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Linear Algebra

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72 Chapter 1. <strong>Linear</strong> Systems<br />

Topic: Analyzing Networks<br />

This is the diagram of an electrical circuit. It happens to describe some of the<br />

connections between a car’s battery and lights, but it is typical of such diagrams.<br />

To read it, we can think of the electricity as coming out of one end of the battery<br />

(labeled 6V OR 12V), flowing through the wires (drawn as straight lines to make<br />

the diagram more readable), and back into the other end of the battery. If, in<br />

making its way from one end of the battery to the other through the network of<br />

wires, some electricity flows through a light bulb (drawn as a circle enclosing a<br />

loop of wire), then that light lights. For instance, when the driver steps on the<br />

brake at point A then the switch makes contact and electricity flows through<br />

the brake lights at point B.<br />

This network of connections and components is complicated enough that to<br />

analyze it — for instance, to find out how much electricity is used when both<br />

the headlights and the brake lights are on — then we need systematic tools.<br />

One such tool is linear systems. To illustrate this application, we first need a<br />

few facts about electricity and networks.<br />

The two facts that we need about electricity concern how the electrical components<br />

act. First, the battery is like a pump for electricity; it provides a force<br />

or push so that the electricity will flow, if there is at least one available path for<br />

it. The second fact about the components is the observation that (in the materials<br />

commonly used in components) the amount of current flow is proportional<br />

to the force pushing it. For each electrical component there is a constant of<br />

proportionality, called its resistance, satisfying that potential = flow·resistance.<br />

(The units are: potential to flow is described in volts, the rate of flow itself is<br />

given in amperes, and resistance to the flow is in ohms. These units are set up<br />

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

For example, suppose a bulb has a resistance of 25 ohms. Wiring its ends<br />

to a battery with 12 volts results in a flow of electrical current of 12/25 =<br />

0.48 amperes. Conversely, with that same bulb, if we have flow of electrical<br />

current of 2 amperes through it, then the potential difference between one end

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