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Microwave Hybrid
Circuits
MR. HIMANSHU DIWAKAR
Assistant Professor
JETGI
MR. HIMANSHU DIWAKAR JETGI 1
MICROWAVE HYBRID CIRCUITS
• A microwave circuit ordinarily consists of several microwave
devices connected in some way to achieve the desired
transmission of a microwave signal.
• The interconnection of two or more microwave devices may
be regarded as a microwave junction.
MR. HIMANSHU DIWAKAR JETGI 2
Commonly used microwave junctions include
such waveguide tees as
• E-plane tee,
• H -plane tee,
• Magic tee,
• Hybrid ring (rat-race circuit),
• Directional coupler,
• The circulator.
MR. HIMANSHU DIWAKAR JETGI 3
E-plane tee H-plane tee
MR. HIMANSHU DIWAKAR JETGI 4
Magic tee, Hybrid ring
MR. HIMANSHU DIWAKAR JETGI 5
Directional coupler, Circulator
MR. HIMANSHU DIWAKAR JETGI 6
S parameters (the heart of RF/MW
measurements)
• A two-port network is shown in Fig. From network theory a two-port
device can be described by a number of parameter sets, such as the H,
Y, Z, and ABCD parameters.
MR. HIMANSHU DIWAKAR JETGI 7
• All these network parameters relate total voltages and total currents at
each of the two ports. For instance,
• If the frequencies are in the microwave range, however, the H, Y, and
Z parameters cannot be measured for the following reasons:
MR. HIMANSHU DIWAKAR JETGI 8
a) Equipment is not readily available to measure total voltage and total
current at the ports of the network.
b) Short and open circuits are difficult to achieve over a broad band of
frequencies.
c) Active devices, such as power transistors and tunnel diodes,
frequently will not have stability for a short or open circuit i.e.
unstable system.
MR. HIMANSHU DIWAKAR JETGI 9
Consequently, some new method of characterization
is needed to overcome these problems.
• The logical variables to use at the microwave frequencies are traveling
waves rather than total voltages and total currents. These are the S
parameters, which are expressed as
MR. HIMANSHU DIWAKAR JETGI 10
Waveguide Tees
• Tee junctions: In microwave circuits a waveguide or coaxial-line
junction with three independent ports is commonly referred to as a tee
junction.
• A tee junction should be characterized by S matrix of third order
containing nine elements, six of which should be independent.
MR. HIMANSHU DIWAKAR JETGI 11
The characteristics of a three-port junction can be
explained by three theorems
• 1. A short circuit may always be placed in one of the arms of a three-
port junction in such a way that no power can be transferred through
the other two arms.
• 2. If the junction is symmetric about one of its arms, a short circuit can
always be placed in that arm so that no reflections occur in power
transmission between the other two arms. (That is, the arms present
matched impedances.)
• 3. It is impossible for a general three-port junction of arbitrary
symmetry to present matched impedances at all three arms.
MR. HIMANSHU DIWAKAR JETGI 12
E-plane tee (series tee).
• An E-plane tee is a waveguide tee in which the axis of its side arm is
parallel to the E field of the main guide.
• If E-plane tee is perfectly matched the diagonal components of the
scattering matrix, 𝑆11, 𝑆22, 𝑎𝑛𝑑 𝑆33 are zero because there will be no
reflection.
• 𝑆13 = −𝑆23 -----(1)
MR. HIMANSHU DIWAKAR JETGI 13
Cont’d
• It should be noted that Eq. (1) does not mean that S13 is always
positive and S23 is always negative. The negative sign merely means
that SB and S23 have opposite signs. For a matched junction, the S
matrix is given by
• From the symmetry property of S matrix
𝑆12 = 𝑆21, 𝑆13 = 𝑆31, 𝑆23 = 𝑆32-----(2)
MR. HIMANSHU DIWAKAR JETGI 14
Cont’d
• From the zero property of S matrix, the sum of the products of each
term of any column (or row) multiplied by the complex conjugate of
the corresponding terms of any other column (or row) is zero
MR. HIMANSHU DIWAKAR JETGI 15
Cont’d
• However, from the unity property of S matrix
𝑆21 𝑆21
∗
+ 𝑆31 𝑆31
∗
= 1 −−− −(3)
𝑆12 𝑆12
∗
+ 𝑆32 𝑆32
∗
= 1 −−− −(4)
𝑆13 𝑆13
∗
+ 𝑆23 𝑆23
∗
= 1 −−− −(5)
From eq.(2) put in (3) ----------(6)
Eq. (5) and (6) are contradictory for if 𝑆13 = 0 𝑡ℎ𝑒𝑛 𝑆23 is also Zero.
MR. HIMANSHU DIWAKAR JETGI 16
Cont’d
• In Similar fashion, if 𝑆23 = 0 𝑡ℎ𝑒𝑛 𝑆13 is also Zero and Therefore
eq.(6) is not true.
• This inconsistency proves the statement that the diagonal elements of
the S matrix of a tee junction are not all zeros.
• In general, when an E-plane tee is constructed of an empty waveguide,
it is poorly matched at the tee junction
MR. HIMANSHU DIWAKAR JETGI 17
Cont’d
• Hence 𝑆𝑖𝑗 ≠ 0 if i = j. However, since the collinear arm is usually
symmetric about the side arm, 𝑆13 = 𝑆23 and 𝑆11 = 𝑆22. Then the S
matrix can be simplified to
MR. HIMANSHU DIWAKAR JETGI 18
H-plane tee (shunt tee)
• An H-plane tee is a waveguide tee in which the axis of its side arm is
"shunting" the E field or parallel to the H field of the main guide as
shown in Fig.
MR. HIMANSHU DIWAKAR JETGI 19
Cont’d
• It can be seen that if two input waves are fed into port 1 and port
2 of the collinear arm, the output wave at port 3 will be in phase
and additive.
• On the other hand, if the input is fed into port 3, the wave will
split equally into port 1 and port 2 in phase and in the same
magnitude.
• Therefore the S matrix of the H-plane tee is similar to E-plane
tee. Except that
𝑆13 = 𝑆23
MR. HIMANSHU DIWAKAR JETGI 20
Magic Tees (Hybrid Tees)
• A magic tee is a combination of the E-plane tee and H -plane tee
MR. HIMANSHU DIWAKAR JETGI 21
Cont’d
1. If two waves of equal magnitude and the same phase are fed
into port 1 and port 2, the output will be zero at port 3 and
additive at port 4.
2. If a wave is fed into port 4 (the Harm), it will be divided
equally between port 1 and port 2 of the collinear arms and
will not appear at port 3 (the E arm).
MR. HIMANSHU DIWAKAR JETGI 22
Cont’d
1. If a wave is fed into port 3 (the E arm), it will produce an output of
equal magnitude and opposite phase at port 1 and port 2. The output
at port 4 is zero. That is, 𝑆43 = 𝑆34 = 0.
2. If a wave is fed into one of the collinear arms at port 1 or port 2, it
will not appear in the other collinear arm at port 2 or port 1 because
the E arm causes a phase delay while the Harm causes a phase
advance. That is, 𝑆12 = 𝑆21 = 0.
MR. HIMANSHU DIWAKAR JETGI 23
• Therefore the S matrix of a magic tee can be expressed as
• The magic tee is commonly used for mixing, duplexing, and
impedance measurements.
MR. HIMANSHU DIWAKAR JETGI 24
For example
• Suppose, there are two identical radar transmitters in equipment stock.
• A particular application requires twice more input power to an antenna
than either transmitter can deliver.
• A magic tee may be used to couple the two transmitters to the antenna
in such a way that the transmitters do not load each other.
MR. HIMANSHU DIWAKAR JETGI 25
Cont’d
• The two transmitters should be connected to ports 3 and 4,
respectively, as shown in Fig. Transmitter 1, connected to port 3,
causes a wave to emanate from port 1 and another to emanate from
port 2;
MR. HIMANSHU DIWAKAR JETGI 26
Magic tee-coupled transmitters to antenna.
Cont’d
• These waves are equal in magnitude but opposite in phase. Similarly,
transmitter 2, connected to port 4, gives rise to a wave at port 1 and
another at port 2, both equal in magnitude and in phase.
• At port 1 the two opposite waves cancel each other. At port 2 the two
in-phase waves add together; so double output power at port 2 is
obtained for the antenna as shown in above Fig.
MR. HIMANSHU DIWAKAR JETGI 27
Hybrid Rings (Rat-Race Circuits)
• A hybrid ring consists of an
annular line of proper
electrical length to sustain
standing waves, to which
four arms are connected at
proper intervals by means of
series or parallel junctions.
• Figure shows a hybrid ring
with series junctions.
MR. HIMANSHU DIWAKAR JETGI 28
Cont’d
• The hybrid ring has characteristics similar to those of the hybrid tee.
• When a wave is fed into port 1, it will not appear at port 3 because the
difference of phase shifts for the waves traveling in the clockwise and
counterclockwise directions is 180°.
• Thus the waves are canceled at port 3. For the same reason, the waves
fed into port 2 will not emerge at port 4 and so on.
MR. HIMANSHU DIWAKAR JETGI 29
Cont’d
• The S matrix for an ideal hybrid ring can be
MR. HIMANSHU DIWAKAR JETGI 30
Thank you
MR. HIMANSHU DIWAKAR JETGI 31

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Microwave Hybrid Circuits S-Parameters

  • 1. Microwave Hybrid Circuits MR. HIMANSHU DIWAKAR Assistant Professor JETGI MR. HIMANSHU DIWAKAR JETGI 1
  • 2. MICROWAVE HYBRID CIRCUITS • A microwave circuit ordinarily consists of several microwave devices connected in some way to achieve the desired transmission of a microwave signal. • The interconnection of two or more microwave devices may be regarded as a microwave junction. MR. HIMANSHU DIWAKAR JETGI 2
  • 3. Commonly used microwave junctions include such waveguide tees as • E-plane tee, • H -plane tee, • Magic tee, • Hybrid ring (rat-race circuit), • Directional coupler, • The circulator. MR. HIMANSHU DIWAKAR JETGI 3
  • 4. E-plane tee H-plane tee MR. HIMANSHU DIWAKAR JETGI 4
  • 5. Magic tee, Hybrid ring MR. HIMANSHU DIWAKAR JETGI 5
  • 6. Directional coupler, Circulator MR. HIMANSHU DIWAKAR JETGI 6
  • 7. S parameters (the heart of RF/MW measurements) • A two-port network is shown in Fig. From network theory a two-port device can be described by a number of parameter sets, such as the H, Y, Z, and ABCD parameters. MR. HIMANSHU DIWAKAR JETGI 7
  • 8. • All these network parameters relate total voltages and total currents at each of the two ports. For instance, • If the frequencies are in the microwave range, however, the H, Y, and Z parameters cannot be measured for the following reasons: MR. HIMANSHU DIWAKAR JETGI 8
  • 9. a) Equipment is not readily available to measure total voltage and total current at the ports of the network. b) Short and open circuits are difficult to achieve over a broad band of frequencies. c) Active devices, such as power transistors and tunnel diodes, frequently will not have stability for a short or open circuit i.e. unstable system. MR. HIMANSHU DIWAKAR JETGI 9
  • 10. Consequently, some new method of characterization is needed to overcome these problems. • The logical variables to use at the microwave frequencies are traveling waves rather than total voltages and total currents. These are the S parameters, which are expressed as MR. HIMANSHU DIWAKAR JETGI 10
  • 11. Waveguide Tees • Tee junctions: In microwave circuits a waveguide or coaxial-line junction with three independent ports is commonly referred to as a tee junction. • A tee junction should be characterized by S matrix of third order containing nine elements, six of which should be independent. MR. HIMANSHU DIWAKAR JETGI 11
  • 12. The characteristics of a three-port junction can be explained by three theorems • 1. A short circuit may always be placed in one of the arms of a three- port junction in such a way that no power can be transferred through the other two arms. • 2. If the junction is symmetric about one of its arms, a short circuit can always be placed in that arm so that no reflections occur in power transmission between the other two arms. (That is, the arms present matched impedances.) • 3. It is impossible for a general three-port junction of arbitrary symmetry to present matched impedances at all three arms. MR. HIMANSHU DIWAKAR JETGI 12
  • 13. E-plane tee (series tee). • An E-plane tee is a waveguide tee in which the axis of its side arm is parallel to the E field of the main guide. • If E-plane tee is perfectly matched the diagonal components of the scattering matrix, 𝑆11, 𝑆22, 𝑎𝑛𝑑 𝑆33 are zero because there will be no reflection. • 𝑆13 = −𝑆23 -----(1) MR. HIMANSHU DIWAKAR JETGI 13
  • 14. Cont’d • It should be noted that Eq. (1) does not mean that S13 is always positive and S23 is always negative. The negative sign merely means that SB and S23 have opposite signs. For a matched junction, the S matrix is given by • From the symmetry property of S matrix 𝑆12 = 𝑆21, 𝑆13 = 𝑆31, 𝑆23 = 𝑆32-----(2) MR. HIMANSHU DIWAKAR JETGI 14
  • 15. Cont’d • From the zero property of S matrix, the sum of the products of each term of any column (or row) multiplied by the complex conjugate of the corresponding terms of any other column (or row) is zero MR. HIMANSHU DIWAKAR JETGI 15
  • 16. Cont’d • However, from the unity property of S matrix 𝑆21 𝑆21 ∗ + 𝑆31 𝑆31 ∗ = 1 −−− −(3) 𝑆12 𝑆12 ∗ + 𝑆32 𝑆32 ∗ = 1 −−− −(4) 𝑆13 𝑆13 ∗ + 𝑆23 𝑆23 ∗ = 1 −−− −(5) From eq.(2) put in (3) ----------(6) Eq. (5) and (6) are contradictory for if 𝑆13 = 0 𝑡ℎ𝑒𝑛 𝑆23 is also Zero. MR. HIMANSHU DIWAKAR JETGI 16
  • 17. Cont’d • In Similar fashion, if 𝑆23 = 0 𝑡ℎ𝑒𝑛 𝑆13 is also Zero and Therefore eq.(6) is not true. • This inconsistency proves the statement that the diagonal elements of the S matrix of a tee junction are not all zeros. • In general, when an E-plane tee is constructed of an empty waveguide, it is poorly matched at the tee junction MR. HIMANSHU DIWAKAR JETGI 17
  • 18. Cont’d • Hence 𝑆𝑖𝑗 ≠ 0 if i = j. However, since the collinear arm is usually symmetric about the side arm, 𝑆13 = 𝑆23 and 𝑆11 = 𝑆22. Then the S matrix can be simplified to MR. HIMANSHU DIWAKAR JETGI 18
  • 19. H-plane tee (shunt tee) • An H-plane tee is a waveguide tee in which the axis of its side arm is "shunting" the E field or parallel to the H field of the main guide as shown in Fig. MR. HIMANSHU DIWAKAR JETGI 19
  • 20. Cont’d • It can be seen that if two input waves are fed into port 1 and port 2 of the collinear arm, the output wave at port 3 will be in phase and additive. • On the other hand, if the input is fed into port 3, the wave will split equally into port 1 and port 2 in phase and in the same magnitude. • Therefore the S matrix of the H-plane tee is similar to E-plane tee. Except that 𝑆13 = 𝑆23 MR. HIMANSHU DIWAKAR JETGI 20
  • 21. Magic Tees (Hybrid Tees) • A magic tee is a combination of the E-plane tee and H -plane tee MR. HIMANSHU DIWAKAR JETGI 21
  • 22. Cont’d 1. If two waves of equal magnitude and the same phase are fed into port 1 and port 2, the output will be zero at port 3 and additive at port 4. 2. If a wave is fed into port 4 (the Harm), it will be divided equally between port 1 and port 2 of the collinear arms and will not appear at port 3 (the E arm). MR. HIMANSHU DIWAKAR JETGI 22
  • 23. Cont’d 1. If a wave is fed into port 3 (the E arm), it will produce an output of equal magnitude and opposite phase at port 1 and port 2. The output at port 4 is zero. That is, 𝑆43 = 𝑆34 = 0. 2. If a wave is fed into one of the collinear arms at port 1 or port 2, it will not appear in the other collinear arm at port 2 or port 1 because the E arm causes a phase delay while the Harm causes a phase advance. That is, 𝑆12 = 𝑆21 = 0. MR. HIMANSHU DIWAKAR JETGI 23
  • 24. • Therefore the S matrix of a magic tee can be expressed as • The magic tee is commonly used for mixing, duplexing, and impedance measurements. MR. HIMANSHU DIWAKAR JETGI 24
  • 25. For example • Suppose, there are two identical radar transmitters in equipment stock. • A particular application requires twice more input power to an antenna than either transmitter can deliver. • A magic tee may be used to couple the two transmitters to the antenna in such a way that the transmitters do not load each other. MR. HIMANSHU DIWAKAR JETGI 25
  • 26. Cont’d • The two transmitters should be connected to ports 3 and 4, respectively, as shown in Fig. Transmitter 1, connected to port 3, causes a wave to emanate from port 1 and another to emanate from port 2; MR. HIMANSHU DIWAKAR JETGI 26 Magic tee-coupled transmitters to antenna.
  • 27. Cont’d • These waves are equal in magnitude but opposite in phase. Similarly, transmitter 2, connected to port 4, gives rise to a wave at port 1 and another at port 2, both equal in magnitude and in phase. • At port 1 the two opposite waves cancel each other. At port 2 the two in-phase waves add together; so double output power at port 2 is obtained for the antenna as shown in above Fig. MR. HIMANSHU DIWAKAR JETGI 27
  • 28. Hybrid Rings (Rat-Race Circuits) • A hybrid ring consists of an annular line of proper electrical length to sustain standing waves, to which four arms are connected at proper intervals by means of series or parallel junctions. • Figure shows a hybrid ring with series junctions. MR. HIMANSHU DIWAKAR JETGI 28
  • 29. Cont’d • The hybrid ring has characteristics similar to those of the hybrid tee. • When a wave is fed into port 1, it will not appear at port 3 because the difference of phase shifts for the waves traveling in the clockwise and counterclockwise directions is 180°. • Thus the waves are canceled at port 3. For the same reason, the waves fed into port 2 will not emerge at port 4 and so on. MR. HIMANSHU DIWAKAR JETGI 29
  • 30. Cont’d • The S matrix for an ideal hybrid ring can be MR. HIMANSHU DIWAKAR JETGI 30
  • 31. Thank you MR. HIMANSHU DIWAKAR JETGI 31