Fig. 8 A comparison between the RANS-analyzed nondimensional axial velocity with the standard logarithmic law at θ = 90 deg and θ = 270 deg for simulations without and with the effect of gravity More
Image
in New Insights in Turbulent Heat Transfer With Oil and Hybrid Nano-Oils, Subject to Discrete Heating, for Parabolic Trough Absorbers
> ASME Journal of Heat and Mass Transfer
Published Online: March 20, 2023
Fig. 9 ( a )–( h ) The RANS-analyzed streamlines at various axial locations for q r = 1 and q r = 50 considering the effect of gravity at Re = 5000 More
Image
in New Insights in Turbulent Heat Transfer With Oil and Hybrid Nano-Oils, Subject to Discrete Heating, for Parabolic Trough Absorbers
> ASME Journal of Heat and Mass Transfer
Published Online: March 20, 2023
Fig. 10 The RANS-analyzed, statistical, fluid temperature contour at different axial locations for Re = 5000, g = 0, 9.81 m/s 2 , and different heat flux ratios q r = 1 and 50 More
Image
in New Insights in Turbulent Heat Transfer With Oil and Hybrid Nano-Oils, Subject to Discrete Heating, for Parabolic Trough Absorbers
> ASME Journal of Heat and Mass Transfer
Published Online: March 20, 2023
Fig. 11 The RANS-analyzed, statistical, fluid temperature contour at different axial locations for Re = 20, 000, g = 0, 9.81 m/s 2 , and different heat flux ratios q r = 1 and 50 More
Image
in New Insights in Turbulent Heat Transfer With Oil and Hybrid Nano-Oils, Subject to Discrete Heating, for Parabolic Trough Absorbers
> ASME Journal of Heat and Mass Transfer
Published Online: March 20, 2023
Fig. 12 ( a )–( h ) RANS-based statistic fluid and solid temperatures for simulations without gravity effect and with gravity effect, different Reynolds number Re = 5000 and 20,000, and different heat flux ratios q r = 1 and 50 More
Image
in New Insights in Turbulent Heat Transfer With Oil and Hybrid Nano-Oils, Subject to Discrete Heating, for Parabolic Trough Absorbers
> ASME Journal of Heat and Mass Transfer
Published Online: March 20, 2023
Fig. 13 RANS-based ( a ) fluid and solid temperatures for simulations with gravity effect at z = 3.75 m, Re = 5000, and q r = 5, 10, 20, 40, and 50, and ( b ) Richardson number using the maximum temperature difference, local thermophysical properties for TVP1, and Re = 5000 and 2... More