Waveguide discontinuity with centered circular aperture

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SUMMARY

The discussion centers on a rectangular waveguide discontinuity featuring a centered circular aperture, analyzed under the Edge Theorem. The theorem states that field components parallel to an edge are diffracted without generating new components, while orthogonal components can generate new field components. The fundamental TE10 mode is examined, revealing interactions among field components EY, HZ, and HX, leading to a complex six-component field. The conversation highlights the need for further exploration of the generation of components HY and EX, which remain unclear.

PREREQUISITES
  • Understanding of waveguide theory and modes, specifically TE10 mode.
  • Familiarity with the Edge Theorem in electromagnetic theory.
  • Knowledge of microwave engineering principles, particularly regarding discontinuities.
  • Ability to interpret field component interactions in waveguides.
NEXT STEPS
  • Research the Edge Theorem and its applications in waveguide analysis.
  • Study the generation of field components in waveguide discontinuities.
  • Examine the concept of Bethe holes and their relevance in microwave engineering.
  • Explore Marcuvitz's Microwave Handbook for insights on equivalent circuits and field interactions.
USEFUL FOR

Electromagnetic engineers, microwave engineers, and researchers focusing on waveguide design and analysis, particularly those interested in field component interactions and discontinuities.

EmilyRuck
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Hello!
This is the first time I write in the forum. I hope to be fully in-topic.
I'm dealing with a rectangular waveguide discontinuity: a perfect-conductor plane orthogonal to the propagation direction, with a circular aperture in the centre of the guide section. The structure is symmetrical along the x-axis and the y-axis and I drew it in the attachment, where the z axis is outgoing from the screen.
In my note the professor talked about a strange "Edge Theorem" (which we didn't demonstrate and which I can't find in any book). The Theorem says that:
- a field component which is parallel to an edge is diffracted but not folded (and so it doesn't generate any new field component);
- a field component which is orthogonal to an edge is diffracted and folded along the plane perpendicular to the edge (so it could generate a new field component).
The discontinuity is reached by the fundamental TE10 mode: in my coordinate system, it has EY, HX and HZ field components.
According to the Theorem, when EY reaches the upper and the lower part of the circle (points A and D in the picture) it is orthogonal to the circle edge and it generates an EZ component.
When HZ reaches the left and the right part of the circle (points B and C in the picture) it generates HX; similarly, in those points HX generates HZ.
But what about HY and EX? I can't see how they are generated, but they are, because I wrote in my notes that the field becomes a 6-components field.
The only electric field component is EY, but when it reaches the oblique edge between A and B, it generates an EZ again and not an EY! What is wrong?
Thank you anyway!
Bye,

Emily
 

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I don't have a copy of the article, but Hans Bethe wrote a paper during the War on microwave couplers using small holes. These later became referred to as Bethe holes. See http://prola.aps.org/abstract/PR/v66/i7-8/p163_1.
I would also look in Marcuvitz's Microwave Handbook..
 
Bob S said:
I don't have a copy of the article, but Hans Bethe wrote a paper during the War on microwave couplers using small holes. These later became referred to as Bethe holes.
I would also look in Marcuvitz's Microwave Handbook..

I tried to read the article but it's not available, unfortunately. Thank you anyway for your reference! I read also the Marcuvitz's Microwave Handbook: it deals with such a discontinuity, but it considers just the equivalent circuit (an admittance) and not which field components arise from it.

Emily
 
Most likely this can only be answered by an "old timer". I am making measurements on an uA709 op amp (metal can). I would like to calculate the frequency rolloff curves (I can measure them). I assume the compensation is via the miller effect. To do the calculations I would need to know the gain of the transistors and the effective resistance seen at the compensation terminals, not including the values I put there. Anyone know those values?

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