Chapter 9: Electromagnetic Waves - MIT OpenCourseWare
We also need a trial solution for z > 0. Inside the conductor EH= =0 , and boundary conditions (2.6.17) require a surface current: Js =×nˆ HA ⎣⎡ m-1⎤⎦ (9.1.10) The fourth and final step of this problem-solving method is to test the full trial solution
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