Simple Transmission Line Question

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In a lossless transmission line scenario with a 50-ohm source and a 100-ohm load, a pulse sent down the line experiences reflection due to impedance mismatch, resulting in a transmitted pulse that is larger in voltage but smaller in current than the incident pulse. The energy reconciliation occurs because the product of voltage and current in the transmitted pulse is less than that of the incident pulse. The discussion also touches on the geometry changes associated with impedance variations, suggesting that the dielectric cross-section may need to increase. Participants emphasize the importance of considering both voltage and current at the mismatch to accurately analyze the situation, with equations provided for simulation purposes. Overall, the conversation highlights the complexities of energy distribution in transmission lines under varying impedance conditions.
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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
 
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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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