Control Example

10
April 5, 2014 FAHEM_HW 06 Page 1 of 10 Problem -1- Solution: a) Transfer frequency function is : () b) Bode diagram : clc close s=tf('s') T=8; G=1/(T*s+1); bode(G) -40 -35 -30 -25 -20 -15 -10 -5 0 Magnitude (dB) System: G Frequency (rad/s): 0.125 Magnitude (dB): -3.01 10 -3 10 -2 10 -1 10 0 10 1 -90 -45 0 System: G Frequency (rad/s): 0.125 Phase (deg): -45 Phase (deg) Bode Diagram Frequency (rad/s) G

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  • April 5, 2014 FAHEM_HW 06

    Page 1 of 10

    Problem -1- Solution:

    a) Transfer frequency function is :

    ( )

    b) Bode diagram :

    clc

    close

    s=tf('s')

    T=8;

    G=1/(T*s+1);

    bode(G)

    -40

    -35

    -30

    -25

    -20

    -15

    -10

    -5

    0

    Ma

    gn

    itu

    de

    (d

    B)

    System: G

    Frequency (rad/s): 0.125

    Magnitude (dB): -3.01

    10-3

    10-2

    10-1

    100

    101

    -90

    -45

    0

    System: G

    Frequency (rad/s): 0.125

    Phase (deg): -45

    Ph

    as

    e (

    de

    g)

    Bode Diagram

    Frequency (rad/s)

    G

  • April 5, 2014 FAHEM_HW 06

    Page 2 of 10

    From the bode diagram the cutoff frequency is ( )

    Recall to the lecture:

    Discussion: I can get the from the figure by moving the cursor on the

    intersection point between the 45 deg. And the phase curve. Also this is the

    same result when I calculated this value theoretically. Also, at this point the low

    and high frequencies are equal.

    c)

    Form the bode diagram we choose two point in high frequency:

    Point -1- has:

    Point -2- has:

    Slope=

    ( )

    (

    )

    -80

    -70

    -60

    -50

    -40

    -30

    -20

    -10

    0

    Ma

    gn

    itud

    e (

    dB

    )

    System: G

    Frequency (rad/s): 10

    Magnitude (dB): -38.1

    System: G

    Frequency (rad/s): 100

    Magnitude (dB): -58.1

    10-1

    100

    101

    102

    103

    -90

    -60

    -30

    Ph

    as

    e (

    de

    g)

    Bode Diagram

    Frequency (rad/s)

  • April 5, 2014 FAHEM_HW 06

    Page 3 of 10

    Theoretically:

    The magnitude of first order system is :

    | |

    | |

    | | ( )

    | |

    | | ( )

    Then : | | | |

    d)

    Then: ( )

    ( )

  • April 5, 2014 FAHEM_HW 06

    Page 4 of 10

    -30

    -25

    -20

    -15

    -10

    -5

    0M

    ag

    nit

    ud

    e (

    dB

    )

    System: G

    Frequency (rad/s): 50.1

    Magnitude (dB): -3

    100

    101

    102

    103

    -90

    -45

    0

    System: G

    Frequency (rad/s): 50.3

    Phase (deg): -45

    Ph

    as

    e (

    de

    g)

    Bode Diagram

    Frequency (rad/s)

    G

  • April 5, 2014 FAHEM_HW 06

    Page 5 of 10

    Problem -2- Solution:

    a) Transfer frequency function is :

    ( )

    Bode diagram :

    clc

    close

    s=tf('s')

    T=5;

    G=2/(T*s+1);

    bode(G)

    From the figure the system bandwidth is : ( )

    -30

    -25

    -20

    -15

    -10

    -5

    0

    5

    10

    System: G

    Frequency (rad/s): 0.2

    Magnitude (dB): 3.01

    Ma

    gn

    itu

    de

    (d

    B)

    10-2

    10-1

    100

    101

    -90

    -45

    0

    System: G

    Frequency (rad/s): 0.2

    Phase (deg): -45Ph

    as

    e (

    de

    g)

    Bode Diagram

    Frequency (rad/s)

    G

  • April 5, 2014 FAHEM_HW 06

    Page 6 of 10

    b)

    s =

    RiseTime: 11.5109 SettlingTime: 19.5490

    SettlingMin: 1.7999

    SettlingMax: 1.9999

    Overshoot: 0

    Undershoot: 0

    Peak: 1.9999

    PeakTime: 50

    clc

    close

    s=tf('s')

    T1=5;

    t=0:0.001:50;

    figure(1)

    G1=2/(T1*s+1);

    step(G1,t);

    x=step(G1,t);

    S=stepinfo(x,t,'RiseTimeLimits',[0 0.9])

    figure(2)

    bode(G1)

    hold on

    T2=.5;

    G2=2/(T*s+1);

    bode(G2)

    0 5 10 15 20 25 30 35 40 45 500

    0.2

    0.4

    0.6

    0.8

    1

    1.2

    1.4

    1.6

    1.8

    2

    Step Response

    Time (seconds)

    Amplitu

    de

  • April 5, 2014 FAHEM_HW 06

    Page 7 of 10

    c)

    Then: ( )

    ( )

    -60

    -50

    -40

    -30

    -20

    -10

    0

    10

    20

    Ma

    gn

    itu

    de

    (d

    B)

    System: G2

    Frequency (rad/s): 50.3

    Magnitude (dB): 3.01

    System: G1

    Frequency (rad/s): 0.2

    Magnitude (dB): 3.01

    10-2

    10-1

    100

    101

    102

    103

    -90

    -45

    0

    Ph

    as

    e (

    de

    g)

    System: G2

    Frequency (rad/s): 50.3

    Phase (deg): -45

    System: G1

    Frequency (rad/s): 0.2

    Phase (deg): -45

    Bode Diagram

    Frequency (rad/s)

    G1

    G2

    T=0.5

    T=5

  • April 5, 2014 FAHEM_HW 06

    Page 8 of 10

    Problem -3- Solution :

    a) ( )

    ( )

    b) From the characteristic equation , we can find :

    -80

    -60

    -40

    -20

    0

    20

    Ma

    gn

    itu

    de

    (d

    B)

    10-1

    100

    101

    102

    -180

    -135

    -90

    -45

    0

    Ph

    as

    e (

    de

    g)

    Bode Diagram

    Frequency (rad/s)

    G

  • April 5, 2014 FAHEM_HW 06

    Page 9 of 10

    c)

    From the bode diagram

    d) the cutoff frequency from bode diagram is :

    -15

    -10

    -5

    0

    5

    10

    Ma

    gn

    itu

    de

    (d

    B)

    System: G

    Frequency (rad/s): 2.83

    Magnitude (dB): 8.93

    System: G

    Frequency (rad/s): 2.74

    Magnitude (dB): 9.17

    System: G

    Frequency (rad/s): 4.3

    Magnitude (dB): -3

    100.4

    100.5

    100.6

    100.7

    -180

    -135

    -90

    -45

    System: G

    Frequency (rad/s): 2.83

    Phase (deg): -90

    Ph

    as

    e (

    de

    g)

    System: G

    Frequency (rad/s): 2.74

    Phase (deg): -79.4

    System: G

    Frequency (rad/s): 4.3

    Phase (deg): -157

    Bode Diagram

    Frequency (rad/s)

    G

  • April 5, 2014 FAHEM_HW 06

    Page 10 of 10

    e) From the characteristic equation , and use FRF, we can

    calculate :

    And:

    ( )

    ( )

    Discussion:

    The result I got from these two methods (c and e), are very close.

    So, the frequency value and amplitude show me the real resonance ( )

    accrued before theoretical resonance states, also the system at real

    resonance state has bigger value of amplitude then theoretical value. As

    a result, the designer should give the good tension, because the

    systems maybe go to failure before it arrives to theoretical value of

    resonance.

    clc

    close

    s=tf('s')

    z=0.1768;

    wn=8^0.5

    G=wn^2/(s^2+2*z*wn*s+wn^2);

    bode(G)