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Question

Any length of a transmission line may be made to appear as an infinitely long line by

The correct answer is

terminating the line in its characteristic impedance

Transmission Line Behavior: Simulating an Infinite Line

The question asks how a finite transmission line can be made to behave like an infinitely long one. An infinitely long transmission line is an ideal concept where a signal propagating along the line never reaches an end and therefore never reflects. The key characteristic of such a line is that the impedance seen by the source connected to it remains constant, regardless of how much further the line extends. This constant impedance is known as the characteristic impedance, often denoted as $Z_0$.

Understanding Transmission Line Terminations

When a transmission line of finite length is terminated with a specific load impedance ($Z_L$), any signal that reaches the end of the line can be reflected back towards the source, depending on the relationship between $Z_L$ and the line's characteristic impedance $Z_0$.

  • Characteristic Impedance ($Z_0$): This is a property of the transmission line itself, determined by its physical characteristics (like conductor size, spacing, and dielectric material). It represents the ratio of voltage to current for a wave traveling in one direction along the line.
  • Load Impedance ($Z_L$): This is the impedance of the component connected to the far end of the transmission line (e.g., a resistor, antenna, or another circuit).
  • Reflections: When $Z_L$ is not equal to $Z_0$, part of the incident wave is reflected from the termination back towards the source. This causes voltage and current waves to exist simultaneously in both directions, leading to phenomena like standing waves.

Matching for Infinite Line Behavior

To make a finite transmission line behave like an infinite one, we need to prevent reflections from occurring at the termination. This happens when the load impedance ($Z_L$) perfectly matches the characteristic impedance ($Z_0$) of the line.

Specifically, if we choose terminating the line in its characteristic impedance ($Z_L = Z_0$), the incident wave encountering the load is completely absorbed. There is no reflected wave. Without reflections, the voltage and current at any point along the line are determined solely by the forward-traveling wave, just as they would be on an infinitely long line.

Analyzing Other Options:

  • Leaving the line open: This means the load impedance is infinite ($Z_L = \infty$). This causes a voltage reflection, and the reflected voltage wave has the same polarity as the incident wave. This clearly does not simulate an infinite line.
  • Increasing the standing wave ratio (SWR) above unity: A Standing Wave Ratio (SWR) greater than 1 indicates that reflections are present on the line. An SWR of 1 signifies a perfect match (no reflections), which is the condition for simulating an infinite line. Therefore, increasing SWR means moving away from the desired behavior.
  • Shorting the line at the end: This means the load impedance is zero ($Z_L = 0$). This causes a current reflection, and the reflected voltage wave has the opposite polarity to the incident wave. This also does not simulate an infinite line.

Therefore, the only way to make a finite transmission line appear infinitely long is by terminating it with its characteristic impedance.

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Important Questions from Transmission Lines

  1. A characteristic impedance does NOT satisfy which of the following statements?

  2. Twisting of live and return lines in long signal lines is done to reduce the effect of

  3. For transmission line load matching over a range of frequencies, it is best to use a

  4. Inductance and capacitance per unit length of a lossless transmission line are 250 nH/m and 0.1 nF/m respectively. The velocity of the wave propagation and characteristic impedance of the transmission line are respectively

  5. What are the characteristics of a coaxial cable?

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