Simple Transmission Line Question

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Discussion Overview

The discussion revolves around the behavior of a lossless transmission line with varying impedances, specifically focusing on the energy reconciliation when a pulse encounters an impedance mismatch. Participants explore the implications of voltage and current changes at the mismatch and the geometry of the transmission line.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Experimental/applied

Main Points Raised

  • One participant describes a scenario involving a pulse traveling down a transmission line with different impedances and questions how energy is reconciled when a reflection occurs.
  • Another participant notes that while the voltage increases in the transmitted pulse, the current decreases, leading to a lower product of voltage and current compared to the incident pulse.
  • A participant acknowledges a mistake in calculating field energy and seeks clarification on how geometry changes with impedance variations, suggesting that the cross-section of the dielectric may need to increase.
  • One participant questions whether the ideal source has a 50-ohm output impedance and emphasizes the need to consider both voltage and current at the mismatch, providing equations for forward and reflected signals.
  • A later reply presents simulation results from LTSpice, detailing the voltages and currents at the mismatch and confirming the relationships between them.

Areas of Agreement / Disagreement

Participants express differing views on the implications of impedance mismatch and energy reconciliation, with no consensus reached on the geometry changes or the ideal source's characteristics.

Contextual Notes

Participants rely on specific assumptions about the ideal source and the nature of the transmission line, which may not be universally applicable. The discussion includes unresolved mathematical relationships and varying interpretations of the physical behavior at the impedance mismatch.

HasuChObe
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Say you had a lossless transmission line that consists of an ideal source, a 50 ohm impedance, a 100 ohm impedance, and a 100 ohm terminator. The material is the same. You send a pulse down the line. When the pulse hits the impedance mismatch, you get a smaller reflection back, and a pulse bigger than the original pulse going toward the terminator. Since the material is the same, the pulse should have the same width (in space and time) as it did originally going down the line (prior to reflection) except now you have them where one is actually bigger than the initial pulse. How is energy reconciled in this case?
 
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The short answer is that the voltage is more but the current is less (in the transmitted pulse, compared to what it was in the incident pulse). More importantly, the product of voltage times current is also less.
 
uart said:
The short answer is that the voltage is more but the current is less (in the transmitted pulse, compared to what it was in the incident pulse). More importantly, the product of voltage times current is also less.

Hah; Of course I try to calculate field energy with only the E field :/ Good answer. Should be further along now :P Any inputs on the geometry changes from a smaller to larger impedance? I've concluded that the cross section of the dielectric part has to get bigger, but I could be wrong again -.-
 
Are you assuming your ideal source has a 50 ohm output impedance? To solve the mismatch equation at the transmission line impedance step, you have to consider both the voltage V and the current I at the mismatch. For a forward (F) and reflected (R) signal you have 3 equations for the voltages and currents at the mismatch (Z1=50 ohms, and Z2=100 ohms). This is easily simulated in SPICE.

VF1 = +Z1·IF1

VF2 = +Z2·IF2,

VR1 = -Z1·IR1

where F = forward, R = reflected.

[added] The minus sign comes from the direction of the Poynting vector.

Bob S
 
Last edited:
Here in thumbnail is a simulation of the mismatch using LTSpice. A back-terminated voltage source drives a 50-ohm transmission line, which is connected to a 100-ohm transmission line, terminated at the end. For 1 volt in,

VF1 = 1 volt
VR1 = 0.333 volts
VF2 = 1.333 volts
IF1 = +20 mA
IR1 = - 6.667 mA (note minus sign)
IF2 = +13.333 mA

So VF1 + VR1 = VF2
and IF1 + IR1 = IF2

Bob S
 

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