Can coax cause distortion in signals?

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Discussion Overview

The discussion revolves around the potential for coaxial cables to cause distortion in signals, particularly in the context of lossless transmission lines and their properties. Participants explore theoretical aspects, practical experiences, and the implications of frequency on signal integrity.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Experimental/applied

Main Points Raised

  • Some participants question whether lossless transmission lines can truly exist, suggesting that while they may approach losslessness, practical limitations prevent them from being entirely lossless.
  • There is a discussion about the characteristics of coaxial cables, with some participants noting that the propagation velocity is relatively constant with frequency, while others argue that different frequencies can experience varying propagation velocities, leading to distortion.
  • One participant highlights the importance of the attenuation constant and phase constant in determining whether a transmission line is distortionless, emphasizing that both must remain constant with frequency for distortion-free propagation.
  • Another participant shares a practical experience with coaxial cables, detailing how they encountered significant distortion when using RG-175 cables for high-frequency applications, necessitating the design of compensation networks.
  • Some participants assert that for single frequency applications, distortion may not be apparent, but for broadband applications, the effects of distortion become more pronounced.
  • There is mention of the relationship between the dielectric properties of materials and their frequency dependence, with a focus on how this impacts signal propagation in coaxial cables.

Areas of Agreement / Disagreement

Participants express differing views on the existence of lossless transmission lines and the extent to which coaxial cables can distort signals. While some argue that coax can distort signals under certain conditions, others maintain that distortion is not a significant issue in typical applications. The discussion remains unresolved with multiple competing perspectives.

Contextual Notes

Limitations include the dependence on specific cable types, the frequency range of applications, and the assumptions about ideal conditions versus practical implementations. The discussion highlights the complexity of signal transmission and the factors that contribute to distortion.

seang
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Is it true that lossless transmission lines don't distort signals?

to me, they seem like low pass filters.

i had this class a while ago, but I guess i forgot this, or never understood it

thanks
 
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I was under the impression they don't really exist...hmm

you can probably get very close at least
 
Are speaking things like a 50 ohm coaxial cables, or the ideal model in terms of the L-C ladder network in the limit as the ladder is more finely divided?
 
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seang said:
Is it true that lossless transmission lines don't distort signals?

no. losslessness is an independent property of distortion free propagation.

i don't remember the equations that express \alpha and \beta (expressed in terms of nepers per unit length and radians per unit length) in terms of R, L, G, C of the transmission line. all of these parameters are functions of frequency \omega. if \alpha and \frac{\beta}{\omega} are both constant with frequency, then you have a distortionless line. if \alpha=0, then you have a lossless line.
 
P=alpha+j * beta
where P is the propagation constant
alpha = (R/(2*z))
where alpha is the attenuation constant
beta = (2*pi/lambda)
where beta is the phase constant
z= characteristic impedence (usually z0)
For a lossless line alpha is 0
 
seang said:
Is it true that lossless transmission lines don't distort signals?

to me, they seem like low pass filters.

i had this class a while ago, but I guess i forgot this, or never understood it

thanks

Theoractically yes!

But there is not lossless Tx lines. Just how much. They are not exactly low past. For lossy Tx line, different frequencies have slightly different propagation velocities. So for a long line, signals don't arrive at the same time. Of cause the higher the frequency, the more attenuation on the line. Because the attenuation constant is proportional to frequency.
 
I can't see that there are any ways that coax can distort a signal.

The velocity is more or less constant with frequency.

There is no frequency cut-off as such except when the diameter is half a wavelength or more and waveguide modes appear. This limits the maximum diameter of coax at a given freq.
 
Pumblechook said:
I can't see that there are any ways that coax can distort a signal.

The velocity is more or less constant with frequency.

There is no frequency cut-off as such except when the diameter is half a wavelength or more and waveguide modes appear. This limits the maximum diameter of coax at a given freq.

Not true, depend on how long the coax is. I have experience with this very issue. I worked for LeCroy before that design digital scope and transient recorder in the 80s. Those days, you can't buy 8bits 100MHz ADC. We had to design subrange configuration using two 4 bits ADC of 100MHz. We have to do summing of two signals and delay using coax as delay lines. The wave form get distorted and I have to design compensation networks for different frequencies to line the signal up again. We started out with RG-175, that has so much distortion that no networks can even compensate it back. I end up using big RG-58 and 4 compensating network in order to make it work.

For single frequency application in typical RF application, you don't see this problem because the frequencies are close together. You see attenuation only and it is easy to get the signal back. For broadband, it is very very obvious! We were using about 12 feet and it really showed.

Check out "group velocity" in EM books, they talk about the exact issue. There are no lossless dielectric, just how much. Not even taflon or any of the fancy dielectrics from Rogers or 3M.

Velocity=\frac{1}{\sqrt{\epsilon\mu}} Where \epsilon is frequency dependent. The imaginary part is \sigma/ \omega.
 
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