Presentation is loading. Please wait.

Presentation is loading. Please wait.

Induction and Inductance III

Similar presentations


Presentation on theme: "Induction and Inductance III"— Presentation transcript:

1 Induction and Inductance III
Physics 2113 Jonathan Dowling Lecture 34: WED 15 APR Induction and Inductance III Fender Stratocaster Solenoid Pickup

2 I n a s e r i o f x p m t , M c h l F d y E g J H U . S w b u ' T h e c i r u t s o w n f g a l p d v m ( k " ) . I b y A c u r e n t a p s o l y i f h v m b w g d . 1 F a s t e r m o i n u l g c . 2 I f 3 . w e r v s t h d i c o n m p l a y g , u T h e c u r n t g a d i s k o w " ; m f p l .

3 loop 1 loop 2

4 Lenz’s Law The Loop Current Produces a B Field that Opposes the CHANGE in the bar magnet field. Upper Drawing: B Field from Magnet is INCREASING so Loop Current is Clockwise and Produces an Opposing B Field that Tries to CANCEL the INCREASING Magnet Field Lower Drawing: B Field from Magnet is DECREASING so Loop Current is Counterclockwise and Tries to BOOST the Decreasing Magnet Field.

5 loop 1 loop 2 (30–17)

6 The RL circuit Key insights:
Set up a single loop series circuit with a battery, a resistor, a solenoid and a switch. Describe what happens when the switch is closed. Key processes to understand: What happens JUST AFTER the switch is closed? What happens a LONG TIME after switch has been closed? What happens in between? Key insights: You cannot change the CURRENT in an inductor instantaneously! If you wait long enough, the current in an RL circuit stops changing! At t = 0, a capacitor acts like a closed wire and inductor acts like break in the wire. At t = ∞ a capacitor acts like a break in the wire and inductor acts like an closed wire.

7 30.8: Self-Induction:

8 30.9: RL Circuits:

9 30.9: RL Circuits: If we suddenly remove the emf from this same circuit, the flux does not immediately fall to zero but approaches zero in an exponential fashion:

10 30.9: RL Circuits:

11 RC vs RL Circuits In an RL circuit, while fluxing up (rising current), E = Ldi/dt and the loop rule mean: magnetic field increases from 0 to B current increases from 0 to E/R voltage across inductor decreases from -E to 0 In an RC circuit, while charging, Q = CV and the loop rule mean: charge increases from 0 to CE current decreases from E/R to 0 voltage across capacitor increases from 0 to E

12 ICPP Immediately after the switch is closed, what is the potential difference across the inductor? (a) 0 V (b) 9 V (c) 0.9 V 10 Ω 10 H 9 V Immediately after the switch, current in circuit = 0. So, potential difference across the resistor = 0! So, the potential difference across the inductor = E = 9 V!

13 ICPP 40 Ω 10 H 3 V 10 Ω Immediately after the switch is closed, what is the current i through the 10 Ω resistor? (a) A (b) 0.3 A (c) 0 Immediately after switch is closed, current through inductor = 0. Why??? Hence, current through battery and through 10 Ω resistor is i = (3 V)/(10 Ω) = 0.3 A Long after the switch has been closed, what is the current in the 40 Ω resistor? (a) A (b) 0.3 A (c) A Long after switch is closed, potential across inductor = 0. Why??? Hence, current through 40 Ω resistor i = (3 V)/(10 Ω) = A (Par-V)

14 Fluxing Up The Inductor
How does the current in the circuit change with time? i i(t) Fast = Small τ E/R Slow= Large τ Time constant of RL circuit: τLR = L/R

15 RL Circuit Movie

16 Fluxing Down an Inductor
The switch is at a for a long time, until the inductor is charged. Then, the switch is closed to b. What is the current in the circuit? Loop rule around the new circuit: i E/R Exponential defluxing i(t)

17 Inductors & Energy Recall that capacitors store energy in an electric field Inductors store energy in a magnetic field. i P = iV = i2R = power dissipated by R Power delivered by battery + (d/dt) energy stored in L

18 Inductors & Energy Magnetic Potential Energy UB Stored in an Inductor.
Magnetic Power Returned from Defluxing Inductor to Circuit.

19 Example The switch has been in position “a” for a long time.
It is now moved to position “b” without breaking the circuit. What is the total energy dissipated by the resistor until the circuit reaches equilibrium? 9 V 10 Ω 10 H When switch has been in position “a” for long time, current through inductor = (9V)/(10Ω) = 0.9A. Energy stored in inductor = (0.5)(10H)(0.9A)2 = 4.05 J When inductor de-fluxes through the resistor, all this stored energy is dissipated as heat = 4.05 J.

20 E=120V, R1=10Ω, R2=20Ω, R3=30Ω, L=3H. What are i1 and i2 immediately after closing the switch? What are i1 and i2 a long time after closing the switch? What are i1 and i2 immediately after reopening the switch? What are i1 and i2 a long time after reopening the switch?

21

22 Energy Density in E and B Fields

23 The Energy Density of the Earth’s Magnetic Field Protects us from the Solar Wind!

24 Example, RL circuit, immediately after switching and after a long time:

25

26

27

28 Example, RL circuit, during a transition:

29 Example, Energy stored in a magnetic field:


Download ppt "Induction and Inductance III"

Similar presentations


Ads by Google