Other Parts Discussed in Thread: TPS56C215, TPS54020, LMZ31710, TPS54A20, TPSM84A21
Hello,
Is there any conducted and/or radiated EMI data available for the TPS54824 ?
e.g. a CISPR22 or CISPR25 report for the TPS54824EVM.
Thanks, Ken
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Hello Ryan,
Thanks for the reply. Yes, I understand that the EMI is very layout dependant, but some manufacturers are starting to give EVM EMI data as an indication of how the part performs.
It seems that quite a few are getting on the symmetrical pin-out bandwagon (e.g. LT8640, MPQ8636). But it makes sense to keep the circulating currents balanced so they cancel out, and hence low EMI. Some of these parts also have spread spectrum which is nice (e.g. LT8640, your LM53635). What would be nice for my design is something that can do 5-12Vin to 1V1out @ 10A, symmetrical pin-out, and spread spectrum. Something for the wish list…
Best regards, Ken
Hello Ken,
Thanks for the part numbers. I was unaware that some suppliers have started inserting such information into their datasheets. I will have to keep on the look out.
I am curious if you have looked at the TPS56C215 it is a 12A part that has a similar symmetric configuration on the GND pins around the SW node. Also the fact that is a DCAP-3 control method it leverages a form of constant-on-time which is inherently somewhat spread spectrum. I am curious what you think after you have a chance to look at that part.
There might be a few other parts that could also fit the bill but that would be a good place to start in the TI catalog.
Hi Ryan,
Just thought I would give you an update on my progress...
Got hold of several evaluation boards so that I could estimate radiated noise. Used a near field loop probe and a Cleverscope CS328 oscilloscope which has a spectrum analyser built in. OK, it’s not as good as a proper EMI chamber, but at least it can give me an indication. Here are the results:
Test Board |
Type |
RMS noise |
Spectral Peak |
F peak |
Vin Range |
Part cost US$ (100) |
Efficiency (data sheet) 12Vin, 1V1, 6.4A out |
LMZ31710EVM |
Module |
95mV |
-26dB |
312kHz |
3-17V |
11.68 |
85 |
TPS54020EVM |
Chip |
117mV |
-22dB |
500kHz |
4.5-17V |
5.11 |
? |
TPSM84A21EVM |
Module |
49mV |
-33dB |
1995kHz |
8-14V |
12.75 |
85 |
TPS54A20EVM |
Chip |
38mV |
-35dB |
3928kHz |
8-14V |
5.35 |
86 |
MPM3682 |
Module |
78mV |
-26dB |
436kHz |
4.5-18V |
9.80 |
90 |
MPQ8636 |
Chip |
94mV |
-25dB |
300kHz |
4.5-18V |
3.13 |
90 |
TPS56C215EVM |
Chip |
62mV |
-29dB |
1243kHz |
4.5-17V |
3.95 |
83 |
The TPS54A20 & TPSM84A21 are dual phase 2MHz parts and give the best performance for radiated noise, but they do not operate below 8Vin. There is an internal 7.65V UVLO which shuts the part down. So these parts cannot be used for the automotive start condition (ISO 16750 normal cold start 4.5V for 19ms, rising to 6.5V over 50ms).
Next best part which could keep running through cold start is the TPS56C215. It has symmetrical pin-out so good for EMI. So will use the TPS56C215 for the design.
Then I started experimenting…
The idea of these symmetrical pin-out parts (e.g. LT8640, LM53635, TPS56C215, MPQ8636, etc) is that current flows in balanced loops to cancel out the generated EMI:
All good, except there’s only one inductor so it can’t be symmetrical and cancel out. So try with 2 inductors…
The LM53635 board has the most symmetrical layout of the ones I have, so modify it with 2x 4.7uH inductors in parallel. Placed them with “pin 1” in opposite directions so that flux will cancel; e.g. with current flowing from left to right, one inductor will have flux going into board and the other will have flux coming out of board.
LM53635 board: Original single 2.2uH:
LM53635 board: Modified with 2x 4.7uH, pin 1 opposite directions:
Frequency display: Dark trace 2.2uH original inductor, light trace 2x 4.7uH (peak about 6dB better):
Time display: Loop centred over inductor(s). Dark trace with 2x 4.7uH, light trace with original 2.2uH. For the 2 inductor case the flux is cancelled directly above the centre of them.
Using dual inductors seems to improve the peak radiated noise (at least for near field) by about 6dB, and directly above the inductors the flux is cancelled. This also has the advantage that the current is half in each inductor, so flux density and RMS losses will lower.
We will implement parallel inductors in our design.