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Circuit Analysis – II (EE-201)Variable-frequency Networks
Part 2
Sinusoidal Frequency Analysis
Bode plots to display frequency response data
VARIABLE-FREQUENCY NETWORK
PERFORMANCE
LEARNING GOALS
SINUSOIDAL FREQUENCY ANALYSIS
)(sH
Circuit represented by
network function





)cos(0
)(
0


tB
eA tj
 




)(cos|)(|
)(
0
)(
0

 
jHtjHB
ejHA tj
)(
)()(
)()(
|)(|)(




j
eMjH
jH
jHM



Notation
stics.characteriphaseandmagnitude
calledgenerallyareoffunctionasofPlots  ),(),(M
)(log
)(
))(log20
10
10



PLOTSBODE vs
(M



.offunctionaasfunctionnetworkthe
analyzewefrequencytheoffunctionaasnetworkaofbehaviorthestudyTo
)( jH
HISTORY OF THE DECIBEL
Originated as a measure of relative (radio) power
1
2
)2 log10(|
P
P
P dB 1
Pover
2
1
2
2
2
1
2
2
)2
2
2
log10log10(|
I
I
V
V
P
R
V
RIP dB  1
Pover
By extension
||log20|
||log20|
||log20|
10
10
10
GG
II
VV
dB
dB
dB



Using log scales the frequency characteristics of network functions
have simple asymptotic behavior.
The asymptotes can be used as reasonable and efficient approximations
Bode Plots
• These are Magnitude and Phase based pair of plots
• The Horizontal Access is always a logarithmic scale frequency (f or ꙍ)
• The vertical is a 20log(k + jꙍ) Magnitude plot in 1st part
• The vertical access is tan-1(jꙍ/k) Phase plot in 2nd part
• Most of the times, we take all k’s common from the tf and thus we use
1+jꙍ/k instead k+jꙍ,
• The common terms are multiplied with Constant gain portion so the overall
effect on the graph is none.
• It is calculated for a transfer function of
H(w) = Gain* Polynomial(Zeros)/ Polynomial( Poles)
Zeros, Poles and Gains
• The zeros are on the top of transfer function (tf) equation (numerators) so the
magnitude is positive elevation
• Poles are the denominator of tf equation so are negative depressions on graph
• Two polos or Zeros at the same value makes the elevation or depression doubled
• A pair of a pole and a zero cancels out the effect on graph
• When a pole or zero is already drawn, and a second pole or stars its effect, the
previous depression or elevation is effected and thus a composite plot is formed.
• Constant terms with H(w) such as Gains are straight lines with a fixed magnitude.
• We add up all gains, poles and zeros to get our overall plot
Drawing a Zero on Bode plot
• A zero has 20dB/decade elevation starting from its position.
• We always convert the zeros and poles to 1+jꙍ/k or 1+s/k form
• Before the value of s or jꙍ is reached on the x-axis, the 20log(1+jꙍ/k) is negligible because ꙍ is
small hence jꙍ/k is more small. Also 20log(1+0) is 0.
• If a zero is at origin, jꙍ=0, then it is a +20dB/decade increasing line, crossing ꙍ axis at 0
• It is an approximation and real plots may be more smooth due to continuous values.
Drawing a Pole on Bode plot
• A Pole has -20dB/decade depression starting from its position.
• We always convert the poles to 1+jꙍ/k or 1+s/k form
• Before the value of s or jꙍ is reached on the graph, the -20log(1+jꙍ/k) is negligible because ꙍ is
small jꙍ/k is more small. Also -20log(1+0) is 0.
• If a pole is at origin, jꙍ=0, then it is a -20dB/decade decreasing line, crossing ꙍ axis at 1
• Approximation encounters difference between plots
Drawing Phase in bode plot
• We calculate Phase by using tan-1(imaginary/real) method for individual terms in the tf.
• Phase of a constant term is 0 since the imaginary term in such case is zero.
• (jꙍ+0), jw=0 has a 90o phase, always, throughout the graph
• For zero, it is positive
• For pole it is negative
• jꙍ=k has a phase change of +90o or -90o between k and 10 x k
• If we consider a zero such as (1+jꙍ/k), the 0 to 90 degree phase inversion will start from k and will complete at 10k
• If we consider a pole such as (1+jꙍ/m), the 0 to -90 degree phase inversion will start from k and will complete at 10k
• The slope is 45o/decade
H(s) =
H(s) =
Book and Notes available at www.eedmd.weebly.com/ca2

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Varibale frequency response lecturer 2 - audio+

  • 1. Circuit Analysis – II (EE-201)Variable-frequency Networks Part 2
  • 2. Sinusoidal Frequency Analysis Bode plots to display frequency response data VARIABLE-FREQUENCY NETWORK PERFORMANCE LEARNING GOALS
  • 3. SINUSOIDAL FREQUENCY ANALYSIS )(sH Circuit represented by network function      )cos(0 )( 0   tB eA tj       )(cos|)(| )( 0 )( 0    jHtjHB ejHA tj )( )()( )()( |)(|)(     j eMjH jH jHM    Notation stics.characteriphaseandmagnitude calledgenerallyareoffunctionasofPlots  ),(),(M )(log )( ))(log20 10 10    PLOTSBODE vs (M    .offunctionaasfunctionnetworkthe analyzewefrequencytheoffunctionaasnetworkaofbehaviorthestudyTo )( jH
  • 4. HISTORY OF THE DECIBEL Originated as a measure of relative (radio) power 1 2 )2 log10(| P P P dB 1 Pover 2 1 2 2 2 1 2 2 )2 2 2 log10log10(| I I V V P R V RIP dB  1 Pover By extension ||log20| ||log20| ||log20| 10 10 10 GG II VV dB dB dB    Using log scales the frequency characteristics of network functions have simple asymptotic behavior. The asymptotes can be used as reasonable and efficient approximations
  • 5. Bode Plots • These are Magnitude and Phase based pair of plots • The Horizontal Access is always a logarithmic scale frequency (f or ꙍ) • The vertical is a 20log(k + jꙍ) Magnitude plot in 1st part • The vertical access is tan-1(jꙍ/k) Phase plot in 2nd part • Most of the times, we take all k’s common from the tf and thus we use 1+jꙍ/k instead k+jꙍ, • The common terms are multiplied with Constant gain portion so the overall effect on the graph is none. • It is calculated for a transfer function of H(w) = Gain* Polynomial(Zeros)/ Polynomial( Poles)
  • 6. Zeros, Poles and Gains • The zeros are on the top of transfer function (tf) equation (numerators) so the magnitude is positive elevation • Poles are the denominator of tf equation so are negative depressions on graph • Two polos or Zeros at the same value makes the elevation or depression doubled • A pair of a pole and a zero cancels out the effect on graph • When a pole or zero is already drawn, and a second pole or stars its effect, the previous depression or elevation is effected and thus a composite plot is formed. • Constant terms with H(w) such as Gains are straight lines with a fixed magnitude. • We add up all gains, poles and zeros to get our overall plot
  • 7. Drawing a Zero on Bode plot • A zero has 20dB/decade elevation starting from its position. • We always convert the zeros and poles to 1+jꙍ/k or 1+s/k form • Before the value of s or jꙍ is reached on the x-axis, the 20log(1+jꙍ/k) is negligible because ꙍ is small hence jꙍ/k is more small. Also 20log(1+0) is 0. • If a zero is at origin, jꙍ=0, then it is a +20dB/decade increasing line, crossing ꙍ axis at 0 • It is an approximation and real plots may be more smooth due to continuous values.
  • 8. Drawing a Pole on Bode plot • A Pole has -20dB/decade depression starting from its position. • We always convert the poles to 1+jꙍ/k or 1+s/k form • Before the value of s or jꙍ is reached on the graph, the -20log(1+jꙍ/k) is negligible because ꙍ is small jꙍ/k is more small. Also -20log(1+0) is 0. • If a pole is at origin, jꙍ=0, then it is a -20dB/decade decreasing line, crossing ꙍ axis at 1 • Approximation encounters difference between plots
  • 9. Drawing Phase in bode plot • We calculate Phase by using tan-1(imaginary/real) method for individual terms in the tf. • Phase of a constant term is 0 since the imaginary term in such case is zero. • (jꙍ+0), jw=0 has a 90o phase, always, throughout the graph • For zero, it is positive • For pole it is negative • jꙍ=k has a phase change of +90o or -90o between k and 10 x k • If we consider a zero such as (1+jꙍ/k), the 0 to 90 degree phase inversion will start from k and will complete at 10k • If we consider a pole such as (1+jꙍ/m), the 0 to -90 degree phase inversion will start from k and will complete at 10k • The slope is 45o/decade
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  • 16. Book and Notes available at www.eedmd.weebly.com/ca2