PHY 114 A General Physics II Plan for Lecture 14 (Chapter 32):

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Presentation transcript:

PHY 114 A General Physics II Plan for Lecture 14 (Chapter 32): 11 AM-12:15 PM TR Olin 101 Plan for Lecture 14 (Chapter 32): Inductance Inductors as a circuit element RL, LC, and RLC circuits Energy stored in an inductor 12/4/2018 PHY 114 A Spring 2012 -- Lecture 14

Remember to send in your chapter reading questions… 12/4/2018 PHY 114 A Spring 2012 -- Lecture 14

Web assign question -- hint 1000 turns/m 12/4/2018 PHY 114 A Spring 2012 -- Lecture 14

Web assign question -- hint q = wt 12/4/2018 PHY 114 A Spring 2012 -- Lecture 14

Electric generator: q = wt 12/4/2018 PHY 114 A Spring 2012 -- Lecture 14

Electric generator: I t 12/4/2018 PHY 114 A Spring 2012 -- Lecture 14

Summary: 12/4/2018 PHY 114 A Spring 2012 -- Lecture 14

Faraday’s law for EMF induced in a current loop: 12/4/2018 PHY 114 A Spring 2012 -- Lecture 14

“Mutual” inductance =Nc A 12/4/2018 PHY 114 A Spring 2012 -- Lecture 14

“Self” inductance L inductance 12/4/2018 PHY 114 A Spring 2012 -- Lecture 14

Inductors in a circuit Example: LR circuit 12/4/2018 PHY 114 A Spring 2012 -- Lecture 14

Example: LR circuit 12/4/2018 PHY 114 A Spring 2012 -- Lecture 14

Example: LR circuit I t 12/4/2018 PHY 114 A Spring 2012 -- Lecture 14

The LR circuit reminds us of: Why physics class is so beautiful. Why physics class is so terrible. RC circuit. Money in the bank. 12/4/2018 PHY 114 A Spring 2012 -- Lecture 14

Energy storage in inductor: 12/4/2018 PHY 114 A Spring 2012 -- Lecture 14

Example: LR circuit continued 12/4/2018 PHY 114 A Spring 2012 -- Lecture 14

Charge decays with time Charge increases with time LC circuit This circuit has the following time dependence after the switch is closed: Charge decays with time Charge increases with time Charge remains constant with time Charge increases and decreases with time 12/4/2018 PHY 114 A Spring 2012 -- Lecture 14

LC circuit 12/4/2018 PHY 114 A Spring 2012 -- Lecture 14

LC circuit For L=1 H, C=1 F; w=1 rad/s Q/Qmax w=2pf t 12/4/2018 PHY 114 A Spring 2012 -- Lecture 14

The LC circuit is mathematically analogous to: Nothing seen previously seen in class An elastic bouncing ball A swinging pendulum A mass attached to a spring All above, except A The LC circuit is useful: Because of its mathematical analogies Physicists like simple formulae like cos(wt) It could be useful in science experiments It could be useful for toys It could be useful for everyday appliances 12/4/2018 PHY 114 A Spring 2012 -- Lecture 14

LRC circuit: Q/CE t 12/4/2018 PHY 114 A Spring 2012 -- Lecture 14