The cutoff frequency \(f_{c,mn}\) for TE\(_{mn}\) or TM\(_{mn}\) modes in a rectangular waveguide with dimensions \(a\) (width) and \(b\) (height) is given by:
\( f_{c,mn} = \frac{c}{2} \sqrt{\left(\frac{m}{a}\right)^2 + \left(\frac{n}{b}\right)^2} \) where \(c\) is the speed of light, and \(m\) and \(n\) are mode indices (integers).
For TE modes, \(m, n\) can be 0, 1, 2, ... but not both \(m=0\) and \(n=0\) simultaneously. For TM modes, \(m, n\) must be 1, 2, 3, ... (neither \(m\) nor \(n\) can be zero).
Given: \(a=2b\). The cutoff frequency for TE\(_{01}\) mode is 12 GHz.
For TE\(_{01}\) mode, \(m=0\), \(n=1\). Using the formula for cutoff frequency:
For TE\(_{01}\) mode: \( f_{c,01} = \frac{c}{2} \sqrt{\left(\frac{0}{a}\right)^2 + \left(\frac{1}{b}\right)^2} = \frac{c}{2} \sqrt{\frac{1}{b^2}} = \frac{c}{2b} \)
We are given \(f_{c,01} = 12 \text{ GHz}\). So, \( \frac{c}{2b} = 12 \text{ GHz} \). This gives us a relation for \(c/b\): \( c/b = 24 \text{ GHz} \).
Now, we need to find the cutoff frequency for TM\(_{11}\) mode.
For TM\(_{11}\) mode, \(m=1\), \(n=1\). Using the formula:
For TM\(_{11}\) mode: \( f_{c,11} = \frac{c}{2} \sqrt{\left(\frac{1}{a}\right)^2 + \left(\frac{1}{b}\right)^2} \)
Substitute \(a = 2b\):
\( f_{c,11} = \frac{c}{2} \sqrt{\left(\frac{1}{2b}\right)^2 + \left(\frac{1}{b}\right)^2} = \frac{c}{2} \sqrt{\frac{1}{4b^2} + \frac{1}{b^2}} \)
Now simplifying:
\( f_{c,11} = \frac{c}{2} \sqrt{\frac{1+4}{4b^2}} = \frac{c}{2} \sqrt{\frac{5}{4b^2}} = \frac{c}{2} \frac{\sqrt{5}}{2b} = \frac{c\sqrt{5}}{4b} \)
We can write this as:
\( f_{c,11} = \left( \frac{c}{2b} \right) \frac{\sqrt{5}}{2} \)
We know \( \frac{c}{2b} = 12 \text{ GHz} \).
So:
\( f_{c,11} = (12 \text{ GHz}) \times \frac{\sqrt{5}}{2} = 6\sqrt{5} \text{ GHz} \)
This matches option (b).
The final answer is: \( \boxed{6\sqrt{5} \text{ GHz}} \)
| LIST I | LIST II | ||
|---|---|---|---|
| A. | Bipolar npn transistor operate in the cut-off mode. | I. The base-emitter is reverse biased and | |
| B. | Bipolar npn transistor operate in the saturation mode. | II. Both the base-emitter and base | |
| C. | Bipolar npn transistor operate in the inverse active mode. | III. The base-emitter is forward biased | |
| D. | Bipolar npn transistor operate in the forward active mode. | IV. Both the base-emitter and bas |
| LIST I | LIST II |
|---|---|
| A. Maxwell's First Equation | I. Modified Ampere's Law |
| B. Maxwell's Second Equation | II. Faraday's Laws of Electromagnetic Induction |
| C. Maxwell's Third Equation | III. Gauss Law in Electrostatics |
| D. Maxwell's Fourth Equation | IV. Gauss Law in Magnetostatics |