Summary of Class 23 8.02 Topic: Inductors & Magnetic Energy; RL Circuits Related Reading: Course Notes (Liao et al.): Sections 11.1 – 11.4; Topic Introduction Today we continue thinking about self inductance, in which the changing flux from a circuit induces an EMF in itself. We will then discuss the use of inductors in circuits. Self Inductance Remember that we defined the self inductance L by the amount of flux that an object generates through itself when a current I flows through it (Φ = LI) and, from Faradays Law, found that inductors will generate a back EMF: ε =−LdI dt . An inductor is a circuit element whose main characteristic is its inductance, L. It is drawn as a coil in circuit diagrams. The strong resemblance to a solenoid is intentional – solenoids make very good inductors both because of their ability to make a strong field inside themselves, and also because the field they produce is fairly well contained, and hence doesn’t produce flux (and induce EMFs) in other, nearby circuits. The role of an inductor is to oppose changing currents. At steady state, in a DC circuit, an inductor is off – it induces no EMF as long as the current through it is constant. As soon as you try to change the current through an inductor though, it will fight back. In this sense an inductor is the opposite of a capacitor. If a capacitor is placed in a steady state current it will eventually fill up and “open” the circuit, whereas an inductor looks like a short in this case. On the other hand, when starting from its uncharged state, a capacitor looks like a short when you first try to move current through it (no voltage drop), while an inductor looks like an open circuit, as it prevents the change (from no current to some current). Energy in B Fields Where do inductors get the energy to source current when they need to? In capacitors we found that energy was stored in the electric field between their plates. In inductors, energy is similarly stored, only now its in the magnetic field. Just as with capacitors, where the electric field was created by a charge on the capacitor, we now have a magnetic field created when there is a current through the inductor. Thus, just as with the capacitor, we can discuss both the energy in the inductor, U = 12 LI 2 , and the more generic energy density uB = 2 B µ 20 , stored in the magnetic field. Again, although we introduce the magnetic field energy density when talking about energy in inductors, it is a generic concept – whenever a magnetic field is created it takes energy to do so, and that energy is stored in the field itself. Summary for Class 23 W10D1 p. 1/3Summary of Class 23 8.02 RL Circuits A simple RL circuit is shown below. When the switch is closed, no current will initially flow in the circuit, Decay Down “Decay” Up but as time goes on this current will increase. We can write down the differential equation for current flow by using Faraday’s Law. We begin by calculating the line integral of the electric field around the loop. There are two contributions to this integral: the electric field in the wire and the electric field in the battery. If we orient the line integral in the direction of the electric field in the wire (the electric field in the battery points in the opposite direction) then GG v∫ Er⋅ d = IR −εbattery . oriented We now use Faraday’s law: GG d GG v∫ Er⋅ d =εelectromotive =− dt ∫∫ ⋅ dBa . oriented For a loop with only self induction, d GG dI − ⋅ d =− L .∫∫Badt dt So combining the two results in Faraday’s Law yields IR−εbattery =− L dI dt which is first order linear differential equation with constant coefficients. The solution to this differential equation εbattery −t/τIt() = (1 − e )R shows that the current increases exponentially from its initial value of zero to a final constant value of εbattery / R . The rate at which this change happens is dictated by the “time constant” τ, which for this circuit is given by τ= /LR. Summary for Class 23 W10D1 p. 2/3Summary of Class 23 8.02 Now the current starts at zero and “decays” upward to a constant value, now with a time constant τ = L/R (a big inductance slows down the circuit as it is more effective at opposing changes, but now a big resistance reduces the size of the current and hence changes in the current that the inductor will see, and thus decreases the time constant – speeds things up). Interestingly, in RL circuits any value that you could ask about (current, potential drop across the resistor, …) “decays” exponentially (either down or up). You should be able to determine which of the two plots (above and to the right a value) will follow just by thinking about it. Important Equations Self Inductance, L: L =ΦB I EMF Induced by Inductor: ε=−L dI dt Energy stored in Inductor: U = 1 LI 2 2 B2 Energy Density in B Field: uB = 2µ0 Exponential Decay: Value =Value initial e−t τ Exponential “Decay Upwards”: Value =Value final (1− e−t τ) Simple RL Time Constant: τ= L/R Summary for Class 23 W10D1 p.
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