cad techniques for rf electromagnetics

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    CAD TECHNIQUES FOR RF ELECTROMAGNETICS

    EXPERIMENT 01, NETWORK ANALYSER

    INTRODUCTION:

    The main objective of the experiment is to measure the S-parameters. S-parameters

    have got an important position in the field of RF Electromagnetics. S-parameters

    measurements are complex functions of frequency and are used for high-frequency

    measurements, for example microwave design etc. S-parameters are defined and

    measured with the ports terminated in characteristic reference impedance. Modern

    network analyzers are well suited for measuring S-parameters. Because the networksbeing analyzed are often employed by insertion in a transmission medium with

    common characteristic reference impedance, S-parameters have the additional

    advantage that they relate directly to commonly specified performance parameters

    such as insertion gain and return loss. S-parameters can be easily measured using an

    s-parameter test set. S-Parameters are the reflection and transmission coefficient of

    waves, normalized to the incident wave. They describe the input/output behaviour of a

    device under linear conditions at microwave frequencies. S-parameters are measured

    based on properly terminated transmission lines (and not open/short Circuit

    conditions).

    Network analyzers have become one of the most important measurement tools for

    characterizing the performance of high-frequency components and devices.

    We used Hewlett Packard HP8720 Network Analyser to measure the S-parameters for

    some simple devices. Beside this tool we used one another important tool, which is

    coaxial cable with small SMA connectors. It should be remember that these cables

    cannot be correctly mated unless tightened by a spanner (but not over tightened),

    although hand tight is not good.

    THEORY

    RESULT

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    1. Amplitude response for matched load

    -45

    -40

    -35

    -30

    -25

    -20

    -15

    -10

    -5

    0

    0 5E+ 09 1E +10 1.5E +1

    0

    2E+10 2.5E+1

    0

    Series1

    Series2

    DB

    HZ

    2. Amplitude open circuit

    -5

    -4

    -3

    -2

    -1

    0

    1

    2

    3

    4

    0 5E +09 1 E+ 10 1.5E+ 1

    0

    2E+10 2.5E+1

    0

    Series1

    Series2

    db

    hz

    3. Phase open circuit

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    -2.50E+02

    -2.00E+02

    -1.50E+02

    -1.00E+02

    -5.00E+01

    0.00E+00

    5.00E+01

    1.00E+02

    1.50E+02

    2.00E+02

    2.50E+02

    0 5E+0

    9

    1E+1

    0

    2E+1

    0

    2E+1

    0

    3E+1

    0

    Series1

    Series2

    dg

    HZ

    4. Phase matched load (106)

    -6.00E+01

    -4.00E+01

    -2.00E+01

    0.00E+00

    2.00E+01

    4.00E+01

    6.00E+01

    8.00E+01

    1.00E+02

    1.20E+02

    1.40E+02

    1.60E+02

    0 5E+0

    9

    1E+1

    0

    2E+1

    0

    2E+1

    0

    3E+1

    0

    Series1

    Series2

    HZ

    DG

    5. Amplitude response RF cable 107

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    Amplitude Response

    -30

    -25

    -20

    -15

    -10

    -5

    0

    0 5E +09 1E+ 10 1.5E +1

    0

    2E+10 2.5E+1

    0

    f(Hz)

    db dB

    6. Forward Amplitude Response S11 jpg 00

    7. Forward phase response S21 text109

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    Forward Phase Response S21

    -40

    -30

    -20

    -10

    0

    0 5E +09 1E+ 10 1.5E+1

    0

    2E+10 2.5E+1

    0

    f(Hz)

    dg dB

    8. Reverse Amplitude Response S12

    Reverse Amplitude Response S12

    -40

    -30

    -20

    -10

    0

    0 5E+ 09 1E+10 1.5E+ 1

    0

    2E+10 2.5E+1

    0

    Hz

    db dB

    9. Reverse phase response S22

    Reverse Phase Response S22

    -60

    -50

    -40

    -30

    -20

    -10

    0

    0 5E+09 1E+10 2E+10 2E+10 3E+10

    Hz

    dg dB

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    PART TWO

    REFLECTION AND TRANSMISSION TEST SET

    TRANSMISSION MEASUREMENT

    In this section, we will investigate the transmission properties of a microwave

    waveguide device. This is would be important in the design of microwave system to

    ensure that the device operates correctly.

    1. Attenuator at 0 dB, attenuation is 2.044 dB, Frequency 10GHz

    Value of attenuation at 10 GHz

    -14

    -12

    -10

    -8

    -6

    -4

    -2

    0

    2

    0 5000000000 1E+10 1.5E+10

    Hz

    dB dB

    2. Attenuator 10 dB, Attenuation is 10.97dB, Frequency 10GHz

    Value of attenuation at 10 GHz

    -25

    -20

    -15

    -10

    -5

    0

    0 5000000000 1E+10 1.5E+10

    Hz

    dB dB

    3. Attenuator 20 dB, Attenuation is 28.00, at 10GHz

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    Value of Attenuation at 10 GHz

    -50

    -40

    -30

    -20

    -10

    0

    0 5E+09 1E+10 1.5E+10

    Hz

    dB dB

    .

    4. Attenuator at 0 db and phase shifter range is set to 0 at 10 GHz frequencies theresponse would be 2.2030 dB

    5. Attenuator at 0 dB, phase shift range is set to 5, frequency 10 GHz the response

    would be 1.1080

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    6. Attenuator at 0 dB, phase shift range is set to 10 dB, frequency at 10 GHz the

    response would be 1.7070

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    7. Attenuator at 10 dB, phase shift range is set to 0 dB, frequency at 10 GHz the

    response would be 12.220 dB

    8. Attenuator at 10 dB, phase shift range is set to 5 dB, frequency at 10 GHz the

    response would be 11.992 dB

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    9. Attenuator at 10 dB, phase shift range is set to 10 dB, frequency at 10 GHz the

    response would be 11.697dB

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    10. Attenuator at 20 dB, phase shift range is set to 0 dB, frequency at 10 GHz the

    response would be 27.628dB

    11. Attenuator at 20 dB, phase shift range is set to 5 dB, frequency at 10 GHz the

    response would be 27.608dB

    12. Attenuator at 20 dB, phase shift range is set to 5 dB, frequency at 10 GHz theresponse would be 27.006dB

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