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Development of Synthetic Air Jet Technology for Applications in Electronics Cooling Dr. Tadhg S. O’Donovan School of Engineering and Physical Sciences Heriot-Watt University 27 th HEXAG Meeting, Heriot-Watt University, Edinburgh

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Development of Synthetic Air Jet Technology for Applications in

Electronics Cooling

Dr. Tadhg S. O’Donovan

School of Engineering and Physical SciencesHeriot-Watt University

27th HEXAG Meeting, Heriot-Watt University, Edinburgh

Synthetic Air Jet Electronics Cooling

27th HEXAG Meeting, Heriot-Watt University, Edinburgh

• A flexible membrane or diaphragm forms one end of a partially enclosed chamber

• Opposite to the membrane is an opening, such as a jet nozzle or orifice plate

• A mechanical actuator or a piezoelectric diaphragm causes the membrane to oscillate and periodically forces air into and out of the opening

• Thus creating a pulsating jet that can be directed at a heated surface, such as an electronic device

What is a Synthetic Air Jet?

• Instabilities in the flow at a jet nozzle develop into vortices that impinge on the heated surface

• The breakdown of vortices along the impingement surface increases velocity fluctuations normal to the impingement surface (O’Donovan and Murray [1], [2])

• These fluctuations result in enhanced heat transfer or secondary peaks in the heat transfer distribution

• Synthetic air jets are comprised entirely of successive vortex rings

• Introduce a stronger entrainment of surrounding air than conventional, steady jets

• These factors combine to give superior heat transfer characteristics

Synthetic Air Jet Electronics Cooling

27th HEXAG Meeting, Heriot-Watt University, Edinburgh

Characteristics of a Jet Impingement Cooling

CoolingDevice

Cooling Efficiency[W/m2K]

2.4 mm Synthetic Jet 96.90

NMB CPU Fan 61.52

Shicoh CPU Fan 44.30

Synthetic Air Jet Electronics Cooling

27th HEXAG Meeting, Heriot-Watt University, Edinburgh

• Current technologies to cool state of the art circuit chips and multi-chip modules (MCMs) rely on global forced air cooling which can dissipate 0.5 to 1 W/cm2.

• It is anticipated that in the next five to ten years this requirement will increase up to 10 to 40 W/cm2

• In a cooling performance benchmark test by Kercher et al. [3], it has been shown that synthetic microjets outperform conventional CPU fan coolers

• Stroke Length

• Reynolds Number

• Strouhal Number

Synthetic Air Jet Electronics Cooling

27th HEXAG Meeting, Heriot-Watt University, Edinburgh

Characterisation of a Synthetic Air Jet

dttUL 2

00

2

00

LU

DU0Re

1

0

0

5.0

D

L

U

fDSr

Nus

selt

Num

ber

Particle Image Velocimetry (PIV)

Synthetic Air Jet Electronics Cooling

27th HEXAG Meeting, Heriot-Watt University, Edinburgh

Experimental Set-up No. 1

Phase Locked Particle Image Velocimetry

Re = 2670 L0 = 15 d

Re = 2670 L0 = 7.7 d

Synthetic Air Jet Electronics Cooling

27th HEXAG Meeting, Heriot-Watt University, Edinburgh

Synthetic Air Jet Electronics Cooling

27th HEXAG Meeting, Heriot-Watt University, Edinburgh

Experimental Set-up No. 2

Flush Mounted Heat Flux Sensors on a UWT Impingement Surface

• RdF MicroFoil Heat Flux Sensor

• Senflex Hot Film Sensor

Synthetic Air Jet Electronics Cooling

27th HEXAG Meeting, Heriot-Watt University, Edinburgh

Heat Transfer Distributions, H/D = 2

At this height above the surface the plate lies in the vortex formation region; this results in a high velocity flow occurring between the vortex and the plate at a radial distance of r/D = 0.7.

It can be seen that the mean heat transfer distribution has a local minimum at the stagnation point for Reynolds numbers of 2300 and above.

Synthetic Air Jet Electronics Cooling

27th HEXAG Meeting, Heriot-Watt University, Edinburgh

Heat Transfer Distributions, H/D = 4

At this height above the surface the plate lies in the vortex are fully formed before impingement

Resulting in a high velocity fluctuations overall and a peak at the geometric centre.

Some increase in surface heat transfer fluctuations can be seen in the wall jet flow region

Synthetic Air Jet Electronics Cooling

27th HEXAG Meeting, Heriot-Watt University, Edinburgh

Phase Locked Vorticity Plot, H/D = 1, Re = 3700, L0/D = 17

Φ = 120°

Φ = 180°

Φ = 240°

Φ = 300°

Φ = 0°

Φ = 60°

y

U

x

V

2

1

Synthetic Air Jet Electronics Cooling

27th HEXAG Meeting, Heriot-Watt University, Edinburgh

Phase Locked Vorticity Plot, H/D = 2, Re = 3700, L0/D = 17

Φ = 120°

Φ = 180°

Φ = 240°

Φ = 300°

Φ = 0°

Φ = 60°

y

U

x

V

2

1

Development of an SAJ Electronics Cooler

Synthetic Air Jet Electronics Cooling

27th HEXAG Meeting, Heriot-Watt University, Edinburgh

• Design a synthetic jet array where jets interact constructivelyjet diameters, array geometries, frequency of oscillation, amplitude etc.

• Encourage the introduction of fresh cold air into the confined region by control of the pulsation characteristics of the individual jets aligned in a channel

phase, frequency, and amplitude

Synthetic Air Jet Electronics Cooling

27th HEXAG Meeting, Heriot-Watt University, Edinburgh

• Synthetic Air Jet Cooling can outperform standard fan-fin CPU coolers and are more effective than similar steady impinging air jets

• The current research addresses the limitations of conventional synthetic jet impingement cooling systems.

• Recycling of the air in a synthetic jet array causes its temperature to continually increase which adversely affects the heat removal capacity of the jets.

• To ensure that the air being forced over the heated surface is sufficiently cool, fresh ambient air must be brought in. This is typically achieved by introducing a secondary cross-flow of air over the heated device via a fan.

• Preliminary results show that synthetic jets can operate in clusters or arrays to achieve enhanced cooling of surfaces such as electronic devices.

Synthetic Air Jet Electronics Cooling

27th HEXAG Meeting, Heriot-Watt University, Edinburgh

Conclusions

1. T. S. O'Donovan and D. B. Murray, "Jet impingement heat transfer - Part I: Mean and root-mean-square heat transfer and velocity distributions," International Journal of Heat and Mass Transfer, vol. 50, pp. 3291-3301, 2007.

2. T. S. O'Donovan and D. B. Murray, "Jet impingement heat transfer - Part II: A temporal investigation of heat transfer and local fluid velocities," International Journal of Heat and Mass Transfer, vol. 50, pp. 3302-3314, 2007.

3. D. S. Kercher, J. B. Lee, O. Brand, M. G. Allen, and A. Glezer, "Microjet cooling devices for thermal management of electronics," IEEE Transactions on Components and Packaging Technologies, vol. 26, pp. 359 - 366, 2003.

4. T. Persoons and T. S. O'Donovan, "A pressure-based estimate of synthetic jet velocity," Physics of Fluids, vol. 19, pp. 128104-4, 2007.

Synthetic Air Jet Electronics Cooling

27th HEXAG Meeting, Heriot-Watt University, Edinburgh

References