How Do You Sketch Voltage and Current Waveforms for a Coaxial Transmission Line?

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Homework Help Overview

The problem involves sketching voltage and current waveforms for a coaxial transmission line with specific parameters, including characteristic impedance, propagation velocity, length, and load resistance. The context is rooted in transmission line theory and wave propagation.

Discussion Character

  • Exploratory, Conceptual clarification, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the relationship between inductance, capacitance, and characteristic impedance, with one participant expressing uncertainty about the approach. Others explore the implications of the pulse generator's internal resistance on waveform reflection and transmission.

Discussion Status

The discussion is ongoing, with participants sharing insights about wave behavior in transmission lines and questioning the role of various parameters. Some guidance has been offered regarding the reflection coefficient and its impact on the waveforms.

Contextual Notes

There is mention of the complexity of the assignment, particularly with respect to the finite-duration pulse and its effects on waveform analysis. Participants are navigating assumptions about the behavior of waves in relation to the source and load impedances.

tim9000
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Homework Statement



As seen in picture: A coaxial transmission line has a characteristic impedance of 50 Ω, propagation
velocity of 200m/μs, length of 400m, and is terminated by a load resistance, RR =
16.7 Ω. At the sending end the line is connected to a pulse generator that has an
internal resistance of 150 Ω and produces a 40 V, 1 μs long pulse at time, t=0. Sketch
the sending end voltage and current waveforms for 0≤t≤15 µsec.

Homework Equations





The Attempt at a Solution



I'm not sure how to approach this, I'm assuming it has something to do with the inductance and capacitance found from Z = Sqrt(L/C), does anyone have any thoughts?
Thanks
 

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IMO this is a very difficult assignment. It would be so even if the input were an infinite-duration pulse, in which case a lattice diagram could be used. Not sure if this type of diagram could be adapted for a finite-duration pulse (duration < L/v). Should in theory but wouldn't want to try it.

The basic idea of course is that
1. the outgoing wave V and I moves with velocity v, I = V/Z_0;
2. the returning wave V' and I' are related by the load reflection coefficient;
3. the returning wave, added to the ingoing wave, force a new V and I at the source, which will depend on the source impedance;
etc.

This keeps going until the input pulse goes back to zero V.
 
thanks

I see, thanks anyway.
Though what does the internal resistance of the pulse generator have to do with it?
 
tim9000 said:
I see, thanks anyway.
Though what does the internal resistance of the pulse generator have to do with it?

The 150 ohm source resistance determines the fraction of the reflected pulse (back to the source) sent back out again as a new pulse in the +x direction. Us your experssion for the reflection coefficient with Z_0 = 50 ohms and Z_L = 150 ohms.
 

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