Condensation in Microchannels


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Research Objectives

Microchannels are increasingly being used to yield compact geometries for heat transfer in wide variety of applications.  Two-phase flow in microchannels have received considerable attention due to growing interest in high heat fluxes made possible by these micro-channel geometries.  Limited research has been done on flow regimes, and the measurement of pressure drop and heat transfer during condensation.  Heat removal and rejection applications can also benefit from high heat flux condensation.  The ultimate rejection of large heat duties, in the electronics cooling industry, through compact condensers has not been addressed adequately. 

Research Objectives:

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To understand condensation flow phenomena and transitions for R134a in mini-channel  geometries

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To study heat transfer and pressure drop for R134a in micro-channel geometries with 100 mm < Dh < 5 mm and understand the effect of Dh and shape

To develop experimentally validated, flow-mechanism-based pressure drop and heat transfer models for each flow regime for a wide range of operating conditions and mini-channel geometries.

Minichannel Geometries

Flow visualization studies were conducted on the circular, rectangular and square tube geometries of varying hydraulic diameter and aspect ratios as shown on the left side.  The flow pattern maps based on these studies were further used to do determine the applicable flow regime for the pressure drop and heat transfer data for a variety of circular and noncircular channels with 0.4 < Dh < 5 mm as shown in center and right side. Experiments were conducted for 0 < x < 1 and 150 < G < 750 kg/m2.

For pressure drop and heat transfer experiments the test sections were fabricated as flat tubes with multiple extruded parallel channels.  Three such tubes were brazed together with refrigerant flowing through the center tube, and coolant flowing in counterflow through the top and bottom tubes. 

Condensation Flow Mechanisms

A novel test facility that enabled visualization of the actual condensation process (and not simulations using air-water mixtures) was developed.  Essentially, two-phase refrigerant of a desired inlet quality was supplied to a glass test section with the cross-section under consideration.  The glass section was enclosed in an outer Plexiglas annulus through which compressed air flowed.  The compressed air decreased the differential pressure to be withstood by the glass channel while also serving as a coolant that enabled condensation.  Air temperatures and flow rates were adjusted to allow a small amount of condensation (0.05 < ∆x < 0.10) in the test section.  With this arrangement, condensation flow mechanisms were recorded using video photography with fast shutter speeds across the entire vapor-liquid dome in small increments (high resolution) of vapor quality.

 

Effect of Geometry on Flow Regimes

Extent of the intermittent flow regime increases as the hydraulic diameter decreases, signifying an increasing influence of surface tension at the small diameters.  Also, the wavy flow regime progressively decreases and disappears as the diameter decreases, giving way to the annular flow regime, signifying a diminishing influence of gravitational forces at the small diameters.  The effect of changing tube shapes (round, square, rectangular with different aspect ratios) was also documented.  Tube shape, however, was found to be less significant than hydraulic diameter in determining the applicable condensation flow pattern.

 

Pressure Drop Modeling

Pressure drop measurements on a multitude of circular and noncircular tubes across the vapor-liquid dome were used, in conjunction with the insights from the flow visualization studies, to develop experimentally validated models for condensation pressure drop.   

The intermittent flow pressure drop model (also shown to apply to discrete-wave flow) treats the overall pressure drop as a combination of the contributions due to the liquid slug, the film-bubble interface region, and the transitions between the slug and the bubble.  A slug frequency model was used to provide closure to the intermittent flow model.

In the annular flow pressure drop model (also shown to apply to disperse-wave and mist flows), the interfacial friction factor derived from the measured pressure drops was correlated in terms of the corresponding liquid-phase Reynolds number and friction factor, the Martinelli parameter, and a surface tension-related parameter. 

The resulting model predicted 82% of the annular flow pressure drop data within ±20%.  It was also shown that at the same mass flux, quality and L/D, the two-phase pressure drop increases as the tube diameter decreases.

 

 

 

 

Heat Transfer Coefficents

Condensation heat transfer coefficients were measured, for a variety of circular and noncircular channels with 0.4 < Dh < 5 mm, using an innovative thermal amplification technique developed to measure heat transfer rates at small scales accurately. 

 

Thermal amplification technique decouples the issue of measuring low heat duties and maintaining high resistance ratios by using a combination of a high flow rate closed loop primary coolant to establish high resistance ratio (Rrefg/Rcoolant) and a low flow rate open loop secondary coolant to ensures the accurate measurement of the small heat duties in these microchannels and the deduction of condensation heat transfer coefficients from measured UA values. Low secondary coolant flow rate ensures high DT, low uncertainty in Q.

 

A model for predicting heat transfer during condensation of refrigerant R134a in three horizontal circular microchannels (0.5 < Dh < 1.5 mm) over the mass flux range 150 < G < 750 kg/m2-s was developed. Results from previous work on condensation flow mechanisms in microchannel geometries were used to interpret the results based on the applicable flow regimes. The utilization of the appropriate existing shear stress models developed specifically for microchannels in the shear driven heat transfer models is able to account for the related heat transfer phenomena accurately.  The heat transfer coefficient increases with an increase in mass flux and quality, and with a decrease in the tube diameter.

 

Fabrication of Channels With 100<Dh<200 µm

The fabrication process starts with the fabrication of an X-ray mask, which is subsequently used to pattern a PMMA mold over a copper wafer. Copper is then deposited into the mold using the process of electroforming followed by planarization. Holes for refrigerant inlet and exit are then drilled into each of the refrigerant channel sets. Figure on left shows the layout of the mask used for X-ray lithography. As shown in the layout, 7 different devices (each set of channels, for example twenty 0.1 ´ 0.1 mm channels, is referred to as device) are obtained. All devices have constant depth of 100 mm, but varying number of channels and widths to test the effect of aspect ratio. Figure on right shows picture of the developed refrigerant channels after the removal of the PMMA mask. Open header area and the location of inlet and exit ports allow for the distribution of refrigerant into various parallel channels.

These channels are then closed using the process of diffusion bonding with another copper wafer on the top of these developed refrigerant channels. No adhesive is used in this process, and bonding is performed in a vacuum oven at 450oC for 3 hours. In this process the bonded joint has almost bulk material like properties, allowing the channels to withhold pressures as high as 10 MPa.

Experimental Setup

The coolant, water flows through the water channel blocks made out of copper shown in figure. Each water channels block has five 1.5 cm long holes of 0.794 mm (1/32”) diameter drilled in them.   These water channel blocks are soldered to the refrigerant channel blocks as shown in figure. Water flows in the counter flow direction.

A novel measurement technique is developed to measure the very high heat transfer coefficients at these microscales, especially due to the low heat transfer rates at extremely small flow rates under consideration.  Energy balances on pre- and post-heaters are used to establish the refrigerant inlet and outlet states at the test section.  Cooling of the refrigerant in the test section is accomplished using water at a high flow rate to ensure that the condensation side presents the governing thermal resistance.

This method yields accurate measurements of heat transfer coefficients for refrigerant R134a for 300 < G < 800 kg/m2-s and 0 < x < 1 over a wide range of saturation temperatures (30 < T < 60oC).  The measured heat transfer coefficients and pressure drops are being analyzed to develop models for pressure drop and heat transfer during condensation at the microscales. The results from this work will directly benefit the design of a variety of high heat flux heat transfer applications at the microscales.

Potential Applications

A fundamental understanding of condensation at the micro-scales will yield far reaching benefits not only for electronics industries, but also for other as-yet untapped applications such as:

        Portable personal cooling devices

        Hazardous duty and high ambient air-conditioning

        Medical/surgical devices

        Fuel cells

        Miniature heat pumps

        Microchannel heat exchangers

Sponsors

This study was supported by a research grant from Modine Manufacturing Company, Racine, WI, and National Science Foundation. 

Papers

1.      Garimella, S., A. Agarwal and J. D. Killion (2005), "Condensation Pressure Drop in Circular Microchannels," Heat Transfer Engineering Vol. 26(3) pp. 1-8.

2.      Garimella, S. (2004), "Condensation Flow Mechanisms in Microchannels: Basis for Pressure Drop and Heat Transfer Models," Heat Transfer Engineering Vol. 25(3) pp. 104-116.

3.      Coleman, J. W. and S. Garimella (2003), "Two-Phase Flow Regimes in Round, Square and Rectangular Tubes During Condensation of Refrigerant R134a," International Journal of Refrigeration Vol. 26(1) pp. 117-128.

4.      Garimella, S., J. D. Killion and J. W. Coleman (2003), "An Experimentally Validated Model for Two-Phase Pressure Drop in the Intermittent Flow Regime for Noncircular Microchannels," Journal of Fluids Engineering Vol. 125(5) pp. 887-894.

5.      Garimella, S., J. D. Killion and J. W. Coleman (2002), "An Experimentally Validated Model for Two-Phase Pressure Drop in the Intermittent Flow Regime for Circular Microchannels," Journal of Fluids Engineering Vol. 124(1) pp. 205-214.

 

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