Mohsen Farzad
Carrier Corporation
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International Journal of Refrigeration-revue Internationale Du Froid | 1994
Mohsen Farzad; Dennis L. O'Neal
Abstract One variable required for modelling the heat transfer and pressure drop of refrigerant inside air conditioner evaporators and condensers is the void fraction. Eight void fraction models were used in a refrigeration system model to evaluate their impact on the estimation of important system variables in an air conditioner as a function of charging. The void fraction models included: (i) homogeneous, (ii) Lockhart and Martinelli, (iii) Thom, (iv) Zivi, (v) Baroczy, (vi) Hughmark, (vii) Premoli and (viii) Tandon. The system variables considered included: power, capacity, refrigerant flow, subcooling and superheat. Comparisons were made with a 10.6 kW capacity air conditioner with capillary tube expansion. Results indicate that the Hughmark void fraction model appeared to provide the best comparison to measured data over the range of charging conditions considered.
Volume 6: Fluids and Thermal Systems; Advances for Process Industries, Parts A and B | 2011
Miad Yazdani; Thomas D. Radcliff; Abbas A. Alahyari; Mohsen Farzad
CO2 is an attractive alternative to conventional refrigerants due to its low direct global warming effects. Unfortunately, CO2 and many alternative refrigerants have lower thermodynamic performance resulting in larger indirect emissions. Effective use of ejectors to recover part of the lost expansion work, which occurs in throttling devices can close this performance gap and enable the use of CO2 . In an ejector, the pressure of the motive fluid is converted into momentum through a choked converging-diverging nozzle, which then entrains and raises the energy of a lower-momentum suction flow. In a two-phase ejector, the motive nozzle flow is complicated by non-equilibrium phase change affecting local sonic velocity and leading to various types of shockwaves, pseudo shocks, and expansion waves inside or outside the exit of the nozzle. Since the characteristics of the jet leaving the motive nozzle greatly affect the performance of the ejector, this paper focuses on the details of flow development and shockwave interaction within and just outside the nozzle. The analysis is based on a high-fidelity model that incorporates real-fluid properties of CO2 , local mass and energy transfer between phases, and a two-phase sonic velocity model in the presence of finite-rate phase change. The model has been validated against literature data for two-phase supersonic nozzles as well as overall ejector performance data. The results show that due to non-equilibrium effects and delayed phase change, the flow can choke well downstream of the minimum-area throat. Also, Mach number profiles show that, although phase change is at a maximum near the boundaries, the flow first becomes supersonic in the interior of the flow where sound speed is lowest. Shock waves occurring within the nozzle can interact with the boundary layer flow and result in a ‘shock train’ and a sequence of subsonic and supersonic flow observed previously in single-phase nozzles. In cases with lower nozzle back pressure, the flow continues to accelerate through the nozzle and the exit pressure adjusts in a series of supersonic expansion waves.Copyright
Archive | 2005
Payman Sadegh; Mohsen Farzad
Archive | 2004
Pengju Kang; Mohsen Farzad; Slaven Stricevic; Payman Sadegh; Alan M. Finn
Archive | 2004
Payman Sadegh; Mohsen Farzad; Alan M. Finn; Pengju Kang; Slaven Stricevic
Archive | 2004
Pengju Kang; Mohsen Farzad; Slaven Stricevic; Payman Sadegh; Alan M. Finn
Archive | 2004
Pengju Kang; Thomas D. Radcliff; Mohsen Farzad; Alan M. Finn
Archive | 2005
Pengju Kang; Mohsen Farzad; Alan M. Finn; Payman Sadegh
Archive | 2005
Pengju Kang; Mohsen Farzad; Alan M. Finn; Payman Sadegh
Archive | 2007
Pengju Kang; Mohsen Farzad; Alan M. Finn; Payman Sadegh; Slaven Stricevic