Friis Path Loss on a Segmented Path Derivation

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Discussion Overview

The discussion revolves around the application of Friis' Path Loss formula in the context of a segmented path between a transmitter and receiver. Participants explore the implications of dividing the path into segments and how to accurately calculate the received power at each segment, considering factors such as reflections and antenna characteristics.

Discussion Character

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

Main Points Raised

  • Some participants propose that dividing the path into segments should yield the same total path loss as treating it as a single path, but they express uncertainty about how to combine the results mathematically.
  • One participant suggests that when calculating two paths in tandem, the losses in decibels should be added, noting that attenuation occurs more significantly at the start of the path.
  • Another participant questions how to define the "start" of a path when reflections occur at an intermediate point, raising the issue of whether to treat the reflected path as a new path or as part of the original path loss.
  • It is mentioned that for the two paths to be treated as one, the receiving antenna on the first hop must be sufficiently large to capture all radiated energy.
  • Some participants clarify that reflections necessitate treating the scenario as two distinct paths, as they represent new wavefronts.

Areas of Agreement / Disagreement

Participants do not reach a consensus on how to handle the calculations for segmented paths, as there are competing views on the treatment of reflections and the definition of path starts. The discussion remains unresolved regarding the best approach to combine path losses in these scenarios.

Contextual Notes

Participants highlight limitations related to assumptions about antenna sizes and the isotropic nature of the Friis' Path Loss formula, as well as the effects of reflections on path loss calculations.

Frov_ken
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Let's say we have a path Length AC. Point A transmits a signal at Ptransmit.
From Friis' Path Loss formula: (assumming Gain for receiver and transmitter antennae are 1.)
##P_{received} = P_{transmit} (\frac{λ}{4π* LengthAC})^2##
,when point C contains the receiver.

What if I divided this into two segments. They should still have the same answer right?
Let's say point B is somewhere between A and C.
Theoretically, the path loss in AB plus the path loss in BC should equal the path loss in AC. If I do this using the formula.

##P_{received at B} = P_{transmit} (\frac{λ}{4π* LengthAB})^2##
##P_{received at C} = P_{received at B} (\frac{λ}{4π* LengthBC})^2##

Combining these two should get me to the total of the equation before. How should I combine them? I couldn't just multiply or add them together. The math would be messy. Am I missing some assumptions here?
 
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Frov_ken said:
Let's say we have a path Length AC. Point A transmits a signal at Ptransmit.
From Friis' Path Loss formula: (assumming Gain for receiver and transmitter antennae are 1.)
##P_{received} = P_{transmit} (\frac{λ}{4π* LengthAC})^2##
,when point C contains the receiver.

What if I divided this into two segments. They should still have the same answer right?
Let's say point B is somewhere between A and C.
Theoretically, the path loss in AB plus the path loss in BC should equal the path loss in AC. If I do this using the formula.

##P_{received at B} = P_{transmit} (\frac{λ}{4π* LengthAB})^2##
##P_{received at C} = P_{received at B} (\frac{λ}{4π* LengthBC})^2##

Combining these two should get me to the total of the equation before. How should I combine them? I couldn't just multiply or add them together. The math would be messy. Am I missing some assumptions here?
If you have two paths in tandem, they should be treated as two paths, each having two antennas and a free space attenuation. The losses in Decibels of the two paths should be added.
The reason that the answer is different to treating it as a single path is that most attenuation occurs at the start of the path, and for two paths this happens twice. For example, suppose a given path has an attenuation of 60dB. If you double the path length, it becomes only 66dB. But if the two paths are used in tandem, say by using a passive repeater, it will give 120dB.
 
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tech99 said:
The reason that the answer is different to treating it as a single path is that most attenuation occurs at the start of the path,
So, how do you exactly define the start of a path when something like this involves an interaction at B?
let's say there's a reflection at point B. Will it "start" a new path? or is it safe to treat the total reflected path distance and treat it as a single path loss?
 
Frov_ken said:
So, how do you exactly define the start of a path when something like this involves an interaction at B?
let's say there's a reflection at point B. Will it "start" a new path? or is it safe to treat the total reflected path distance and treat it as a single path loss?
For the two paths in tandem to be calculated as one, the receiving antenna on the first hop must be large enough to catch all the radiated energy. So it might need to be a kilometre in diameter!
For cases where the intermediate point is back-to-back dishes, passive reflectors, reflections from buildings etc etc, treat it as two paths. The repeater has its gain twice - once for receiving and again for transmitting.
 
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tech99 said:
For the two paths in tandem to be calculated as one, the receiving antenna on the first hop must be large enough to catch all the radiated energy. So it might need to be a kilometre in diameter!
Hmm. I think I'm getting the problem with my equation. As you said, I should be getting all energy. that just means the Friis' Path Loss Formula estimates a certain propagation area and a finite point where it is received. From the wikipedia page, I see it has assumed an isotropic case.

In the case of having reflections, I have to treat it as two paths. since it "starts" again as another wavefront.

I just clarified what you wrote in this text. Thank you!
 

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