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In this scheme, resistance-inductance (RL) combinations form complex impedances (The term impedance comes from the root impede, and fully describes how electrical components impede, or inhibit, the flow of ac You ll learn all about this in Chap 15) Each point on the RL plane corresponds to one unique complex impedance value Conversely, each complex impedance value corresponds to one unique point on the RL plane You might ask, What s the little j doing in Fig 13-5 For reasons that will be made clear in Chap 15, impedances on the RL plane are written in the form R + jXL, where R is the resistance in ohms, and XL is the inductive reactance in ohms The little j is called a j operator and is a mathematical way of expressing the fact that reactance is denoted at right angles to resistance in compleximpedance graphs If you have a pure resistance, say R = 5 , then the complex impedance is 5 + j 0, and is at the point (5,0) on the RL plane If you have a pure inductive reactance, such as XL = 3 , then the complex impedance is 0 + j3, and is at the point (0,j3) on the RL plane These points, and a couple of others, are shown in Fig 13-6 In real life, all coils have some resistance, because no wire is a perfect conductor All resistors have at least a tiny bit of inductive reactance, because they take up some physical space and they have wire leads So there is really no such thing as a mathematically perfect pure resistance such as 5 + j 0, or a mathematically perfect pure reactance like 0 + j3 But sometimes you can get extremely close to theoretical ideals in real life Often, resistance and inductive reactance are both deliberately placed in a circuit Then you get impedances values such as 2 + j3 or 4 + j15 These are shown in Fig 13-6 as points on the RL plane Remember that values for XL are reactances, not actual inductances Because of this, they vary with the frequency in an RL circuit Changing the frequency has the effect of making complex impedance points move around in the RL plane They move vertically, going upward as the ac frequency increases, and downward as the ac frequency decreases If the ac frequency goes down to zero, the inductive reactance vanishes Then XL = 0, we have pure dc, and the point is right on the resistance axis. asp.net pdf 417 ASP . NET PDF-417 Barcode Generator - Generate 2D PDF417 in ...
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