A. The series Series<\/strong><\/span> From the graph above shows that the magnitude of VR is the sum of the voltage drop on each resistor.<\/span> If the series with three resistors connected to the battery voltage, the current will flow from the battery through the three prisoners.<\/span> Strong currents in all parts of the series circuit is as much, not only the three prisoners who can be linked to a row, but the series circuit may comprise two, three, and four or more inmates.<\/span> Because V1 = I1 \u00b7 R1; V2 = I2 \u00b7 R2;<\/span> V3 = I3 \u00b7 R3 and Vs = IS \u00b7 Rt then:<\/span> Because the third series circuit energized prisoners are the same then:<\/span> B. Parallel Resistor Networks<\/strong><\/span>
\n If we connect the two prisoners in a row as in Figure 1:32, then the circuit is called a series of series \/ series.<\/span>
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\n Figure 2.11.<\/span> Series with two resistors<\/span><\/p>\n
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\n Figure 2.12.<\/span> Series with a voltage source<\/span><\/p>\n
\n If we measure the voltage at the first detainees are: V1;<\/span> The second voltage is: V2;<\/span> and the third voltage is: V3, it turns out that the sum of the voltage is the same as the battery voltage.<\/span>
\n Vs = V1 + V2 + V3<\/span><\/p>\n
\n IS \u00b7 Rt = I1 \u00b7 I2 \u00b7 R1 + R2 + I3 \u00b7 R3<\/span><\/p>\n
\n Is = I1 = I2 = I3, so<\/span>
\n Rt = R1 + R2 + R3<\/span><\/p>\n
\n Some users of electrical equipment connected together at one voltage.<\/span> This kind of relationship is called: the relationship rows \/ parallel.<\/span> All electrical equipment is usually associated rows in the voltage available.<\/span>
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\n Figure 2.13.<\/span> Parallel circuit with two resistors<\/span><\/p>\n