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These resistors are said to be in series, and as indicated, it is possible to consider them as one single equivalent resistor R eq . To find this equivalent resistor, we exploit the fact from energy conservation that Vac = Vab + Vbc , which using Ohm's law (17.3) becomes
|
IR eq = IR1 + IR2 | (7) |
| Req = R1 + R2 +...+ RN. | (8) |