Chapter 23: Electromagnetic Induction, AC Circuits, and Electrical Technologies

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51 Terms

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back emf

the emf generated by a running motor, because it consists of a coil turning in a magnetic field; it opposes the voltage powering the motor

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capacitive reactance

the opposition of a capacitor to a change in current; calculated by 𝑋𝐶=12π⁢fC

<p><span><span>the opposition of a capacitor to a change in current; calculated by </span></span>𝑋𝐶=12π⁢fC</p>
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characteristic time constant

denoted by 𝜏, of a particular series RL circuit is calculated by 𝜏=𝐿𝑅, where 𝐿 is the inductance and 𝑅 is the resistance

<p><span><span>denoted by </span></span>𝜏<span><span>, of a particular series </span></span><em>RL</em><span><span> circuit is calculated by </span></span>𝜏=𝐿𝑅<span><span>, where </span></span>𝐿<span><span> is the inductance and </span></span>𝑅<span><span> is the resistance</span></span></p>
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eddy current

a current loop in a conductor caused by motional emf

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electric generator

a device for converting mechanical work into electric energy; it induces an emf by rotating a coil in a magnetic field

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electromagnetic induction

the process of inducing an emf (voltage) with a change in magnetic flux

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emf induced in a generator coil

emf=NAB⁢𝜔⁢sin⁡𝜔𝑡, where 𝐴 is the area of an 𝑁-turn coil rotated at a constant angular velocity 𝜔 in a uniform magnetic field 𝐵, over a period of time 𝑡

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energy stored in a inductor

self-explanatory; calculated by 𝐸ind=12⁢𝐿𝐼2

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Faraday’s Law of Induction

the means of calculating the emf in a coil due to changing magnetic flux, given by emf=−𝑁⁢𝛥𝛷𝛥𝑡

<p><span><span>the means of calculating the emf in a coil due to changing magnetic flux, given by </span></span>emf=−𝑁⁢𝛥𝛷𝛥𝑡</p>
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Henry

the unit of inductance; 1⁢H=1⁢Ω⋅s

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Impedance

the AC analogue to resistance in a DC circuit; it is the combined effect of resistance, inductive reactance, and capacitive reactance in the form 𝑍=√𝑅2+(⁢𝑋𝐿−𝑋𝐶)2

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Inductance

a property of a device describing how efficient it is at inducing emf in another device

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Induction

(magnetic induction) the creation of emfs and hence currents by magnetic fields

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Inductive reactance

the opposition of an inductor to a change in current; calculated by 𝑋𝐿=2π⁢fL

<p><span><span>the opposition of an inductor to a change in current; calculated by </span></span>𝑋𝐿=2π⁢fL</p>
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Inductor

a device that exhibits significant self-inductance, the emf induced in it by a change in current through it is proportional to the rate of change of that current.

<p><span>a device that exhibits significant self-inductance, </span><span><span>the emf induced in it by a change in current through it is proportional to the rate of change of that current. </span></span></p>
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Lenz’s Law

the minus sign in Faraday’s law, signifying that the emf induced in a coil opposes the change in magnetic flux

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Magnetic Damping

the drag produced by eddy currents

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Magnetic Flux

the amount of magnetic field going through a particular area, calculated with 𝛷=BA⁢cos⁡𝜃 where 𝐵 is the magnetic field strength over an area 𝐴 at an angle 𝜃 with the perpendicular to the area

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Mutual Inductance

how effective a pair of devices are at inducing emfs in each other

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Peak emf

emf0=NAB⁢𝜔

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phase angle

denoted by 𝜙, the amount by which the voltage and current are out of phase with each other in a circuit

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power factor

the amount by which the power delivered in the circuit is less than the theoretical maximum of the circuit due to voltage and current being out of phase; calculated by cos⁡𝜙

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resonant frequency

the frequency at which the impedance in a circuit is at a minimum, and also the frequency at which the circuit would oscillate if not driven by a voltage source; calculated by 𝑓0=12π⁢√LC

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self-inductance

how effective a device is at inducing emf in itself

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shock hazard

the term for electrical hazards due to current passing through a human

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step-down transformer

a transformer that decreases voltage

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step-up transformer

a transformer that increases voltage

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thermal hazard

the term for electrical hazards due to overheating

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three-wire system

the wiring system used at present for safety reasons, with live, neutral, and ground wires

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transformer

a device that transforms voltages from one value to another using induction

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transformer equation

the equation showing that the ratio of the secondary to primary voltages in a transformer equals the ratio of the number of loops in their coils; 𝑉s𝑉p=𝑁s𝑁p

<p><span><span>the equation showing that the ratio of the secondary to primary voltages in a transformer equals the ratio of the number of loops in their coils; </span></span>𝑉s𝑉p=𝑁s𝑁p</p>
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Units of Magnetic flux

the measure of the total magnetic field that passes through a given area, measured in Weber (Wb). It quantifies the amount of magnetic field lines passing through a surface.

<p>the measure of the total magnetic field that passes through a given area, measured in Weber (Wb). It quantifies the amount of magnetic field lines passing through a surface. </p>
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motional emf

the electromotive force generated when a conductor moves through a magnetic field, resulting in induced voltage.

<p>the electromotive force generated when a conductor moves through a magnetic field, resulting in induced voltage. </p>
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An electric generator rotates a coil in a magnetic field, inducing an emfgiven as a function of time

that converts mechanical energy into electrical energy, producing alternating current.

<p>that converts mechanical energy into electrical energy, producing alternating current. </p>
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Peak emf of a generator

is the maximum voltage output a generator can produce during its operation, typically occurring when its coil is aligned optimally with the magnetic field.

<p>is the maximum voltage output a generator can produce during its operation, typically occurring when its coil is aligned optimally with the magnetic field. </p>
36
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The currents 𝐼p and 𝐼s in the primary and secondary coils are related

through the turns ratio of the transformer, which determines how voltage and current change between the coils.

<p>through the turns ratio of the transformer, which determines how voltage and current change between the coils. </p>
37
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A change in current Δ⁢𝐼1/Δ⁢𝑡 in one

one induces an emf emf2 in the second according to Faraday's law of electromagnetic induction.

<p><span><span>one induces an emf </span></span>emf2<span><span> in the second according to Faraday's law of electromagnetic induction. </span></span></p>
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a change in current Δ⁢𝐼2/Δ⁢𝑡 through the second device

induces an emf emf1 in the first device, also based on Faraday's law of electromagnetic induction.

<p><span><span>induces an emf emf1 in the first device, also based on Faraday's law of electromagnetic induction. </span></span></p>
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self-inductance 𝐿 of an inductor is

proportional to how much flux changes with current. For an 𝑁-turn inductor,

<p><span><span>proportional to how much flux changes with current. For an </span></span>𝑁<span><span>-turn inductor,</span></span></p>
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The self-inductance of a solenoid

is defined as the ratio of the induced emf to the rate of change of current in the solenoid, considering its geometry and the number of turns.

<p>is defined as the ratio of the induced emf to the rate of change of current in the solenoid, considering its geometry and the number of turns. </p>
41
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Energy stored in a inductor

is given by the formula ( U = \frac{1}{2} L I^2 ), where ( L ) is the inductance and ( I ) is the current through the inductor.

<p>is given by the formula ( U = \frac{1}{2} L I^2 ), where ( L ) is the inductance and ( I ) is the current through the inductor. </p>
42
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When a series connection of a resistor and an inductor—an RL circuit—is connected to a voltage source, the time variation of the current is

exponentially increasing and characterized by a time constant. This behavior results from the inductor opposing changes in current due to self-inductance.

<p>exponentially increasing and characterized by a time constant. This behavior results from the inductor opposing changes in current due to self-inductance. </p>
43
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When the inductor is shorted through a resistor,

current decreases as

<p><span><span>current decreases as  </span></span></p>
44
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Ohm’s law for an inductor

states that the voltage across an inductor is proportional to the rate of change of current through it. Mathematically, it is expressed as V = L (dI/dt), where V is the voltage, L is the inductance, and dI/dt is the time rate of change of the current.

<p>states that the voltage across an inductor is proportional to the rate of change of current through it. Mathematically, it is expressed as V = L (dI/dt), where V is the voltage, L is the inductance, and dI/dt is the time rate of change of the current. </p>
45
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Ohm’s law for a capacitor

states that the current through a capacitor is proportional to the rate of change of voltage across it. Mathematically, it is expressed as I = C (dV/dt), where I is the current, C is the capacitance, and dV/dt is the time rate of change of the voltage.

<p>states that the current through a capacitor is proportional to the rate of change of voltage across it. Mathematically, it is expressed as I = C (dV/dt), where I is the current, C is the capacitance, and dV/dt is the time rate of change of the voltage. </p>
46
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AC version of Ohm’s law:

states that the voltage and current in an AC circuit are related by the impedance of the circuit. It is often represented as V = I Z, where V is the voltage, I is the current, and Z is the impedance.

<p>states that the voltage and current in an AC circuit are related by the impedance of the circuit. It is often represented as V = I Z, where V is the voltage, I is the current, and Z is the impedance. </p>
47
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Impedance units

are measured in ohms (Ω), which indicate the opposition that a circuit presents to the flow of alternating current.

<p>are measured in ohms (Ω), which indicate the opposition that a circuit presents to the flow of alternating current. </p>
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Resonant Frequency

at which 𝑋𝐿=𝑋𝐶

<p><span><span>at which </span></span>𝑋𝐿=𝑋𝐶  </p>
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In an AC circuit, there is a phase angle 𝜙 between source voltage 𝑉 and the current 𝐼

due to the reactive components. This phase difference affects the power factor and the efficiency of energy transfer in the circuit.

<p>due to the reactive components. This phase difference affects the power factor and the efficiency of energy transfer in the circuit. </p>
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for a purely resistive circuit or an RLC circuit at resonance.

The resonant frequency is the frequency at which the inductive reactance equals the capacitive reactance, resulting in maximum circuit current.

<p>The resonant frequency is the frequency at which the inductive reactance equals the capacitive reactance, resulting in maximum circuit current. </p>
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The average power delivered to an RLC circuit is affected by the phase angle and is given by

P = VI cos(φ)

<p>P = VI cos(φ) </p>

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