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Physics 202

Tuesday, March 2, 1999
Announcements: Midterm 2 scheduled for March 18, 1999

Lecture notes:

Temperature dependence of r
  •  R= r L/A
  • For metals: r =ro [ 1+ a(T- To)],  a > 0
  • For Semiconductors such as germanium and silica:

Power Dissipated in a Resistor
  • b to c and d to a the circuit is ideal: There is no resistance
  • c to d is a resistor
  • Let's follow a quantity of positive charge DQ that flows around the circuit.
  • As DQ moves from a to b (through the battery), its electrical potential energy increases by an amount [VDQ ]
    • The chemical potential energy in the battery decreases by the same amount.
  • 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 ]
    • The energy is disipated as heat or thermal energy
  • By the time DQ  reaches point a, it is at the same electric potential again.
    • DU/ Dt = (DQ /Dt) V = IV = P
    • P is the power lost in the resistor; conversely the power supplied by the battery
  • Let's check the units for P...
    • Units of I = coul/sec
    • Units of V= Joul/ Coul
    • Therefore the units of IV= the units of power = Joul/ sec = Watt
  • P =IV if the resistor is ohmic
    • then, if V= IR.... P= I2R  or P = (V/R)V = V2/ R
  • Question: What is the resistance of a light bulb rated at 50 Watts? The effective voltage in a typical household circuit is 110V.
    • P = V2/ R = 50 watts so  V2/ P = R = 242W
  • What is the resistance of a bulb of 100 Watts?
    • P = V2/ R = 100 watts so  V2/ P = R = 121W
      • Therefore, the higher the wattage, the lower the resistance

Direct Current Circuits
  • Let us consider the simple circuit again....
  • The battery acts as a pump that moves positive charges from lower to higher potential.
  • By convention, any device that can increase the potentail energy of positive charges is called an "emf" device
  • There are many different kinds of emf devices; i.e. batteries, solar cells, etc
  • Va + x - iR = Va  so that x - iR = 0 or x = iR
    • x is emf.

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