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Chapter 7 Investigation of the thermal fluid system using direct numerical simulation

  • Alok Dhaundiyal and Laszlo Toth
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Flow Dynamics and Heat Transfer
This chapter is in the book Flow Dynamics and Heat Transfer

Abstract

The chapter focuses on predicting the state properties of the thermodynamic systemthermodynamic system through computational fluid dynamics (CFDcomputational fluid dynamics (CFD)). A laboratory reactor of 1.28 kWth was developed and considered whilst examining the processed loose biomass. The transient change in the thermo-fluid properties of gas in the core element of the unit was evaluated. The wave number and time step considered during the analysis were 18.47 mm−1 and 0.21, respectively. The system’s hydrostatic pressurehydrostatic pressure was omitted in the analysis. The flow is incompressible and subsonic. The standard deviationstandard deviation between the solution sets and the experimental data for velocity, pressure, and temperature were 0.02 m/s, 0.019 mbar, and 0.94 K, respectively. The maximum predicted static gas pressure through the direct numerical simulationdirect numerical simulation (DNS) was 227.60 mbar. Similarly, the gas temperature did not exceed 383 K across the core element.

Abstract

The chapter focuses on predicting the state properties of the thermodynamic systemthermodynamic system through computational fluid dynamics (CFDcomputational fluid dynamics (CFD)). A laboratory reactor of 1.28 kWth was developed and considered whilst examining the processed loose biomass. The transient change in the thermo-fluid properties of gas in the core element of the unit was evaluated. The wave number and time step considered during the analysis were 18.47 mm−1 and 0.21, respectively. The system’s hydrostatic pressurehydrostatic pressure was omitted in the analysis. The flow is incompressible and subsonic. The standard deviationstandard deviation between the solution sets and the experimental data for velocity, pressure, and temperature were 0.02 m/s, 0.019 mbar, and 0.94 K, respectively. The maximum predicted static gas pressure through the direct numerical simulationdirect numerical simulation (DNS) was 227.60 mbar. Similarly, the gas temperature did not exceed 383 K across the core element.

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