What are Aluminum Polymer Capacitors -- KEMET and Mouser Electronics

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Language: en

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00:00:17.930 00:00:17.940 hey we need to talk about capacitors yep
00:00:21.890 00:00:21.900 I know what you're thinking if engineers
00:00:24.230 00:00:24.240 were chefs capacitors would be salt
00:00:26.900 00:00:26.910 never the star of the show you never
00:00:29.810 00:00:29.820 know exactly how much you're going to
00:00:32.210 00:00:32.220 need we all just kind of sprinkle them
00:00:34.850 00:00:34.860 on to our design until it tastes about
00:00:38.030 00:00:38.040 right hmm
00:00:40.840 00:00:40.850 needs more capacitors but there's a lot
00:00:45.080 00:00:45.090 more to choosing the best capacitor than
00:00:47.479 00:00:47.489 just grabbing a shaker full of
00:00:48.920 00:00:48.930 electrolytic sand sprinkle them artfully
00:00:51.229 00:00:51.239 around your PCB hmm pinch more there hi
00:00:56.060 00:00:56.070 I'm Amelia Dalton host of chalk talk it
00:00:59.119 00:00:59.129 turns out that choosing the right kind
00:01:01.250 00:01:01.260 of capacitor can have important
00:01:03.740 00:01:03.750 implications for your design in
00:01:05.930 00:01:05.940 reliability longevity cost board size my
00:01:11.029 00:01:11.039 guest today is James Lewis from Kemet
00:01:13.609 00:01:13.619 and we're gonna dive into some
00:01:15.200 00:01:15.210 fascinating discussion of capacitors
00:01:17.859 00:01:17.869 including some super cool new organic
00:01:21.320 00:01:21.330 polymer aluminum hmm what's all this
00:01:25.460 00:01:25.470 about let's find out and before we get
00:01:29.089 00:01:29.099 started don't forget to click that link
00:01:31.040 00:01:31.050 there you can find out more information
00:01:33.139 00:01:33.149 about capacitors from Kemet hi James
00:01:37.070 00:01:37.080 thank you so much for joining me today
00:01:39.199 00:01:39.209 thanks Melia I'm looking forward to our
00:01:41.240 00:01:41.250 discussion about a certain kind of
00:01:42.889 00:01:42.899 capacitor okay so my relationship with
00:01:45.559 00:01:45.569 capacitors is mainly things like
00:01:47.779 00:01:47.789 decoupling of course and working in
00:01:50.839 00:01:50.849 power and filtering parts of my design
00:01:53.419 00:01:53.429 now I've heard of aluminum electrolytic
00:01:56.979 00:01:56.989 capacitors but what are these organic
00:02:00.309 00:02:00.319 aluminum capacitors I've heard about and
00:02:03.440 00:02:03.450 and are they in that expensive section
00:02:06.499 00:02:06.509 of the grocery store no no they're just
00:02:11.660 00:02:11.670 a different type of aluminum
00:02:13.100 00:02:13.110 electrolytic capacitor okay then why
00:02:15.949 00:02:15.959 don't we talk about the difference
00:02:17.900 00:02:17.910 between organic and traditional aluminum
00:02:21.199 00:02:21.209 all right let's start by talking about
00:02:23.180 00:02:23.190 what's inside of a traditional aluminum
00:02:25.220 00:02:25.230 and then we'll get to these polymer
00:02:26.630 00:02:26.640 stuff in a few minutes so if we look at
00:02:28.880 00:02:28.890 this picture I've got a can
00:02:31.059 00:02:31.069 that we've kind of exploded out a little
00:02:32.559 00:02:32.569 bit and there's two key things inside
00:02:34.899 00:02:34.909 the can there's the anode foil and the
00:02:36.819 00:02:36.829 cathode foil and so these are actually
00:02:38.259 00:02:38.269 the electrode plates that provide our
00:02:40.929 00:02:40.939 positive and negative connection to the
00:02:42.550 00:02:42.560 capacitor in between them is a separator
00:02:45.610 00:02:45.620 paper which as you might imagine from
00:02:47.920 00:02:47.930 the name separates the two plates from
00:02:49.690 00:02:49.700 each other so that we don't have direct
00:02:51.039 00:02:51.049 contact and then within those foils in
00:02:53.890 00:02:53.900 that roll of paper we have foil tabs
00:02:56.080 00:02:56.090 that are connected into them and that's
00:02:57.789 00:02:57.799 what actually provides the actual
00:02:59.020 00:02:59.030 terminal connection so I notice there's
00:03:01.569 00:03:01.579 no electrolyte in this electrolytic
00:03:04.709 00:03:04.719 capacitor at least on this page at least
00:03:08.199 00:03:08.209 so where is this electrolyte hiding it's
00:03:12.670 00:03:12.680 actually that's a good question because
00:03:14.800 00:03:14.810 it's hiding inside of the paper
00:03:16.929 00:03:16.939 separator and so we actually impregnate
00:03:19.240 00:03:19.250 the paper with the electrolyte itself I
00:03:21.369 00:03:21.379 think sometimes people think of kind of
00:03:23.379 00:03:23.389 like this picture shows a actual liquid
00:03:25.300 00:03:25.310 kind of rolling around inside the can
00:03:27.099 00:03:27.109 but it's not really like water it's more
00:03:29.379 00:03:29.389 like a paste and so that electrolyte
00:03:31.809 00:03:31.819 does a lot of things for us one thing I
00:03:33.670 00:03:33.680 wanted to point out is that there's a
00:03:35.530 00:03:35.540 lot that goes into what we choose for
00:03:37.300 00:03:37.310 that electrolyte just for example at
00:03:39.129 00:03:39.139 Kemet we have something on the order of
00:03:40.599 00:03:40.609 40 different electrolytes for our
00:03:42.429 00:03:42.439 various products and so we have to
00:03:43.929 00:03:43.939 consider what's the ph of the material
00:03:46.360 00:03:46.370 what kind of operational temperature
00:03:47.770 00:03:47.780 range does it work across what's its
00:03:50.020 00:03:50.030 ability to help us reoxidized a foil
00:03:52.929 00:03:52.939 which we'll probably talk about in a
00:03:54.460 00:03:54.470 little bit then of course with all the
00:03:56.559 00:03:56.569 other materials we've got going on is
00:03:58.179 00:03:58.189 how compatible are they we don't want
00:04:00.699 00:04:00.709 something that eats away at the can
00:04:02.199 00:04:02.209 otherwise be able iki capacitor and then
00:04:04.270 00:04:04.280 of course we need to make sure that it
00:04:06.039 00:04:06.049 doesn't cost too much to use it it's not
00:04:08.020 00:04:08.030 toxic and more importantly it's not
00:04:10.629 00:04:10.639 flammable okay James can you walk me
00:04:13.240 00:04:13.250 through how the elements of an
00:04:15.280 00:04:15.290 electrolytic capacitor work together
00:04:17.349 00:04:17.359 right okay we've got the anode foil the
00:04:19.959 00:04:19.969 cathode foil and we've got the separator
00:04:21.879 00:04:21.889 which is a red line as we show in this
00:04:23.589 00:04:23.599 diagram now what we do on the anode foil
00:04:25.870 00:04:25.880 is when we're processing the foil we do
00:04:28.420 00:04:28.430 two things we acid etch it which gives
00:04:31.120 00:04:31.130 us a really large surface area and then
00:04:33.399 00:04:33.409 the second thing we do is we run it
00:04:34.839 00:04:34.849 through an electrolyte bath where we
00:04:36.700 00:04:36.710 actually grow the dielectric layer and
00:04:38.589 00:04:38.599 so we think about the basic elements of
00:04:40.659 00:04:40.669 a capacitor we get our anode plate and
00:04:42.580 00:04:42.590 then we grow the dielectric
00:04:44.650 00:04:44.660 and that gives us a cathode plate and so
00:04:46.450 00:04:46.460 then over on the other side of the
00:04:48.010 00:04:48.020 capacitor we have another foil which
00:04:49.600 00:04:49.610 called the cathode foil and so in order
00:04:51.850 00:04:51.860 to connect that foil which is connected
00:04:53.800 00:04:53.810 to the terminals we include a conductive
00:04:56.290 00:04:56.300 electrolyte between them and so that way
00:04:58.480 00:04:58.490 we get the electrical connection to the
00:05:00.250 00:05:00.260 actual cathode of the capacitor and so
00:05:02.110 00:05:02.120 that's how we get our anode plate
00:05:04.060 00:05:04.070 gathered plate all connected got okay so
00:05:07.540 00:05:07.550 other than making this electrical
00:05:09.640 00:05:09.650 connection how does the electrolyte do
00:05:12.610 00:05:12.620 anything else for us there's a really
00:05:15.670 00:05:15.680 critical thing that can happen with a
00:05:17.680 00:05:17.690 aluminum electrolytic capacitor and
00:05:19.510 00:05:19.520 that's called reform or heal and so
00:05:22.210 00:05:22.220 remember when I talked about the
00:05:23.470 00:05:23.480 electrolyte I mentioned that we consider
00:05:25.930 00:05:25.940 the pH value of the electrolyte and
00:05:28.360 00:05:28.370 that's because when the oxide is in
00:05:31.000 00:05:31.010 contact with this electrolyte material
00:05:33.130 00:05:33.140 it tends to break down the oxide which
00:05:36.310 00:05:36.320 what we're showing here is a
00:05:37.510 00:05:37.520 cross-section of a aluminum plate where
00:05:40.540 00:05:40.550 we've grown a dielectric which is the
00:05:42.550 00:05:42.560 black region and then the yellow region
00:05:44.140 00:05:44.150 represents the electrolyte and so when
00:05:46.810 00:05:46.820 we grow this dielectric we grow it based
00:05:49.750 00:05:49.760 on what we call the formation voltage
00:05:51.310 00:05:51.320 which is going to be some multiplier of
00:05:53.170 00:05:53.180 the radiant voltage which we hope is
00:05:55.030 00:05:55.040 more than your application voltage and
00:05:57.250 00:05:57.260 so the thing that happens is over time
00:05:59.320 00:05:59.330 the electrolyte will actually eat into
00:06:01.420 00:06:01.430 the dielectric or the oxide and it's
00:06:04.270 00:06:04.280 going to basically eat down to whatever
00:06:06.250 00:06:06.260 voltage is applied and so that's one
00:06:08.980 00:06:08.990 reason why when we do the formation we
00:06:10.780 00:06:10.790 form it much higher than what we say we
00:06:13.630 00:06:13.640 can apply to it so even though the
00:06:15.670 00:06:15.680 electrolyte can eat away at this oxide
00:06:17.380 00:06:17.390 it also has the ability to help regrow
00:06:20.080 00:06:20.090 it and so let's just say for example
00:06:22.120 00:06:22.130 it's sitting on a shelf for a couple of
00:06:24.370 00:06:24.380 years well that oxide over time is going
00:06:26.560 00:06:26.570 to be depleted just from the interaction
00:06:28.810 00:06:28.820 between the oxide and the electrolyte
00:06:30.400 00:06:30.410 when you apply a voltage to it however
00:06:32.230 00:06:32.240 the dielectric will actually regrow or
00:06:35.200 00:06:35.210 what we call reform and the way it does
00:06:37.180 00:06:37.190 that is it pulls oxygen out of the
00:06:39.070 00:06:39.080 electrolyte allowing it to regrow the
00:06:41.140 00:06:41.150 oxide it seems like this electrolyte is
00:06:44.200 00:06:44.210 a bit of a liability in a way then if we
00:06:48.400 00:06:48.410 could just get rid of this electrolyte
00:06:50.520 00:06:50.530 would it be a better capacitor yeah I
00:06:54.159 00:06:54.169 think the thing we need to consider is
00:06:56.260 00:06:56.270 if we have like a long life application
00:06:58.390 00:06:58.400 or application where conductivity is
00:07:00.520 00:07:00.530 important then we might want to consider
00:07:01.870 00:07:01.880 ways to get rid of the electrolyte and
00:07:04.060 00:07:04.070 so one way we can do that is with these
00:07:06.250 00:07:06.260 organic aluminum polymer capacitors and
00:07:08.920 00:07:08.930 in these capacitors we've replaced the
00:07:11.500 00:07:11.510 electrolyte with a polymer material and
00:07:14.140 00:07:14.150 so here I'm showing a cross-section of a
00:07:16.990 00:07:17.000 polymer aluminum capacitor and what you
00:07:19.270 00:07:19.280 might notice is the diagram doesn't look
00:07:21.189 00:07:21.199 all that much different than the
00:07:22.659 00:07:22.669 previous one we looked at in fact all
00:07:24.520 00:07:24.530 we've done in this picture is just said
00:07:26.469 00:07:26.479 that the polymer is now impregnating
00:07:28.480 00:07:28.490 inside of the paper that separates the
00:07:30.430 00:07:30.440 anode and cathode okay so then how do we
00:07:33.400 00:07:33.410 get that electrical connection through
00:07:36.129 00:07:36.139 the paper paper isn't exactly my
00:07:38.860 00:07:38.870 favorite conductor yeah it turns out
00:07:41.500 00:07:41.510 craft paper is not so good at conducting
00:07:43.689 00:07:43.699 electricity so when we actually look
00:07:45.790 00:07:45.800 inside if we think about the wet
00:07:48.189 00:07:48.199 electrolytic the paper was there to
00:07:50.170 00:07:50.180 physically isolate the two connections
00:07:52.750 00:07:52.760 it was also there to provide a
00:07:55.379 00:07:55.389 suspension for the liquid electrolyte
00:07:57.700 00:07:57.710 when we look at a polymer capacitor some
00:08:00.490 00:08:00.500 constructions use actually a film
00:08:01.870 00:08:01.880 material instead of a paper material
00:08:03.400 00:08:03.410 because it's only a physical separation
00:08:05.290 00:08:05.300 the polymer is a solid material and by
00:08:09.250 00:08:09.260 the way I didn't mention this before but
00:08:10.629 00:08:10.639 if you're curious about it it's called P
00:08:12.760 00:08:12.770 dot PE do T and so it's a conductive
00:08:15.879 00:08:15.889 polymer material so is conductive
00:08:18.790 00:08:18.800 polymer really an electrolyte but
00:08:21.790 00:08:21.800 without all the usual gooey mess that's
00:08:24.490 00:08:24.500 pretty close to being exactly the case
00:08:26.830 00:08:26.840 like I said before number one it's a
00:08:28.900 00:08:28.910 solid material it's still there to help
00:08:31.270 00:08:31.280 provide our cathode connection from the
00:08:33.070 00:08:33.080 literal cathode on the dielectric to a
00:08:35.170 00:08:35.180 terminal but it's solid it doesn't dry
00:08:37.390 00:08:37.400 up in the same way that a wet
00:08:38.709 00:08:38.719 electrolyte does because it's solid it's
00:08:41.170 00:08:41.180 not a liquid now that doesn't mean it
00:08:43.449 00:08:43.459 doesn't wear out but it has a completely
00:08:45.280 00:08:45.290 different wear out mechanism and in
00:08:46.780 00:08:46.790 terms of conductivity which is something
00:08:48.370 00:08:48.380 I think you're going to be most
00:08:49.480 00:08:49.490 interested in is it can be orders of
00:08:51.790 00:08:51.800 magnitude higher than a traditional
00:08:53.260 00:08:53.270 electrolyte okay there are always
00:08:56.460 00:08:56.470 compromises let's get this over with
00:08:59.829 00:08:59.839 what do I give up by going with polymer
00:09:03.329 00:09:03.339 electrolytic fantastic question because
00:09:06.490 00:09:06.500 it's very rare we can say you know it's
00:09:09.190 00:09:09.200 actually a lot of upside and only
00:09:11.600 00:09:11.610 few downsides and so in terms of a
00:09:14.210 00:09:14.220 capacitor generally people think okay
00:09:16.220 00:09:16.230 when you change a material you're going
00:09:17.660 00:09:17.670 to lose some of the rate of voltage
00:09:19.460 00:09:19.470 capability or maybe the amount of
00:09:21.860 00:09:21.870 capacitance that you get or you need
00:09:23.690 00:09:23.700 more size the great thing about the
00:09:25.670 00:09:25.680 polymer material is that for about the
00:09:28.220 00:09:28.230 same size we get the same voltage of
00:09:29.990 00:09:30.000 capacitances available because we're
00:09:31.550 00:09:31.560 only replacing out one material the key
00:09:33.710 00:09:33.720 benefit as I mentioned the conductivity
00:09:35.540 00:09:35.550 means we get very very low es R's
00:09:37.730 00:09:37.740 so the one critical trade-off is that
00:09:40.460 00:09:40.470 the polymer material is more temperature
00:09:43.100 00:09:43.110 sensitive in terms of maximum operating
00:09:45.290 00:09:45.300 temperature and so 105 125 are really
00:09:49.009 00:09:49.019 the upper limits for the technologies
00:09:50.449 00:09:50.459 which isn't to say that 150 and maybe
00:09:52.460 00:09:52.470 one day 175 is impossible but that's one
00:09:55.490 00:09:55.500 area where we see that the operational
00:09:57.530 00:09:57.540 temperature does come down a little bit
00:09:59.329 00:09:59.339 compared to the same capacitance voltage
00:10:01.639 00:10:01.649 and size for wet electrolytic alright so
00:10:04.730 00:10:04.740 temperature is the thing then what are
00:10:07.610 00:10:07.620 these temperature characteristics you're
00:10:09.769 00:10:09.779 talking about
00:10:10.550 00:10:10.560 okay so let's say you're okay with the
00:10:12.860 00:10:12.870 temperature range and you want to
00:10:13.880 00:10:13.890 operate the capacitor within its
00:10:15.319 00:10:15.329 temperature range whether it's 105 over
00:10:17.030 00:10:17.040 125 or some de 150 one thing to know
00:10:19.730 00:10:19.740 with just about any wet electrolyte is
00:10:21.860 00:10:21.870 that you're going to see a huge shift in
00:10:24.230 00:10:24.240 conductivity or probably what we're more
00:10:26.509 00:10:26.519 interested in with the capacitor is a
00:10:27.889 00:10:27.899 shift in resistance across its
00:10:30.230 00:10:30.240 temperature range so here the red graph
00:10:32.449 00:10:32.459 is showing us an aluminum electrolytic
00:10:34.400 00:10:34.410 from negative 55 to 125 degrees C and it
00:10:37.610 00:10:37.620 shifts it changes over 250 ohms from
00:10:41.480 00:10:41.490 it's cold hot temperature that's kind of
00:10:43.939 00:10:43.949 tough to design for right whereas if we
00:10:45.769 00:10:45.779 look at a similar-sized voltage
00:10:48.290 00:10:48.300 capacitance of a conductive polymer
00:10:51.079 00:10:51.089 electrolytic the same range the shift is
00:10:53.720 00:10:53.730 only 233 millions and so obviously the
00:10:57.620 00:10:57.630 range is much tighter but also by the
00:11:00.110 00:11:00.120 way pay attention to the change in
00:11:02.389 00:11:02.399 overall ESR we're talking about a
00:11:04.519 00:11:04.529 capacitor that is over a home versus one
00:11:06.889 00:11:06.899 that's less than 100 milli ohms for my
00:11:09.590 00:11:09.600 de coupling needs for say a switching
00:11:12.710 00:11:12.720 power supply how does the switching
00:11:15.590 00:11:15.600 frequency affect these capacitors right
00:11:18.650 00:11:18.660 sometimes a non-obvious characteristic
00:11:21.230 00:11:21.240 of a capacitor especially electrolytic
00:11:23.000 00:11:23.010 capacitor is that the ESR
00:11:25.400 00:11:25.410 is affected by frequency and it turns
00:11:27.619 00:11:27.629 out it's because internally there's an
00:11:29.240 00:11:29.250 RC ladder construction that's going on
00:11:31.100 00:11:31.110 and so we see the response change with
00:11:33.829 00:11:33.839 frequency again because it's such a
00:11:35.629 00:11:35.639 highly conductive material the overall
00:11:37.610 00:11:37.620 ESR is lower and it's stability is
00:11:40.309 00:11:40.319 relatively high and so here we're just
00:11:41.960 00:11:41.970 gonna compare an aluminum electrolytic
00:11:43.639 00:11:43.649 which again is much much higher ESR but
00:11:46.249 00:11:46.259 it shifts quite a bit from say DC to
00:11:48.079 00:11:48.089 tens of megahertz whereas if we look at
00:11:50.179 00:11:50.189 the conductive polymer it's relatively
00:11:52.400 00:11:52.410 stable right around 100 million it drops
00:11:54.470 00:11:54.480 down a little bit around 100 K but it's
00:11:56.480 00:11:56.490 mostly stable across the frequency sweep
00:11:58.519 00:11:58.529 and then back on temperature a little
00:12:00.769 00:12:00.779 bit how does temperature translate into
00:12:03.860 00:12:03.870 life expectancy this is probably one of
00:12:06.920 00:12:06.930 the most misunderstood and critical
00:12:09.470 00:12:09.480 differences between a wet electrolyte
00:12:11.389 00:12:11.399 and a conductive polymer electrolytic
00:12:13.400 00:12:13.410 the lifetime of a conductive polymer is
00:12:16.300 00:12:16.310 significantly better than a traditional
00:12:19.129 00:12:19.139 aluminum electrolytic one of the main
00:12:21.379 00:12:21.389 reasons why is that as the alumina
00:12:24.079 00:12:24.089 electrolytic is used over a period of
00:12:26.210 00:12:26.220 time its electrolyte dries up and so
00:12:28.790 00:12:28.800 that affects its lifetime now if we look
00:12:31.730 00:12:31.740 at this graph a common rule of thumb is
00:12:34.340 00:12:34.350 that for every 10 degree decrease you'll
00:12:37.040 00:12:37.050 double the life of an aluminum
00:12:38.870 00:12:38.880 electrolytic which is typically true for
00:12:41.120 00:12:41.130 a standard wet electrolyte however if we
00:12:43.579 00:12:43.589 look at the conductive polymer life is
00:12:46.280 00:12:46.290 10 times longer with every 20 degree
00:12:49.249 00:12:49.259 decrease and so it's not a linear
00:12:51.590 00:12:51.600 relationship between their lifetimes now
00:12:53.929 00:12:53.939 the way you can kind of think about this
00:12:55.670 00:12:55.680 is look at these lower temperatures
00:12:57.079 00:12:57.089 right under 85 degrees C you're getting
00:12:59.780 00:12:59.790 significantly more life out of that
00:13:01.550 00:13:01.560 conductive polymer now like I said the
00:13:03.530 00:13:03.540 one kind of trade-off here is that as
00:13:05.120 00:13:05.130 you get closer to 105 125 that's not
00:13:07.550 00:13:07.560 quite the same advantage but you still
00:13:09.650 00:13:09.660 do get the benefit of lower ESR and
00:13:12.290 00:13:12.300 since temperature isn't a big factor in
00:13:14.900 00:13:14.910 the life of my capacitor what about self
00:13:18.499 00:13:18.509 heating and internal resistance
00:13:20.900 00:13:20.910 good follow-up because if we think about
00:13:23.150 00:13:23.160 temperature it's easy to think about
00:13:24.559 00:13:24.569 ambient but most of the time we're
00:13:26.720 00:13:26.730 worried about what does the self heating
00:13:28.189 00:13:28.199 due to the capacitor with in an ambient
00:13:30.379 00:13:30.389 situation and so because the ESR is so
00:13:33.530 00:13:33.540 low on these parts they can take on
00:13:35.540 00:13:35.550 higher amounts of ripple current before
00:13:37.699 00:13:37.709 their self heating contribu
00:13:39.049 00:13:39.059 it's to the overall maximum temperature
00:13:40.909 00:13:40.919 and so we've tried to normalize out some
00:13:42.889 00:13:42.899 information here so this graph we're
00:13:44.689 00:13:44.699 going to look at aluminum electrolytic
00:13:45.979 00:13:45.989 versus conductive polymer and we're
00:13:48.349 00:13:48.359 looking at the same voltage and
00:13:50.209 00:13:50.219 capacitance and when possible in the
00:13:51.859 00:13:51.869 same case sizes and so what's
00:13:53.569 00:13:53.579 interesting is when you look at this
00:13:55.099 00:13:55.109 you've got quite a bit more ripple
00:13:57.349 00:13:57.359 current available from the conductive
00:13:59.449 00:13:59.459 polymer and so basically we've done the
00:14:01.189 00:14:01.199 math for you we've looked at what the
00:14:02.629 00:14:02.639 self-heating would be and then we added
00:14:04.429 00:14:04.439 it to an room temperature ambient to get
00:14:06.619 00:14:06.629 to 105 C so if you're not calculating
00:14:08.839 00:14:08.849 with room temperature then we have to do
00:14:10.159 00:14:10.169 a little bit different math but the same
00:14:11.599 00:14:11.609 trend holds the conductive polymers can
00:14:13.549 00:14:13.559 handle quite a bit more ripple current
00:14:15.379 00:14:15.389 than a traditional aluminum what oolitic
00:14:17.359 00:14:17.369 which by the way it might mean you don't
00:14:19.099 00:14:19.109 need as much capacitance or really where
00:14:21.739 00:14:21.749 I'm getting is you don't need as many
00:14:22.819 00:14:22.829 capacitors and so you might actually be
00:14:24.589 00:14:24.599 able to reduce the size of your design
00:14:26.389 00:14:26.399 just with a single polymer capacitor
00:14:28.639 00:14:28.649 okay I think I've got a pretty good
00:14:31.039 00:14:31.049 handle on all of this
00:14:32.599 00:14:32.609 hit me with some of that datasheet stuff
00:14:35.119 00:14:35.129 okay let's let's look at some things
00:14:37.459 00:14:37.469 that maybe don't look so good on a graph
00:14:39.559 00:14:39.569 but I think they're important to
00:14:40.729 00:14:40.739 understand about the aluminum polymers
00:14:42.319 00:14:42.329 so first of all they do have a shelf
00:14:44.299 00:14:44.309 life but it's not really much different
00:14:46.039 00:14:46.049 than any other surface mount capacitor
00:14:48.469 00:14:48.479 the shelf life is really related to the
00:14:50.779 00:14:50.789 solder ability of the component not
00:14:52.909 00:14:52.919 necessarily the degradation of the
00:14:54.619 00:14:54.629 capacitive element now the one exception
00:14:56.509 00:14:56.519 here is that aluminum polymer capacitors
00:14:58.579 00:14:58.589 and we see this with almost any
00:15:00.469 00:15:00.479 capacitor using P dot is going to be
00:15:02.629 00:15:02.639 rated as an MSL one rating in terms of
00:15:05.149 00:15:05.159 surge voltage there are similar search
00:15:07.009 00:15:07.019 capabilities to a traditional aluminum
00:15:09.019 00:15:09.029 electrolytic but it's gonna be series
00:15:11.089 00:15:11.099 dependent so you're gonna have to look
00:15:12.229 00:15:12.239 at the parts datasheet to understand
00:15:13.789 00:15:13.799 what it's search capabilities are in
00:15:15.349 00:15:15.359 terms of D rating voltage D rating even
00:15:17.809 00:15:17.819 temperature D rating to some extent it's
00:15:20.149 00:15:20.159 not like other polymer capacitor
00:15:22.309 00:15:22.319 technologies where you're told you need
00:15:23.959 00:15:23.969 a ten to twenty percent voltage D rate
00:15:25.759 00:15:25.769 you can use 100 percent of the applied
00:15:28.009 00:15:28.019 voltage to the capacitor obviously the
00:15:30.109 00:15:30.119 less volts that you apply you'll
00:15:31.459 00:15:31.469 probably increase the life but it's not
00:15:33.619 00:15:33.629 gonna have a significant effect on the
00:15:35.209 00:15:35.219 wear out unlike traditional what
00:15:37.069 00:15:37.079 electrolytic and then finally the
00:15:38.689 00:15:38.699 failure mode sort of like Illumina
00:15:40.369 00:15:40.379 electrolytic the ESR will change over
00:15:42.199 00:15:42.209 time the mechanism for that ESR change
00:15:44.179 00:15:44.189 is different but what we'll see is that
00:15:45.679 00:15:45.689 the ESR will increase which will
00:15:47.749 00:15:47.759 effectively turn it into an open as it
00:15:50.509 00:15:50.519 reaches end-of-life
00:15:51.530 00:15:51.540 okay James remind me again how
00:15:53.840 00:15:53.850 traditional electrolytic and polymer are
00:15:56.720 00:15:56.730 similar and different okay so they're
00:15:59.540 00:15:59.550 similar in their form factors Radio lead
00:16:02.450 00:16:02.460 it surface mount snapping all available
00:16:04.790 00:16:04.800 in the same sort of packages that are
00:16:06.770 00:16:06.780 used to quite honestly the big
00:16:08.600 00:16:08.610 difference you'll notice is the colors
00:16:10.130 00:16:10.140 that we use on the silkscreen are
00:16:11.480 00:16:11.490 different you'll see very similar
00:16:13.040 00:16:13.050 voltages and capacitances between the
00:16:15.290 00:16:15.300 two now for the highest voltage parts
00:16:17.360 00:16:17.370 it's still going to be done with a wet
00:16:18.890 00:16:18.900 electrolytic but we keep seeing the
00:16:20.690 00:16:20.700 voltages on the polymers go up higher
00:16:22.640 00:16:22.650 and higher and just for context I'm
00:16:24.350 00:16:24.360 talking about things like in the 300 400
00:16:26.390 00:16:26.400 volt range if we're talking anything 50
00:16:28.070 00:16:28.080 volts and below nearly identical and
00:16:29.930 00:16:29.940 then in terms of price of course my
00:16:31.760 00:16:31.770 favorite answer with capacitors is price
00:16:33.560 00:16:33.570 as always it depends on a number of
00:16:35.120 00:16:35.130 factors but when we look at the
00:16:36.650 00:16:36.660 differences between these two we
00:16:38.240 00:16:38.250 typically see things that are in the
00:16:40.040 00:16:40.050 same ballpark and then of course keep in
00:16:41.990 00:16:42.000 mind with lower ESR you get more
00:16:44.390 00:16:44.400 effective capacitance at switching
00:16:46.010 00:16:46.020 frequencies and so in a switching
00:16:47.330 00:16:47.340 application you may actually be able to
00:16:48.800 00:16:48.810 use fewer components which will
00:16:50.480 00:16:50.490 contribute to a lower overall cost and
00:16:53.260 00:16:53.270 polymer is better at what number one
00:16:56.120 00:16:56.130 message if you didn't hear it before is
00:16:57.830 00:16:57.840 that there is so much less ESR at these
00:17:00.470 00:17:00.480 parts and so if you can't relate how
00:17:02.990 00:17:03.000 that could it be helpful in your circuit
00:17:04.490 00:17:04.500 just remember less ESR means less heat
00:17:07.040 00:17:07.050 and almost everybody wants less heat in
00:17:09.050 00:17:09.060 their designs basically allows us to
00:17:11.120 00:17:11.130 address more ripple current with these
00:17:12.980 00:17:12.990 devices because there is no liquid
00:17:15.170 00:17:15.180 electrolyte there is a much longer
00:17:17.870 00:17:17.880 lifetime associated with them now there
00:17:20.210 00:17:20.220 are wear out mechanisms associated with
00:17:22.250 00:17:22.260 polymer and field application engineer
00:17:24.260 00:17:24.270 can talk to you about what that's going
00:17:25.400 00:17:25.410 to be but the mechanism is completely
00:17:27.319 00:17:27.329 different and then lastly as we saw
00:17:29.060 00:17:29.070 especially with temperature the
00:17:30.440 00:17:30.450 parameters for the capacitor are
00:17:32.090 00:17:32.100 extremely stable we're getting much
00:17:34.190 00:17:34.200 closer to a solid device which is in a
00:17:36.260 00:17:36.270 surprise they are solid devices and so
00:17:38.360 00:17:38.370 it just makes it much easier to design
00:17:39.830 00:17:39.840 in with these parts because the range of
00:17:41.660 00:17:41.670 change is much lower well I think that's
00:17:43.820 00:17:43.830 all I have time for today thank you so
00:17:45.860 00:17:45.870 much for joining me James oh you're very
00:17:47.750 00:17:47.760 welcome Amelia I think aluminum
00:17:49.610 00:17:49.620 capacitors are very popular and I think
00:17:51.470 00:17:51.480 it's really important to understand the
00:17:52.730 00:17:52.740 difference between these two types and
00:17:54.260 00:17:54.270 before we go you didn't forget to click
00:17:56.390 00:17:56.400 that
00:17:56.830 00:17:56.840 did you there you can find out more
00:17:59.259 00:17:59.269 information about capacitors from Kemet
00:18:02.310 00:18:02.320 for chalk talks I'm Amelia Dalton from a
00:18:05.529 00:18:05.539 journal comm for more chalk talks
00:18:08.619 00:18:08.629 check out the chalk talks section of a
00:18:11.619 00:18:11.629 journal calm or head on over to youtube
00:18:15.119 00:18:15.129 keyword EEE journal
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