Simple Transmission Line Question

In summary, the mismatch results in a decrease in voltage and current at the mismatch point, and the net result is that the voltage is more but the current is less (in the transmitted pulse, compared to what it was in the incident pulse).
  • #1
HasuChObe
31
0
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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  • #2
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.
 
  • #3
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 -.-
 
  • #4
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:
  • #5
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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1. What is a simple transmission line?

A simple transmission line is a two-wire circuit that is used to transfer electrical energy from one point to another. It consists of two parallel conductors, typically made of copper or aluminum, separated by a dielectric material.

2. What is the purpose of a simple transmission line?

The purpose of a simple transmission line is to transmit electrical signals with minimal loss and distortion over long distances. It is commonly used in telecommunication systems, power distribution networks, and electronic devices.

3. How does a simple transmission line work?

A simple transmission line works by propagating electromagnetic waves along its length. These waves are created by an alternating voltage applied to one end of the line, and they travel to the other end at a constant velocity determined by the physical properties of the line.

4. What are the key parameters of a simple transmission line?

The key parameters of a simple transmission line include its length, impedance, and characteristic impedance. Length affects the propagation time of the signal, while impedance determines the amount of signal loss. Characteristic impedance is the ratio of voltage to current at any point along the line.

5. How can the performance of a simple transmission line be improved?

The performance of a simple transmission line can be improved by minimizing the length of the line, using high-quality materials for the conductors and dielectric, and properly terminating the line with its characteristic impedance. Additionally, using techniques such as impedance matching and shielding can also improve the performance of the line.

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