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A 150 MHz uniform plane wave is normally incident from air onto a material. Measurements yield a SWR of 3 and the appearance of an electric field minimum at 0.3λ in front of the interface. The impedance of material is
  • a)
    502 - j641 Ω 
  • b)
    641 -  j502 Ω
  • c)
    641 + j502 Ω 
  • d)
    502 + j641Ω
Correct answer is option 'C'. Can you explain this answer?
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A 150 MHz uniform plane wave is normally incident from air onto a mate...
Given information:
- Frequency of the incident plane wave: 150 MHz
- SWR (Standing Wave Ratio): 3
- Electric field minimum observed at 0.3 inches in front of the interface

Explanation:

1. Understanding SWR (Standing Wave Ratio):
- SWR is a measure of how well a load is matched to a transmission line.
- It is defined as the ratio of the maximum amplitude of the forward wave to the maximum amplitude of the reflected wave.
- SWR = (1 + Γ) / (1 - Γ), where Γ is the reflection coefficient.

2. Relationship between SWR and Reflection Coefficient:
- SWR can be calculated using the reflection coefficient as follows:
- SWR = (1 + |Γ|) / (1 - |Γ|), where |Γ| is the magnitude of the reflection coefficient.

3. Calculation of Reflection Coefficient:
- We are given SWR = 3. Let's calculate the magnitude of the reflection coefficient using the above formula.
- 3 = (1 + |Γ|) / (1 - |Γ|)
- 3(1 - |Γ|) = 1 + |Γ|
- 3 - 3|Γ| = 1 + |Γ|
- 2|Γ| = 2
- |Γ| = 1

4. Definition of Reflection Coefficient:
- The reflection coefficient (Γ) is the ratio of the amplitude of the reflected wave to the amplitude of the incident wave.

5. Relationship between Reflection Coefficient and Impedance:
- The reflection coefficient (Γ) can be related to the impedance (Z) as follows:
- Γ = (Z - Z0) / (Z + Z0), where Z0 is the characteristic impedance of the transmission line.

6. Calculation of Impedance:
- We are given that an electric field minimum is observed at 0.3 inches in front of the interface.
- At an electric field minimum, the voltage is maximum and the current is minimum. This indicates that the load impedance is purely reactive.
- Let's assume the load impedance (Z) is purely reactive, i.e., Z = jX, where X is the reactive component.
- From the given information, we can conclude that X > 0.

7. Calculation of X:
- Let's calculate X using the relationship between Reflection Coefficient and Impedance.
- From step 3, we know that |Γ| = 1.
- |Γ| = |(Z - Z0) / (Z + Z0)| = 1
- |Z - Z0| = |Z + Z0|
- |jX - Z0| = |jX + Z0|
- √(X^2 + Z0^2) = √(X^2 + Z0^2)
- X = X
- This implies that there is no real component in the load impedance (Z).

8. Final Impedance:
- The impedance (Z) is purely reactive, i.e., Z = jX.
- The magnitude of
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