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Fig. 9.0.1 Typical waveguiding structures
Choice of structure is dictated by: (a) the desired operating frequency band, (b) the amount of
power to be transferred, and (c) the amount of transmission losses that can be tolerated.
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“forward-wave” coupler - if the coupled signal is traveling in the same direction as the through signal.
“backward-wave” coupler -if in opposition to the “forward-wave” coupler.
-is the desirable or undesirable transfer of energy from
one medium, such as a metallic wire or an optical fiber,
to another medium. Microwave couplers are devices
which divert a fraction of the signal on one transmission
line to another transmission line.
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-is to ensure a smooth mechanical junction and suitable electrical characteristics,
particularly low external radiation and low internal reflections.
Plain Flange Flange Coupling
At higher frequencies a much flatter
butted plain flange is used
At lower frequencies the flange will be
brazed or soldered onto the waveguide,
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-consisting of an ordinary flange and a choke flange connected together. The choke
flange is frequency-sensitive, but optimum design can ensure a reasonable bandwidth
(perhaps 10 % of the center frequency) over which SWR does not exceed 1.05.
b.) End view of Choke Flange
a.) Cross section of Choke Coupling
9.
10. Waveguide/Impedance Matching is often
necessary to reduce reflections caused by a
mismatch between the waveguide and the load. The
waveguide impedance can be determined by taking
the ratio of the electric field to the magnetic field at
the center of the waveguide.
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1
𝑍0 =
377
1−(
𝜆
2𝑎
)2
𝛀 (17.8)
Where:
λ = free space wavelength
a= larger dimension of the interior cross section
Or
𝑍0 =
377
1−(
𝑓 𝑐
𝑓
)2
𝛀 (17.9)
Where:
fc = cutoff frequency
f = operating frequency
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2
𝜈 = 𝑓𝜆
𝜆 𝑔 =
𝜈 𝑝
𝑓
(17.10)
Where, 𝜈 𝑝 = phase velocity
𝜆 𝑔 = waveguide wavelength
Given with the free space wavelength 𝜆,
𝜆 𝑔 =
𝜆
1−(
𝜆
2𝑎
)2
(17.11)
And
𝜆 𝑔 =
𝜆
1−(
𝑓 𝑐
𝑓
)2
(17.12)
14. Use of a
waveguide
post or screw
Use of a
Waveguide Iris
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Use of gradual
changes in
dimensions of
waveguide.
15. Inductive Waveguide Iris
-placed within the electric field
Capacitive Waveguide Iris
-portions across both the magnetic
and electric fields.
Inductive and Capacitive
Waveguide Iris
-placed within the magnetic field
16. -used to give a similar effect
like the iris and thereby
provide waveguide
impedance matching.
17. -A decrease in intensity of energy to
spreading of energy, transmission line
losses or path losses between two
antennas
• Due to losses in the conducting
walls of the waveguide
• Due to the shunt conductivity of the
dielectric filling in the waveguide
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Types of Waveguide bends:
a.) Waveguide E bends b.) Waveguide H bends c.) Waveguide Twist
-Used to direct high frequency signals propagating
through a waveguide in a specific direction. These bends
allow the change in direction of a signal within a
waveguide, with minimal loss, reflection and distortion of
the electric and magnetic fields.
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Waveguide E bends
An E-bend changes or distorts the E-Field (Electric
Field) of the propagating signal. In order to minimize
reflections, the radius of the bend should be greater
than two wavelengths of the signal.
Waveguide Sharp E bends
The techniques is to use a 45° bend in the waveguide.
Effectively the signal is reflected, and using a 45° surface
the reflections occur in such a way that the fields are left
undisturbed, although the phase is inverted and in some
applications this may need accounting for or correcting
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This for of waveguide bend is the same as the
sharp E bend, except that the waveguide bend
affects the H field rather than the E field.
An H-bend changes or distorts the H-Field
(Magnetic Field) of the propagating signal. In
order to minimize reflections, the radius of the
bend should be greater than two wavelengths of
the signal.
Waveguide Sharp H bendsWaveguide H bends
22. Waveguide twists are also useful in many applications to ensure the polarisation is correct.
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There are two main types of Waveguide Tees:
a.) E-Plane Waveguide Tee b.) H-Plane Waveguide Tee c.) Hybrid Waveguide Tee
-a 3-port device that can be used to either
divide or combine two or more signals in a waveguide
system. It is formed when three waveguides tubes are
connected in the form of the English alphabet 'T'. This
is where its name is derived from.
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E-Plane Waveguide Tee
When the axis of the side arm is parallel to the
Electric Field (E) of the collinear, then the tee is called
a E-Plane Tee Junction. The outputs we get in this
type of tee are 180° out of phase with each other,
irrespective of from which port the input is fed.
When the axis of the side arm of the waveguide tee is
parallel to the flow of the Magnetic Field (H) from port 1
and is perpendicular to the flow of the Electric Field (E),
then the tee is called a H-Plane Waveguide Tee.
H-Plane Waveguide Tee
A waveguide is essentially a pipe through which an EM wave travels. As it travels along the guide, it reflects from the walls.
Most high power microwave energy transmission above about 6GHz is handled by waveguides.
It can be used to carry energy between pieces of equipment or over longer distances to carry transmitter power to an antenna or microwave signals from an antenna to a receiver
-are made of copper, aluminum, or brass
Waveguides are used to transfer electromagnetic power efficiently from one point in space to another. Some common guiding structures are shown in the figure.
These include the typical coaxial cable, the two-wire and mictrostrip transmission lines, hollow conducting waveguides, and optical fibers.
The signal exiting the output port of the first transmission line is called the “through” (sometimes called the “direct”) signal since it is directly connected to the input port and the signal exiting the other transmission line is called the “coupled” signal.
Because these coupled signals are related to the direction of the through signals, couplers are called directional couplers.
Port 1 and 2 is your primary waveguide. “through” (sometimes called the “direct”)
3 and 4 is the secondary waveguide. “coupled” signal
Directional couplers are characterized by their insertion loss, coupling, and directivity. All three are normally specified in decibels.
Insertion Loss - is the amount by which a signal in the main guide is attenuated.
Coupling - is the specification that gives the amount by which the signal in the main waveguide is greater than that coupled to the secondary waveguide.
Directivity-Refers to the ratio between the power coupled to the secondary guide, for signals traveling in the two possible directions along the main guide.
Waveguide Coupling is generally by means of some sort of flange. The function of such flange is to ensure…
A typical piece of waveguide will have a flange at either end.
When two pieces are joined, the flanges are bolted together, to ensure perfect mechanical alignment if adjustment is provided. This prevents an unwanted bend or step, either of which would produce undesirable reflections. It follows that the guide ends and flanges must be smoothly finished to avoid discontinuities at the junction.
With Waveguide Coupling naturally reduced in size when frequencies are raised, a coupling discontinuity becomes larger in proportion to the signal wavelength and the guide dimensions.
Thus discontinuities at higher frequencies become more troublesome.
To compensate for the discontinuity which would otherwise be present, a small gap circular choke ring of L cross section is used in the choke flange, in order to reflect a short
circuit at the junction of the waveguides. This is possible because the total length of the ring cross section, as shown, is λp/2, and the far end is short-circuited. Thus an electrical short circuit is placed at a surface where a mechanical short circuit would be difficult to achieve.
Reflections in a waveguide system cause impedance mismatches.
When this happens, the solution is identical to the one that would be employed for transmission lines: lumped impedance or stubs.
In transmission lines there is a need of matching Impedance for maximum power transfer.
That is in Microwave, a lumped
impedance of required value is placed at a precalculated point in the waveguide to overcome the mismatch, canceling the effects of the reflections.
Similarly, If the waveguide impedance is matched to the source or load, then a greater level of power transfer will occur.
When waveguides are not accurately matched to their loads, standing waves appear, and not all the power is transferred.
To overcome the mismatch it is necessary to use some waveguide impedance matching techniques.
Like any transmission line, a waveguide has a characteristic impedance.
Characteristic impedance of a waveguide is a function of frequency.
377 ohms comes from the intrinsic empedance (eta 𝜼) in free space in which 𝜼 = 𝝻 0 𝞊 𝑜
There are two velocities in a waveguide, and both change with frequency.
Uses a probe resembling a quarter-wave monopole antenna. The probe couples to the electric field in the guide, and it should therefore be located at an electric field maximum.
Shows another way to couple power to a guide. A loop is used to couple with the magnetic field in the guide. It is placed in a location of maximum magnetic field.
Is simply to put a hole in the waveguide, so that electromagnetic energy can propagate into or out of the guide from the region exterior to it.
It is found that abrupt changes in a waveguide will give rise to a discontinuity that will create standing waves. However gradual changes
in impedance do not cause this.
This approach is used with horn antennas - these are funnel shaped antennas that provide the waveguide impedance match between the waveguide itself and free space by gradually expanding the waveguide dimensions.
Matching Devices or Waveguide Irises
Inductive Iris: The iris places a shunt inductive reactance across the waveguide that is directly proportional to the size of the opening. Notice that the edges of the inductive iris are perpendicular to the magnetic plane.
Capacitive Waveguide Iris: The shunt capacitive reactance, illustrated in view (B), basically acts the same way. Again, the reactance is directly proportional to the size of the opening but the edges of the iris are perpendicular to the electric plane.
Inductive and Capacitive Waveguide Iris: The iris, illustrated in view (C), has portions across both the magnetic and electric planes and forms an equivalent parallel-LC circuit across the waveguide. At the resonant frequency, the iris acts as a high shunt resistance. Above or below resonance, the iris acts as a capacitive or inductive reactance.
In addition to using a waveguide iris, post or screw can also be used to give a similar effect and thereby provide waveguide impedance
matching. The waveguide post or screw is made from a conductive material.
To make the post or screw inductive, it should extend through the
waveguide completely making contact with both top and bottom walls.
For a capacitive reactance the post or screw should only extend part of the way through.
When a screw is used, the level can be varied to adjust the waveguide to the right conditions
The attenuators are basically passive devices which control power levels in microwave system by absorpsion of the signal. Attenuator which attenuates the RF signal in a waveguide system is referred as waveguide attenuator. There are two main types fixed and variable. They are achieved by insertion of resistive films.
Using waveguides require some passive components that are used with feed-lines.
E-bend: The bend must have a radius greater than two wavelengths.
H-Bend: It creates a bend around the thinner side of the waveguide. This also must have a radius greater than two times the wavelength.
The bend angle is usually 30 degrees, 45 degrees or 90 degrees, however this can be customized based on the requirement. When selecting the waveguide bend the waveguide size and the flange type need to be selected - these usually vary based on the frequency at which you are planning to use the specific waveguide bend.
Waveguide Twist
There are also instances where the waveguide may require twisting. This too, can be accomplished. If a complete inversion is required, e.g. for phasing requirements, the overall inversion or 180° twist should be undertaken over a four wavelength distance.
used to change the signal polarization.
E-Plane Waveguide Tee: Also called series tee.
• If a signal is applied to port C, the output will appear at port A and B
but half the power and the same phase.
• If two input waves at port A and B are in phase, the output at port C is additive and in phase
H-Plane Waveguide Tee: Also called shunt tee.
• Input at port D has an equal output at port A and B but 1800 out of phase
Hybrid tee - Magic tee
•It can provide an isolation between signal.
•If two in-phase and equal signals are fed to port A and B, cancellation will be in port D but reinforcement in port C. Similarly, if energy is fed to port C, energy appears at port A and B but not port D.