Abstract
In this paper, based on the Li-Peterson pumping consumption-thermal resistance optimization model, a single-phase structure-optimized large-scale microchannel heat sink with each channel having 0.2 mm width and 0.8 mm height for extremely high heat flux cooling was proposed and investigated. Employing deionized water as coolant, two different heat source areas were designed and the results were compared under different pumping power from 0.1 W to 6.5 W. The experimental and simulation results indicates that the proposed copper-based microchannel thermal management system can dissipate heat flux of 1000 W/cm2 over 1cm2 and 500 W/cm2 over 5cm2, respectively, adding critical data support to the database of single-phase microchannel heat sink with heat removal capacity exceeding 1000 W/cm2. Moreover, the possible minimum thermal resistance over a broad pumping power range of 0.1 W to 6.5 W was explored. Extremely low thermal resistance of 0.065 K/W and 0.019 K/W were obtained for these two heating area scenarios. Overall, the proposed copper-based optimized microchannel heat sink is an ideal solution to cool high heat flux devices.
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Abbreviations
- \({A}_{ch}\) :
-
Effective heat transfer area (m2)
- \({A}_{hs}\) :
-
Source dimension (m2)
- \({c}_{p}\) :
-
Specific heat capacity (J/(kg∙K))
- \({D}_{h}\) :
-
The characteristic dimension of microchannel (m)
- \({D}_{tube}\) :
-
The inner diameter of tube (m)
- \(f\) :
-
Fanning friction factor
- \({f}_{app}\) :
-
Apparent friction factor
- \(G\) :
-
Flow rate (L/h)
- \(h\) :
-
Convective heat transfer coefficient (W/(m2∙K))
- \(H\) :
-
Height of channel (mm)
- \({H}_{b}\) :
-
Thickness of microchannel substrate (mm)
- \(I\) :
-
Current (A)
- \({K}_{w}\) :
-
Thermal conductivity of deionized water (W/(m∙K))
- \(L\) :
-
Length of channel (mm)
- \(m\) :
-
Mass flow (kg/s)
- \(N\) :
-
Number of microchannels
- \(Nu\) :
-
Nusselt number
- \(P\) :
-
Pressure (kPa)
- \({P}_{w}\) :
-
Pumping power (W)
- \({P}_{Q}\) :
-
Input heating power by AC power (W)
- \(\Delta P\) :
-
Pressure drop (kPa)
- Pr :
-
Prandt number
- \(Q\) :
-
Heating power (W)
- \(q\) :
-
Heat flux (W/cm2)
- \(R\) :
-
Total thermal resistance of heat sink (K/W)
- \({R}_{cd}\) :
-
Conduction thermal resistance of heat sink (K/W)
- \({R}_{cv}\) :
-
Convection thermal resistance of heat sink (K/W)
- \({R}_{c}\) :
-
Capacity thermal resistance of heat sink (K/W)
- Re :
-
Reynolds number
- \(T\) :
-
Temperature (°C)
- \({T}_{hs}\) :
-
Junction temperature of heat sink (°C)
- \({T}_{m}\) :
-
Mean temperature (°C)
- \({T}_{a}\) :
-
Ambient temperature (°C)
- \(\Delta T\) :
-
Temperature difference (°C)
- \(U\) :
-
Voltage (V)
- \(u\) :
-
Velocity (m/s)
- \(W\) :
-
Width of channel (mm)
- \(\mu\) :
-
Viscosity (kg/(m∙s))
- \(\rho\) :
-
Density (kg/m3)
- MEMS:
-
Micro electro mechanical systems
- DC:
-
Direct current
- AC:
-
Alternating current
- ch:
-
Microchannel
- hs:
-
Heat sink
- in/inlet:
-
Inlet
- out/outlet:
-
Outlet
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Acknowledgements
This work is supported by the National Natural Science Foundation of China (Project No.51776195).
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Higlights
• A structure-optimized large microchannel heat sink for extremely high heat flux was designed.
• Rough surface promotes heat transfer through creating flow disturbance at low Re number.
• Actual heat fluxes of 1104.54W/cm2 and 480.60W/cm2 were dissipated over 1cm2 and 5cm2 area.
• Dependence of thermal resistance on pumping power between 0.1W and 6.5W was identified.
• Unprecedented low thermal resistance of 0.065K/W and 0.019K/W were obtained respectively.
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Sun, B., Wang, H., Shi, Z. et al. Pumping power and heating area dependence of thermal resistance for a large-scale microchannel heat sink under extremely high heat flux. Heat Mass Transfer 58, 195–208 (2022). https://doi.org/10.1007/s00231-021-03104-y
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DOI: https://doi.org/10.1007/s00231-021-03104-y