How Does High-Frequency Affect the Line Equation in AC Circuits?

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Discussion Overview

The discussion revolves around the behavior of alternating currents at high frequencies in AC circuits, specifically focusing on the high-frequency line equation and the roles of inductance, capacitance, resistance, and conductance in this context. Participants explore theoretical aspects, derivations, and implications of these parameters in transmission lines.

Discussion Character

  • Homework-related
  • Technical explanation
  • Exploratory

Main Points Raised

  • Some participants suggest that at very-high frequencies, the inductor's high reactance leads it to behave almost like an open circuit, potentially allowing the resistance to be ignored.
  • There is a question regarding whether the quantities L, C, R, and G are defined per unit length, which some participants confirm.
  • Participants request a derivation of the high-frequency line equation and discuss the arrangement of R and G in relation to L and C, referencing the Characteristic Impedance model.
  • Concerns are raised about the interpretation of current flow in the presence of high reactance, with a clarification that current does flow in transmission lines despite the high impedance of inductors.
  • One participant mentions the need to compare the impedance of R and L per unit length, as well as C and G, to justify the neglect of R in high-frequency scenarios.
  • There is a discussion about calculating the impedance for G, with a note that G represents parasitic parallel leakage conductance, which is typically small.

Areas of Agreement / Disagreement

Participants express varying views on the implications of high-frequency behavior on the circuit parameters, particularly regarding the neglect of resistance and the role of conductance. The discussion remains unresolved with multiple competing perspectives on these points.

Contextual Notes

Participants highlight the importance of understanding the definitions and arrangements of the circuit components, as well as the frequency dependence of the parameters involved. There are unresolved aspects regarding the derivation of equations and the specific values for typical transmission lines.

CalvinB
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Homework Statement


Show that in the case of alternating currents of high frequencies the equation

attachment.php?attachmentid=30513&stc=1&d=1291853375.jpg


can be approximated by the so-called high-frequency line equation

attachment.php?attachmentid=30514&stc=1&d=1291853392.jpg


L = Inductance, C = Capacitance, R = Resistance, G = Conductance

Homework Equations


At very-high frequencies the inductor has a high reactance and acts almost like an open circuit. Thus, the current is low, so the resistance can be ignored (correct me if i am wrong :P). But how about G?
 

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CalvinB said:

Homework Statement


Show that in the case of alternating currents of high frequencies the equation

attachment.php?attachmentid=30513&stc=1&d=1291853375.jpg


can be approximated by the so-called high-frequency line equation

attachment.php?attachmentid=30514&stc=1&d=1291853392.jpg


L = Inductance, C = Capacitance, R = Resistance, G = Conductance

Homework Equations


At very-high frequencies the inductor has a high reactance and acts almost like an open circuit. Thus, the current is low, so the resistance can be ignored (correct me if i am wrong :P). But how about G?


First, I think that those 4 quantities (L, C, R and G) are per unit length, right?

Second, can you show how the first equation is derived?

Third, the R term is in series with the L term, and the G term is in parallel with the C term? Like in the Characteristic Impedance Zo model:

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

And if you want to say that the R term is negligible, you need to say that in contrast to the value of the impedance of the L term, not say that no current flows, since certainly current flows in a transmission line. Look at the impedance of the R resistance per unit length versus the impedance of the L inductance per unit length of a typical transmission line cable (like Cat-5). Do a similar comparison of impedances for C and G...
 
Last edited:
berkeman said:
First, I think that those 4 quantities (L, C, R and G) are per unit length, right?

Second, can you show how the first equation is derived?

Third, the R term is in series with the L term, and the G term is in parallel with the C term? Like in the Characteristic Impedance Zo model:

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

And if you want to say that the R term is negligible, you need to say that in contrast to the value of the impedance of the L term, not say that no current flows, since certainly current flows in a transmission line. Look at the impedance of the R resistance per unit length versus the impedance of the L inductance per unit length of a typical transmission line cable (like Cat-5). Do a similar comparison of impedances for C and G...


I do have the first equation derived. I tried to type it in here, but somehow the Latex Reference keep messing up my equations >:(

And yes, since the problem did not clearly state how the RLCG are placed, i assumed they are like the Characteristic Impedance Zo model.

Since the impedance of L depends on the frequency, as the frequency increases, the impedance of L increases, so R can be neglected because the frequency does not change the resistance.(Again, correct me if I'm wrong :P) But how do i calculate the impedance for G?
 
CalvinB said:
Since the impedance of L depends on the frequency, as the frequency increases, the impedance of L increases, so R can be neglected because the frequency does not change the resistance.(Again, correct me if I'm wrong :P) But how do i calculate the impedance for G?

I would start with the values of L', C', R', and G' (the primes often are used to indicate that the quantity is per unit length, like per meter or per foot) for a typical transmission line cable, like Cat-5 or RG-58. That will give you some numbers that you can use to justify your simplification of the equation, and will let you calculate a reasonable frequency for starting to use the 2nd equation in your post.

The G' value is basically the parasitic parallel leakage conductance, and is typically quite small.
 

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