0:00:00.000,0:00:03.810 >> Hello, this is Dr. Cynthia Furse at the University of Utah. 0:00:03.810,0:00:07.305 Today, I'd like to do an Introduction to Capacitors. 0:00:07.305,0:00:11.430 Let's talk about what is capacitance and how it relates to current and charges, 0:00:11.430,0:00:13.110 what are the effects of the parameters of 0:00:13.110,0:00:16.440 the capacitor and what does it do to voltage and current? 0:00:16.440,0:00:20.600 A capacitor is a passive element that stores energy in the electric field. 0:00:20.600,0:00:22.380 This means that it does not require 0:00:22.380,0:00:25.245 an external voltage source in order to act like a capacitor. 0:00:25.245,0:00:27.945 Remember that it is actually storing energy. 0:00:27.945,0:00:30.660 The capacitance, which you remember from physics, 0:00:30.660,0:00:35.265 of a parallel plate is epsilon A over d. Epsilon is the dielectric material. 0:00:35.265,0:00:38.415 It is a constant epsilon knot times epsilon r. 0:00:38.415,0:00:40.910 The smallest epsilon r is one for air and 0:00:40.910,0:00:43.795 a large epsilon r would be something like 80 for water. 0:00:43.795,0:00:46.435 Plastics, glasses, et cetera are very close to air. 0:00:46.435,0:00:47.780 Maybe there epsilon value is 0:00:47.780,0:00:52.535 about two or even four and things that are getting closer to water would be more like 80. 0:00:52.535,0:00:56.375 When epsilon increases, their capacitance increases. 0:00:56.375,0:01:00.080 A is the area of the two plates that's the part that's actually is parallel between them. 0:01:00.080,0:01:01.730 So, as I increase that area, 0:01:01.730,0:01:05.720 the capacitance increases and as I decrease the distance of the place, 0:01:05.720,0:01:08.310 the capacitance would also increase. 0:01:08.740,0:01:11.915 Capacitors effect that flow of charges. 0:01:11.915,0:01:15.515 The current is the change of charge dq dt. 0:01:15.515,0:01:19.025 So, it's how much charge changes over a period of time. 0:01:19.025,0:01:21.650 The way this works is charges flow from 0:01:21.650,0:01:24.535 the positive voltage source onto the top of the capacitor. 0:01:24.535,0:01:29.945 They are stored there, they get hung up there, and then they force positive charges 0:01:29.945,0:01:32.780 away from the bottom plate leaving the bottom plate negatively 0:01:32.780,0:01:35.960 charged and the top plate positively charged, 0:01:35.960,0:01:37.310 that creates a voltage difference. 0:01:37.310,0:01:39.875 That allows us to be able to do work. 0:01:39.875,0:01:44.360 Displacement current is the current that appears between the two plates. 0:01:44.360,0:01:46.340 You're more familiar with conduction current. 0:01:46.340,0:01:48.440 Conduction current is actually the flow of charges. 0:01:48.440,0:01:52.550 The fact that these charges are flowing or moving that's conducting electricity. 0:01:52.550,0:01:55.100 But then right here between the two plates, 0:01:55.100,0:01:58.970 it looks like there should be no current because there are no charges that can move. 0:01:58.970,0:02:01.265 But the electric field forcing the charges 0:02:01.265,0:02:04.160 makes a current that we called displacement current. 0:02:04.160,0:02:07.010 It's the appearance that acts like there's a flow of charges, even though 0:02:07.010,0:02:10.205 there aren't actually charges flowing in between the two plates. 0:02:10.205,0:02:13.130 Again remember, that the conduction current is 0:02:13.130,0:02:17.600 calculated as the change of charge divided by time. 0:02:17.600,0:02:21.200 So, what does it mean when we talk about epsilon A over d? 0:02:21.200,0:02:23.825 Of course a larger A can store more charges. 0:02:23.825,0:02:28.580 Epsilon means that the attraction between the two charges or the ability to set up 0:02:28.580,0:02:31.820 this strong electric field increases with larger epsilon and 0:02:31.820,0:02:36.130 d of course means that it reduces the attraction between the two charges. 0:02:36.130,0:02:38.220 How can we build with this? 0:02:38.220,0:02:40.700 So, here's a simple parallel plate capacitor. 0:02:40.700,0:02:43.970 Let's suppose that we wanted to be able to use these as a sensor. 0:02:43.970,0:02:47.060 Let's consider two metal pieces with foam in between them. 0:02:47.060,0:02:49.340 If we switched them or push them together, 0:02:49.340,0:02:52.175 we'd be changing d, there would be change in the capacitance. 0:02:52.175,0:02:53.870 If we split them back and forth, 0:02:53.870,0:02:56.060 that would be changing the effective area because 0:02:56.060,0:02:58.820 the area is only this where they are overlapping. 0:02:58.820,0:03:01.580 Then, if wet them off with some other material between it, 0:03:01.580,0:03:03.125 we'll be changing the epsilon. 0:03:03.125,0:03:06.115 That's how we can use capacitors as sensors. 0:03:06.115,0:03:10.490 So basically, we talked about what is capacitance and how does it relate to 0:03:10.490,0:03:14.930 current and charges and the effect of epsilon A and d. In the next video, 0:03:14.930,0:03:19.270 we're going to talk about what this does to current and voltage.