0:00:00.000,0:00:03.480 >> Now, let's consider how we combine 0:00:03.480,0:00:07.935 impedances that are connected in[br]either series or in parallel. 0:00:07.935,0:00:10.290 We might get a hint from[br]the fact that because 0:00:10.290,0:00:12.420 impedances have the units of ohms, 0:00:12.420,0:00:14.640 we would expect them to combine in 0:00:14.640,0:00:16.680 exactly the same way that resistances 0:00:16.680,0:00:19.185 do and we're going to see[br]that is in fact the case. 0:00:19.185,0:00:24.390 So for example, we've got Z_1 and Z_2[br]connected in series with each other. 0:00:24.390,0:00:32.235 The equivalent impedance Z equivalent[br]is just equal to Z_1 plus Z_2. 0:00:32.235,0:00:35.040 So Z_1 equals 3 plus J_2. 0:00:35.040,0:00:39.050 Three being the real part sometimes[br]referred to as the resistance, 0:00:39.050,0:00:45.275 and J_2 the imaginary part also[br]sometimes referred to as the reactants. 0:00:45.275,0:00:49.835 A second impedance Z_2 equaling 5 minus J, 0:00:49.835,0:00:52.490 then the equivalent impedance of[br]those two connected in series 0:00:52.490,0:00:57.960 will simply be 3 plus J_2 plus 5, 0:00:57.960,0:01:02.265 minus J, which equals 3 plus five is 8. 0:01:02.265,0:01:07.375 J_2 minus J_1 is plus J. 0:01:07.375,0:01:09.710 That's its rectangular form, 0:01:09.710,0:01:12.520 and we can also write[br]that it is parallel form, 0:01:12.520,0:01:18.580 which would give us then[br]8.06 for the magnitude E to 0:01:18.580,0:01:24.990 the J at 7.103. 0:01:24.990,0:01:27.875 All right, now let's look[br]at these two in parallel. 0:01:27.875,0:01:32.225 In parallel, it turns out that as[br]it was with resistance is also 0:01:32.225,0:01:38.580 1 over Z_eq is equal to 1 over Z_1, 0:01:38.580,0:01:42.750 plus 1 over Z_2. 0:01:42.750,0:01:45.730 Now, sometimes we refer[br]to instead of impedances, 0:01:45.730,0:01:53.330 we'll refer to admittances where admittance[br]is called y is equal to 1 over Z. 0:01:53.330,0:02:04.170 So in this case, we could say then[br]that Y_eq equals Y_1, plus Y_2. 0:02:04.540,0:02:08.720 All right. Let's just simplify[br]this in terms of impedances. 0:02:08.720,0:02:11.850 We know then that 1 over Z_eq. 0:02:12.940,0:02:15.530 We need to combine these two terms to get 0:02:15.530,0:02:18.210 the common denominator or to get[br]a common denominator to combine them. 0:02:18.210,0:02:22.055 So it would be the common denominator[br]would be Z_1 times Z_2, 0:02:22.055,0:02:26.520 and in the numerator[br]would have Z_2 plus Z_1. 0:02:27.560,0:02:31.200 Thus that now we can invert them, 0:02:31.200,0:02:38.700 and we get Z_eq is equal[br]to Z_1 Z_2 over Z_1, 0:02:38.700,0:02:41.030 plus Z_2 or the 0:02:41.030,0:02:43.850 product of the impedances divided[br]by the sum of the impedances. 0:02:43.850,0:02:47.570 I'll leave it to you to go ahead[br]and plug in Z_1 and Z_2 on these, 0:02:47.570,0:02:51.905 but let me just give you that[br]for these values of Z_1 and Z_2, 0:02:51.905,0:02:54.730 we get Z_eq is equal to 0:02:54.730,0:03:04.635 2.2 plus 0.6J in rectangular coordinates, 0:03:04.635,0:03:07.040 and in parallel coordinates that turns 0:03:07.040,0:03:09.515 out to be around a site[br]in polar coordinates. 0:03:09.515,0:03:14.630 That turns out to be 2.28 e to 0:03:14.630,0:03:23.100 the positive J15.3 degrees.