Table 2.
Cooling Method | Advantages | Limitations |
---|---|---|
Conduction |
• Good with low current density systems. • No moving parts required. • Can be coupled with convective cooling methods. |
• There is a limit to how much heat transfer material is to be used. • Not suitable for high current density values. • Significant increase in system weight if more heat conductive material is added. • Eddy currents in case of excess material [42] and from changing fields |
Air cooling |
• Cooling medium is readily available. • Can easily be coupled with conductive cooling and indirect liquid cooling. • Dry method hence no fear of shocks from leakage. |
• Limited to current densities of 2 A/mm2. • Low coefficient of heat transfer (between 2.5–10 (natural convection) 10–500 W/m2K (forced convection) [64]). • Often bulky with high space requirements. |
Liquid cooling |
• Relatively high coefficient of heat transfer (100–15,000 W/m2K [64]) • Compact design is possible hence lower space requirements. • No thermal barriers when direct cooling through hollow conductors is used |
• Possible electric shocks in case of leakages • Corrosion of cooling channels due to high flow rate and pressure requirements • Additional power and operational costs from pumping |