Published on: Mar 2, 2015. Updated on: Jan 15, 2018.

This is chapter 6 of the DRSSTC design guide: Snubber capacitor

When we switch on and off very large peak currents in a DRSSTC, residual energy will be trapped in the circuit stray inductance of the switching devices and busbar, that causes a voltage transient that can be many times higher than the IGBT ratings.

Snubber capacitors should never be used to make up for a bad circuit layout. It is will very important to design a circuit with low inductance as discussed in chapter 2 on Busbar and primary circuit design.

The following oscilloscope shots show a IGBT switching on and the resulting voltage overshoot from the stray inductance. The black curve show the switching waveform without any kind of suppression and the brown curve show a switching transient that is suppressed by a capacitor.

**Snubber capacitor selection
**

Snubber capacitors are subjected to high peak and rms currents and high dV/dt. All types of high frequency polypropylene film capacitors are suitable to be used as a snubber capacitor, there is however a magnitude of difference in internal inductance from normal capacitors with through hole leads and those made for direct mounting on IGBT terminals. [1]

Aim to use polypropylene capacitors with a voltage rating that at least matches the IGBT and have a dV/dt rating at at least 500-5000 V/μs and above.

Snubber capacitors can come in many different packages and sizes.

**Calculation of snubber capacitance**

A approximation of the needed snubber capacitance can be found using stray inductance L_{S} in H, peak current I_{peak} in A, allowed transient voltage peak V_{transient} in V and DC bus voltage V_{bus} in V. [2]

Let us of look at the same example, as used earlier, where we have some numbers from my large DRSSTC. With 564 V on the DC bus, 2000 A primary peak current, maximum allowed transient voltage of 1000 V on a 1200 V IGBT and assuming 200 nH stray inductance.

There is also another estimation method that uses a rule of thumb with two assumed scenarios. Where a snubber capacitor is used alone in a circuit where a low or high inductance is expected, the following quick rules can used. [3]

A design where you expect a low inductance you can use 0.5 μF for each 100 A the IGBT is switching. That would result in 10 μF needed snubber capacitance for the above calculation.

A design where you expect a high inductance you can use 1 μF for each 100 A the IGBT is switching. That would result in 20 μF needed snubber capacitance for the above calculation.

The estimations will naturally give a higher value needed than the calculations as the estimation will have to make up for the lack of knowledge about the exact stray inductance that the snubber capacitance will have to act against.

**Snubber capacitor power dissipation**

The transient voltage caused by the IGBT switching a current would normally oscillate until the energy was dissipated in the resistive part of the busbar and components circuit. The snubber capacitors forms a shorter DC loop where the oscillation dies out faster due to its low ESR. The ESR of the snubber capacitor is also the dominant resistive part in this new loop and it will be here the energy from the oscillations is dissipated.

The overall power dissipation is however very low due to the very low duty cycles used in a DRSSTC and it is not necessary to take extra precautions in regard to RMS current if IGBT snubber capacitors mounted directly on the terminals are used.

**A word on physical dimensions of capacitors for either DC link or MMC**

As demonstrated by El-Husseini, Venet, Rojat and Joubert in their article “Thermal Simulation for Geometric Optimization of Metallized Polypropylene Film Capacitors”, the physical geometry of a capacitor can have an impact on capacitor temperature, power loss and life. They demonstrated that for the same electrical stress, taller capacitors experienced higher temperature and losses than shorter capacitors.

As stated in their article, in taller capacitors, the current must travel a longer distance through the very thin metal films, thus the total I²R losses are higher compared to a short capacitor. The authors demonstrated that the total power loss in the capacitor is proportional to Equivalent Series Resistance (ESR) and to the square of the true rms current.

ESR represents the eddy current and dielectric losses, which are affected by both frequency and current. If capacitor current is elevated, power loss increases. Likewise, power loss in a metallized film capacitor increases if the frequency of the current increases. Thus, harmonic current flowing in a metallized film capacitor, the power loss will be higher than if pure sinusoidal current were to flow. [4]

As the following equation shows, it is the RMS current flowing through a capacitor that is the most vital parameter in temperature rise and too high temperatures lowers life time dramatically.

Cooling of capacitors by forced air can be a solution to get a longer life time. Approximately 2/3 generated heat rise moves out axial and 1/3 radial. So it is most important to cool a capacitor at its terminals as it does not radiate the heat evenly from all over its surface.

Some capacitors have a metal mounting stud in the opposite end of the terminals, these are meant for installation in heat sinks or other material that can lead the heat away. Be aware that the metal can and stud might not be isolated from the negative terminal, depends on manufacturer and capacitor type.

The thermal resistance (Rth) from case to ambient is given for still air in most datasheets, so if forced air cooling is used the thermal resistance can be de-rated. Some manufacturers supply equations to calculate a exact thermal resistance in regard to capacitor surface and forced air speed velocity.

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### References

[1] Rudy Severns. “Design of snubbers for power circuits”, cde.com

[2] Yi Zhang, Saed Sobhani, Rahul Chokhawala. “Snubber Considerations for IGBT Applications”, International Rectifier Applications Engineering 233 Kansas St., El Segundo, CA, 90245 USA.

[3] Kemet. “Film Snubber Capacitors for IGBT Modules”, SA1211. Kemet 2011.

[4] M.H. El-Husseini, Pacal Venet, Gerard Rojat and Charles Joubert, “Thermal Simulation for Geometric Optimization of Metallized Polypropylene Film Capacitors”, IEEE Trans. Industry Appl, vol. 38, pp713-718, May/June 2002.

Is the recommended rating really 500-5000 dV/dt? I know that these capacitors need an insanely high peak current to suppress the voltage transients, but for an average snubber capacitance of 5uF, 500-5000 dV/dt means 2.5-25kA peak current capability, while it gets relatively difficult to find snubbers with over 2kA. I’ve also seen quite a few inverter desings on the web with snubbers of 50-500 dV/dt rating.

I’m just wondering if perhaps there is something I’m not getting, or some sort of typo? Or does the rating really need to be this high?

Hi Jeremi

A non-decoupled bridge will often have transients in the range of several thousands. It is a frequency dependant calculation and historically looking back at older inverters, these hard switching drives usually run at much lower frequencies than we see today.

So 5 uF might be too big and it is really your bus layout that should be optimized for lower stray inductance than trying to fix it with decoupling/snubbering.

Take a look at page 2 and 3 here for some additional calculations to estimate a pure decoupling capacitor: https://www.infineon.com/dgdl/Infineon-Snubber_Considerations_for_IGBT_Applications-Article-v01_00-EN.pdf?fileId=5546d462533600a401535748b5103fe8

Kind regards

Mads

Hi, thanks for the quick response!

I have one more question regarding caps:

I’m planning to upgrade my FGY75N60SMD full-bridge, to a SKM195GB066D brick half-bridge, but would like to keep my single DC bus cap. Since this means no center tap between two series bus caps (as is often done in half-bridge designs), two extra series caps across the bus will be needed to create the tap for the other end of the primary circut.

Are there any recommended specs/desing rules I should follow with them, besides being polypropylene pulse capaictors? I’ve seen people using ~2uF caps for this purpose, but that might not have been the correct choice.

Regards

Jeremi

Hi Jeremi

I covered that part slightly on the topic of DC bus capacitors, scroll down to halfbridge header: http://kaizerpowerelectronics.dk/tesla-coils/drsstc-design-guide/dc-bus-capacitor/

You also omit the center point and run the other end of the primary coil directly to the negative rail. If you look at this schematic and -400 is ground potential instead.

Kind regards

Mads

Hello Mads, When you say “stray inductance” Does this only mean the inverter part of the DRSSTC? Which does not include the inductance of the primary coil correct?

Hi Chris

The stray inductance is only the busbar inductance between the bulk DC bus capacitance and your switches. The resonant LC circuit is not a part of stray inductance as it is a designed specific inductance for resonance, this is designed to have oscillations.

Kind regards

Mads

Right! Thanks Mads!

Hi, great tutorials throughout.

I am trying to estimate snubber capacitance using your calculator. Would it be possible to measure the stray inductance with an LCR meter? I have one but I am not sure between which points I should measure; I suspect I should measure while setting the LCR meter frequency close to what the system resonance frequency would be?

I could also just estimate it off high/low but since I have a tool, I’d rather do that (if it makes sense).

Cheers

Hi Steve

You are right about using a LCR meter would have to be near your resonant frequency, usually they can only do 1/10/100 kHz, so 100 kHz will properly cover most coils and noone gets near 10 kHz 🙂

Measure all conducting parts of the bridge, without components mounted, from the point of view from the DC bus capacitors and make a short circuit at the load. This should give you the best simulation of supply and return paths cancelling each-other out.

Kind regards

Mads