circuits ii ee221 unit 4 instructor: kevin d. donohue

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Circuits II EE221 Unit 4 Instructor: Kevin D. Donohue Transfer Function, Complex Frequency, Poles and Zeros, and Bode Plots, Resonant Circuits

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Circuits II EE221 Unit 4 Instructor: Kevin D. Donohue. Transfer Function, Complex Frequency, Poles and Zeros, and Bode Plots, Resonant Circuits. Node Voltage Example. - PowerPoint PPT Presentation

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Page 1: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Circuits IIEE221

Unit 4Instructor: Kevin D. Donohue

Transfer Function, Complex Frequency, Poles and Zeros, and Bode Plots,

Resonant Circuits

Page 2: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Node Voltage Example Perform phasor analysis to determine vo(t). Since the frequency of the

source is not specified, leave impedances in terms of j = s. Express the phasor of vo(t) in terms of a product between a rational polynomial in s and the phasor of the input. Then substitute = 2 and solve for vo(t) .

Show that

Show v0(t) = .33cos(2t-9.46) V , when =2

vs(t) = cos(t) V

2 4

0.5 F 2 H+vo(t)

-

21

222

2

2 33tan90ˆ

9)3(ˆ

33ˆˆ

ssso VV

sssVV

Page 3: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Transfer Functions From the last example let:

Note that for s = j, the above function represents the phasor ratio of output to input for any :

Therefore, for any input magnitude, phase, and frequency of i the output can be determined by multiplying the input magnitude by and adding to the input phase. In this sense, describes how to transfer the input value to the output value.

33)(ˆ

2

ssssH

21

222

2

33tan90

9)3()(ˆ

)(ˆ)(ˆ

jHjVjV

s

o

)(ˆijH )(ˆ

ijH

)(ˆ sH

Page 4: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Transfer Functions Definition: A transfer function (TF) is a complex-valued

function of frequency associated with an input-output system, such that for a sinusoidal input and the TF evaluated at the input frequency, the TF magnitude indicates the scaling between the input and output magnitudes, and the TF phase indicates the phase shifting between the input and output phases.

The transfer function indicates this relationship for all input frequencies.

To find a transfer function, convert to impedance circuit, but leave the impedance values as functions of j=s. Then solve for the ratio of the phasor output divided by the phasor input.

Page 5: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Transfer Function ExampleDetermine the transfer function for the circuit below, where the input is vi(t) and the output is io(t).

Show transfer function is given by:

vi(t)

R1

R2C

io(t)

21

21

210

1

ˆˆ

)(ˆ

RCRRRs

RCRVIsHi

Page 6: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Transfer Function Example Determine the transfer function for the circuit below,

where the input is vi(t) and the output is vo(t).

Show transfer function is given by:

-

+

vi(t)

RfR1

Rh

C

+vo(t)

-

CRs

sRR

VVsH

h

i

f

i1

1

ˆˆ

)(ˆ 0

Page 7: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Evaluating/Plotting TFsThe following Matlab commands can be used to plot the results of the last TF. Let Rf = 50k, Ri = 10k , Rh=1.59k , C = 1FRf = 50e3; Ri = 10e3; Rh=1.59e3; C = 1e-6;f = [0:500]; % generate x-axis pointss = j*2*pi*f;h = (1+Rf/Ri)*s ./ (s + (1/(Rh*C))); % Evaluate TF at every pointfigure(1) % Plot Magnitudeplot(f,abs(h))xlabel('Hertz')ylabel('Magnitude')figure(2) % Plot Phase in Degreesplot(f,phase(h)*180/pi)xlabel('Hertz')ylabel('Degrees')

Page 8: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Resulting Plots

0 50 100 150 200 250 300 350 400 450 5000

20

40

60

80

100

Hertz

Degree

s

0 50 100 150 200 250 300 350 400 450 5000

1

2

3

4

5

6

Hertz

Magni

tude

Page 9: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

TF UnitsThere are 4 possible ratios of voltages and currents that can be used for a TF. List all possibilities and indicate the units for each one.

)(ˆ)(ˆ

)(ˆjVjVjH

in

out

)(ˆ)(ˆ

)(ˆjVjIjH

in

out)(ˆ)(ˆ

)(ˆjIjIjH

in

out

)(ˆ)(ˆ

)(ˆjIjVjH

in

out

Page 10: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Decibel ScaleA decibel is a logarithmic measure of gain (or attenuation). A power gain between the designated system input and output is denoted in Decibels (or dB) as:

Express power in terms of voltage over a load to get another version of the dB formula:

in

outdB P

PG 10log10

out

in

in

outdB

out

in

in

out

inin

outoutdB

RR

VVG

RR

VV

RVRVG

1010

2

2

102

2

10

log10log20

log10//log10

Page 11: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Decibel ScaleIf input and output impedances are considered equal (Rin= Rout) the formula reduces to:

Linear gain is always positive (between 0 and ). Describe the gain in dB when the system is attenuating. Describe the gain in dB when the linear gain is unity.

in

outdB V

VG 10log20

Page 12: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Bode Plot Bode plots provide information on the general behavior

of circuits over a broad range of frequencies and magnitudes where important features exist.

A Bode plot of a TF shows the magnitude in dB and phase in degrees on a frequency scale over the range where all important features exist.

Important features of the plot include resonances, nulls, transitions between pass and stop bands, and asymptotic gains (not flat regions that do not change!).

Page 13: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Bode Plot (with Matlab) Before building our understanding on how to manipulate TF

polynomials for convenient plotting, consider using Matlab to generate the plot from polynomials evaluated over a complex field.

Matlab functions behave like a subroutine in a main program. Specify input and output arguments for your function (subroutine). Only the input and output arguments exist in the Matlab workspace or main program. Help information for the function is the first set of comments you include after the function definition. These comments must provide all user needs to know in order to use it properly. At the Matlab prompt, typing >> help “function name” will display these comments.

Example: Create a Matlab function that evaluates a TF based on its polynomial coefficients. Generate a script that calls this function to show how it works.

Page 14: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Matlab Example For a function, start the first line with the word

“function” followed by the function syntax (input and output arguments). Comments immediately following this first line will be used as the “help” for this function and must show the complete syntax on how to use function along with descriptions of input and output. An example of how to call the function is helpful in the comments as well.

First line of text file when creating a function

function p = tfeval(ns, ds, f)

Page 15: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Matlab ExampleThe file should be saved with the same name as the function as defined in the first line. In this case it would be saved as “tfeval.m’

function p = tfeval(ns, ds, f)

% This function evaluates a transfer function for a given frequency(s)% p = tfeval(ns, ds, f)% where NS => the vector representing the numerator polynomial% DS => the vector representing the denominator polynomial% F => vector of frequency values in Hz at which the TF is% to be evaluated% P => vector of TF values corresponding to F.% ns(1)*s^N + ns(2)*s^(N-1) ...+ ns(N)*s^1 + ns(N+1)% H(s) = ---------------------------------------------------% ds(1)*s^M + ds(2)*s^(M-1) ...+ ds(M)*s^1 + ds(M+1)

Page 16: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Matlab ExampleContinued ….% Example:% for linear frequency evaluation% >> freq = [0:10:10000]; % Frequency points% >> numc = [10 0]; % Numerator coefficients% >> denc = [1 5000*2*pi]; % Denominator coefficients % >> tf = tfeval(numc, denc, freq); % Compute complex TF points% >> figure; plot(f,abs(p)); ylabel('Magnitude') % Plot magnitude% >> figure; plot(f,angle(p)*180/pi); ylabel('Degrees') % Plot Phase%% Updated by Kevin D. Donohue ( [email protected] ) February 1, 2010

num_order = length(ns)-1; % Determine order of numeratorden_order = length(ds)-1; % Determine order of denominator s = 2j*pi*f; % Create s vector for evaluating TF

Page 17: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Matlab ExampleContinued … % Loop to sum up every term in numerator sumn = zeros(size(s)); % Initialize accumulation variablefor k=1:num_order+1 sumn = sumn + ns(k)*s.^(num_order-k+1);end % Loop to sum up every term in numerator sumd = zeros(size(s)); % Initialize accumulation variablefor k=1:den_order+1 sumd = sumd + ds(k)*s.^(den_order-k+1);end p = sumn ./ sumd; % Divide numerator and denominator points

Page 18: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Matlab Example Test Script The following script will create the input variables for the function

and plot the output.% This scripts demonstrates the TFEVAL function by evaluating% a transfer function at many points and plotting the result% on both a linear and log scale% Updated by Kevin D. Donohue ( [email protected] ) 2/1/2010

% Generate 1000 points equally spaced on a Log Scale from% 20 to 20kHzf = logspace(log10(20),log10(20000),1000);% 3*s% H(s) = --------------------------------% s^2 + 1.81k*s + 900Mnu = [3 0]; % Numerator polynomialde = [1, 1.81e3, 900e6]; % Denominator polynomialtf = tfeval(nu, de, f); % Evaluate Transfer function

Page 19: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Matlab ExampleContinued …

figure(1)% Plot result on a linear scaleplot(f,abs(tf)) % Plot magnitudetitle('Transfer Function Example - Linear')xlabel('Hertz')ylabel('TF magnitude') figure(2)plot(f,phase(tf)*180/pi) % Plot phasetitle('Transfer Function Example - Linear Scale')xlabel('Hertz')ylabel('TF phase (degrees)')

Page 20: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Matlab ExampleContinued …

figure(3)% Plot result on a log scalesemilogx(f,20*log10(abs(tf))) % Plot magnitudetitle('Transfer Function Example - Log (dB) scale')xlabel('Hertz')ylabel('TF magnitude in dB') figure(4)semilogx(f,phase(tf)*180/pi) % Plot phasetitle('Transfer Function Example - Log Scale')xlabel('Hertz')ylabel('TF phase (degrees)')

Page 21: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Plot ResultsLinear Scales

0 0.5 1 1.5 2 2.5

x 104

-100

-50

0

50

100Transfer Function Example - Linear Scale

Hertz

TF p

hase

(deg

rees

)0 0.5 1 1.5 2 2.5

x 104

0

0.5

1

1.5

2x 10

-3 Transfer Function Example - Linear

Hertz

TF m

agni

tude

Page 22: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Plot ResultsBode Plots (Log Scales)

101

102

103

104

105

-140

-120

-100

-80

-60

-40Transfer Function Example - Log (dB) scale

Hertz

TF m

agni

tude

in d

B

101

102

103

104

105

-100

-50

0

50

100Transfer Function Example - Log Scale

Hertz

TF p

hase

(deg

rees

)

Page 23: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Plot RangesThe interesting parts of the plot occurs near the roots of the numerator (zeros) and denominator (poles). The only exception to this is roots at zero (which actually correspond to negative infinity on a log scale). So by doing an analysis of the roots of the TF, the plot range can be determined by starting a decade before the smallest root magnitude and going a decade after the largest root magnitude.

Example: Graph the magnitude and phase of the transfer function. Create both a linear scaled plot and a log (Bode) scaled plot.

45

146

54

)(23

2

sss

ssH

Page 24: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Plot RangesThe following Matlab script can be used to determine plot range:% Define range for w% Find poles:ps = roots([1, 6, (14/5), 4]); % Vector of polynomial coefficients% ps will be a vector containing the poles% Find zeroszs = roots([(4/5), 0, 0]); % Vector containing polynomial% coefficients, zs will be a vector containing the roots

% Find maximum magnitude pole and zerofend1 = max(abs(ps)) % fend1 will be the maximum of the % magnitudes of ps. (fend1 = 5.6288)fend2 = max(abs(zs)) % fend2 will be the maximum of the % magnitudes of zs. (fend2 = 0)

Page 25: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Plot Ranges% Pick maximum value between the two (5.6 in this case), round up to the% next decade (which is 10) and increment to next decade (100 in this case)

% Find minimum magnitude pole and zerofbeg1 = min(abs(ps)) % fbeg1 is the minimum of the magnitudes of ps.%% (fbeg1 = 0.8430)fbeg2 = min(abs(zs) % fbeg2 is the minimum of the magnitudes of zs.%% (fbeg2 = 0)% Pick the minimum non-zero value between the two (.84 in this case),% round down to next decade (which .1) and decrement to next decade% (.01 in this case).

% Now create the w-axis vector with 201 equally spaced points% on a log (base 10) scale:w = logspace(-2, 2, 201); % w is now a vector of points from 10^-2 to 10^2 % Note that the transfer function is computed for s=j*w, therefore assign:s=j*w; % now s is a vector of imaginary numbers (j=sqrt(-1) by default)% Now evaluate the transfer function at all points defined by s:h = (4/5)*s.^2 ./ (s.^3 + 6*s.^2 + (14/5)*s + 4);

Page 26: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Plot Ranges% Plot magnitude on semilog axis in decibels:figure(1)semilogx(w, 20*log10(abs(h)))grid % Add gridlines to the plotxlabel('Radians per Second') % Add x-axis labelylabel('TF Magnitude in Decibels') % Add y-axis label

% Plot phase on semilog axis in degrees:figure(2)% angle return in radians, convert to phase.semilogx(w, (180/pi)*(angle(h)))grid % Add gridlines to the plotxlabel('Radians per Second') % Add x-axis labelylabel('TF Phase in Degrees') % Add y-axis label

Page 27: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Plot Results

10-2

10-1

100

101

102

-100

-80

-60

-40

-20

0

Radians per Second

TF M

agni

tude

in D

ecib

els

10-2

10-1

100

101

102

-100

-50

0

50

100

150

200

Radians per Second

TF P

hase

in D

egre

es

Plot output (Log)

Page 28: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Plot Ranges% For the linear plot redefine the range for w, the interesting part% looks like it's between .1 and 20.% So create a new w-axis:wl= [0:0.1:20]; % This creates and array of points starting at 0 % and goes up to 20 in increments of 0.1s=j*wl;h = (4/5)*s.^2 ./ (s.^3 + 6*s.^2 + (14/5)*s + 4);% Now Create a linear plot for the magnitude:figure(3)plot(wl, abs(h))grid % Add gridlines to the plotxlabel('Radians per Second') % Add x-axis labelylabel('TF Magnitude') % Add y-axis label% Now Create a linear plot for the phase:figure(4)plot(wl, angle(h))grid % Add gridlines to the plotxlabel('Radians per Second') % Add x-axis labelylabel('TF Phase') % Add y-axis label

Page 29: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Plot ResultsPlot output (linear)

0 5 10 15 200

0.05

0.1

0.15

0.2

0.25

0.3

0.35

Radians per Second

TF M

agni

tude

0 5 10 15 20-2

-1

0

1

2

3

4

Radians per Second

TF P

hase

Page 30: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Complex Frequency Since the poles and zeros of a transfer function can be complex (having a real and imaginary part), the s variable in the transfer function is referred to as complex frequency:

So a full plot of the TF is over the entire real and imaginary values in the complex number plane. For now we will only be concerned with evaluating the TF on the j axis (i.e. = 0).

js

Page 31: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Bode SketchesBode plots are also useful for generating simple sketches of the transfer function due to the dB scale, which converts mulplicative factors to additive terms.

Recall logarithmic relationship:

21121

1 logloglog))((

log pspszspsps

zs

Page 32: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Bode SketchesTransfer function sketches can be performed by knowing the shape of 4 basic factors that any transfer function can be decomposed into:

constant factors non-zero real pole or zeros factors pole or zero factors at zero complex conjugate pole or zero factors

Sketches are simplified by only considering asymptoticbehavior of each factor (i.e. as and as 0).

The phase and magnitude for each factor can be sketched individually and summed together in the final step.

Page 33: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Bode SketchesSketch the Bode plot of the transfer function:Show for magnitude sketch in dB:

Show for phase sketch:

10010)100(10)(ˆ

2

sssssH

1100

1010

log201100

log20log2010log20)(ˆlog202

jjjjjH

2040

-20-40

1 10 100 1000

|H(j)| dB

4590

-45-90

1 10 100 1000

H(j)

1

10010

101

10010)(ˆ

2 jjjjjH

Page 34: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

ResonanceResonance occurs when the capacitive and inductive reactance is equal in magnitude, leaving a purely resistive impedance.Resonance results in a maximum (or minimum) point on the transfer function magnitude.The Bandwidth (B) is the distance between the frequencies where the amplitude is down by a factor of from the maximum. These frequencies are sometimes called the half power points.

100

101

102

103

104

105

106

0

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.9

1

Hertz

Am

plitu

de

Half PowerPoints

Bandwidth B

Resonance

2

Page 35: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Quality Factor

The Quality Factor (Q) is the ratio of the resonant frequency to its bandwidth.

BQ o

Page 36: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Resonant Circuit Example

Find 0 , B, Q, and the gain at resonance (G0) in terms of the circuit parameters where the input is vi(t) and the output is io(t).Show:

where (B and 0 are in Radians/Second)

Note: This formula set is only valid for this circuit. Similar formulae must be derived for different resonant circuits.

In general a 2nd order resonant circuit can always be put in the form:

22)(ˆo

o

BssBsGsH

vi(t)io(t)

1 LC1

o RLQ

RG

LRB o

o

Page 37: Circuits II EE221 Unit 4 Instructor:  Kevin D. Donohue

Resonant Circuit ExampleFind 0 , B, Q, and the gain at resonance (G0) in terms of the circuit parameters where the input is ii(t) and the output is vo(t):

Show:

(B and 0 are in Radians/Second)

Note: This formula set is only valid for this circuit (Sometimes called a tank circuit). Similar formulae must be derived for different resonant circuits.

ii(t) R C L+vo(t)_

01 1

LC

BRC

R Q = RCL

Go