Near-Critical-Pressure Condensation of Refrigerant Blends


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Background

The use of vapor compression cycles for high-temperature-lift space-conditioning systems and concern about the depletion of the stratospheric ozone level has created an interest in high pressure, zero-ozone-depletion-potential, near-azeotropic refrigerant blends such as R404A and R410A as substitutes for refrigerants such as R22. At the desired high heat rejection temperatures in such space-conditioning and water heating systems, the saturation pressures of these blends approach and even exceed the critical pressure. 

Motivation

Phase change at near-critical pressures in these refrigerant blends is not well understood.  Much of the literature available for the prediction of condensation heat transfer is at relatively low operating pressures, and the validity of extrapolating these models to near-critical pressures is not well established

Past Work

Most prior investigations focused on:

bulletAnnular Flow
bulletPure refrigerants
bulletLow critical pressures
bulletPressure drop in adiabatic flow

 Commonly used correlations fail to predict the heat transfer and pressure gradient at higher reduced pressures.

 

 

Liquid-Vapor Dome for 410A

 

Specific Objectives
bulletExperimentally determine local h and ΔP across V-L dome in small quality increments at Pr= 0.8 and 0.9×Pcritical
bulletMass flux range 200 < G < 800 kg/m2-s
bulletRound, horizontal tubes, with diameters ranging from 0.5 < D < 9 mm
bulletDevelop flow mechanism based h and ΔP models
Approach

Experimental Facility

Schematic of Test Facility

 

Condensation:

bulletPre-condenser energy balance -> Inlet quality (enthalpy)
bulletPost-condenser energy balance -> Outlet quality (enthalpy)
bulletSecondary coolant energy balance -> Test section heat duty

 

Thermal Amplification Technique

 

 

Thermal Amplification Technique

 

bulletDecouple heat duty determination and resistance ratio issues
bulletUse high flow rate primary coolant (closed loop) to establish high resistance ratio (Rrefg/Rcoolant)
bulletAddress heat duty determination in secondary coolant (open loop) at low flow rates
bulletLow secondary coolant flow rate ensures high DT, low uncertainty in Q
Sample Findings

 

Experimental Data

bulleth increases at higher x and G
bulleth slightly decreases at higher Pr

 

Model Development

For larger diameters (6 and 9 mm I.D.), the data is divided into the following flow regimes:

·         Wavy Flow

·         Annular Flow

·         Wavy-Annular Transition

 

FrSO (Soliman modified Froude Number) is used to divide the different flow regimes.

 

Applications

This study will aid the understanding of refrigerant blend behavior at elevated pressures and will help the HVAC industry to develop safer and more efficient high-temperature-lift space-conditioning and water heating systems with less adverse impact on the environment. 

Ongoing Work/Future Directions

The Air-Conditioning and Refrigeration Technology Institute (ARTI) is the primary sponsor of this project and has particular interest in small diameter tubes, which can withstand higher operating pressures. In addition to the diameter, the effects of mass flux, operating pressure, quality (during condensation) will be experimentally investigated.

Sponsors

ARTI

Papers
  1. Mitra, B. and S. Garimella (2003), "Heat Transfer and Pressure Drop for Condensation of Refrigerant R410a at near-Critical Pressures," 2003 ASME International Mechanical Engineering Congress, Nov 15-21 2003, Washington, DC., United States, American Society of Mechanical Engineers, pp. 87-97.
  2. Jiang, Y. and S. Garimella (2003), "Heat Transfer and Pressure Drop for Condensation of Refrigerant R-404a at near-Critical Pressures," Technical and Symposium Papers Presented At the 2003 Winter Meeting of The ASHRAE, Jan 26-29 2003, Chicago, IL, United States, Amer. Soc. Heating, Ref. Air-Conditoning Eng. Inc., pp. 677-688.

 

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