Performance of a complimentary antenna?

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Discussion Overview

The discussion revolves around the performance of complementary antennas, exploring their properties, relationships, and theoretical underpinnings. Participants examine concepts such as Babinet's Principle, input impedance, radiation patterns, and the implications of self-complementary antennas. The scope includes theoretical considerations and practical applications in antenna design.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants inquire about the specific aspects of performance being considered, such as drive impedance or radiation patterns.
  • Babinet's Principle is referenced as a foundational concept relating the input impedance of an antenna and its complement, with examples provided for specific antenna types.
  • There is mention of uncertainty regarding the exact replication of radiation patterns between complementary antennas, particularly between dipoles and slots.
  • Some participants discuss the self-complementary antenna, noting its symmetric properties and specific input impedance, while others clarify that their focus is not on self-complementary antennas.
  • The near-field behavior of complementary antennas is examined, with observations about how electric and magnetic fields behave differently as one approaches the antennas.
  • Concerns are raised about the assumption of total equivalence between complementary antennas, with references to the principle of reciprocity and its limitations in close proximity scenarios.

Areas of Agreement / Disagreement

Participants express a range of views, with some agreeing on the relevance of Babinet's Principle while others question its applicability to antenna performance. There is no consensus on the equivalence of complementary antennas, as differing opinions on their radiation patterns and properties persist.

Contextual Notes

Limitations include the dependence on specific definitions of performance and the unresolved nature of certain mathematical relationships between complementary antennas. The discussion also highlights the complexity of near-field interactions and the challenges in applying theoretical principles to practical scenarios.

qnach
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Suppose the performance of an antenna is calculated.
How about its complimentary antenna?
 
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An antenna and its complement are related by Babinet's Principle, which was originally devised for simple problems with light.
The input impedance, for instance, of the two antennas is related by 2 x SQRT(Z1 x Z2) = Zo, where Zo is 377 Ohms, the intrinsic impedance of free space. For instance, a strip dipole might have an input impedance of 70 Ohms. Its complement will be a slot having the same dimensions and cut in a large sheet of metal. The input impedance across the centre of the slot will be 507 Ohms.
The radiation pattern of one antenna in its E-plane should be the same as the other in its H-plane. However, there is a little uncertainty about this because a half wave slot does not seem to replicate a dipole pattern exactly.
In his book "Antennas", J D Kraus introduces the term "Magnetic Dipole" for antennas which are complementary to a dipole. By this he meant that the E plane pattern of a dipole resembles the H plane pattern of a slot or loop. Unfortunately, this has led to some confusion over the radiation mechanism of the two. For both classes of antenna, radiation is caused by the acceleration of electrons.
 
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tech99 said:
An antenna and its complement are related by Babinet's Principle, which was originally devised for simple problems with light.
The input impedance, for instance, of the two antennas is related by 2 x SQRT(Z1 x Z2) = Zo, where Zo is 377 Ohms, the intrinsic impedance of free space. For instance, a strip dipole might have an input impedance of 70 Ohms. Its complement will be a slot having the same dimensions and cut in a large sheet of metal. The input impedance across the centre of the slot will be 507 Ohms.
The radiation pattern of one antenna in its E-plane should be the same as the other in its H-plane. However, there is a little uncertainty about this because a half wave slot does not seem to replicate a dipole pattern exactly.
In his book "Antennas", J D Kraus introduces the term "Magnetic Dipole" for antennas which are complementary to a dipole. By this he meant that the E plane pattern of a dipole resembles the H plane pattern of a slot or loop. Unfortunately, this has led to some confusion over the radiation mechanism of the two. For both classes of antenna, radiation is caused by the acceleration of electrons.

You mentioned impedance and the radiation pattern of such antenna. How about other properties?
I did not found much study in the web about complementary antenna.
Babinet's Principle seems more about diffraction pattern instead of antenna performance?
 
qnach said:
Suppose the performance of an antenna is calculated.
How about its complimentary antenna?
By performance, do you mean the drive impedance or the radiation pattern?

qnach said:
Babinet's Principle seems more about diffraction pattern instead of antenna performance?
The radiation pattern of an array of elements is important. This becomes very important with arrays of slots in a waveguide, such as often used for marine radar antennas. Are you only interested in single elements and their complement?

There is an elegant design, halfway between the electric-dipole and it's complement, the magnetic-slot.
That special case is the self-complementary antenna, where the conductor and space are symmetric in pattern.
The self-complementary antenna has an input impedance of 376.73 / 2 = 188.365 ohm.
http://bbs.hwrf.com.cn/downrf/self-complementary Antenna.pdf
 
Baluncore said:
By performance, do you mean the drive impedance or the radiation pattern?The radiation pattern of an array of elements is important. This becomes very important with arrays of slots in a waveguide, such as often used for marine radar antennas. Are you only interested in single elements and their complement?

There is an elegant design, halfway between the electric-dipole and it's complement, the magnetic-slot.
That special case is the self-complementary antenna, where the conductor and space are symmetric in pattern.
The self-complementary antenna has an input impedance of 376.73 / 2 = 188.365 ohm.
http://bbs.hwrf.com.cn/downrf/self-complementary Antenna.pdf

There are many self-complementary antenna on the web.
However, I am not talking about self-complementary antenna.
 
qnach said:
You mentioned impedance and the radiation pattern of such antenna. How about other properties?
What other properties are there that you are interested in?
 
Baluncore said:
What other properties are there that you are interested in?

Everything we can calculated from an antenna.
 
  • #10
qnach said:
Everything we can calculated from an antenna.
The near fields also seem to be complementary. For instance, if we approach a dipole along the equatorial plane, when we get closer than about lambda/6, the power flux density no longer grows with 1/D^2 but flattens off until we reach the antenna. The E-field remains uniform from lambda/6 until we almost touch the antenna, whilst the B field continues upward with 1/D. But for a slot antenna, the opposite happens; the E field grows with 1/D whilst the B field remains constant as the antenna is approached.
If we bring two dipoles towards each other, the loss between them is reaches 3dB approx. at a spacing of lambda/6 and then flattens off and is still 3dB when they touch. But I am sad to say, with a slot and a dipole, once they touch the same thing does not happen.
 
  • #11
A bit of a necropost but I have to wonder what fundamental laws are being used to lead one to expect that a 'similarity' is several respects (Kraus) should demand that there would be total equivalence. I know that this complementary idea is always taught in EM courses but that doesn't mean there should be any significant principle involved.
The principle of Reciprocity tells us that transmit and receive antennae could be interchanged and the loss over any path would be the same but reciprocity has to run out of steam once the antennae are near enough together. We also tend to analyse antennae as either Transmit or Receive, depending on which suits us and we assume the patterns will come out right.
 
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  • #12
sophiecentaur said:
A bit of a nectar post but I have to wonder what fundamental laws are being used to lead one to expect that a 'similarity' is several respects (Kraus) should demand that there would be total equivalence. I know that this complementary idea is always taught in EM courses but that doesn't mean there should be any significant principle involved.
The principle of Reciprocity tells us that transmit and receive antennae could be interchanged and the loss over any path would be the same but reciprocity has to run out of steam once the antennae are near enough together. We also tend to analyse antennae as either Transmit or Receive, depending on which suits us and we assume the patterns will come out right.
The reciprocity idea seems hard to disprove. For instance, if I have two dipoles very close to one another, the loss between them is fixed at approx 3dB. As the antennas are identical, I measure 3dB whichever way round I do the test.
Regarding complementary antennas, it is based on Babinet's Principle with additional work by Booker. However, I have a nagging doubt about it as a slot does not seem to have exactly the same pattern as an equivalent dipole.
 
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  • #13
tech99 said:
However, I have a nagging doubt about it as a slot does not seem to have exactly the same pattern as an equivalent dipole.
For a slot to have the same pattern as a dipole requires the slot be cut in an infinite conductive sheet. But the sheet will not be truly infinite, so external peripheral currents will flow that distort the field. Likewise a wire dipole will not be in free space, so nearby conductive structures will distort the dipole's field in ways different to the periphery of a slot's actual conductive sheet.
An ideal slot antenna exists as a portal between two semi-infinite universes. Half the energy is radiated into each half of free space.
 

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