DRSSTC design guide updated with MMC design guide
It only took me a mere 4 years from I first started this article about the MMC until it is now done for public released 🙂 …
High voltage enthusiasm
It only took me a mere 4 years from I first started this article about the MMC until it is now done for public released 🙂 …
Published on: 07. February 2019
This is chapter 7 of the DRSSTC design guide: MMC / resonant tank capacitor design for Tesla coils and inverters.
MMC is short for multi mini capacitor and is used to describe a resonant tank capacitor made from many smaller capacitors to achieve the needed ratings.
As with all the other aspects of designing a Tesla coil, many of the choices on component and design selection are interrelated in a nonlogical way and it often makes it difficult to split up the design as I try to in this guide. That means some data and input used in selecting a MMC is based on prior choices regarding IGBT, topology or secondary circuit. For most people a MMC will first and foremost be designed from a money perspective, high power pulse rated capacitors are not cheap.
I will discuss the following three roads to take in the design of a MMC:
1. Designing by DC voltage rating and peak current rating is a quick, dirty and easy method. The result is a working and cheap MMC, but failure at long runtimes and shortened life time should be expected.
2. Designing by peak / RMS current rating and temperature rise results in a set of data where it has to be chosen what is acceptable, DC voltage rating is also a part of it and it is necessary to always adjust the design to have around 1020 % voltage rating overhead by this method. Results in a robust and medium cost MMC.
3. Designing by peak voltage rating and maximum ontime for the current to flow in the LC circuit before the voltage rating of the MMC is hit. A conservative approach, especially if the AC voltage rating is used. Results in a indestructible but also very expensive MMC.
I use and recommend the peak current, RMS current and temperature rise method, which is also the method used in my MMC calculator. It is a more thorough result set, but I will demonstrate all three methods here.
If you are looking for a list of good MMC capacitors or the MMC calculator, follow these links. Examples and explanations from the list and the calculator will be used throughout this guide.
The first important decision to make is what the expected life time of the Tesla coil is.
The further down you get on this list, the more important it is that the Tesla coil is reliable and here the MMC is often a part that fails due to inadequate design and abuse of a underrated part that is working under great stress.
For 1 and 2 it will be okay to design simple and cheap as it will be shown in the budget example, for 3 and 4 it is highly recommended that you use the advanced and more expensive design criteria that will be shown in advanced examples.
This choice is also revolving around the money issue, high impedance primary circuits have lower capacitance, operate at longer ontimes, lower peak currents and is generally cheaper to build. Low impedance primary circuits have higher capacitance, operate at short ontimes, have very high peak currents and is generally more expensive to build due to more capacitors needed to get the capacitance and appropriate voltage rating for the higher peak currents. More details on low and high impedance is also covered in Secondary coil part of this guide.
The larger a system is, the larger should the MMC also be, in order to match the energy needed to push out longer and longer sparks, more pulse energy storage is also needed.
A general guide, using the same Tesla coil sizes as in the secondary coil design part, can be seen in Table 1. I will look at five different sizes of coil systems with a rough power input estimate:
Coil diameter  Coil length  Capacitance range  
Micro  40 mm 50 mm 
160200 mm 200250 mm 
0.1 – 0.2 uF 
Mini  75 mm  300375 mm  0.15 – 0.45 uF 
Medium  110 mm 160 mm 
440550 mm 640800 mm 
0.3 – 0.6 uF 
Large  200 mm 250 mm 
8001000 mm 10001250 mm 
0.45 – 1 uF 
Very large  315 mm 400 mm 
12501575 mm 16002000 mm 
0.6 – 2 uF 
I find that the easiest way to design a DRSSTC primary circuit is so choose a maximum primary peak current that the IGBTs can handle and then design the MMC from this. So with a known value in the following example, I will demonstrate how to design a 0.45 uF MMC for use in a 70 kHz coil with 800 Ampere peak primary current, a medium size system that can produce somewhere around 1.5 to 2 meter sparks.
First we need to calculate the reactance of the MMC, F is frequency in Hertz and C is capacitance in Farad.
Now we can calculate the impedance of the MMC, ESR is the combined ESR of the series and parallel connected capacitors in the MMC. For the 0.45 uF MMC I chose to use 6 parallel strings of 2 CDE 942C20P15KF capacitors in series. Each capacitor has a DC voltage rating of 2000 V and a ESR rating of 5 mΩ, which results in 4000 V series rating and a 1.66 mΩ rating for the chosen MMC.
As it can be seen, with low ESR polypropylene pulse capacitors, the ESR is almost negligible when calculating the impedance.
Last we can calculate the peak voltage across the MMC and see if it is higher or lower than the combined series VDC rating of the capacitors. Zc is the MMC impedance from above and primary peak current in Ampere.
The multiplied DC rating of the capacitors in series is just on spot of what is needed to run the system at 800 Ampere peak. You can now just adjust the primary peak current in this last formula to find out when you will be below or above the voltage rating of your MMC.
This will be a fairly long part, as the calculations and explanations will go hand in hand with my MMC calculator, as that is the tool I made after this design method but also to give a more indepth introduction to those that use the MMC calculator.
This method is based on designing a MMC from a certain maximum peak current, as the IGBTs often is a setinstone parameter and they are the limiting factor in the design.
Then there is seven important capacitor specifications in order to get the most precise results. It is Capacitance, Voltage rating, Peak current rating, RMS current rating, dV/dt rating, ESR rating and specific dissipation factor. These values also have to be calculated / extrapolated for the chosen resonant frequency. Help on getting these values can found bottom of the good MMC capacitors list.
Input parameters for the Tesla coils primary circuit is also important to be able to calculate the ratings of the MMC. When all these numbers have been plotted in, it is just as simple as using the +/ buttons to adjust number of capacitors, ontime, BPS or primary peak current to see that the results are equal to or better than the requirements.
To use the same example I will once again use the 0.45 uF MMC where I choose to use six parallel strings of two CDE 942C20P15KF capacitors in series. Each capacitor has a DC voltage rating of 2000 V in a 4000 V series rating. A MMC to be used in a 70 kHz coil with 800 Ampere peak primary current.
We can reuse the calculations and results from the example above, so we can continue from where the calculated MMC impedance is 5.05 Ω and peak voltage across the MMC is 4040 V.
Steve McConner proposed the following equation to calculate the RMS current across the MMC based on a square waveform, BPS and ontime
The 6 parallel strings of CDE 942C20P15KF capacitors, which has a 13.5 A RMS current rating each, gives us a 81 A rating, so the actual load is just shy of hitting the rating, so we should think seriously about limiting ontime, BPS, peak current or overall run times lengths. The peak current rating of these capacitors are 432 A each, so multiplied by 6 strings in parallel that gives us a total peak current rating of 2592 A which is with plenty of headroom in respect to the 800 A peak current we planned to run this coil at.
We also need to check that the rate of voltage change across the MMC does not exceed that rating of the MMC. First we calculate the actual dV/dt imposed on the MMC. V is peak DC voltage over MMC and F is frequency in Hertz. This will give a result in V/uS.
The actual dV/dt rating of the MMC is a simple equation and this number have to be higher than the above calculated imposed dV/dt. Primary peak current in A and MMC capacitance in F.
In this case there is plenty of headroom for the dV/dt.
The last step to ensure that we have a sturdy MMC that can be operated for extended periods of time is to calculate the temperature rise of the single capacitor according to its dissipated power.
First we need to calculate the dissipated energy in a single capacitor for a 1 second time period. So this means we divide the combined Irms result of 80A from earlier with the six strings in parallel and that gives us 13.33A.
Temperature rise for a single capacitor can now be calculated, this now the last simple task of multiplying the dissipation with the dissipation factor. For this example I have it given in the datasheet as 11ºC/W, which means that this capacitor will rise 11ºC for each 1 Watt of power dissipation. If you can only find a rating given in W/K, look at the bottom of this page on how to convert that value.
While almost 10ºC does not sound like much, we have to remember that this is for a single second of operation. It is important that we let the capacitor be able to cool down enough between pulses that the temperature does not just keep adding up until disaster happens.
To give a better idea of how much is tolerable, here is a rule of thumb list for temperature rise per second.
This path of design is from Matt “Sigurthr” Giordano and he starts his design by asking two questions, “how long a burst length can I use?” and “which voltage rating do I need on the tank capacitor?”.
This is not so much designing a MMC, but more a method to check how hard you can drive a existing MMC without damaging the capacitors.
Maximum ontime in uS and the voltage rating needed for the MMC are interrelated, but the link is not straight forward as it has to do with some inductive load inverter theory.
Each half cycle the inverter switches polarity it adds more voltage, and thus more current is flowing into the tank circuit. The longer your burst length, the more the voltage and current can ring up. So, how do we know when voltage or current is too high?
We would like to know the maximum primary peak current that we can adjust our OCD circuit to. This is dependent on the voltage we will allow according to the voltage derating that we choose for the MMC capacitors. Here we can either use the AC voltage rating or use the DC voltage rating with a head room between 20 to 50%.
So to avoid damage to the MMC, we can limit the voltage across it by calculating a OCD maximum peak current value and determine what the maximum ontime is before the voltage is so high that the interrelated current is too high aswell.
These calculations disregard the fact that primary current is, in normal operation, limited by the secondary arc load. A well tuned and built coil should never have its OCD trip as all the energy should be transferred into making sparks.
To use the same example I will once again use the 0.45 uF MMC where I choose to use six parallel strings of two CDE 942C20P15KF capacitors in series. Each capacitor has a DC voltage rating of 2000 V in a 4000 V series rating, but for protection I will derate that 20% so the calculations are done with a maximum allowed 3200 V across the MMC.
Peak voltage V_peak is given in Volt, Primary inductance L_primary is given in Henry and frequency F_resonant is given in Hertz.
The result shows with good precision why I ran my DRSSTC1 at 500 Ampere OCD settings, as this corresponds to the low voltage rating of the MMC, but not lower than it was a good match with the IGBTs used.
The maximum ontime to stay below 3200 V across the MMC, and thus also stay below 472 A peak primary current can be calculated, but it is dependent of the inverter type.
The maximum ontime for a halfbridge
10 halfcycles at 70 kHz on a halfbridge, according to table 2 is around 72 uS before we have either 3200 V across the MMC or 472 A flowing in the primary circuit.
The maximum ontime for a fullbridge
5 halfcycles at 70 kHz on a fullbridge, according to table 2 is around 35 uS before we have either 3200 V across the MMC or 472 A flowing in the primary circuit.
The table below can be used as reference for these calculations, as a general lookup table instead of calculating the time half a period lasts at a given frequency or just for sanity check of your own calculations.
Halfcycles:  1  2  3  4  5  6  7 
40 kHz  12  25  37  50  62  75  87 
60 kHz  8  17  25  33  41  50  58 
80 kHz  6  12  18  25  31  37  43 
100 kHz  5  10  15  20  25  30  35 
150 kHz  3  7  10  13  17  20  23 
200 kHz  2  5  7  10  12  15  17 
250 kHz  2  4  6  8  10  12  14 
300 kHz  2  3  5  7  9  10  12 
350 kHz  1  3  4  6  7  8  10 
Halfcycles:  8  9  10  11  12  13  14 
40 kHz  100  112  125  137  150  162  175 
60 kHz  66  75  83  91  100  108  116 
80 kHz  50  56  62  69  75  81  88 
100 kHz  40  45  50  55  60  65  70 
150 kHz  27  30  33  37  40  43  47 
200 kHz  20  22  25  27  30  32  35 
250 kHz  16  18  20  22  24  26  30 
300 kHz  14  15  16  18  20  21  23 
350 kHz  11  13  14  15  17  18  20 
Halfcycles:  15  16  17  18  19  20  21 
40 kHz  187  200  212  225  237  250  262 
60 kHz  124  132  141  149  158  166  175 
80 kHz  94  100  107  113  119  125  131 
100 kHz  75  80  85  90  95  100  105 
150 kHz  50  53  57  60  63  67  70 
200 kHz  37  40  42  45  47  50  52 
250 kHz  32  34  36  38  40  42  44 
300 kHz  25  26  28  30  31  33  35 
350 kHz  21  22  24  25  27  28  29 
RMS current rating is often overlooked as people focus on the voltage and peak current rating. Too high RMS current will slowly heat up the capacitors to a point where failure is imminent. Pay close attention to the achieved RMS current rating and be sure to honor this as well.
Capacitors with a larger physical size will often have a advantage over many smaller capacitors due to their large thermal mass, but they are also slower to cool down again.
Path resistance to each capacitor should be equal to assure equal current sharing, as it was described in Chapter 1: Rectifiers. The rectifier closest to the supply would conduct the most current, it is the capacitor closest to the load that will conduct the most current. The 40% current derating rule can also be used for capacitors in parallel to correct for uneven current sharing.
While ripple current divides among the capacitors in proportion to capacitance values for lowfrequency ripple, high frequency ripple current divides in inverse proportion to ESR values and path resistance. [3]
This means that parallel capacitors in applications with low frequency load will share the current according to the capacitance of each capacitor in parallel. Whereas a load operating at a high frequency, like a DRSSTC does, the current sharing is up to ESR values and resistance of the busbar and wires in the circuit.
Here is a example from Amaury Poulain where the MMC failed from asymmetrical current sharing and the result is heating damage of the strings that carry the most current, those with the shortest current path between MMC conection terminals.
Another example of a unblanced MMC that failed due to uneven current sharing. A capacitor was melted completely apart from excessive heat dissipation.
Even current sharing can easily be obtained from ensuring even length current paths between the strings in regard to the MMC connection terminals.
Amaury Poulain’s failed MMC from above was remade with better cooling and even current paths in mind.
Here is a another example of a PCB designed by Franzoli Electronics after the same principles.
Here Jeroen Van Dijk made a very compact MMC, could have better air cooling distance between the capacitors, but the even current sharing is ensured.
Here are some of my own MMC constructions and it is always important that terminals are connected in a way so that current paths are an even length.
Film and Mica capacitors are generally the best for Tesla coil tank circuit use, Mica capacitors can however be hard or expensive to find at the capacitance needed for a DRSSTC.
Lets first have a look at a comparison between some film capacitors that have ratings in the range of what we could use for a MMC.
Film characteristics  Polyester PET MKT 
Polyethylene PEN 
Polyphenylene PPS MKI 
Polypropylene PP FKP/MKP 


Dielectric str. (V/µm)  580  500  470  650  
Max (V/µm)  280  300  220  400  
Max DC (V)  1000  250  100  2000  
Capacitance  100pF+  100pF+  100pF+  100pF+  
Max temp. °C  +125  +150  +150  +105  
Dissipation factor (•10^{−4})  
10 kHz  110150  54150  2.525  28  
100 kHz  170300  120300  1260  225  
1 MHz  200350  –  1870  440 
If we solely look at the voltage rating and capacitance of a film capacitor when building a MMC, there could be problems with heat dissipation at DRSSTC frequencies. As it can be seen, polypropylene capacitors have a very low dissipation factor even at high frequencies, which makes them our preferred choice.
The FKP type of polypropylene capacitors are made from layers of film and foil, the FKP type does not have selfhealing capabilities and will fail short circuit. The MKP type is made from metallized film that is self healing, if a local punch through of the film happens, the small internal explosion will burn away the metallized layer around the punch through hole and thus isolates it from the rest of the layer. This way a punch through in a MKP type will fail open circuit, which makes them our preferred choice.
The temperature and frequency dependencies of electrical parameters for polypropylene film capacitors are very low. Polypropylene film capacitors have a linear, negative temperature coefficient of capacitance of ±2,5 % within their temperature range.
The dissipation factor of polypropylene film capacitors is smaller than that of other film capacitors. Due to the low and very stable dissipation factor over a wide temperature and frequency range, even at very high frequencies, and their high dielectric strength of 650 V/µm, polypropylene film capacitors can be used in metallized and in film/foil versions as capacitors for pulse applications, such as CRTscan deflection circuits, or as socalled “snubber” capacitors, or in IGBT applications. In addition, polypropylene film capacitors are used in AC power applications, such as motor run capacitors or PFC capacitors.
Most power capacitors, the largest capacitors made, generally use polypropylene film as the dielectric. Polypropylene film capacitors are used for highfrequency highpower applications such as induction heating, for pulsed power energy discharge applications, and as AC capacitors for electrical distribution. [1]
As demonstrated by ElHusseini, 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 is 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. [2]
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.
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 derated. Some manufacturers supply equations to calculate a exact thermal resistance in regard to capacitor surface and forced air speed velocity.
Capacitive reactance Xc, where f is frequency given in Hertz and C is capacitance given in Farad
ESR can be calculated from the tangent of loss angle given as TANδ in the data sheets. ESR is frequency dependent. C is capacitance given in Farad, f is frequency given in Hertz.
Thermal resistance (Rth) when given in data sheets are either Watt needed to raise the temperature by one Kelvin or degree Celsius the temperature raises by one Watt dissipation. Conversion from W/K to °C/W is to divide one by W/K dissipation factor.
Ipeak or Ipulse is calculated from the dV/dt rating times the capacitance of the capacitor. Capacitance given in micro Farad times pulse rise time given in micro seconds will give a result in Ampere.
As a rule of thumb ESL is about 1.6 nH per millimeter of lead distance between the capacitor itself and the rest of the circuit. This also includes the leads of the capacitor itself. This only applies to well designed capacitors.
[1] http://en.wikipedia.org/wiki/Film_capacitor
[2] M.H. ElHusseini, Pacal Venet, Gerard Rojat and Charles Joubert, “Thermal Simulation for Geometric Optimization of Metallized Polypropylene Film Capacitors”, IEEE Trans. Industry Appl, vol. 38, pp713718, May/June 2002.
[3] CDM Cornell Dubilier, “Aluminum Electrolytic Capacitor Application Guide”, http://www.cde.com/resources/catalogs/AEappGUIDE.pdf
A live broadcast that I did on Sunday, February 4, 2018 with focus on designing Tesla coils with special focus on the DRSSTC topology. Questions …
Here is the recording of the live stream I did on 2018 January 31, Wednesday at 2000 CET, I performed a live stream on youtube …
This is a guide that aims to explain a few in depth details and best practices that one should have in mind when designing and building a Dual Resonant Solid State Tesla Coil (DRSSTC).
It is not a complete instruction in how to make a entire DRSSTC system work, but food for thought and explanations on why some parts are chosen over others. The lessons learned over the years by other people who built Tesla coils have resulted in some parts being the only one used, just due to the fact that they were used by the original designer and proven to work good.
This guide should hopefully give you an insight to chose among a wider selection of parts for your DRSSTC and that could help on lowering the construction price and time spent looking for parts. The math and calculations used are simplified for practical use.
Remember that reading is only a fraction of the learning process. Design, build, blow it up, redesign, rebuild, blow it up again, redesign, rebuild and you are on your way to become a master of lightning 🙂
It is not as simple as pushing a button and receiving lightning, prepare to make an effort yourself.
Thanks to the fellow experimenters that helped me proof read, check data and many of them for providing much of the information and experiences collected in this guide.
Here is a list of capacitors tested by the high voltage community to be known to withhold the use as primary capacitor in Tesla coils.
Capacitor specifications are taken from data sheets at 100kHz and some values for peak current, rms current, ESR and dv/dt are estimates(* marked) from similar capacitors and graph read outs.
Product  Ipeak  Irms  ESR  dV/dT  Rth  
data sheet  V  μF  A  A  mΩ  V/μS  °C/W 
Aerovox RBPS20591KR6G  1000  2  854  22  7  427  15* 
CDE 942C20P15KF 
2000  0.15  432  13.5  5  2879  11 
CDE 940C20P1KF 
2000  0.1  171  8.3  7  1712  11 
EFD SP 25502 
1000  3.75  2500*  152  1  810*  10* 
Kemet R474N247000A1K 
900  0.047  28  4*  135  600  51 
Kemet R76UR3150SE30K 
2000  0.15  345  10  26  2300  23 
Panasonic ECWH16333 
1600  0.033  198  3.5  350*  6000  40 
Panasonic ECWH16473 
1600  0.047  282  4.3  250*  6000  40 
Panasonic ECWH16563 
1600  0.056  333  5  150*  6000  40 
TPC CMPPX4K0K0405 
3000  4  5000  80*  0.75  1250  6.9 
WIMA FKP1O131007C00 
1000  0.1  1100  6  10  11000  33 
WIMA FKP1T031007E00 
1600  0.1  1100  6  10  11000  33 
WIMA FKP1R032207F00 
1250  0.22  2420  6  9  11000  33 
Capacitive reactance Xc = 1 / ( 2 * π * f * C)
ESR can be calculated from the tangent of loss angle given as TANδ in the data sheets. ESR is frequency dependant. Capacitance is given in Farad, frequency in Hertz. ESR = (1 / (2 * π * f * C)) * TANδ = TANδ * Xc.
Thermal resistance (Rth) when given in data sheets are either Watt needed to raise the temperature by one Kelvin or degree Celsius the temperature raises by one Watt dissipation. Conversion from W/K to °C/W is to divide one by W/K dissipation factor. °C/W = 1 / (W/K).
Ipeak is calculated from the dV/dT rating times the capacitance of the capacitor. Capacitance given in micro Farad times pulse rise time given in micro seconds will give a result in Ampere. Ipeak or Ipulse = C * dV/dT.
As a rule of thumb ESL is about 1.6 nH per millimetre of lead distance between the capacitor itself and the rest of the circuit. This also includes the leads of the capacitor itself. This only applies to well designed capacitors.
MMC tank design calculator for SGTC, VTTC, DRSSTC and QCWDRSSTC Tesla coils. Results are guidelines to designing a MMC and should always be double checked in your final design! Most importantly is that voltage rating is the DC voltage rating, from experience this can used for good quality capacitors, AC voltage rating with frequency derating would be much lower.
Capacitor specifications are taken from data sheets at 100 kHz and some values for peak current, rms current, ESR and dv/dt are estimates from similar capacitors and graph read outs.
Inputs are in green. Outputs are in red. Formulas used can be seen below the calculator.