0:00:00.000,0:00:03.660 >> Okay. Now let's talk[br]about the antenna block. 0:00:03.660,0:00:05.880 The antenna right here is what's 0:00:05.880,0:00:08.085 used to receive the signal[br]in the first place. 0:00:08.085,0:00:11.520 The antenna is a 2.4 or 2.6 0:00:11.520,0:00:15.225 gigahertz antenna so they can receive[br]both of the possible frequencies. 0:00:15.225,0:00:19.385 They come into this antenna which[br]is a quarter of a wavelength long, 0:00:19.385,0:00:24.060 and underneath there's copper[br]underneath each of these strips. 0:00:24.060,0:00:28.080 So, that this thing right here is[br]a microstrip as a transmission line. 0:00:28.080,0:00:31.530 Now, the transmission lines are[br]normally modeled like this. 0:00:31.530,0:00:35.804 Their model is a combination of[br]resistors, inductors, capacitors, 0:00:35.804,0:00:39.335 and conductors G so that[br]each little distance 0:00:39.335,0:00:42.920 along this transmission line can[br]be assumed to be a resistive, 0:00:42.920,0:00:46.090 capacitive, inductive, conductive network. 0:00:46.090,0:00:47.645 So that's a transmission line. 0:00:47.645,0:00:51.950 Okay now, as the signal is[br]received by this antenna, 0:00:51.950,0:00:54.740 the antenna has[br]a particular input impedance. 0:00:54.740,0:00:58.520 On the other side, the amplifier has[br]a particular input impedance as well, 0:00:58.520,0:01:01.080 and these two impedances[br]need to be matched at 0:01:01.080,0:01:04.535 the stub and they wouldn't be and[br]so we have to manually match them. 0:01:04.535,0:01:08.930 This thing right here is an open-circuited[br]stub that's used to impedance match 0:01:08.930,0:01:11.630 the antenna to the transmission line and 0:01:11.630,0:01:14.705 then the amplifiers also matched[br]to this transmission line. 0:01:14.705,0:01:18.080 This particular transmission line[br]is a 50 Ohm transmission line. 0:01:18.080,0:01:21.245 So, we need this antenna[br]to be matched to 50 Ohm's. 0:01:21.245,0:01:22.610 The way we do it is we have 0:01:22.610,0:01:27.545 a particular distance here and a[br]particular length of the stub. 0:01:27.545,0:01:30.290 It's literally just a little stub[br]of copper that we 0:01:30.290,0:01:33.230 cut with scissors and stuck down, 0:01:33.230,0:01:35.090 this literally stuck it right down there 0:01:35.090,0:01:37.160 so it's touching this transmission line. 0:01:37.160,0:01:39.905 The length of the stub is[br]going to make it either 0:01:39.905,0:01:43.295 capacitive or inductive depending[br]on the length of the stub. 0:01:43.295,0:01:46.970 Remember that inductors and[br]capacitors create phase shifts. 0:01:46.970,0:01:48.950 A phase shift is just a time delay. 0:01:48.950,0:01:52.460 So as a little bit of signal goes[br]up this line and comes back, 0:01:52.460,0:01:55.130 that's the time delay[br]that it experiences and 0:01:55.130,0:01:58.105 consequently the phase[br]shift that it also obtains. 0:01:58.105,0:02:00.225 So, once we get past this point, 0:02:00.225,0:02:02.570 the antenna and this combination of 0:02:02.570,0:02:07.110 impedance matching network are[br]now matched to a 50 Ohm line.