Inductance, RL Circuits, LC Circuits, RLC Circuits
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1 Inductance, R Circuits, C Circuits, RC Circuits
2 Inductance What happens when we close the switch? The current flows What does the current look like as a function of time? Does it look like this? I t
3 Inductance What happens when we close the switch? The current flows What does the current look like as a function of time? If there is current in the loop, then there is a magnetic field The flux would change infinitely fast if the current looked like this, so there would be an (infinite) EMF I t 3
4 Inductance In fact any loop resists having it s current changed by generating an EMF, call this (self) inductance, di E V s E =, 1 Henry (H) 1 dt di dt A 4
5 Inductance For a solenoid of N turns, we have di dφ NΦ B E = = N = solenoid dt dt I µ Φ B = solenoid BA; = B = NBA I ni = µ nna = µ n Al = µ n B V 5
6 R Circuits OK, what really happens when we close the switch Move all the inductance into a new circuit element Use Kirchhoff s Rule for voltages around a loop E E IR E = IR = solenoid di dt 6
7 E R Circuits Solving the 1 st Order Differential Equation di di IR = dt = dt E IR E I t = I E di IR = log R R ( E IR) E IR E = log e ( ) E R R t = 1 = E IR ( R ) t ( e ) I 7
8 R Circuits What happens when we disconnect the ery (but still have the loop with the resistor and inductor)? E = = R I e I e ( R ) t ( ) R t 8
9 R Circuits The important idea is that an inductor acts like an infinite resistor when you initially try to push current through it and then after the current has been flowing for a long time it acts like a wire. Once you remove the current flowing through it, it creates its own current to cancel out the change in magnetic flux through its center, but that current quickly decreases to zero (if there is resistance in the wire) 9
10 Energy in the Magnetic Field Consider the Kirchhoff loop equation again E = IR + di dt A voltage is just an energy per charge So when the current is changing the inductor is storing up or releasing energy! How much, energy? Consider the power: di P = IE = I R + I dt 1
11 Energy in the Magnetic Field Consider the Kirchhoff loop equation again E = IR + E di dt P = I = I R + I dt For the inductor du di P = = I ind dt dt Compare to capacitor I di U = du = IdI = I 1 U U C = = 1 1 CV I 11
12 C Circuits and Oscillations What happens when we have a (charged) capacitor and inductor in a circuit Start with charged capacitor, and throw the switch 1
13 C Circuits and Oscillations 1) At t =, all the energy is stored in the capacitor 13
14 C Circuits and Oscillations 1) At t =, all the energy is stored in the capacitor ) When the capacitor is discharged, all the energy is stored in the inductor 14
15 C Circuits and Oscillations 1) At t =, all the energy is stored in the capacitor ) When the capacitor is discharged, all the energy is stored in the inductor 3) The current then recharges the capacitor (oppositely) 15
16 C Circuits and Oscillations 1) At t =, all the energy is stored in the capacitor ) When the capacitor is discharged, all the energy is stored in the inductor 3) The current then recharges the capacitor (oppositely) 4) And the cycle repeats 16
17 C Circuits and Oscillations How do we find the current quantitatively? Use Kirchhoff s aw again V C + E = Q di Q d Q + = + = C dt C dt d Q 1 = Q dt C This is the same equation as a simple harmonic oscillator 17
18 C Circuits and Oscillations How do we find the current quantitatively? Use Kirchhoff s aw again V C + E = Q di Q d Q + = + = C dt C dt d Q 1 = Q dt C This is the same equation as a simple harmonic oscillator C 1 ; k m; ω = k m ω = 1 C 18
19 C Circuits and Oscillations How do we find the current quantitatively? V C + E = Q di Q d Q + = + = C dt C dt d Q 1 = Q = ω Q dt C Q( t) = Q cos ωt + ϕ ( ) dq I( t) = = ωq sin( ωt + ϕ ) dt 19
20 U C Circuits and Oscillations What about the energy? With no resistor, energy is conserved = U C + U Q = cos ωt + C Q = cos ωt + C Q = C Q 1 = = I max C 1 1 I ( ωq ) max ( cos ωt + sin ωt) sin sin ωt ωt
21 RC Circuits Now, what if we add a resistor? This is like the damped harmonic oscillator RI = du dt Q = C Q RI = C d Q = dt + C di I dt dq dt di dt 1 I Q dq + R + C dt Rt Q t = Q e ( ) d Q = dt cosω t d for small R ω d = 1 C R 1
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