Abstract
One of the prevalent phenomena that significantly affects thermal-vapor compressors is the moisture in the motive steam. It has a dominant effect on the thermodynamic and design parameters of a thermal-vapor compressor (TVC), such as entrainment ratio, compression ratio, and flow density. This study investigates a numerical simulation of a thermal-vapor compressor operated with a two-phase flow motive steam that is composed of saturated water vapor and dispersed water droplets. The droplets injected into the computational domain are represented as the second phase and are simulated by the discrete phase model. In this method, transport equations are solved for the continuous phase, whereas droplets regarded in the Lagrangian frame are involved through interaction in source terms. Three critical factors for understanding the effect of moisture on TVC are studied: the mass flow rate, the diameter, and the number of droplets. It will be shown that the presence of moisture in motive steam, which is inevitable to be ignored in the desalination industry and vapor lines, has a negative impact on the efficiency of the thermal-vapor compressors. Eventually, the numerical results are compared with the experimental data, which are accepted with less than 5% error from the actual TVC.
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Abbreviations
- \(a_{1}\), \(a_{2}\), \(a_{3}\) :
-
Constant experimental parameters
- B.C.:
-
Boundary condition
- C D :
-
Drag coefficient
- C m :
-
Momentum exchange coefficient
- c p :
-
Specific heat capacity (J/kg. K)
- CFD:
-
Computational fluid dynamics
- CR:
-
Compression ratio
- C s :
-
Thermal slip coefficient
- C t :
-
Temperature jump coefficient
- DPM:
-
Discrete phase model
- DNS:
-
Direct numerical simulation
- D T,P :
-
Thermophoretic coefficient
- d P :
-
Particle diameter (m)
- ER:
-
Entrainment ratio
- F:
-
Momentum source term (kg/m2s2)
- F Saff :
-
Saffman's lift force (N/kg)
- F T :
-
Thermophoretic force (N/kg)
- F v :
-
Virtual mass force (N/kg)
- F x :
-
Additional acceleration force (N/kg)
- g :
-
Gravitational acceleration (m/s2)
- G k :
-
Generation of turbulence kinetic energy (kg/ms3)
- h :
-
Convective heat transfer coefficient (W/m2K)
- h fg :
-
Latent heat of vaporization (J/kg)
- HMI:
-
Human–machine interface
- kn:
-
Knudsen number
- Kr:
-
The ratio of thermal conductivity
- M:
-
Mass source term (kg/m3s)
- m p :
-
Particle mass (kg)
- ṁ :
-
Mass flow rate (kg/s)
- MED:
-
Multi-effect desalination
- MDP:
-
Maximum discharge pressure (KPa)
- P :
-
Pressure (Pa)
- P CO :
-
Cut-off pressure (KPa)
- Q :
-
Energy source term (J/m3s)
- Red :
-
Relative Reynolds number
- S ε :
-
Source terms for dissipation rate (kg/ms3)
- S k :
-
Source terms for turbulent kinetic energy (kg/ms3)
- t :
-
Time (s)
- T :
-
Temperature (K)
- T p :
-
Particle temperature (K)
- TVC:
-
Thermal-vapor compressor
- u :
-
Fluid velocity (m/s)
- u p :
-
Particle velocity (m/s)
- \(\varepsilon\) :
-
Turbulent kinetic energy dissipation rate (m2/s3)
- k :
-
Turbulence kinetic energy (m2/s2)
- ρ :
-
Density (Kg/m3)
- ρ p :
-
Particle density (Kg/m3)
- μ :
-
Dynamic viscosity (Kg/m.s)
- τ :
-
Stress tensor (Pa)
- ν :
-
Kinematic viscosity (m2/s)
- dis:
-
Discharge
- mot:
-
Motive
- p :
-
Particle (water droplet)
- Saff:
-
Saffman's lift force
- suc:
-
Suction
- T:
-
Thermophoretic
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Hakimi, M., Kouhikamali, R., Hassani, M. et al. A numerical investigation of simulating moisture in motive steam in a thermal-vapor compressor with DPM method. J Braz. Soc. Mech. Sci. Eng. 45, 89 (2023). https://doi.org/10.1007/s40430-023-04018-y
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DOI: https://doi.org/10.1007/s40430-023-04018-y