Flow boiling in parallel microchannels enables high-heat-flux cooling but suffers flow maldistribution and self-sustained flow oscillations. Jin, Wen and Narayanan (2020) showed, with a lumped two-channel model and experiments, that flow oscillations of sufficient amplitude synchronize the temperatures of parallel channels coupled thermally (heat conduction through the shared wall, coefficient UtU_t) and/or hydraulically (common inlet/outlet manifolds, coefficient UpU_p), turning oscillation into a maldistribution-mitigation tool — leaving open the quantitative problem: determine the threshold values and ranges of UtU_t and UpU_p that yield synchronization for given evaporator geometry and operating conditions; derive explicit mappings from channel geometry, wall thickness, wall thermal conductivity, manifold design and local convective heat transfer to UtU_t and UpU_p; measure per-channel instantaneous mass flow rates during oscillatory operation; extend the one-zone, channel-averaged model to capture spatial variations; and validate valve/pump actuation strategies.

Background

Microchannel evaporators remove very high heat fluxes, such as those of power electronics and high-performance computing chips, by flow boiling: a pumped liquid coolant vaporizes inside many parallel channels of sub-millimeter scale, absorbing latent heat. Boiling in parallel channels produces two characteristic pathologies. First, flow maldistribution: because the pressure-drop-versus-flow curve of a boiling channel can be non-monotonic, channels sharing inlet and outlet manifolds can settle into asymmetric steady states in which some channels are starved of liquid — the classical static Ledinegg instability (flow excursion). Second, dynamic instabilities: when the loop contains a compressible volume (an accumulator or trapped vapor), the boiling channel can interact with it in a self-sustained limit cycle (a periodic oscillation the system maintains without external forcing) known as pressure-drop oscillation, a large-amplitude, low-frequency oscillation of flow rate, pressure and wall temperature. Both produce uneven wall temperatures, premature dryout (early loss of liquid contact with the channel wall), and degraded cooling.

Two neighboring literatures address these instabilities. For the static problem, models of two-phase flow distribution that include lateral heat conduction through the solid walls between channels — the thermal coupling between channels — show that wall conduction redistributes heat away from flow-starved channels and suppresses maldistribution: Van Oevelen, Weibel and Garimella (2018) predicted, and Miglani, Weibel and Garimella (2021) confirmed experimentally with per-channel flow-rate measurement, that thermally coupled parallel channels maldistribute only beyond a critical heat flux that rises with increasing lateral wall conductance. For the dynamic problem, an experimental line (Rafałko et al., 2020-2026), using high-speed imaging and recurrence analysis (a nonlinear time-series method that detects whether two fluctuating signals visit shared dynamical states), documented that boiling in neighboring minichannels can synchronize — flow patterns and pressure fluctuations lock into common dynamics — with the degree of synchronization depending on the prevailing flow pattern.

Jin, Wen and Narayanan (2020) connected these threads. They studied an evaporator of two parallel channels that interact (i) thermally, by heat conduction through the shared wall between them, summarized by an effective thermal-coupling coefficient UtU_t, and (ii) hydraulically, through the common inlet and outlet manifolds, summarized by a flow-coupling coefficient UpU_p. Operationally, UtU_t measures the strength of the thermal interaction — the heat exchanged between neighboring channels through the shared wall per unit temperature difference between them — and UpU_p measures the strength of the flow interaction — the extent to which a flow disturbance in one channel, such as a sudden change in flow rate or pressure, is transmitted to the other through the common manifolds; both are effective parameters of the channel-averaged description and are, in general, state-dependent during oscillations rather than fixed constants. A lumped, one-zone model — meaning each channel is treated as a single well-mixed control volume with properties averaged over its length, with vapor quality (the vapor mass fraction of the two-phase mixture) treated as a channel average — predicts when the two channels' self-sustained boiling oscillations synchronize. Their experiments on thermally coupled versus decoupled channel pairs showed that flow oscillations of sufficient amplitude synchronize the channel temperatures, in the sense of reducing the wall temperature difference between channels, when the channels are thermally coupled, flow coupled, or both; they proposed deliberately allowing controllable flow oscillations as a simple strategy to mitigate maldistribution.

This made synchronization a potential design tool — but an empirical one. What remains missing to make it quantitative: threshold values and ranges of UtU_t and UpU_p required for synchronization for given evaporator geometries and operating conditions; explicit relations mapping channel geometry, wall thickness, wall thermal conductivity, manifold design and local convective heat transfer onto the effective coupling coefficients used in the lumped model; direct measurement of the instantaneous mass flow rate of each channel during oscillatory operation (their testbed inferred flow redistribution only indirectly, from temperatures and pressures); extension of the model beyond the one-zone channel average to capture spatial variations along the channel, including the subcooled inlet region (liquid cooled below its saturation temperature) and transient local variations of the heat transfer coefficient; and actuation strategies (valve or pump modulation) validated to produce desirable oscillation amplitudes and frequencies without unacceptable reliability or performance penalties.

Problem Statement

The problem arising from the results of Jin, Wen and Narayanan (2020), for a microchannel evaporator with parallel boiling channels, is to convert the observed temperature-synchronization phenomenon into quantitative, design-usable knowledge, so that synchronization can be predicted from geometry and operating conditions and actuated beneficially. Its linked components are:

(1) Determine the threshold values and ranges of the thermal-coupling coefficient UtU_t and the flow-coupling coefficient UpU_p within which the flow-boiling oscillations of the parallel channels synchronize so as to equalize channel temperatures — that is, establish the synchronization boundary in the (UtU_t, UpU_p) plane and how it depends on evaporator geometry and operating conditions (heat load, total flow rate, inlet subcooling). The UtU_t and UpU_p of this boundary are the effective scalar coefficients of the one-zone, channel-averaged model that characterize the two coupled channels at the stated operating conditions — their nominal, cycle-averaged values at that operating point — so that the threshold is a well-defined locus in the plane. The instantaneous, state-dependent variation of these coefficients along an oscillation cycle is the subject of the model extension in component (4), not of the boundary itself.

(2) Derive explicit relations that map the physical design parameters — channel geometry, wall thickness, wall thermal conductivity, manifold design, and local convective heat transfer — onto the effective coupling coefficients UtU_t and UpU_p used in the lumped model, so that the thresholds from (1) become predictable design quantities rather than fitted constants.

(3) Measure, experimentally, the instantaneous mass flow rate of each channel during oscillatory operation, in order to directly quantify how the flow redistributes on average as synchronization develops, replacing the present indirect inference from temperatures and pressures.

(4) Extend the theoretical model beyond the one-zone, channel-averaged approximation so that it captures spatial variations along the channels — including the subcooled inlet region and local variations of the heat transfer coefficient during transients — and thereby improves quantitative agreement with the observed synchronization dynamics.

(5) Design and validate controlled actuation strategies (valve or pump modulation) that generate oscillations of desirable amplitude and frequency, as predicted by the criteria of (1)-(2), without introducing unacceptable reliability or performance penalties.

These components are complementary and serve a single objective — turning the observed synchronization phenomenon into robust design and control prescriptions for practical microchannel evaporators. Components (1)-(2), together with the model extension of (4), form the quantitative core: the synchronization boundary and its geometry-to-coefficient mapping can be established theoretically or by simulation, and a complete answer to them resolves the stated objective. Components (3) and (5) require physical experiment and validated hardware; they are the experimental realization and the design validation that the quantitative core is meant to enable, and they do not gate resolution of a theoretical or simulation answer.

References

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