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Ch. 19-2.  The opposition to the motion of charge in a conductor.  For most metals, resistance is constant over a wide range of applied potential differences.

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Presentation on theme: "Ch. 19-2.  The opposition to the motion of charge in a conductor.  For most metals, resistance is constant over a wide range of applied potential differences."— Presentation transcript:

1 Ch. 19-2

2  The opposition to the motion of charge in a conductor.  For most metals, resistance is constant over a wide range of applied potential differences.  I = amperes (A) V = volts (V) R = ohms ( Ω )

3  Resistance depends on: Length Cross sectional area temperature Material

4  Sample Problem 19B pg. 702

5  Material that has zero resistance below a certain critical temperature.

6 19-3

7  Rate at which charge carriers do work.  P = Watts (W) I = Amperes (A) V = Volts (V)

8  Power companies charge for energy in kilowatt-hours (kWh)

9  Sample Problem 19D pg. 712


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