SDG #061 Ceramic Capacitors will Blow Up your PCB

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Language: en

00:00:00.709
so ceramic capacitors killing your
00:00:03.350 00:00:03.360 electronics what on earth am i talking
00:00:05.120 00:00:05.130 about well I thought this was quite an
00:00:06.860 00:00:06.870 interesting topic because it's something
00:00:08.360 00:00:08.370 that new engineers may not have even
00:00:11.000 00:00:11.010 considered but a situation that occurred
00:00:13.759 00:00:13.769 at work recently on a project that I was
00:00:15.919 00:00:15.929 working on at the situation where there
00:00:18.230 00:00:18.240 was a ceramic capacitor on the input
00:00:20.330 00:00:20.340 circuitry to the electronics there was a
00:00:22.700 00:00:22.710 switch mode power supply and then the
00:00:24.019 00:00:24.029 rest of the device and when we plugged
00:00:26.060 00:00:26.070 in the power to the device under certain
00:00:28.070 00:00:28.080 situations that DC to DC converter no
00:00:31.460 00:00:31.470 longer worked from that point onwards so
00:00:34.010 00:00:34.020 I thought I'd demonstrate what was going
00:00:35.420 00:00:35.430 on here so I've got a little then I
00:00:38.330 00:00:38.340 think this is a 20 2 micro farad ceramic
00:00:41.420 00:00:41.430 capacitor and I've got my bench power
00:00:44.750 00:00:44.760 supply set up so I've got the other lead
00:00:47.750 00:00:47.760 here I think this is set to around 12
00:00:50.720 00:00:50.730 volts or something yeah 12 volts and all
00:00:53.869 00:00:53.879 we're going to do is measure the voltage
00:00:55.459 00:00:55.469 across the ceramic capacitor as we
00:00:57.470 00:00:57.480 connect up the power so here we go and
00:01:02.540 00:01:02.550 if you have a look at the oscilloscope
00:01:03.590 00:01:03.600 you can see actually we've got a massive
00:01:05.690 00:01:05.700 overshoot a nominal voltage here at 12
00:01:08.929 00:01:08.939 volts but the scope is saying that the
00:01:11.630 00:01:11.640 maximum here is actually 20 volts and
00:01:13.820 00:01:13.830 the situation that I saw it was actually
00:01:16.760 00:01:16.770 a lot higher than that and it was
00:01:17.960 00:01:17.970 causing the the input to the DC to DC
00:01:20.660 00:01:20.670 converter to no longer work because it
00:01:22.910 00:01:22.920 was seeing such a high transient and we
00:01:25.070 00:01:25.080 can demonstrate this with a smaller
00:01:26.929 00:01:26.939 capacitor as well so it's not just
00:01:28.399 00:01:28.409 limited to something like one of these
00:01:30.200 00:01:30.210 22 microfarad capacitors this one is a
00:01:34.179 00:01:34.189 22 nano farad capacitor and if we hook
00:01:37.999 00:01:38.009 up the scope again to this and connect
00:01:41.210 00:01:41.220 up the power BAM there we go again so
00:01:44.690 00:01:44.700 this time we're reading a slightly
00:01:46.280 00:01:46.290 higher peak voltage so 22.6 but the
00:01:49.730 00:01:49.740 duration is much much shorter here so
00:01:52.639 00:01:52.649 what on earth is going on so all we've
00:01:54.620 00:01:54.630 got is our 12 volt power supply with our
00:01:56.389 00:01:56.399 ceramic capacitor at the other end of it
00:01:57.950 00:01:57.960 with a scope connected across the
00:01:59.990 00:02:00.000 capacitor and our education and books
00:02:02.240 00:02:02.250 should all tell us that the waveform
00:02:04.459 00:02:04.469 that we should see is this capacitor
00:02:06.649 00:02:06.659 charging waveform that asymptotes
00:02:08.900 00:02:08.910 towards 12 volts so what is giving us
00:02:11.780 00:02:11.790 the big spike
00:02:13.660 00:02:13.670 well basically we've got some non-ideal
00:02:15.460 00:02:15.470 characteristics between the power supply
00:02:17.260 00:02:17.270 and the ceramic capacitor so in my case
00:02:19.480 00:02:19.490 on the bench here I've got some 1 meter
00:02:21.190 00:02:21.200 cables so this distance is just 1 meter
00:02:25.300 00:02:25.310 but what were actually got here is we've
00:02:28.180 00:02:28.190 got some inductance we've got some
00:02:31.080 00:02:31.090 resistance and there would be some
00:02:33.340 00:02:33.350 parallel capacitance along here just to
00:02:36.040 00:02:36.050 buted all the way along but that's
00:02:37.600 00:02:37.610 minimal because we've not got wires that
00:02:40.360 00:02:40.370 are joined together along the whole
00:02:41.620 00:02:41.630 length but what's critical is that this
00:02:43.930 00:02:43.940 inductance here is causing us basically
00:02:46.750 00:02:46.760 to have a big inductive spike so what's
00:02:50.410 00:02:50.420 going on here essentially is that we've
00:02:52.000 00:02:52.010 got this LC circuit and a ceramic
00:02:55.240 00:02:55.250 capacitors are extremely low ESR devices
00:02:57.820 00:02:57.830 which means that they'll charge very
00:02:59.440 00:02:59.450 very quickly so what happens is we start
00:03:02.199 00:03:02.209 charging the capacitor and we know our
00:03:04.780 00:03:04.790 inductors resist a change in current so
00:03:08.140 00:03:08.150 what happens is the current slowly ramps
00:03:10.210 00:03:10.220 up and then the capacitor charges up and
00:03:13.030 00:03:13.040 the inductor still wants that current to
00:03:14.590 00:03:14.600 continue flowing so it does whatever it
00:03:16.180 00:03:16.190 can do to try and keep that current
00:03:17.620 00:03:17.630 flowing and what that happens to be is
00:03:20.199 00:03:20.209 by raising the voltage here as high as
00:03:22.330 00:03:22.340 it can until all of the energy and the
00:03:24.970 00:03:24.980 coil collapses so what we're actually
00:03:27.670 00:03:27.680 seeing is basically an RC tank circuit
00:03:31.180 00:03:31.190 which is why we're also seeing a bit of
00:03:32.770 00:03:32.780 ringing as well so this is a particular
00:03:34.810 00:03:34.820 problem in certain applications because
00:03:37.030 00:03:37.040 for example where you've got a plug top
00:03:38.949 00:03:38.959 power supply if you have this plugged in
00:03:43.210 00:03:43.220 and then connect up your DC connector
00:03:46.180 00:03:46.190 this is all charged up ready at 12 volts
00:03:48.789 00:03:48.799 so you just shove it in 12 volts
00:03:51.039 00:03:51.049 directly to this capacitor which wants
00:03:52.690 00:03:52.700 to create a really huge current and then
00:03:54.940 00:03:54.950 we see a big current and then the
00:03:56.560 00:03:56.570 inductor really wants to get that high
00:03:57.940 00:03:57.950 current flowing and you see a really
00:03:59.830 00:03:59.840 high voltage in the situation where your
00:04:01.960 00:04:01.970 power supply is permanently connected
00:04:03.670 00:04:03.680 and you turn on the mains instead you
00:04:06.039 00:04:06.049 won't see this because the the voltage
00:04:08.410 00:04:08.420 on the output of your power supply will
00:04:11.259 00:04:11.269 slowly increase and you won't see such a
00:04:13.780 00:04:13.790 high current being drawn by your
00:04:16.090 00:04:16.100 capacitors so I thought it might be
00:04:18.789 00:04:18.799 interesting just to see what other
00:04:19.900 00:04:19.910 capacitors are affected by this it's
00:04:22.029 00:04:22.039 typically going to be those with a
00:04:23.500 00:04:23.510 particularly low ESR so in this case
00:04:26.260 00:04:26.270 we've got a winner
00:04:27.129 00:04:27.139 film capacitor so let's do the test on
00:04:30.040 00:04:30.050 this one and yet there we go so we see
00:04:33.820 00:04:33.830 in the same sort of twenty two point six
00:04:35.679 00:04:35.689 peak voltage then we've got another type
00:04:39.040 00:04:39.050 of film capacitor and there we go very
00:04:43.029 00:04:43.039 similar we've got a lot of ringing on
00:04:44.260 00:04:44.270 this one I think this is a particularly
00:04:45.790 00:04:45.800 low impedance caster and I've got an
00:04:48.580 00:04:48.590 electrolytic capacitor so here we go
00:04:51.119 00:04:51.129 they were going a very small amount of
00:04:53.589 00:04:53.599 overshoot here so only thirteen point
00:04:55.510 00:04:55.520 four dropping down to twelve volts so
00:04:58.600 00:04:58.610 you might say to yourself well have
00:04:59.740 00:04:59.750 normally got a load on the output here
00:05:01.300 00:05:01.310 we haven't just got a capacitor with
00:05:03.070 00:05:03.080 nothing there
00:05:03.909 00:05:03.919 so what I've done now is I've just
00:05:05.559 00:05:05.569 connected a resistor across here so this
00:05:08.800 00:05:08.810 is a 22 ohm resistor which should
00:05:10.689 00:05:10.699 present quite a load so let's connect up
00:05:14.050 00:05:14.060 the power supply again and you can see
00:05:17.589 00:05:17.599 look we're still getting a very similar
00:05:18.939 00:05:18.949 reading nineteen point nine volts at the
00:05:21.640 00:05:21.650 peak here settling down to twelve volts
00:05:24.309 00:05:24.319 so even with a relatively large load
00:05:26.499 00:05:26.509 like this it's having virtually no
00:05:29.379 00:05:29.389 effect on that initial spike which is
00:05:31.420 00:05:31.430 just passed straight through to our
00:05:32.740 00:05:32.750 electronics in our DC to DC and causing
00:05:35.559 00:05:35.569 the input circuitry to blow up so to try
00:05:38.379 00:05:38.389 and combat this what we actually need to
00:05:39.760 00:05:39.770 do is to limit the current through the
00:05:43.209 00:05:43.219 capacitor so that we don't see such a
00:05:45.189 00:05:45.199 high peak current and thus we don't see
00:05:46.959 00:05:46.969 such a high peak voltage when the
00:05:49.300 00:05:49.310 capacitor is charged up so basically the
00:05:52.570 00:05:52.580 simplest way that we can do this is by
00:05:54.040 00:05:54.050 adding some resistance in here
00:05:55.929 00:05:55.939 as much as we can get away with without
00:05:58.179 00:05:58.189 affecting our electronics but enough to
00:06:01.149 00:06:01.159 dampen the effect of the increased
00:06:04.269 00:06:04.279 current right so here we are with our
00:06:06.070 00:06:06.080 capacitor and our resist a combination
00:06:08.079 00:06:08.089 the scope is across the capacitor and
00:06:09.670 00:06:09.680 the resistor and if we repeat the
00:06:11.589 00:06:11.599 experiment there you go we can see we
00:06:14.589 00:06:14.599 get basically no overshoot here it's
00:06:16.869 00:06:16.879 just gone over by about one volt at this
00:06:18.999 00:06:19.009 point and what we actually do is have
00:06:21.519 00:06:21.529 this resistor in series with our
00:06:23.230 00:06:23.240 capacitor but our load would still be
00:06:25.629 00:06:25.639 across and the overall combination of
00:06:27.909 00:06:27.919 the R and the C so what we're actually
00:06:30.219 00:06:30.229 doing here is effectively adding some
00:06:32.230 00:06:32.240 impedance to our capacitor so we're
00:06:33.969 00:06:33.979 increasing the ESR we've still got our
00:06:36.129 00:06:36.139 load connected across the combination of
00:06:38.469 00:06:38.479 the R on the C so we don't connect our
00:06:40.119 00:06:40.129 low
00:06:40.460 00:06:40.470 across the sea because that will affect
00:06:42.850 00:06:42.860 maximum current that we can draw from
00:06:44.780 00:06:44.790 our power supply so I'm just simulating
00:06:47.330 00:06:47.340 that here with our resistor across the
00:06:49.700 00:06:49.710 combination of the two and if we apply
00:06:51.560 00:06:51.570 power again there we go we get basically
00:06:54.920 00:06:54.930 no overshoot on the oscilloscope so
00:06:57.830 00:06:57.840 essentially we want to get this
00:06:59.480 00:06:59.490 resistance as low as possible so that
00:07:01.910 00:07:01.920 our circuit still functions as best as
00:07:03.710 00:07:03.720 possible because DC to DC converters and
00:07:05.900 00:07:05.910 that kind of thing
00:07:06.620 00:07:06.630 want extremely high transient currents
00:07:09.140 00:07:09.150 so if we start adding big resistances
00:07:11.480 00:07:11.490 here you start getting poor behavior of
00:07:13.970 00:07:13.980 your DC to DC converter so what you want
00:07:17.150 00:07:17.160 to do is get this as low as possible and
00:07:19.010 00:07:19.020 basically what all we're doing is
00:07:20.060 00:07:20.070 increasing the ESR of this capacitor by
00:07:22.070 00:07:22.080 having this series resistance what may
00:07:24.470 00:07:24.480 work better for you depending on your
00:07:26.030 00:07:26.040 application is to have cascaded stages
00:07:28.300 00:07:28.310 so you might want a COC type filter or
00:07:31.640 00:07:31.650 something like that so that you still
00:07:32.840 00:07:32.850 get a high transient current capability
00:07:36.290 00:07:36.300 if your DC to DC converter but you're
00:07:38.600 00:07:38.610 just limiting that inrush current the
00:07:40.760 00:07:40.770 other thing that you can do is you can
00:07:42.350 00:07:42.360 design something like a soft start
00:07:43.760 00:07:43.770 circuit and there's lots of ICS that do
00:07:45.590 00:07:45.600 this for you and basically during
00:07:48.140 00:07:48.150 startup you've got a resistance in
00:07:50.870 00:07:50.880 series with all of your electronics and
00:07:52.640 00:07:52.650 then a predefined time later it shorts
00:07:55.130 00:07:55.140 out that resistor and then from then
00:07:57.080 00:07:57.090 onwards your electronics can draw as
00:07:59.180 00:07:59.190 much power as it likes so there we go
00:08:01.070 00:08:01.080 hopefully found that video useful and
00:08:02.600 00:08:02.610 particularly if you're designing
00:08:03.500 00:08:03.510 electronics if you come across this
00:08:05.060 00:08:05.070 problem in the future you might know
00:08:06.920 00:08:06.930 what to start looking for but until next
00:08:09.320 00:08:09.330 time thanks for watching
00:08:12.810 00:08:12.820 you
00:08:23.100 00:08:23.110
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