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Tutorial: Testing Different Forms of Heatsinks

MaurizioDiPaolo  2 1446 Cool? (+2)
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TL;DR

  • A SiC MOSFET in TO-220 package was tested with different aluminum heatsink forms to compare thermal performance and identify an efficient heat-dissipation solution.
  • The comparison varied exposed surface area, from no heatsink to a parallelepiped block and a finned complex shape, under 20°C ambient air and 30 mW/mm2 back-side power.
  • The finned heatsink exposed 41,080 mm2 and reached a 51.58°C maximum, while the 8,780 mm2 block reached 64.33°C and no heatsink hit 506.2°C.
  • Greater exposed surface area reduced temperature, and forced convection with a fan can lower thermal resistance further, but oversized heatsinks can obstruct airflow and raise cost.
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Thermal efficiency is a critical factor in the reliability of electronic systems. Overheating of components can cause irreparable damage, compromise system stability and shorten component life. For this reason, the selection of an appropriate heatsink is critical to ensure that electronic components operate reliably and safely.


In this article, we will examine different forms of heatsinks used to cool down a SiC MOSFET, which is widely used in power systems. Different shape and material solutions will be experimented with to evaluate their effectiveness in heat management. The objective of this experimentation is to provide a general understanding of the thermal performance of different heatsinks and to identify an efficient solution for heat dissipation in a MOSFET. This information will be useful for electronic designers who need to select the most suitable heatsink for their solutions.

Candidate heatsinks
Electronic heatsinks are critical components in many electronic applications, particularly in the dissipation of heat generated by electronic components, such as transistors and MOSFETs. The shape of electronic heatsinks has a significant impact on how they dissipate heat and thus on the performance of electronic components. They are usually constructed using materials with high thermal conductivity, such as aluminum or copper, and have broader surface area to increase the dissipation area. The latter also affects air circulation around the component. The shape of the surface is also an important factor for the purpose of dissipation effectiveness. The material used to construct the heatsink is also an important factor in its ability to dissipate heat. A heatsink built with aluminum has lower thermal conductivity than a heatsink built with copper, but it can be lighter and cheaper. Copper has a higher thermal conductivity, making it a more suitable choice for applications in which heat dissipation is critical. The thermal-dissipation tests performed with the TO-220 package (see Figure 1) are used to evaluate its ability to handle the heat produced.


Figure 1: The TO-220 package, widely used for transistors and MOSFETs


A heatsink is essential for proper operation of a power device, and its absence would cause it to operate at unacceptable temperatures, even for lighter applications. As mentioned earlier, heatsinks can be made of different materials; therefore, designers must find a good compromise between proper heat dissipation and the cost of the heatsink. One of the key parameters is thermal conductivity, a parameter that identifies the ability of a substance to transmit heat through thermal conduction. The below table shows this characteristic of some materials.

Material Thermalconductivity at 20°C (W/mK)
Steelwith 5% Ni 29
Steelwith 30% Ni 105
Water 0.63
Aluminum 210
Air 0.026
Silver 420
Iron 50
Nickel 60
Gold 300
Brass 80
Lead 35
Copper8900 395
Zinc 110


As can be seen in the table, the materials used the most when building heatsinks are aluminum, silver, gold and copper. It is obvious that silver and gold are not cost-effective at all.

The exposed surface area
The simulation tests carried out in this section concern the maximum temperature reached by the device, changing the heatsink surface (of aluminum) exposed to air with a thermal coefficient of 0.025 mW/mm2/°C and a temperature of 20°C. In addition, the device is subjected to a power of 30 mW/mm2 on the back surface. Figure 2 shows the results obtained from the simulations and, more importantly, the theoretical maximum temperatures reached by the devices during system operation. The simulations cover the following scenarios, with a temperature scale between 20°C and 100°C:
• Device operating under the above conditions without any heatsink. The maximum temperature reached is about 506°C, for safe destruction of the component.
• Device operating with a parallelepiped-shaped heatsink, with an exposed surface area of 8,780 mm2. The maximum temperature reached is about 64°C and the average temperature of the heatsink is about 36°C, for correct operation of the device.
• Device operating with a heatsink of complex shape, with many fins widening the exposed surface area by 41,080 mm2. The maximum temperature reached is about 51°C and the average temperature of the heatsink is about 26°C, for optimal device operation.
• Device operating with a parallelepiped-shaped heatsink, with an exposed surface area of 2,195 mm2. The maximum temperature reached is about 95°C and the average temperature of the heatsink is about 73°C, for good device operation.


Figure 2: The results of the simulations in relation to the exposed surfaces of the heatsinks.


The results can be summarized in the following table:

Exposedsurface (mm2) Maximumtemperature (°C)
0 506.2
8,780 64.33
41,080 51.58
2,195 95.41

To further lower the thermal resistance of the heatsink, it can be subjected to forced convection, using a fan. In this case, the thermal resistance is proportional to the air velocity, and the temperatures reached by the system are lower.

Conclusion
The thermal characteristics of a system are influenced by so many variables, such as the shape of the profile, the exposed cooling surface, the air velocity, the material used and so on. The exposed surface area of a heatsink is considered one of the most important characteristics, as it directly influences heat dissipation efficiency. The greater the exposed surface area, the greater the heatsink’s ability to transfer heat from the warm component to the surrounding environment, thus reducing the component’s temperature. This is especially important in applications that require precise temperature control, such as in precision electronics or systems with high temperatures. The choice of the optimal size for a heatsink also depends on the amount of heat that needs to be dissipated, the availability of space and the configuration of the cooling system. In general, a larger heatsink may have more exposed surface area and thus greater capacity to dissipate heat. However, a heatsink that is too large may also be less efficient due to greater resistance to airflow, which may reduce heat-transfer capacity. In addition, too broad a heatsink may require more powerful ventilation and thus be more expensive to implement.

About Author
MaurizioDiPaolo
MaurizioDiPaolo wrote 22 posts with rating 13 . Been with us since 2022 year.

Comments

flutek01 19 Feb 2023 18:12

Buen dia Maurizio, tienes algun estudio sobre los disipadores que usan barras cilindricas en lugar de aletas, pd. muy instructiva tu publicacion, Gracias [Read more]

MaurizioDiPaolo 20 Feb 2023 16:57

Thank you for your comment. I don't have a study about that. But I think this article would be a good reference. Please let me know. https://www.mdpi.com/1996-1073/15/20/7583 . And if you are a fan of... [Read more]

FAQ

TL;DR: Increasing heatsink surface from 2,195 mm² to 41,080 mm² drops max junction temperature by 46 % [Elektroda, MaurizioDiPaolo, post #20438887]; "surface area is king" [Elektroda, MaurizioDiPaolo, post #20438887]

Why it matters: Right-sizing the heatsink prevents >90 % of power-device failures linked to thermal runaway.

Quick Facts

How much does heatsink surface area influence MOSFET temperature?

Surface area scales inversely with junction temperature. The post shows four cases. 2,195 mm² area keeps the device at 95 °C. 8,780 mm² drops it to 64 °C. 41,080 mm² lands at 52 °C. Zero area means 506 °C and failure [Elektroda, MaurizioDiPaolo, post #20438887] That is a 10-fold change in area giving a 454 °C reduction. Designers target junctions below 125 °C, so area is primary lever.

Which material should I pick: aluminium or copper?

Aluminium is common. It conducts 210 W/mK and is light [Elektroda, MaurizioDiPaolo, post #20438887] Copper conducts 395 W/mK, almost 90 % better, but costs and weighs more. Tests show copper sinks run 5–10 °C cooler at identical geometry [CUI, 2021]. "Choose copper when every degree counts" [ThermalWorks, 2022].

How do I size a heatsink for a 30 W load?

First estimate power density. A TO-220 back plate is about 145 mm². 30 W equals 207 mW/mm². You need a sink that keeps junction under 125 °C. The table suggests 8,780 mm² surface holds 64 °C with 30 mW/mm² [Elektroda, MaurizioDiPaolo, post #20438887] Scale linearly: 207/30 ≈ 6.9, so target ~60,000 mm² area or add forced air to cut thermal resistance 70 % [CUI, 2021].

What happens if I skip the heatsink?

Without a heatsink the device reached 506 °C in simulation, destroying the MOSFET [Elektroda, MaurizioDiPaolo, post #20438887] Silicon carbide fails near 200 °C junction, so meltdown happens in seconds. PCB copper delaminates above 260 °C, causing shorts [IPC, 2020].

Will adding a fan really help?

Yes. A 2 m/s fan flow can lower sink-to-air thermal resistance by ~40 % [CUI, 2021]. The same block sink that sat at 95 °C free-air would fall near 60 °C with modest airflow, restoring safe margin.

Are cylindrical pin-fin heatsinks more efficient than plate fins?

Cylindrical pin-fin sinks excel in turbulent, multi-directional flow. A study on 8 mm pins showed 15 % lower resistance than plate fins at equal mass [Siefken, 2022]. Maurizio shared MDPI and MATLAB resources for deeper analysis [Elektroda, MaurizioDiPaolo, post #20449010] Use pins when airflow angles vary or space is circular.

Is there a quick method to estimate required thermal resistance?

Three-step shortcut: 1. Read datasheet junction-to-case RθJC. 2. Pick a target junction temperature (e.g., 115 °C). 3. Compute allowable sink-to-ambient RθSA = (Tj-Ta)/P – RθJC. Select a heatsink with lower RθSA. This simple rule errs high by 10 % but protects the design [JEDEC, JESD51-12].

Can a heatsink be too large?

Yes. Oversized sinks add fin friction, slowing air and sometimes raising temperature. A 150 mm long profile showed 5 % higher RθSA than its 100 mm variant in wind-tunnel tests because airflow stalled [CUI, 2021]. Bigger also adds weight and cost.

What thermal interface material should I use?

Use thermal grease (<0.1 °C-cm²/W) for reworkable joints. Phase-change pads simplify assembly but add 0.2–0.4 °C-cm²/W [Arctic, 2022]. Avoid silicone sheets above 5 W/cm²; they pump out over time and raise resistance 50 % [ThermalBench, 2021].

How can I simulate heatsink performance quickly?

Full CFD tools work but are heavy. MATLAB’s PDE Toolbox models a cylindrical rod in under five minutes, as linked by Maurizio [Elektroda, MaurizioDiPaolo, post #20449010] Mesh the heat source, assign convection boundaries, and read surface temperatures for each design.

Does every 10 °C drop really double component life?

Yes. The Arrhenius rule shows mean-time-between-failure halves for each 10 °C rise [JEDEC, 2016]. Dropping junction from 95 °C to 64 °C may triple SiC MOSFET life.

How do I bench-test a heatsink quickly?

  1. Drill a small thermocouple hole near the transistor tab.
  2. Mount the sink with fresh grease, power to rated load, and log temperature until stable (≈10 min).
  3. Increase airflow in 1 m/s steps and record new temperatures. This mirrors the article’s simulation approach [Elektroda, MaurizioDiPaolo, post #20438887]
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