Rectangular Waveguide at 9 GHz with a = 2.0 cm: Compute the group velocity for the dominant TE10 mode (air-filled guide).
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A1.8 × 10^8 m/s
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B5 × 10^8 m/s
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C3 × 10^8 m/s
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D1.5 × 10^8 m/s
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E9 × 10^7 m/s
Answer
Correct Answer: 1.8 × 10^8 m/s
Explanation
Introduction / Context:In rectangular waveguides, the dominant mode is TE10 with cutoff frequency fc = c/(2a). Group velocity in a dispersive guide depends on the operating frequency relative to cutoff. This exercise checks your understanding of TE modes and waveguide dispersion relations.
Given Data / Assumptions:
- Air-filled rectangular waveguide.
- Broad wall dimension a = 2 cm = 0.02 m (dominant TE10).
- Frequency f = 9 GHz.
- Speed of light c ≈ 3 × 10^8 m/s.
Concept / Approach:
For TE10 in air: fc = c/(2a). Group velocity: v_g = c * sqrt(1 − (fc/f)^2). v_g is always less than c and increases as f moves far above fc.
Step-by-Step Solution:
Compute cutoff: fc = 3×10^8 / (2*0.02) = 7.5 GHz.Form ratio: (fc/f) = 7.5/9 ≈ 0.8333; square → ≈ 0.6944.Inside root: 1 − 0.6944 = 0.3056; sqrt ≈ 0.5528.Group velocity: v_g = 0.5528 * 3×10^8 ≈ 1.66×10^8 m/s ≈ 1.8×10^8 m/s (nearest option).Verification / Alternative check:
Since f > fc but not by a large margin, v_g should be well below c; 1.8×10^8 m/s is reasonable and closest to the calculated value ~1.66×10^8 m/s.
Why Other Options Are Wrong:
- 3×10^8 m/s and 5×10^8 m/s: exceed or equal c, impossible for group velocity in a guide near cutoff.
- 1.5×10^8 m/s and 9×10^7 m/s: lower than the computed value; less accurate than 1.8×10^8 m/s.
Common Pitfalls:
- Using phase velocity formula instead of group velocity.
- Taking a as 1 cm instead of 2 cm, which changes fc.
Final Answer:
1.8 × 10^8 m/s