0:00:00.000,0:00:00.830 0:00:00.830,0:00:03.510 Before we move on, I want to[br]clarify something that I've 0:00:03.510,0:00:04.490 inadvertently done. 0:00:04.490,0:00:06.660 I think I was not exact[br]with some of the 0:00:06.660,0:00:07.550 terminology I used. 0:00:07.550,0:00:10.920 So I want to highlight the[br]difference between two things 0:00:10.920,0:00:12.590 that I've used almost[br]interchangeably up to this 0:00:12.590,0:00:15.100 point, but now that we are about[br]to embark on learning 0:00:15.100,0:00:18.260 what voltage is, I think it's[br]important that I highlight the 0:00:18.260,0:00:20.200 difference, because initially,[br]this can be very confusing. 0:00:20.200,0:00:23.430 I remember when I first learned[br]this, I found I often 0:00:23.430,0:00:26.680 mixed up these words and didn't[br]quite understand why 0:00:26.680,0:00:27.540 there was a difference. 0:00:27.540,0:00:31.280 So the two words are[br]electrical-- or sometimes 0:00:31.280,0:00:33.580 you'll see electric instead[br]of electrical. 0:00:33.580,0:00:49.110 So "electric potential energy"[br]and "electric potential." I 0:00:49.110,0:00:51.380 think even in the last video,[br]I used these almost 0:00:51.380,0:00:53.630 interchangeably, and I shouldn't[br]have. I really 0:00:53.630,0:00:56.500 should have always used[br]electrical or electric 0:00:56.500,0:00:57.390 potential energy. 0:00:57.390,0:00:58.850 And what's the difference? 0:00:58.850,0:01:05.379 Electrical potential energy is[br]associated with a charge. 0:01:05.379,0:01:08.830 It's associated with a particle[br]that has some charge. 0:01:08.830,0:01:12.390 Only that particle[br]can have energy. 0:01:12.390,0:01:16.520 Electrical potential, or[br]electric potential, this is 0:01:16.520,0:01:18.860 associated with a position. 0:01:18.860,0:01:23.170 So, for example, if I have a[br]charge and I know that it's at 0:01:23.170,0:01:26.720 some point with a given electric[br]potential, I can 0:01:26.720,0:01:29.590 figure out the electric[br]potential energy at that point 0:01:29.590,0:01:32.710 by just multiplying actually[br]this value by the charge. 0:01:32.710,0:01:34.970 Let me give you some examples. 0:01:34.970,0:01:38.380 Let's say that I have[br]an infinite 0:01:38.380,0:01:39.740 uniformly charged plate. 0:01:39.740,0:01:41.290 So that we don't have to do[br]calculus, we can have a 0:01:41.290,0:01:43.050 uniform electric field. 0:01:43.050,0:01:44.640 Let's say that this[br]is the plate. 0:01:44.640,0:01:47.130 I'll make it vertical just so we[br]get a little bit of change 0:01:47.130,0:01:55.760 of pace, and let's say it's[br]positively charged plate. 0:01:55.760,0:01:57.170 And let's say that the[br]electric field 0:01:57.170,0:01:59.010 is constant, right? 0:01:59.010,0:02:00.060 It's constant. 0:02:00.060,0:02:05.580 No matter what point we pick,[br]these field vectors should all 0:02:05.580,0:02:08.156 be the same length because the[br]electric field does not change 0:02:08.156,0:02:12.290 in magnitude it's pushing out,[br]because we assume when we draw 0:02:12.290,0:02:14.810 field lines that we're using a[br]test charge with a positive 0:02:14.810,0:02:16.060 charge so it's pushing[br]outward. 0:02:16.060,0:02:18.370 0:02:18.370,0:02:22.640 Let's say I have a[br]1-coulomb charge. 0:02:22.640,0:02:24.420 Actually, let me make[br]it 2 coulombs just 0:02:24.420,0:02:26.320 to hit a point home. 0:02:26.320,0:02:33.532 Say I have a 2-coulomb charge[br]right here, and it's positive. 0:02:33.532,0:02:40.750 A positive 2-coulomb charge, and[br]it starts off at 3 meters 0:02:40.750,0:02:46.430 away, and I want to bring[br]it in 2 meters. 0:02:46.430,0:02:48.560 I want to bring it in 2 meters,[br]so it's 1 meter away. 0:02:48.560,0:02:51.800 0:02:51.800,0:02:56.250 So what is the electric-- or[br]electrical-- potential energy 0:02:56.250,0:03:00.600 difference between the particle[br]at this point and at 0:03:00.600,0:03:02.200 this point? 0:03:02.200,0:03:05.270 Well, the electrical potential[br]energy difference is the 0:03:05.270,0:03:07.860 amount of work, as we've learned[br]in the previous two 0:03:07.860,0:03:11.390 videos, we need to apply to this[br]particle to take it from 0:03:11.390,0:03:12.770 here to here. 0:03:12.770,0:03:14.200 So how much work do[br]we have to apply? 0:03:14.200,0:03:21.290 We have to apply a force that[br]directly-- that exactly-- we 0:03:21.290,0:03:22.990 assume that maybe this is[br]already moving with a constant 0:03:22.990,0:03:24.840 velocity, or maybe we have to[br]start with a slightly higher 0:03:24.840,0:03:27.210 force just to get it moving, but[br]we have to apply a force 0:03:27.210,0:03:34.000 that's exactly opposite the[br]force provided by Coulomb's 0:03:34.000,0:03:37.570 Law, the electrostatic force. 0:03:37.570,0:03:40.030 And so what is that force we're[br]going to have to apply? 0:03:40.030,0:03:42.620 Well, we actually have to know[br]what the electric field is, 0:03:42.620,0:03:44.650 which I have not told you yet. 0:03:44.650,0:03:46.220 I just realized that,[br]as you can tell. 0:03:46.220,0:03:54.330 So let's say all of these[br]electric field lines are 3 0:03:54.330,0:03:57.100 newtons per coulomb. 0:03:57.100,0:04:01.260 So at any point, what is the[br]force being exerted from this 0:04:01.260,0:04:02.940 field onto this particle? 0:04:02.940,0:04:07.630 Well, the electrostatic force[br]on this particle is equal to 0:04:07.630,0:04:16.269 the electric field times the[br]charge, which is equal to-- I 0:04:16.269,0:04:19.829 just defined the electric field[br]as being 3 newtons per 0:04:19.829,0:04:25.220 coulomb times 2 coulombs. 0:04:25.220,0:04:27.000 It equals 6 newtons. 0:04:27.000,0:04:30.940 So at any point, the electric[br]field is pushing this way 6 0:04:30.940,0:04:33.416 newtons, so in order to push the[br]particle this way, I have 0:04:33.416,0:04:35.930 to completely offset that, and[br]actually, I have to get it 0:04:35.930,0:04:37.170 moving initially, and I'll[br]keep saying that. 0:04:37.170,0:04:39.570 I just want to hit[br]that point home. 0:04:39.570,0:04:42.690 So I have to apply a force of[br]6 newtons in the leftward 0:04:42.690,0:04:45.560 direction and I have to apply[br]it for 2 meters to get the 0:04:45.560,0:04:46.660 point here. 0:04:46.660,0:04:54.370 So the total work is equal to[br]6 newtons times 2 meters, 0:04:54.370,0:04:58.920 which is equal to 12[br]newton-meters or 12 joules. 0:04:58.920,0:05:04.200 So we could say that the[br]electrical potential energy-- 0:05:04.200,0:05:05.570 and energy is always joules. 0:05:05.570,0:05:07.950 The electrical potential energy[br]difference between this 0:05:07.950,0:05:10.850 point and this point[br]is 12 joules. 0:05:10.850,0:05:13.520 Or another way to say it[br]is-- and which one 0:05:13.520,0:05:14.530 has a higher potential? 0:05:14.530,0:05:16.140 Well, this one does, right? 0:05:16.140,0:05:19.610 Because at this point, we're[br]closer to the thing that's 0:05:19.610,0:05:22.170 trying to repel it, so if we[br]were to just let go, it would 0:05:22.170,0:05:25.530 start accelerating in this[br]direction, and a lot of that 0:05:25.530,0:05:27.250 energy would be converted to[br]kinetic energy by the time we 0:05:27.250,0:05:28.480 get to this point, right? 0:05:28.480,0:05:33.520 So we could also say that the[br]electric potential energy at 0:05:33.520,0:05:38.400 this point right here is 12[br]joules higher than the 0:05:38.400,0:05:41.480 electric potential energy[br]at this point. 0:05:41.480,0:05:43.680 Now that's potential energy. 0:05:43.680,0:05:46.300 What is electric potential? 0:05:46.300,0:05:51.330 Well, electric potential tells[br]us essentially how much work 0:05:51.330,0:05:55.550 is necessary per unit[br]of charge, right? 0:05:55.550,0:05:58.220 Electric potential energy was[br]just how much total work is 0:05:58.220,0:06:01.650 needed to move it from[br]here to here. 0:06:01.650,0:06:05.890 Electric potential says, per[br]unit charge, how much work 0:06:05.890,0:06:09.340 does it take to move any charge[br]per unit charge from 0:06:09.340,0:06:11.010 here to here? 0:06:11.010,0:06:14.070 Well, in our example we just[br]did, the total work to move it 0:06:14.070,0:06:15.780 from here to here[br]was 12 joules. 0:06:15.780,0:06:20.130 But how much work did it take to[br]move it from there to there 0:06:20.130,0:06:21.500 per charge? 0:06:21.500,0:06:29.640 Well, work per charge is equal[br]to 12 joules for what? 0:06:29.640,0:06:32.280 What was the charge[br]that we moved? 0:06:32.280,0:06:35.040 Well, it was 2 coulombs. 0:06:35.040,0:06:41.520 It equals 6 joules[br]per coulomb. 0:06:41.520,0:06:48.930 That is the electric potential[br]difference between this point 0:06:48.930,0:06:49.760 and this point. 0:06:49.760,0:06:51.180 So what is the distinction? 0:06:51.180,0:06:54.150 Electric potential energy was[br]associated with a particle. 0:06:54.150,0:06:57.980 How much more energy did the[br]particle have here than here? 0:06:57.980,0:07:00.140 When we say electric potential,[br]because we 0:07:00.140,0:07:03.490 essentially divide by the[br]size of the particle, it 0:07:03.490,0:07:05.720 essentially is independent of[br]the size of the particle. 0:07:05.720,0:07:07.960 It actually just depends[br]on our position. 0:07:07.960,0:07:12.130 So electric potential, we're[br]just saying how much more 0:07:12.130,0:07:15.180 potential, irrespective of the[br]charge we're using, does this 0:07:15.180,0:07:18.240 position have relative[br]to this position? 0:07:18.240,0:07:21.960 And this electric potential,[br]that's just another way of 0:07:21.960,0:07:27.980 saying voltage, and the unit[br]for voltage is volts. 0:07:27.980,0:07:30.600 So 6 joules per coulomb,[br]that's the 0:07:30.600,0:07:34.030 same thing as 6 volts. 0:07:34.030,0:07:42.060 And so if we think of the[br]analogy to gravitation, we 0:07:42.060,0:07:46.170 said gravitational potential[br]energy was mgh, right? 0:07:46.170,0:07:46.860 This was force. 0:07:46.860,0:07:49.040 This was distance, right? 0:07:49.040,0:07:52.970 Electric potential is[br]essentially the amount of 0:07:52.970,0:07:55.820 gravitational-- if we extend[br]the analogy, the amount of 0:07:55.820,0:07:58.890 gravitational potential energy[br]per mass, right? 0:07:58.890,0:08:04.500 So if we wanted a quick way of[br]knowing what the gravitational 0:08:04.500,0:08:06.640 potential is at any point[br]without having to care about 0:08:06.640,0:08:09.340 the mass, we divide by the[br]mass, and it would be the 0:08:09.340,0:08:11.130 acceleration of gravity[br]times height. 0:08:11.130,0:08:13.750 Ignore that if it[br]confused you. 0:08:13.750,0:08:15.590 So what is useful[br]about voltage? 0:08:15.590,0:08:19.650 It tells us regardless of how[br]small or big or actually 0:08:19.650,0:08:23.170 positive or negative a charge[br]is, what the difference in 0:08:23.170,0:08:26.980 potential energy would be if[br]we're at two different points. 0:08:26.980,0:08:31.390 So electric potential, we're[br]comparing points in space. 0:08:31.390,0:08:37.760 Electric potential energy, we're[br]comparing charges at 0:08:37.760,0:08:39.330 points in space. 0:08:39.330,0:08:40.789 Hopefully, I didn't[br]confuse you. 0:08:40.789,0:08:43.059 In the next video, we'll[br]actually do a couple of 0:08:43.059,0:08:45.690 problems where we figure out[br]the electric potential 0:08:45.690,0:08:48.960 difference or the voltage[br]difference between two points 0:08:48.960,0:08:51.050 in space as opposed[br]to a charge at two 0:08:51.050,0:08:52.190 different points in space. 0:08:52.190,0:08:54.760 I will see you in[br]the next video. 0:08:54.760,0:08:54.900