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NO MYTHS ALLOWED How Does Return Current Really Return? In ‘short,’ through the capacitance between the signal and return conductors. However, suppose we were to change the voltage across the capacitor. The only way we can increase the voltage into the signal conductor of a transmisacross a capacitor is if we add some additional positive sion line, it returns on the other conduccharge to the top conductor and add some negative charge tor – the return path conductor. But how to the bottom conductor. does it get to the other conductor, espeAdding negative charge to the bottom conductor is the cially if there is an insulating dielectric same as pushing out some positive charge from the bottom between the signal and return path? conductor. When voltage is increased across a capacitor, it Suppose our transmission line is a DR. ERIC BOGATIN looks like some positive charge is added to the top conduc50Ω coax cable, 10’ in length. The onetor and some negative charge pushed out from the bottom way time delay is about 15 nsec. If we conductor. From the outside, it looks like current has gone launch a 1 V signal into the line, the curthrough the capacitor. rent will be I = V/R = 1 V/50Ω = 20 mA. This 20 mA of Do we actually have positive charge carriers flowing current goes into the signal line. If at the far end of the through the insulating dielectric? No, but it sure acts that cable, we short the center conductor and outer shield, how way. The only way we get current through a capacitor is to long do we have to wait for the return current to come out change the voltage across it. of the shield conductor at the front end? When we launch a current into the signal conductor of a Most engineers might think we have to wait one roundtransmission line, how could the current flow through the trip time, or 30 nsec. After all, how can else can the current insulating dielectric to get to the return conductor? It flows launched into the signal line get back to the shield, acting as through the capacitance between the the return path, except by going down signal and return conductors. After to the end of the line and connecting all, the signal is a changing voltage. to the return path at the far-end’s Wherever that changing voltage wave short? front is, the return current is flowing For those that think the return curbetween the signal and return path rent will come back out the shield at conductors. For this reason, the signal the same instant we launch the current is not just a voltage transition propainto the signal line, think about how FIGURE 1. The return current in a transmisgating down the line; it is also a curthe current could possibly flow sion line returns through the capacitance between the signal and return conductors. rent loop between the signal and through the insulating dielectric return currents. between the signal conductor and The instantaneous impedance the signal sees is really the outer shield. How could current flow (20 mA) possibly get ratio of this transition voltage to the current loop, and for a through this insulating dielectric? It’s all about how current uniform transmission line, this ratio is constant as the signal goes through a capacitor (FIGURE 1). propagates down the line, which is why we refer to this A capacitor is composed of any two conductors with constant instantaneous impedance, this impedance that is an insulating dielectric between them. Dump some plus characteristic to the line, as the characteristic impedance of charge on one conductor and an equal amount of negative the transmission line. PCD&M charge on the other, and a voltage is generated between the conductors. The capacitance between these two conductors that Ed.: An online lecture on this topic can be viewed at make up a capacitor is a measure of the capacity of these BogEnt.com. Many of the details on this and other topics conductors to hold charge, at the price of the voltage can be found in Bogatin’s new book, Signal Integrity – between them. The more charge they can hold for the same Simplified (Prentice Hall). voltage, the higher their capacitance. Capacitance is a property of geometry. It depends only upon the physical features of the conductors and the dielectric constant of the insulation between them. It is completely independent of the voltage between the conductors. Because there is an insulting dielectric between the conDR. ERIC BOGATIN is the CTO of Synergetix (synergetix.com). ductors at DC, current cannot flow between them. The He is scheduled to speak at PCB Design Conference East in impedance of the capacitor at DC is infinite. October. He can be reached at [email protected]. WE KNOW THAT if a current is launched 20 PRINTED CIRCUIT DESIGN & MANUFACTURE AUGUST 2004