A waveguide Ras a square cross section of side 2a. For the TM modes of wave...
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A waveguide Ras a square cross section of side 2a. For the TM modes of wave vector K, the transverse em modes are obtained in terms of a function 4(x,y) which obeys the equation: (² + y + (10²-1³]] 4(x,y) = 0 لولى with the boundary condition & (±a, y) = 4(x, t0) = 0 the frequency w of the lowest mode is : as we²² = ²(kª² + 4x² / Q9²) by ² (²+²/a²) c) w²²=²(K²+x²²²) d) ₁²² =²² (1²^² + x^²/0²) A waveguide Ras a square cross section of side 2a. For the TM modes of wave vector K, the transverse em modes are obtained in terms of a function 4(x,y) which obeys the equation: (² + y + (10²-1³]] 4(x,y) = 0 لولى with the boundary condition & (±a, y) = 4(x, t0) = 0 the frequency w of the lowest mode is : as we²² = ²(kª² + 4x² / Q9²) by ² (²+²/a²) c) w²²=²(K²+x²²²) d) ₁²² =²² (1²^² + x^²/0²)
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Physics
ISBN: 978-0077339685
2nd edition
Authors: Alan Giambattista, Betty Richardson, Robert Richardson
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