The incident wave fields:
"\u03b2=\\frac {\u03c9} {c}=\\frac {2\\pi\\times10 \\times10^3} {c}=\\frac {\\pi} {150} (2)"
"E_i=3 \\times 10^5 \\times {\\cos (2\\pi \\times 10^4- \\frac {\\pi} {150} y)} \\widehat{-x}"
We assume that the incident electric field is reflected with a reflection coefficient Γ and transmitted with a transmitted with a transmission coefficient τ. That implies that if the electric field intensity of the incident, reflected and transmitted waves at the boundary (z = 0) are Ei0, Er0 and Et0 respectively, then Er0= rEi0 and Et0= tEi0
"r= \\frac {k_2-k_1} { k_2+k_1} (3)""k_1=\\sqrt{\\frac {\\mu_0} { \u025b_0}}=120\\pi"
"k_2=\\sqrt{\\frac {\\mu_2} { \u025b_2}}=180\\pi"
Using (3) we got: r=0.2
Reflected vector
Transmitted vector
Answer:
incident
reflected
transmitted
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