Series Resonance. For an R-L-C series circuit, when inductive reactance XL = capacitive reactance XC, the applied voltage V and the current I are in phase. This effect is called series resonance. At resonance: Impedance, Z Current, / | Z = XL or Z = Xc The series resonant circuit is often described as an acceptor circuit sinc it has its minimum impedance, and thus maximum current, at the reson- ant frequency. VL = Vc X₂ -Frequency Z =R (i.e. the minimum circuit imped- ance possible in an L-C-R circuit) XL > XC XL =XC, then 2πfr L=1/2nfr C, where fi is resonant frequency VL > Vc or VL < Vc I=V/R (i.e. the maximum current pos sible in an L-C-R circuit)

Delmar's Standard Textbook Of Electricity
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ISBN:9781337900348
Author:Stephen L. Herman
Publisher:Stephen L. Herman
Chapter24: Resistive-inductive-capacitive Parallel Circuits
Section: Chapter Questions
Problem 4RQ: A tank circuit contains a capacitor and an inductor that produce 30 of reactance at the resonant...
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Series Resonance. For an R-L-C
series circuit, when inductive
reactance XL = capacitive reactance
XC, the applied voltage V and the
current I are in phase. This effect is
called series resonance. At
resonance:
Impedance, Z
Current, /
R
Z = XL or Z = Xc
The series resonant circuit is often
described as an acceptor circuit sinc
it has its minimum impedance, and
thus maximum current, at the reson-
ant frequency.
VL = Vc
Xc
--Frequency
Z =R (i.e. the minimum circuit imped-
ance possible in an L-C-R circuit)
XL > Xc
XL =XC, then 2nfr L=1/2rfr C, where fi
is resonant frequency
VL > Vc or VL < Vc
I=V/R (i.e. the maximum current pos
sible in an L-C-R circuit)
Transcribed Image Text:Series Resonance. For an R-L-C series circuit, when inductive reactance XL = capacitive reactance XC, the applied voltage V and the current I are in phase. This effect is called series resonance. At resonance: Impedance, Z Current, / R Z = XL or Z = Xc The series resonant circuit is often described as an acceptor circuit sinc it has its minimum impedance, and thus maximum current, at the reson- ant frequency. VL = Vc Xc --Frequency Z =R (i.e. the minimum circuit imped- ance possible in an L-C-R circuit) XL > Xc XL =XC, then 2nfr L=1/2rfr C, where fi is resonant frequency VL > Vc or VL < Vc I=V/R (i.e. the maximum current pos sible in an L-C-R circuit)
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