772 CHAPTER 7 Applications of Trigonometry 7-62
b. From the table we note when and
. Using the intersection of graphs method places these values
at and (see graph).
Now try Exercises 53 and 54
The chief components of AC circuits are voltage (V) and current (I). Due to the
nature of how the current is generated, V and I can be modeled by sine functions. Other
characteristics of electricity include pure resistance (R),
inductive reactance (X
L
), and capacitive reactance (X
C
)
(see Figure 7.75). Each of these is measured in a unit called
ohms ( while current I is measured in amperes (A), and
voltages are measured in volts (V). These components of
electricity are related by fixed and inherent traits,
which include the following: (1) voltage across a
resistor is always in phase with the current,
meaning the phase shift or phase angle between
them is (Figure 7.76);(2) voltage across an
inductor leads the current by (Figure 7.77);
(3) voltage across a capacitor lags the current by
(Figure 7.78); and (4) voltage is equal to the
product of the current times the resistance or
reactance: and
Different combinations of R, X
L
, and X
C
in a
combined (series) circuit alter the phase angle and the resulting voltage. Since voltage
across a resistance is always in phase with the current (trait 1), we can model the resis-
tance as a vector along the positive real axis (since the phase angle is ). For traits
(2) and (3), X
L
is modeled on the positive imaginary axis since voltage leads current
by and X
C
on the negative imaginary axis since voltage lags current by (see
Figure 7.79). These natural characteristics make the complex plane a perfect fit for
describing the characteristics of the circuit.
Consider a series circuit (Figure 7.75), where and
For a current of through this circuit, the voltage across each
individual element would be (A to B),
(B to C), and (C to D). However, the resulting voltage across this
circuit cannot be an arithmetic sum, since R is real while X
L
and X
C
are represented by
imaginary numbers. The joint effect of resistance (R) and reactance (X
L
, X
C
) in a circuit
is called the impedance, denoted by the letter Z, and is a measure of the total resis-
tance to the flow of electrons. It is computed (see Worthy of
Note), due to the phase angle relationship of the voltage in each element (X
L
and X
C
point in opposite directions, hence the subtraction). The expression for Z is more
commonly written where we more clearly note Z is a complex
number whose magnitude and angle with the x-axis can be found as before:
and The angle represents the
phase angle between the voltage and current brought about by this combination of ele-
ments. The resulting voltage of the circuit is then calculated as the product of the
current with the magnitude of the impedance, or (Z is also measured in
ohms, ).
EXAMPLE 7
Finding the Impedence and Phase Angle of the Current in a Circuit
For the circuit diagrammed in the figure, (a) find the magnitude of Z, the phase
angle between current and voltage, and write the result in trigonometric form; and
(b) find the total voltage across this circuit.
V
RLC
I
Z
r
tan
1
a
X
L
X
C
R
b.
Z
2R
2
1X
L
X
C
2
2
R 1X
L
X
C
2j,
Z R X
L
j X
C
j
V
C
122142 8 V
V
L
122192 18 VV
R
1221122 24 V
I 2 amps
X
C
4 .
R 12 , X
L
9 ,
90°90°,
0°
V IX
C
.V IR, V IX
L
,
90°
90°
0°
2,
t 0.0069t 0.0014
t 10.006, 0.0072
t 10.001, 0.0022V1t2 160
X
C
X
L
R
BCD
sin
Voltage and current
are in phase
(phase angle 0)
90 180 270
sin
Voltage leads current
by 90
(phase angle 90)
90 180 270
sin
Voltage lags current
by 90
(phase angle 90)
90 180 270
R
X
L
X
C
yi
Figure 7.75
Figure 7.76
Figure 7.77
Figure 7.78
Figure 7.79
WORTHY OF NOTE
While mathematicians
generally use the symbol i to
represent the “i” is
used in other fields to
represent an electric current
so the symbol is
used instead. In conformance
with this convention, we will
temporarily use j for
as well.
11
j 11
11,
College Algebra & Trignometry—
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