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Chapter 23: Magnetic Flux and Faraday's Law of Induction Chapter Review |
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Chapter Review
23-8 RL Circuits
A coil with a finite inductance (and negligible resistance) is called an inductor. Inductors are often used as circuit elements; a circuit with a resistor and an inductor in series is called an RL circuit. Recall that induction in a coil tends to resist changes in the current. As a result of this, the current in a circuit that contains an inductor does not rise and fall as quickly as it otherwise would; the inductance causes it to rise and fall gradually, the larger the inductance the more gradual the change in current.
Similar to what happens in RC circuits, when an emf is first
applied (or shut off) in an RL circuit, the current increases (or
decreases) exponentially with a characteristic time given by the
time constant
.
For a current that is building up from zero in a RL circuit the
result is
For a current that is falling off from the maximum value
Imax = E/R the result is
We can see that in the case where the current is falling off,
t
represents the amount of time it takes for the current to fall to
(e-1)Imax =
(0.368)Imax, that is, to 36.8% of its
maximum value.
Physlet Illustration: RL Circuit |
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| In this simulation, a resistor and an inductor are connected in series to a 12-Volt battery. When the switch closes, the current in the circuit begins to flow. An ammeter is included in the circuit, and a graph of the current vs. time is also shown. Vary the values of the resistor (1 W < R < 10 W) and inductor (1 H < L < 5 H). How do these affect the flow of current through the circuit? | |
Hints:
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Practice Quiz
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23-9 Energy Stored in a Magnetic Field
Because the induced current in an inductor resists the build up
of current in the coil, it therefore requires energy to build up
the current in an inductor against this "resistance." Once the
current has been established, so has the magnetic field within the
coil. The energy needed to build up this current is stored in the
magnetic field. For an inductor of inductance L, sustaining a
current I, the amount of energy U (the text uses E) stored in the
magnetic field is
.
Just like with the energy stored in the electric field of a
capacitor, the relationship between the energy stored in an
inductor and its magnetic field is nicely expressed in terms of the
energy density (energy per unit volume) of the magnetic field
.
This expression for the energy density applies to any magnetic field, not just those for an inductor.
Practice Quiz
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23-10 Transformers
A very important practical device that relies on the phenomenon
of induction is the transformer. A transformer is a device
that uses induction to increase or decrease the voltage in a
circuit. A transformer consists of a primary coil,
containing Np turns, across which an AC
voltage Vp is applied. The primary coild
is bound by an iron core to a secondary coil, containing
Ns turns. By induction there will be an
induced potential differece Vs across the
secondary coil. The relationship between the primary and secondary
voltages is given by the transformer equation:
.
When Vs > Vp we have a step-up transformer and when Vs << Vp we have a step-down transformer.
By conservation of energy, the average power in the secondary
circuit must equal the average power in the primary circuit,
IsVs =
IpVp.
Therefore,
.
So that a step-up transformer steps down the current and vice versa.
Exercise 23.5 A Big Step Down: Suppose you want to use one transformer to step down from a power line voltage of 50,000 V to a household voltage of 120 V. If your primary coil consists of 10,000 turns, how many turns would you need in your secondary coil?
Solution: We are given the following information:
Given: Vp = 50,000 V, Vs = 120 V, Np = 10,000 Find: Ns
The transformer equation gives,
Insight In practice the voltage from power lines is stepped down in several stages, not all at once.
Practice Quiz
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