Capacitors in AC Circuits with Phasors _ Doc Physics

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Kind: captions
Language: en

00:00:00.030
hey if I hook up a capacitor to a
00:00:03.740 00:00:03.750 battery let's say I've got this D
00:00:05.690 00:00:05.700 battery here and this sides positive and
00:00:09.169 00:00:09.179 this side is negative and here I have a
00:00:10.669 00:00:10.679 parallel plate capacitor and my
00:00:13.070 00:00:13.080 intention is to put a wire between here
00:00:16.039 00:00:16.049 and then a wire between here and as soon
00:00:19.490 00:00:19.500 as I connect that see as soon as I
00:00:22.370 00:00:22.380 connect that the voltage on the
00:00:25.730 00:00:25.740 capacitor will gradually increase like
00:00:27.800 00:00:27.810 this voltage will go like this and
00:00:30.830 00:00:30.840 approach some some maximum level
00:00:33.319 00:00:33.329 probably the voltage of the battery if
00:00:35.630 00:00:35.640 this is a function of time but if I'm
00:00:37.700 00:00:37.710 going to also want to know what's
00:00:40.130 00:00:40.140 happening to the current see the current
00:00:43.270 00:00:43.280 immediately will be huge
00:00:45.470 00:00:45.480 they'll immediately be a very large
00:00:47.660 00:00:47.670 current as soon as I connect that
00:00:50.389 00:00:50.399 there'll be a huge current and then the
00:00:52.639 00:00:52.649 current will taper off and approach zero
00:00:56.510 00:00:56.520 where these guys are acting very
00:00:59.180 00:00:59.190 differently right the current in this
00:01:02.450 00:01:02.460 circuit is going to be falling to zero
00:01:04.939 00:01:04.949 and the voltage will be rising up and
00:01:06.859 00:01:06.869 and that's because we can intuitively
00:01:08.390 00:01:08.400 understand this because as soon as I
00:01:10.730 00:01:10.740 make this connection here there is no
00:01:14.000 00:01:14.010 force against the electrons initially
00:01:17.330 00:01:17.340 going this direction there's no force
00:01:19.640 00:01:19.650 initially against the current going that
00:01:21.170 00:01:21.180 direction but as the capacitor becomes
00:01:22.760 00:01:22.770 more and more charged than the voltage
00:01:24.530 00:01:24.540 difference between the capacitor and the
00:01:26.210 00:01:26.220 battery is approaching zero because well
00:01:28.580 00:01:28.590 the voltage of the and the voltage of
00:01:31.249 00:01:31.259 the capacitor is approaching the voltage
00:01:32.630 00:01:32.640 of the battery so we want to think now
00:01:35.660 00:01:35.670 about what happens if instead we connect
00:01:38.480 00:01:38.490 a capacitor to an alternating source I'm
00:01:43.399 00:01:43.409 going to connect a capacitor to an AC
00:01:45.710 00:01:45.720 source and I want you to think about
00:01:48.139 00:01:48.149 what this means
00:01:49.190 00:01:49.200 see if I connect it to a DC source then
00:01:54.050 00:01:54.060 the capacitor actually looks like a
00:01:55.760 00:01:55.770 break in the circuit it will just
00:01:57.050 00:01:57.060 prevent any current from flowing but if
00:02:00.289 00:02:00.299 I connect it to a very fast AC source
00:02:02.330 00:02:02.340 it's almost as if the capacitor isn't
00:02:04.130 00:02:04.140 there because as soon as I begin to
00:02:05.569 00:02:05.579 charge the capacitor the current from
00:02:07.670 00:02:07.680 the source changes directions and then
00:02:10.100 00:02:10.110 discharges it and can charge it and
00:02:11.960 00:02:11.970 discharge it and charge and discharge it
00:02:13.760 00:02:13.770 so it's just as if there were a wire
00:02:15.380 00:02:15.390 right here so let me summarize that
00:02:17.300 00:02:17.310 little observation I will say at oh and
00:02:20.540 00:02:20.550 of course I'm going to use Omega to
00:02:23.930 00:02:23.940 symbolize how fast I'm sloshing right
00:02:26.540 00:02:26.550 here this is the frequency the angular
00:02:29.450 00:02:29.460 frequency of my of my AC power source at
00:02:33.680 00:02:33.690 low Omega capacitors look like what and
00:02:43.970 00:02:43.980 at high Omega this is very important so
00:02:47.690 00:02:47.700 I'm going to ask you to fill those in
00:02:48.950 00:02:48.960 you have to think about what it means
00:02:50.710 00:02:50.720 capacitors and I don't need to say look
00:02:54.770 00:02:54.780 I could say they act like what in a
00:03:02.540 00:03:02.550 circuit this is very important to think
00:03:07.970 00:03:07.980 about in a DC circuit a capacitor looks
00:03:11.150 00:03:11.160 like a break in the circuit and so at
00:03:14.150 00:03:14.160 low Omega that's what capacitors look
00:03:16.010 00:03:16.020 like it looks as if the circuit is
00:03:17.690 00:03:17.700 broken but at high omegas sloshing back
00:03:20.750 00:03:20.760 and forth shoo-shoo shoo-shoo the
00:03:22.490 00:03:22.500 capacitor doesn't affect the sloshing at
00:03:24.920 00:03:24.930 all assuming the capacitor is large
00:03:26.870 00:03:26.880 enough right so that it doesn't reach
00:03:28.670 00:03:28.680 its maximum voltage very quickly
00:03:30.110 00:03:30.120 capacitors that are tiny reach the
00:03:32.090 00:03:32.100 maximum voltage very quickly and could
00:03:33.740 00:03:33.750 still impede the flow of charge through
00:03:36.050 00:03:36.060 this part of the circuit of course there
00:03:37.760 00:03:37.770 aren't actually charges going that
00:03:39.800 00:03:39.810 direction or that direction it's just
00:03:42.230 00:03:42.240 everywhere along here and everywhere
00:03:43.880 00:03:43.890 along here so as long as you're outside
00:03:45.320 00:03:45.330 the capacitor it looks as if there's
00:03:47.120 00:03:47.130 just a wire right there so here we put
00:03:49.640 00:03:49.650 wire and there we put break or here you
00:03:52.190 00:03:52.200 could put short and here you could put
00:03:53.720 00:03:53.730 break a break in a shorter very
00:03:55.100 00:03:55.110 different things think about that for a
00:03:56.720 00:03:56.730 moment now as we go into this we're
00:03:59.600 00:03:59.610 going to have to do a little bit of
00:04:00.680 00:04:00.690 thumb we're going to have to do a little
00:04:03.140 00:04:03.150 bit of calculus and I think that's
00:04:04.400 00:04:04.410 probably very good for us so let's do it
00:04:05.990 00:04:06.000 you know that the voltage across a
00:04:08.360 00:04:08.370 capacitor is the charge on the capacitor
00:04:10.699 00:04:10.709 divided by its capacitance and this
00:04:13.670 00:04:13.680 charge is actually the integral of the
00:04:15.800 00:04:15.810 current going into the capacitor so as
00:04:18.500 00:04:18.510 current goes into a capacitor it fills
00:04:20.510 00:04:20.520 up the capacitor and that's what gives
00:04:22.580 00:04:22.590 the capacitor charge on its positive
00:04:24.740 00:04:24.750 plate so let's write that of again the
00:04:26.659 00:04:26.669 voltage on the capacitor
00:04:27.629 00:04:27.639 charge / capacitance so that's going to
00:04:30.959 00:04:30.969 be well it's going to be the integral
00:04:33.570 00:04:33.580 well it'll be one over C times the
00:04:35.399 00:04:35.409 integral of current over time and with
00:04:38.490 00:04:38.500 my AC generator now I'm going to say
00:04:41.129 00:04:41.139 that I have current that does depend on
00:04:44.070 00:04:44.080 time and I'm going to say that the
00:04:46.679 00:04:46.689 current is well this is current as a
00:04:49.890 00:04:49.900 function of time it's going to be IMAX
00:04:51.929 00:04:51.939 times the sine of Omega times T that's
00:04:56.520 00:04:56.530 my current I plug that in right there
00:04:58.619 00:04:58.629 and see what happens it's going to be
00:05:01.499 00:05:01.509 some really enjoyable calculus 1 over C
00:05:05.129 00:05:05.139 times the integral of IMAX times the
00:05:09.959 00:05:09.969 sine of Omega T over time IMAX as a
00:05:15.450 00:05:15.460 constant and pulls out and we just have
00:05:17.399 00:05:17.409 to do the integral of the sine of Omega
00:05:19.769 00:05:19.779 T it gives us the negative cosine and
00:05:21.869 00:05:21.879 then we have to do the chain rule for
00:05:23.490 00:05:23.500 integrals oh man so we get negative IMAX
00:05:30.529 00:05:30.539 over C and and then we have cosine of
00:05:36.529 00:05:36.539 Omega T and we've also got to note what
00:05:40.800 00:05:40.810 the integral of that sucker is and that
00:05:44.159 00:05:44.169 would be oh man I think I'm going to get
00:05:46.260 00:05:46.270 divided by Omega right here so that's
00:05:50.249 00:05:50.259 really lovely and I could write it just
00:05:52.980 00:05:52.990 slightly differently I'm going to write
00:05:54.659 00:05:54.669 it as oh gosh well this is negative
00:05:57.779 00:05:57.789 cosine here but I happen to know that
00:06:00.209 00:06:00.219 negative cosine of theta is the sine of
00:06:03.929 00:06:03.939 theta this is spelled this is really
00:06:05.610 00:06:05.620 lovely sine of theta minus PI by 2 all
00:06:10.740 00:06:10.750 right so that's a substitution I'm about
00:06:13.170 00:06:13.180 to use and I'm just going to clean
00:06:14.429 00:06:14.439 things up a little bit I'm going to say
00:06:16.019 00:06:16.029 that this is 1 over Omega times C times
00:06:21.329 00:06:21.339 the maximum current possible times the
00:06:25.649 00:06:25.659 sine of well what do we have to put we
00:06:29.279 00:06:29.289 have to put Omega t minus PI over 2
00:06:35.249 00:06:35.259 this equation is a very powerful
00:06:37.110 00:06:37.120 equation we call this constant here
00:06:40.820 00:06:40.830 phase-shift and thats related to the
00:06:43.290 00:06:43.300 term fazer of course and what we're
00:06:46.320 00:06:46.330 seeing is that the fazer for voltage is
00:06:50.160 00:06:50.170 not facing the same direction as the
00:06:53.100 00:06:53.110 fazer for the current so first of all we
00:06:57.690 00:06:57.700 can identify some maximum values when
00:07:00.240 00:07:00.250 the sine function is at a maximum it
00:07:02.130 00:07:02.140 just disappears it becomes 1 so then we
00:07:04.320 00:07:04.330 say that V cap is 1 over Omega C times
00:07:08.570 00:07:08.580 IMAX on the cap so that would be the
00:07:11.910 00:07:11.920 maximum voltage so I can say V Max is 1
00:07:16.560 00:07:16.570 over Omega C times IMAX I hope that you
00:07:20.550 00:07:20.560 believed that particular observation and
00:07:23.490 00:07:23.500 I want to make a substitution also
00:07:25.950 00:07:25.960 because I like I mean it's one of my
00:07:28.470 00:07:28.480 favorite electrical equations I like the
00:07:30.750 00:07:30.760 idea of a resistor where V is I times R
00:07:34.650 00:07:34.660 and for a resistor we also find that V
00:07:37.470 00:07:37.480 Max is I max times the resistance of the
00:07:41.010 00:07:41.020 resistor so what if capacitor is acted
00:07:43.500 00:07:43.510 kind of like resistors and and they sort
00:07:46.140 00:07:46.150 of do because they are sometimes able to
00:07:49.470 00:07:49.480 act like a line in the circuit a short
00:07:52.590 00:07:52.600 circuit sometimes they're able to act
00:07:54.420 00:07:54.430 like a break in the circuit so that's
00:07:56.250 00:07:56.260 sort of a resistance it's not exactly a
00:07:59.310 00:07:59.320 resistance we call it a reactance so I
00:08:02.880 00:08:02.890 want to say that this is V V is equal to
00:08:06.570 00:08:06.580 I times something so I'm going to define
00:08:08.910 00:08:08.920 1 over Omega C to be the reactance of a
00:08:13.590 00:08:13.600 capacitor and it's abbreviated with the
00:08:15.300 00:08:15.310 letter X this is the reactance of the
00:08:17.430 00:08:17.440 capacitor and you'll find that it
00:08:18.900 00:08:18.910 actually has the same units of
00:08:20.340 00:08:20.350 resistance this is radians per second
00:08:22.380 00:08:22.390 and that is the capacitance in farad's
00:08:24.450 00:08:24.460 and you get units of ohms Wow go figure
00:08:28.200 00:08:28.210 try that out it's really beautiful so we
00:08:30.270 00:08:30.280 have this analogy of Ohm's law for well
00:08:34.770 00:08:34.780 we can write it here the analogy of
00:08:36.510 00:08:36.520 Ohm's law for capacitors is that voltage
00:08:39.480 00:08:39.490 on a capacitor is and sorry I have to
00:08:44.490 00:08:44.500 put Max's in here or rms is in here
00:08:46.740 00:08:46.750 because it's not an instantaneous
00:08:49.020 00:08:49.030 equation at all it's going to be I
00:08:51.990 00:08:52.000 max times the reactive capacitance now
00:08:57.329 00:08:57.339 my next plan is to show you how this
00:09:00.449 00:09:00.459 works we've got we've got no I'm gonna
00:09:04.619 00:09:04.629 have to use a different page because
00:09:05.670 00:09:05.680 this is really important stuff um I'll
00:09:08.579 00:09:08.589 set up my axes and I've got Y and X and
00:09:11.280 00:09:11.290 this is where my phasor is going to live
00:09:12.900 00:09:12.910 before I go on though I want to remind
00:09:15.300 00:09:15.310 you this is what the phasor of a
00:09:16.949 00:09:16.959 resistor looks like starts here and if
00:09:19.470 00:09:19.480 the voltage is max then the current
00:09:21.269 00:09:21.279 through the resistor will be max at that
00:09:22.559 00:09:22.569 same time so right now I'm saying what
00:09:24.929 00:09:24.939 does the y-component gives the value the
00:09:32.699 00:09:32.709 Y component of the phasor at any instant
00:09:34.980 00:09:34.990 in time gives the actual value of that
00:09:36.990 00:09:37.000 variable so right now I've got no y
00:09:39.150 00:09:39.160 component for anything
00:09:40.050 00:09:40.060 and now I've got maximum remember this
00:09:42.840 00:09:42.850 is this is everything here is rotating
00:09:46.050 00:09:46.060 at Omega so that's the frequency of my
00:09:49.889 00:09:49.899 power source and as I reach this point
00:09:53.129 00:09:53.139 right here I get maximum value for
00:09:55.800 00:09:55.810 current and maximum value for voltage
00:09:57.900 00:09:57.910 and that's a resistor and then I get
00:10:00.329 00:10:00.339 none and then I get negative current and
00:10:04.530 00:10:04.540 negative voltage right because you're
00:10:07.230 00:10:07.240 pushing the other way it's going the
00:10:08.460 00:10:08.470 other way and then I get none again and
00:10:10.769 00:10:10.779 so if I draw this graph for a resistor
00:10:15.949 00:10:15.959 I'm going to find that the voltage might
00:10:19.230 00:10:19.240 do this and the current one we want to
00:10:24.929 00:10:24.939 use for current let's use orange for
00:10:26.280 00:10:26.290 current the current would do this for
00:10:28.980 00:10:28.990 instance where these guys have the same
00:10:34.170 00:10:34.180 time dependence and they are we can call
00:10:36.329 00:10:36.339 these in phase and they differ only by
00:10:41.819 00:10:41.829 this this Ohm's law relationship this is
00:10:45.660 00:10:45.670 going to be let's see this is V and this
00:10:49.499 00:10:49.509 level is the Max and the orange is I and
00:10:55.639 00:10:55.649 this value here is I max and we can
00:11:01.199 00:11:01.209 define I max by Ohm's law these
00:11:04.110 00:11:04.120 are so I is V over our IMAX is going to
00:11:08.340 00:11:08.350 be V Max divided by the resistance of my
00:11:11.430 00:11:11.440 resistor it's time to go to capacitors
00:11:14.430 00:11:14.440 though so resistors are really really
00:11:16.350 00:11:16.360 Pleasant
00:11:16.829 00:11:16.839 everybody likes resistors because
00:11:18.180 00:11:18.190 they're super simple it's time to go to
00:11:20.760 00:11:20.770 capacitors and in a capacitor let me get
00:11:23.550 00:11:23.560 you the same idea of a graph in a
00:11:26.400 00:11:26.410 capacitor graph if the voltage starts
00:11:29.820 00:11:29.830 out well let's see I'm actually going to
00:11:32.550 00:11:32.560 say that the voltage on the capacitor is
00:11:34.560 00:11:34.570 going to start out I mean it really
00:11:36.930 00:11:36.940 doesn't matter where start will just
00:11:37.890 00:11:37.900 start you let you go voltage big voltage
00:11:42.540 00:11:42.550 small I'm zooming in a little bit I
00:11:44.610 00:11:44.620 changed my angular frequency so that you
00:11:46.410 00:11:46.420 can study this a little bit better so
00:11:47.970 00:11:47.980 this is my voltage and this is all as a
00:11:51.780 00:11:51.790 function of time sorry I should have
00:11:53.130 00:11:53.140 labeled that up there now the
00:11:55.290 00:11:55.300 interesting thing about a capacitor is
00:11:57.000 00:11:57.010 that if you have a large voltage across
00:12:00.840 00:12:00.850 the capacitor then that's when the
00:12:03.750 00:12:03.760 current actually stops so let's go back
00:12:06.300 00:12:06.310 to this diagram right here as I'm
00:12:08.130 00:12:08.140 putting a really large voltage across
00:12:10.079 00:12:10.089 the capacitor that means the capacitor
00:12:11.880 00:12:11.890 is fully charged because Q is CV and
00:12:15.690 00:12:15.700 when Q reaches a maximum that means the
00:12:17.699 00:12:17.709 capacitor is going to be impeding the
00:12:19.680 00:12:19.690 flow of charge you won't have any charge
00:12:22.820 00:12:22.830 flowing at that time so the current is
00:12:26.280 00:12:26.290 zero when the voltage reaches a maximum
00:12:29.820 00:12:29.830 and we can also argue that the current
00:12:32.970 00:12:32.980 is zero when the voltage reaches a
00:12:35.310 00:12:35.320 minimum so we're going to have these
00:12:36.630 00:12:36.640 zeros right here I want to also say that
00:12:40.920 00:12:40.930 if the if the voltage is decreasing then
00:12:46.890 00:12:46.900 you can imagine that will be what are we
00:12:49.590 00:12:49.600 doing here this is going to be a graph
00:12:51.000 00:12:51.010 of current ultimately and I'm going to
00:12:53.610 00:12:53.620 say that the current will be going the
00:12:57.090 00:12:57.100 opposite direction as the voltage
00:12:59.190 00:12:59.200 decreases so there we've got voltage at
00:13:02.190 00:13:02.200 a peak and the current now is going
00:13:04.530 00:13:04.540 below zero and then it comes up and goes
00:13:08.940 00:13:08.950 above zero and comes down and goes below
00:13:11.610 00:13:11.620 zero and comes up and goes above zero so
00:13:15.540 00:13:15.550 you've got this very interesting pattern
00:13:18.030 00:13:18.040 notice in this case we can look at in
00:13:19.889 00:13:19.899 terms of current the current is a
00:13:21.660 00:13:21.670 minimum when the voltage across the
00:13:23.879 00:13:23.889 capacitor is zero and the current is
00:13:26.879 00:13:26.889 zero when the voltage across the
00:13:28.379 00:13:28.389 capacitor is very negative
00:13:30.180 00:13:30.190 if the voltage across the capacitor is
00:13:32.550 00:13:32.560 very negative then you can bet that that
00:13:35.160 00:13:35.170 will induce a current to start going the
00:13:37.199 00:13:37.209 other direction so it's sloshing Chuchu
00:13:39.509 00:13:39.519 Chuchu
00:13:40.139 00:13:40.149 but the key fact is that they are out of
00:13:43.170 00:13:43.180 phase we've already seen that they're
00:13:45.780 00:13:45.790 out of phase I want to remind you that
00:13:47.639 00:13:47.649 they're out of phase by this equation
00:13:49.170 00:13:49.180 right here it says the voltage on a
00:13:50.759 00:13:50.769 capacitor is the current max on the
00:13:54.120 00:13:54.130 capacitor with this stuff right here
00:13:56.280 00:13:56.290 this reactance but it's out of phase of
00:13:59.400 00:13:59.410 the same Omega it's minus PI over 2 or
00:14:02.610 00:14:02.620 90 degrees or it's a quarter revolution
00:14:05.400 00:14:05.410 out of phase that's what it means to be
00:14:07.680 00:14:07.690 a quarter revolution out of phase these
00:14:09.180 00:14:09.190 guys are in phase and these guys are a
00:14:11.220 00:14:11.230 quarter out of phase so I'll say PI by
00:14:13.889 00:14:13.899 two out of phase hi Kira and if I take
00:14:21.150 00:14:21.160 this capacitor phase or you see that
00:14:25.199 00:14:25.209 initially if I start it out like this I
00:14:28.680 00:14:28.690 didn't actually start it out like this
00:14:29.850 00:14:29.860 but look at this instant right here this
00:14:32.040 00:14:32.050 is the instant right here
00:14:33.449 00:14:33.459 where the voltage that's my purple is a
00:14:35.819 00:14:35.829 oh no sorry this is maximum current oh
00:14:38.819 00:14:38.829 that is right there yeah good so I get
00:14:40.650 00:14:40.660 maximum current initially before the
00:14:43.139 00:14:43.149 capacitor is charged right and there's
00:14:45.900 00:14:45.910 no voltage on the capacitor as I start
00:14:47.550 00:14:47.560 so I start charging the capacitor
00:14:49.470 00:14:49.480 there's a huge current and the voltage
00:14:52.189 00:14:52.199 rises up as I'm going to here the
00:14:55.110 00:14:55.120 voltage is rising up because I'm
00:14:56.910 00:14:56.920 charging my capacitor boom now the
00:15:00.360 00:15:00.370 capacitor is fully charged so the
00:15:02.069 00:15:02.079 voltage is huge but the current has
00:15:04.110 00:15:04.120 dropped to zero because the capacitor is
00:15:05.879 00:15:05.889 fully charged and the power supply
00:15:07.650 00:15:07.660 starts and no let's go the other
00:15:10.230 00:15:10.240 direction so the current actually starts
00:15:12.240 00:15:12.250 unloading going away from the capacitor
00:15:14.790 00:15:14.800 and back towards the power supply and
00:15:17.040 00:15:17.050 that's here right now and now we have no
00:15:20.460 00:15:20.470 voltage C the Y component of this phasor
00:15:23.819 00:15:23.829 right here is at zero but we have a very
00:15:26.970 00:15:26.980 negative current and if we continue
00:15:28.920 00:15:28.930 going counterclockwise
00:15:30.990 00:15:31.000 right here for instance we've got no
00:15:33.390 00:15:33.400 current but we've got a very very
00:15:35.730 00:15:35.740 negative voltage and as I continue
00:15:38.190 00:15:38.200 spinning this around you see how these
00:15:39.720 00:15:39.730 two things interact which one is leading
00:15:41.850 00:15:41.860 would you say that the current is
00:15:44.520 00:15:44.530 leading the voltage or that the voltage
00:15:47.820 00:15:47.830 is leading the current now take that
00:15:50.910 00:15:50.920 answer that you got right there the
00:15:52.740 00:15:52.750 voltage leading the current and the
00:15:53.880 00:15:53.890 current leading the voltage and see what
00:15:56.250 00:15:56.260 you think if you look at this which one
00:15:57.930 00:15:57.940 of these does it look like is leading
00:15:59.780 00:15:59.790 does it look like the voltage is leading
00:16:01.890 00:16:01.900 here or the current is leading I mean I
00:16:03.870 00:16:03.880 guess if it's erased that direction then
00:16:05.640 00:16:05.650 it looks like the voltage is leading but
00:16:07.140 00:16:07.150 it's not what we're doing is we're
00:16:08.850 00:16:08.860 scrolling across this so we're saying at
00:16:11.370 00:16:11.380 this instant right here we've got that
00:16:13.050 00:16:13.060 and then oh man see that's going down
00:16:15.210 00:16:15.220 and now that's going up which one looks
00:16:18.000 00:16:18.010 like it's leading now it looks to me
00:16:20.460 00:16:20.470 like the orange is leading because the
00:16:22.620 00:16:22.630 orange leaps up and then the purple is
00:16:24.210 00:16:24.220 like okay we can go up and then the
00:16:26.010 00:16:26.020 orange shoots down the Purple's like
00:16:27.450 00:16:27.460 okay we can go down and then the orange
00:16:29.220 00:16:29.230 shoots up and purple says okay we can go
00:16:31.320 00:16:31.330 up all right so that's why it's
00:16:33.300 00:16:33.310 consistent to say that the voltage lags
00:16:36.210 00:16:36.220 the current for a capacitor and that
00:16:38.610 00:16:38.620 will be our final statement here voltage
00:16:42.829 00:16:42.839 lags current by a phase shift of PI over
00:16:50.250 00:16:50.260 2 they are 90 degrees out of phase I'm
00:16:54.210 00:16:54.220 gonna go get some lunch I think you
00:16:55.740 00:16:55.750 should have some
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