ECEN3714 Network Analysis Lecture #16 18 February 2015 Dr. George Scheets n Read 14.4 n Problems:...
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Transcript of ECEN3714 Network Analysis Lecture #16 18 February 2015 Dr. George Scheets n Read 14.4 n Problems:...
![Page 1: ECEN3714 Network Analysis Lecture #16 18 February 2015 Dr. George Scheets n Read 14.4 n Problems: Old Quiz #4.](https://reader035.fdocuments.us/reader035/viewer/2022062222/5697c01b1a28abf838ccf7bd/html5/thumbnails/1.jpg)
ECEN3714 Network AnalysisECEN3714 Network AnalysisLecture #16 18 February 2015Lecture #16 18 February 2015Dr. George ScheetsDr. George Scheetswww.okstate.edu/elec-eng/scheets/ecen3714www.okstate.edu/elec-eng/scheets/ecen3714
ECEN3714 Network AnalysisECEN3714 Network AnalysisLecture #16 18 February 2015Lecture #16 18 February 2015Dr. George ScheetsDr. George Scheetswww.okstate.edu/elec-eng/scheets/ecen3714www.okstate.edu/elec-eng/scheets/ecen3714
Read 14.4Read 14.4 Problems: Old Quiz #4Problems: Old Quiz #4 Quiz #4 this FridayQuiz #4 this Friday Quiz #3 ResultsQuiz #3 Results
Hi = 9.0, Low = 0.5, Average = 5.50Hi = 9.0, Low = 0.5, Average = 5.50Standard Deviation = 2.69Standard Deviation = 2.69
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ECEN3714 Network AnalysisECEN3714 Network AnalysisLecture #18 23 February 2015Lecture #18 23 February 2015Dr. George ScheetsDr. George Scheetswww.okstate.edu/elec-eng/scheets/ecen3714www.okstate.edu/elec-eng/scheets/ecen3714
ECEN3714 Network AnalysisECEN3714 Network AnalysisLecture #18 23 February 2015Lecture #18 23 February 2015Dr. George ScheetsDr. George Scheetswww.okstate.edu/elec-eng/scheets/ecen3714www.okstate.edu/elec-eng/scheets/ecen3714
Read 14.5Read 14.5 Problems: 13.55, 13.57, 14.2Problems: 13.55, 13.57, 14.2 Quiz #5 this FridayQuiz #5 this Friday
![Page 3: ECEN3714 Network Analysis Lecture #16 18 February 2015 Dr. George Scheets n Read 14.4 n Problems: Old Quiz #4.](https://reader035.fdocuments.us/reader035/viewer/2022062222/5697c01b1a28abf838ccf7bd/html5/thumbnails/3.jpg)
ECEN3714 Network AnalysisECEN3714 Network AnalysisLecture #19 25 February 2015Lecture #19 25 February 2015Dr. George ScheetsDr. George Scheetswww.okstate.edu/elec-eng/scheets/ecen3714www.okstate.edu/elec-eng/scheets/ecen3714
ECEN3714 Network AnalysisECEN3714 Network AnalysisLecture #19 25 February 2015Lecture #19 25 February 2015Dr. George ScheetsDr. George Scheetswww.okstate.edu/elec-eng/scheets/ecen3714www.okstate.edu/elec-eng/scheets/ecen3714
Read 14.6Read 14.6 Problems: Old Quiz #5Problems: Old Quiz #5 Quiz #5 this FridayQuiz #5 this Friday Quiz 4 ResultsQuiz 4 Results
Hi = 10, Low = 3, Average = 8.06Hi = 10, Low = 3, Average = 8.06Standard Deviation = 1.97Standard Deviation = 1.97
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Gustav KirchoffGustav Kirchoff Born 1824Born 1824 Died 1887Died 1887 German PhysicistGerman Physicist KCL & KVL formulated in 1852KCL & KVL formulated in 1852
Doctoral DissertationDoctoral Dissertation
KVL: KVL: ΣΣ(voltage drops around a closed loop) = 0(voltage drops around a closed loop) = 0 KCL: KCL: ΣΣ(current entering or exiting a node) = 0(current entering or exiting a node) = 0 High side voltage on device end a current entersHigh side voltage on device end a current enters
source: Wikipedia
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V(s) = (100s + 106)/(s + 5000)2V(s) = (100s + 106)/(s + 5000)2
v(t) = 500,000te-5000t + 100e-5000t
Re
Im
xx-5000 t
v(t)
100
.001
Stability Issues:Location of poles on Real axis sets decay rate.
Shape of curve indicates not pure exponential.
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v(t) = 500,000te-5,000t + 100e-5,000t)v(t) = 500,000te-5,000t + 100e-5,000t)
t
500,000te-5,000t
100
.001
t
100
.001
100e-5,000t
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Pulse in: u(t) – u(t-1)... Pulse in: u(t) – u(t-1)...
t
1
10
xin(t)
1
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Smeared pulse out: u(t)(1–e-0.5t) - u(t-1)(1+e-0.5(t-1))
Smeared pulse out: u(t)(1–e-0.5t) - u(t-1)(1+e-0.5(t-1))
t
1
10
xin(t)
1
t
0.632
101
xout(t)
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V(s) = 4/(s [4Cs2 +(1+4C)s +5])Roots at [ –[1+4C] + {[1+4C]2 – 80C}0.5 ]/2
V(s) = 4/(s [4Cs2 +(1+4C)s +5])Roots at [ –[1+4C] + {[1+4C]2 – 80C}0.5 ]/2
vout
vin 1 Ω
C
1 H
4 Ω
Quiz 4B2005
Will not oscillate when 0 < C < 13 mF
Im
xx-5 Re
C = 0
Im
xx-5.27 Re
C = 3 mF
x-79.04
Im
xx-6.13 Re
x-22.64
C = 9 mFIm
xx-7.04 Re
x-14.79
C = 12 mF
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V(s) = 4/(s(4Cs2 +(1+4C)s +5)V(s) = 4/(s(4Cs2 +(1+4C)s +5)
vout
vin 1 Ω
C
1 H
4 Ω
Quiz 4B
Oscillates when 14 mF < C < 4.49 F
Im
xx
-.75 Rex
1.39C = .5 F
Im
x
x-4.96
Re
C = 28 mF
x
4.47
Im
xx
-9.43 Re
C = 14 mF
.627x
C = 3 F Im
xx
-.54Rex
.35
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V(s) = 4/(s(4Cs2 +(1+4C)s +5)V(s) = 4/(s(4Cs2 +(1+4C)s +5)
vout
vin 1 Ω
C
1 H
4 Ω
Quiz 4B
Will not oscillate when C > 4.49 F
Im
xx-.2 Rex
-.83C = 7.5 F
Im
xx-.36
Re
C = 5 F
x-.69
C = 4.48 F Im
xx
-.53Re
x.02
Im
xx-.14 Re
x-.88
C = 10 F
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s = σ + jω…s = σ + jω… Pole real (x axis) coordinate Pole real (x axis) coordinate σσ
Provides time constantProvides time constant Time Waveform fades away if < 0Time Waveform fades away if < 0
Pole imaginary (y axis) coordinate Pole imaginary (y axis) coordinate ωω Frequency of oscillationFrequency of oscillation
0 = no oscillation0 = no oscillation
1st Order Equation "s"1st Order Equation "s" Has 1 poleHas 1 pole
2nd Order Equation "s2nd Order Equation "s22"" Has 2 polesHas 2 poles
Etc.Etc.
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y(t) = x(t) + y(t-1) → H(s) = 1/[1 – e–s]y(t) = x(t) + y(t-1) → H(s) = 1/[1 – e–s]
σ
Frequency Responseσ = 0 axisThis system, with a
feedback loop, has anInfinite # of poles alongThe σ = 0 (jω) axis.
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V(s) = 10s/(s2+2s+25)V(s) = 10s/(s2+2s+25)
Im
x
x
-1 Ret
10.2
v(t) = 10.2e-tcos(4.899t + .0641π)
Stability Issues: UnderdampedLocation of poles on Real axis sets decay rate.Location of poles on Imagninary axis sets oscillation rate.
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V(s) = 105/(s2 + 2*105s + 108)V(s) = 105/(s2 + 2*105s + 108)
t
v(t)
.5
.002
v(t) = .5025(e-500t - e-199,500t)
Im
xx-500 Re-199,500
Stability Issues: OverdampedNo complex poles = no oscillation.Location of poles on real axis sets decay rate.
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V(s) = (100s + 106)/(s + 5000)2V(s) = (100s + 106)/(s + 5000)2
v(t) = 500,000te-5000t + 100e-5000t
Re
Im
xx-5000 t
v(t)
100
.001
Stability Issues: Critically dampedLocation of poles on Real axis sets decay rate.
![Page 17: ECEN3714 Network Analysis Lecture #16 18 February 2015 Dr. George Scheets n Read 14.4 n Problems: Old Quiz #4.](https://reader035.fdocuments.us/reader035/viewer/2022062222/5697c01b1a28abf838ccf7bd/html5/thumbnails/17.jpg)
If system is under damped it'seasy to get values of α & β
α = decay rate & β = oscillation frequency
If system is under damped it'seasy to get values of α & β
α = decay rate & β = oscillation frequency
Must have imaginaryroots to oscillate.
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