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Series Resonant Circuit
2
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3
CjLjRZin
1
ImpedanceInput
CjLjRI
Z
VZIZVIP
inininin
1
21
2
1
2
1*
2
1
2
22
resonatorthetoDeliveredPowerComplex
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4
C
ICV
LI
RIP
c
loss
2
22
2
2
1
4
1
4
1
4
1
21
e
m
W
capacitortheinstoredenergyelectricAverage
W
inductortheinstoredenergymagneticAverage
resistorthebydissipatedPower
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5
22
2
1
22
2
I
WWjP
I
PZ
WWjPP
emlossinin
emlossin
At resonance Wm = We (real),
2
1 2R
I
PZ lossin
Wm = We implies the resonant frequencyLC
10
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6
Quality Factor
loss
em
P
WW
Q
second/lossenergy
storedenergyaverage
RCR
L
P
WQ
loss
m
0
00
12
circuitresonantseriesfor
losslowQHigh
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QBW
1
resonanceatdeliveredthat2
1
iscircuitthetodeliveredpoweraveragereal
2if
bandwidthpowerhalfFractional
22RZin
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Parallel Resonant Circuit
8
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1
11
ImpedanceInput
Cj
LjRZin
CjL
j
RV
VZ
IZVIPin
inin
1
2
1
*
1
2
1
2
1*
2
1resonatorthetoDeliveredPowerComplex
2
22
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CV
LVLI
R
VP
L
loss
2
e
2
22
m
2
4
1W
capacitorin thestoredenergyelectricAverage
1
4
1
4
1W
inductorin thestoredenergymagneticAverage
2
1
resistorby thedissipatedPower
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22
2
1
22
2
I
WWjP
I
PZ
WWjPP
emlossinin
emlossin
At resonance Wm = We (real),
2
1 2R
I
PZ lossin
Wm = We implies the resonant frequencyLC
10
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12
Quality Factor
RC
L
R
P
W
Q
loss
m0
0
2
second/lossenergystoredenergyaverage
resonanceatdeliveredthat2
1
iscircuitthetodeliveredpoweraveragereal2
if
bandwidthpowerhalfFractional
22 R
Zin
QBW
1
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Loaded & Unloaded Q In the absence of any loading effects- no external
circuitry- unloaded Q
Usually- external circuit is coupled to the resonantcircuit Q reduced loaded Q (QL)
13
LLL
LL
R/RRwithRLCparallelRRwithRLCseries
RRR
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circuitsparallelforQ,External
circuitsseriesforQ,External
0
0
L
RQe
RLQe
L
L
QQQ eL
11
1,Qloaded
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Transmission Line Resonators TL sections various lengths & terminations -
resonators
16
Short-Circuited /2 Line
Lossy TL short circuited at one end
Z0,,,l= /2
ljZlZZin
tanhtanh 00
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llj
ljlZZni
tanhtan1
tantanh0
pppvvv
lll
llllTEMAssuming
small)very(,Let
tanh,1lossyTL
0
0
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18
)(,2
00
pvl
0
l
000
tantantan
l
ckt)ResonantRLCseriesofimpedanceinput(2;1
1
0
00
0
00
jLRZl
jlZ
lj
jlZZ
ni
ni
LC
ZLlZR
200
00
1,
2,
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19
The short circuited /2 line resonates for = 0 & its
input impedance at this frequency is Zin = R= Z0lResonance also occurs for l = n/2, n= 1,2,3..
22
0 lR
LQ
l = first resonanceQ decreases as attenuationof the line increases.
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Lossy TL short circuited at one end
Z0,,,l= /4
ljZlZZin tanhtanh 00
Short-Circuited /4 Line
ljl
lljZZ
ljdrnrby
llj
ljlZZ
ni
ni
cottanh
cottanh1
cot.&.
tanhtan1
tantanh
0
0
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21
0
0)(,4
Let
l
022
l
000 22tan22cotcot
l
ckt)ResonantRLCparallelofimpedanceinput(21
1;1
22
21
0
0
0
0
0
0
jCR
Zl
jl
Z
jl
lj
ZZ
ni
ni
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22
CL
ZC
l
ZR
20
00
0
1
4
240
lRCQ
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Practical resonator
Z0,,,l= /2
ljZlZZin cothcoth 00
Open-Circuited /2 Line
ljl
llj
ZZni
tantanh
tanhtan1
0
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0
0)(,2
Let
l
0
l
0
tantan
l
cktResonantRLCparallelofimpedanceinput
0
0
jl
ZZ
ni
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CL
ZC
l
ZR
20
00
0
1
2
220
lRCQ