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Physics 202
Tuesday, March 2, 1999
Announcements: Midterm 2 scheduled for March
18, 1999
Lecture notes:
Temperature dependence of r
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R= r L/A
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For metals: r =ro [ 1+ a(T-
To)], a > 0
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For Semiconductors such as germanium and silica:
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Power Dissipated in a Resistor
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b to c and d to a the circuit is ideal: There is no resistance
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c to d is a resistor
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Let's follow a quantity of positive charge DQ
that flows around the circuit.
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As DQ moves from a to b (through the battery),
its electrical potential energy increases by an amount [VDQ
]
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The chemical potential energy in the battery decreases by the same amount.
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As DQ moves from c to d, through the resistor,
the charge carried suffers "collisions" with the (misplaced) atoms in the
the resistor and loses energy, by the same amount [VDQ
]
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The energy is disipated as heat or thermal energy
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By the time DQ reaches point a, it is
at the same electric potential again.
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DU/ Dt = (DQ
/Dt) V = IV = P
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P is the power lost in the resistor; conversely the power supplied by the
battery
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Let's check the units for P...
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Units of I = coul/sec
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Units of V= Joul/ Coul
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Therefore the units of IV= the units of power = Joul/ sec = Watt
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P =IV if the resistor is ohmic
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then, if V= IR.... P= I2R or P = (V/R)V = V2/
R
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Question: What is the resistance of a light bulb rated at 50 Watts? The
effective voltage in a typical household circuit is 110V.
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P = V2/ R = 50 watts so V2/ P = R = 242W
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What is the resistance of a bulb of 100 Watts?
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P = V2/ R = 100 watts so V2/ P = R = 121W
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Therefore, the higher the wattage, the lower the resistance
Direct Current Circuits
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Let us consider the simple circuit again....
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The battery acts as a pump that moves positive charges from lower to higher
potential.
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By convention, any device that can increase the potentail energy of positive
charges is called an "emf" device
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There are many different kinds of emf devices; i.e. batteries, solar cells,
etc
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Va + x - iR = Va so that x
- iR = 0 or x = iR
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