Transmission lines and Waveguides

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Discussion Overview

The discussion revolves around the relationship between transmission lines (TLs) and waveguides, specifically focusing on how they transmit electromagnetic (EM) waves and AC signals. Participants explore the nature of data transmission in coaxial cables and the implications of current and voltage in these contexts.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants assert that waveguides are specifically for transmitting EM waves, mentioning modes such as TEM, TE, and TM.
  • Others question the nature of transmission lines, noting that they can carry both AC signals (voltage or current) and EM waves, particularly in coaxial cables.
  • One participant suggests that the data entering a TV from a coax cable could be interpreted as either the voltage/current waveform or the EM waveform, raising questions about their relationship.
  • Another participant emphasizes that the EM wave travels through the dielectric of the coax, and that the current observed is a result of boundary conditions related to the H field.
  • It is noted that the apparent current flow in a coax cable is due to the rapid propagation of the EM wave rather than the slow movement of electrons.
  • Participants discuss the definition of current and voltage at terminals along the transmission line, indicating that while these values can be defined at every point, they are not always useful for describing propagation without considering the full fields.
  • One participant reinforces that while current and voltage can be measured at the end of a transmission line, they do not represent actual movement along the line but rather the effects of the EM fields.

Areas of Agreement / Disagreement

Participants express differing views on the relationship between voltage/current and EM waves in transmission lines and waveguides. The discussion remains unresolved, with multiple competing perspectives on how these concepts interrelate.

Contextual Notes

Participants reference Maxwell's equations and the differential forms to support their claims, indicating a reliance on specific mathematical frameworks that may not be fully explored in the discussion.

erst
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Ok, it's clear to me that waveguides are for sending EM waves from one place to another (e.g. TEM, TE, TM modes).

But what about TLs? I've seen them described as carrying AC signals (V or I) but also EM waves, e.g. TEM waves in coax cable. What gives? Does one imply the existence of the other? When the coax cable's signal enters my TV, what is the "data" - the V/I waveform or the EM waveform?
 
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It is EM wave that travel down in the dielectric. The current is the consequence of the boundary condition of the H field which is perpendicular to the direction of propagation( down the coax).

\nabla \times \vec H = \vec J +\frac {\partial \vec D}{\partial t}\;\;\hbox { and }\;\; \vec I = \int_S \vec J \cdot d\vec S

The velocity of electrons moving down the coax is very slow, it is not from the movement of the electrons that create the current flow. It is only because of the EM wave propagation at close to the speed of light that's why you see the apparent current flow instantaneously.
 
Last edited:
erst said:
Ok, it's clear to me that waveguides are for sending EM waves from one place to another (e.g. TEM, TE, TM modes).

But what about TLs? I've seen them described as carrying AC signals (V or I) but also EM waves, e.g. TEM waves in coax cable. What gives? Does one imply the existence of the other? When the coax cable's signal enters my TV, what is the "data" - the V/I waveform or the EM waveform?

In any waveguide or transmission line you can define a set of terminal at which there is an I and V. At these terminals you typically interface a circuit.

In reality there are I and V that could be defined all along the guiding structure but they are not helpful to describe the propagation. You need the full fields for that calculation.
 
Good point about I and V is defined at every point along the Tx line as the consequence of the E and H as you can see the differential form of Mexwell's equation is in point form. It is not that I and V are moving even though it looks like they are moving in very high speed. That's why you can measure the voltage at the end of the Tx line and get current if you put a load at the end.
 

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