Why Does Current Reflect in an Antenna System?

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Discussion Overview

The discussion centers around the behavior of current in antenna systems, particularly focusing on the concepts of voltage standing wave ratio (VSWR), impedance mismatches, and the nature of reflections in transmission lines and dipole antennas. Participants explore theoretical and practical aspects of how current behaves in these systems, especially at high frequencies.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants express confusion about how parasitic capacitance in a dipole antenna completes the circuit while also leading to current reflections at open circuits.
  • There is a suggestion that reflections occur due to impedance mismatches between the feedline and antenna, with a matched system resulting in no reflections.
  • One participant questions the apparent contradiction of current flowing at high frequencies despite the open circuit condition, suggesting that the behavior resembles that of a capacitor.
  • Another participant describes the dipole as an LC circuit that resonates, with energy being radiated away at resonance, but reflects when driven off resonance.
  • Concerns are raised about the adequacy of transmission line theory in explaining these phenomena, with a call for a deeper understanding of how RF behaves compared to low-frequency AC.
  • A visual analogy is provided to illustrate how reflections occur in transmission lines based on the frequency of excitation and the physical characteristics of the line.
  • There is a distinction made between the behavior of antennas at resonance and the nature of breaks in transmission lines, with emphasis on the concept of antennas as matched loads.

Areas of Agreement / Disagreement

Participants do not reach a consensus, as there are multiple competing views regarding the behavior of current in antenna systems and the implications of impedance mismatches. The discussion remains unresolved with ongoing questions and clarifications sought by participants.

Contextual Notes

Limitations include the dependence on definitions of open circuits and impedance, as well as the unresolved nature of how high-frequency behavior contrasts with low-frequency expectations. The discussion also highlights the complexity of RF behavior in practical applications.

david845
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antenna circuit theory help!

Im having trouble understanding vswr and current path in an antenna system. Example is the dipole...Ive read that the parasitic capacitance between the 2 wires forms the complete circuit but then I read about standing waves that reflect at the open circuit. My questions are...if capacitance completes the circuit why does current reflect back ti the source? How does electric current reflect and travel a different direction without emf? If at higher frequencies an open circuit is not actually open then why does the current get reflected back? If current can't flow in an open circuit how the heck did it start flowing toward the load in the first place?
 
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david845 said:
Im having trouble understanding vswr and current path in an antenna system. Example is the dipole...Ive read that the parasitic capacitance between the 2 wires forms the complete circuit but then I read about standing waves that reflect at the open circuit. My questions are...if capacitance completes the circuit why does current reflect back ti the source? How does electric current reflect and travel a different direction without emf? If at higher frequencies an open circuit is not actually open then why does the current get reflected back? If current can't flow in an open circuit how the heck did it start flowing toward the load in the first place?

Welcome to the PF.

You only get a reflection back at the feedline/antenna terminal interface if there is a mismatch in the impedance between the Zo of the feedline cable and the input impedance of the antenna at the terminals. If they are matched, there is no reflection, and SWR = 1.

Do you know the feedpoint impedance of a dipole antenna at its fundamental resonance?
 


I do not know that at all. I am confused if its not an open circuit at high frequency then why does an impedence mismatch which is essentially like a partially open circuit reflect the current? It seems like the description is double edged sword "its not an open circuit at high frequency so current flows but at the open circuit junction the current gets reflected. I guess it is like a capacitor but its the fields were concerned about and not actual currents?
 


david845 said:
I do not know that at all. I am confused if its not an open circuit at high frequency then why does an impedence mismatch which is essentially like a partially open circuit reflect the current? It seems like the description is double edged sword "its not an open circuit at high frequency so current flows but at the open circuit junction the current gets reflected. I guess it is like a capacitor but its the fields were concerned about and not actual currents?

You can sort of think of the dipole as two inductors and a capacitor. Picture each element as an inductor, with a flat plate at the top that serves as half of the capacitor. The traveling RF wave coming down the coax feedline causes this LC circuit to resonate. But the antenna is lossy at its resonant frequiency, so the energy that is fed into it is radiated away.

If you drive it off resonance, some of that energy is not radiated, and is reflected back up the feedline, giving an SWR > 1.

It's probably best to start with standard transmission line theory first, to get a feel for why reflections occur at impedance mismatches in transmission lines:

http://en.wikipedia.org/wiki/Transmission_line

Have you had basic TL theory yet?
 


Yes...the thing is I fully understand what all the texts say but they do not accurately answer my question. You can't just say rf works that way as if it is magic. Rf is still alternating current from accelerating charges. Tl theory doesn't exactly pick up where basic theory left off it simply says a transmission lines behaves as such without making the comparison of how it would behave if it were low freq. Ac
 


To rephrase my question: if the open ends of a dipole behave like a capacitor that passes high frequency then why isn't the same true for current that reaches a break in the TL. Why does it reflect in the TL but radiate at the load when physically theyre the same thing 2 conductors separated by am insulator
 


david845 said:
Yes...the thing is I fully understand what all the texts say but they do not accurately answer my question. You can't just say rf works that way as if it is magic. Rf is still alternating current from accelerating charges. Tl theory doesn't exactly pick up where basic theory left off it simply says a transmission lines behaves as such without making the comparison of how it would behave if it were low freq. Ac
A pair of conductors becomes a transmission line when the length of the line approaches a significant fraction of a wavelength of the excitation waveform. Let me try to give you a visual illustration. Consider a semi-rigid piece of rubber tubing, say 1/4" in diameter and 10 meters long. You are holding one end of it as you are floating weightless in the International Space Station. You can slowly raise and lower your end of the tubing, and if you do it slowly enough, the far end will follow your movements. But as you do it faster and faster, what you see is a traveling wave that propagates down the line, and since the far end is unterminated/free, you get a positive reflection that comes back to you and can create a partial standing wave.

And if you tie the other end to the wall of the ISS, when you move your end very slowly, all you do is make an angle down the tubing to the anchored end. But when you move it more quickly up and down, you send waves down the tubing and the negative reflections from the fixed end (short) also can help to set up partial standing waves.

That is why the frequency of the excitation matters in TLs. If the excitation is slow enough that the TL looks like its lumped parameters, then there are no TL effects like reflections.

david845 said:
To rephrase my question: if the open ends of a dipole behave like a capacitor that passes high frequency then why isn't the same true for current that reaches a break in the TL. Why does it reflect in the TL but radiate at the load when physically theyre the same thing 2 conductors separated by am insulator
An antenna is not an open circuit at resonance. It is an LC tank circuit with 100% loss. A break in the TL is a discontinuity in the Zo of the TL. An antenna is a matched load for the Zo of the TL.

Antennas are not magic. They are very real, physical things. What books are you trying to study antennas from? Stutzman & Thiele (sp?) is my main antenna theory book.
 


Thanks for all the help I truly appreciate it!
 

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