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Transcript
Chapter 33
Inductance, Electromagnetic
Oscillations, and AC Circuits
Part II
Copyright © 2009 Pearson Education, Inc.
AC Circuits with AC Source
Resistors, capacitors, and
inductors have different
phase relationships
between current and
voltage when placed in an
ac circuit.
The current through a
resistor is in phase with
the voltage.
Copyright © 2009 Pearson Education, Inc.
AC Circuits with AC Source
The voltage across the
inductor is given by
or
.
Therefore, the current
through an inductor lags
the voltage by 90°.
Copyright © 2009 Pearson Education, Inc.
AC Circuits with AC Source
The voltage across the inductor is related to the
current through it:
.
The quantity XL is called the inductive
reactance, and has units of ohms:
Copyright © 2009 Pearson Education, Inc.
AC Circuits with AC Source
Example : Reactance of a coil.
A coil has a resistance R = 1.00 Ω and an
inductance of 0.300 H. Determine the
current in the coil if (a) 120-V dc is applied
to it, and (b) 120-V ac (rms) at 60.0 Hz is
applied.
Copyright © 2009 Pearson Education, Inc.
AC Circuits with AC Source
The voltage across the
capacitor is given by
.
Therefore, in a capacitor,
the current leads the voltage
by 90°.
Copyright © 2009 Pearson Education, Inc.
AC Circuits with AC Source
The voltage across the capacitor is related to
the current through it:
.
The quantity XC is called the capacitive
reactance, and (just like the inductive
reactance) has units of ohms:
Copyright © 2009 Pearson Education, Inc.
AC Circuits with AC Source
Example : Capacitor reactance.
What is the rms current in the circuit shown if
C = 1.0 μF and Vrms = 120 V? Calculate (a) for
f = 60 Hz and then (b) for f = 6.0 x 105 Hz.
Copyright © 2009 Pearson Education, Inc.
AC Circuits with AC Source
This figure shows a high-pass filter (allows an ac
signal to pass but blocks a dc voltage) and a lowpass filter (allows a dc voltage to be maintained
but blocks higher-frequency fluctuations).
Copyright © 2009 Pearson Education, Inc.
LRC Series AC Circuit
Analyzing the LRC series AC circuit is complicated,
as the voltages are not in phase – this means we
cannot simply add them. Furthermore, the
reactances depend on the frequency.
Copyright © 2009 Pearson Education, Inc.
LRC Series AC Circuit
We calculate the voltage (and current) using what are
called phasors – these are vectors representing the
individual voltages.
Here, at t = 0, the
current and voltage
are both at a
maximum. As time
goes on, the phasors
will rotate
counterclockwise.
Copyright © 2009 Pearson Education, Inc.
LRC Series AC Circuit
Some time t later,
the phasors have
rotated.
Copyright © 2009 Pearson Education, Inc.
LRC Series AC Circuit
The voltages across each
device are given by the xcomponent of each, and
the current by its xcomponent. The current
is the same throughout
the circuit.
Copyright © 2009 Pearson Education, Inc.
LRC Series AC Circuit
We find from the ratio of voltage to
current that the effective resistance,
called the impedance, of the circuit is
given by
Copyright © 2009 Pearson Education, Inc.
LRC Series AC Circuit
The phase angle between the voltage and the
current is given by
or
The factor cos φ is called the power
factor of the circuit.
Copyright © 2009 Pearson Education, Inc.
LRC Series AC Circuit
Example 30-11: LRC circuit.
Suppose R = 25.0 Ω, L = 30.0 mH, and C =
12.0 μF, and they are connected in series to
a 90.0-V ac (rms) 500-Hz source. Calculate
(a) the current in the circuit, (b) the
voltmeter readings (rms) across each
element, (c) the phase angle , and (d) the
power dissipated in the circuit.
Copyright © 2009 Pearson Education, Inc.
Resonance in AC Circuits
The rms current in an ac circuit is
Clearly, Irms depends on the frequency.
Copyright © 2009 Pearson Education, Inc.
Resonance in AC Circuits
We see that Irms will be a maximum when XC =
XL; the frequency at which this occurs is
f0 = ω0/2π is called the
resonant frequency.
Copyright © 2009 Pearson Education, Inc.
Impedance Matching
When one electrical circuit is connected to another,
maximum power is transmitted when the output
impedance of the first equals the input impedance of
the second.
The power
delivered to the
circuit will be a
minimum when
dP/dt = 0; this
occurs when R1
= R2.
Copyright © 2009 Pearson Education, Inc.
Three-Phase AC
Transmission lines usually transmit threephase ac power, with the phases being
separated by 120°. This makes the power flow
much smoother than if a single phase were
used.
Copyright © 2009 Pearson Education, Inc.
Three-Phase AC
Example : Three-phase circuit.
In a three-phase circuit, 266 V rms exists
between line 1 and ground. What is the
rms voltage between lines 2 and 3?
Copyright © 2009 Pearson Education, Inc.
Summary of Chapter
• Mutual inductance:
• Self-inductance:
• Energy density stored in magnetic field:
Copyright © 2009 Pearson Education, Inc.
Summary of Chapter
• LR circuit:
.
.
• Inductive reactance:
• Capacitive reactance:
Copyright © 2009 Pearson Education, Inc.
Summary of Chapter
• LRC series circuit:
.
• Resonance in LRC series circuit:
Copyright © 2009 Pearson Education, Inc.