Chapter 9: Electromagnetic Waves - MIT OpenCourseWare
o H (z,t )= yˆ (Eo ηo )cos (ωt −kz) ⎡⎣Am-1⎤⎦ (9.1.2) This unambiguously defines the source, and the boundary is similarly unambigous: = ∞ and σ therefore E =0 for z ≥0. This more complete problem definition is sufficient to yield a unique
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