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Linear Algebra, 2020a

Linear Algebra, 2020a

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Topic: Analyzing Networks 77<br />

is equal to the flow times the resistance. Potential is measured in volts, the<br />

rate of flow is in amperes, and resistance to the flow is in ohms; these units are<br />

defined so that volts = amperes · ohms.<br />

Components with this property, that the voltage-amperage response curve is<br />

a line through the origin, are resistors. (Not every component has this property.<br />

For instance, as the light bulbs shown above heat up, their ohmage changes.) An<br />

example is that if a resistor measures 2 ohms then wiring it to a 12 volt battery<br />

results in a flow of 6 amperes. Conversely, if electrical current of 2 amperes flows<br />

through that resistor then there must be a 4 volt potential difference between<br />

its ends. This is the voltage drop across the resistor. One way to think of the<br />

electrical circuits that we consider here is that the battery provides a voltage<br />

rise while the other components are voltage drops.<br />

The facts that we need about networks are Kirchoff’s Current Law, that for<br />

any point in a network the flow in equals the flow out and Kirchoff’s Voltage<br />

Law, that around any circuit the total drop equals the total rise.<br />

We start with the network below. It has a battery that provides the potential<br />

to flow and three resistors, shown as zig-zags. When components are wired one<br />

after another, as here, they are in series.<br />

20 volt<br />

potential<br />

2 ohm<br />

resistance<br />

3 ohm<br />

resistance<br />

5 ohm<br />

resistance<br />

By Kirchoff’s Voltage Law, because the voltage rise is 20 volts, the total voltage<br />

drop must also be 20 volts. Since the resistance from start to finish is 10 ohms<br />

(the resistance of the wire connecting the components is negligible), the current<br />

is (20/10) =2 amperes. Now, by Kirchhoff’s Current Law, there are 2 amperes<br />

through each resistor. Therefore the voltage drops are: 4 volts across the 2 ohm<br />

resistor, 10 volts across the 5 ohm resistor, and 6 volts across the 3 ohm resistor.<br />

The prior network is simple enough that we didn’t use a linear system but<br />

the next one is more complicated. Here the resistors are in parallel.<br />

20 volt 12 ohm 8 ohm<br />

We begin by labeling the branches as below. Let the current through the left<br />

branch of the parallel portion be i 1 and that through the right branch be i 2 ,

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