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Plane EM Wave: Oblique Incidence

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Presentation on theme: "Plane EM Wave: Oblique Incidence"β€” Presentation transcript:

1 Plane EM Wave: Oblique Incidence
𝐸 βŠ₯ π‘Ÿ = 𝐸 0βŠ₯ π‘Ÿ 𝑒 βˆ’π‘— 𝛽 π‘Ÿ βˆ™ π‘Ÿ 𝐸 βŠ₯ 𝑖 = 𝐸 0βŠ₯ 𝑖 𝑒 βˆ’π‘— 𝛽 𝑖 βˆ™ π‘Ÿ 𝐸 || 𝑖 = 𝐸 0|| 𝑖 𝑒 βˆ’π‘— 𝛽 𝑖 βˆ™ π‘Ÿ 𝐸 || π‘Ÿ = 𝐸 0|| π‘Ÿ 𝑒 βˆ’π‘— 𝛽 π‘Ÿ βˆ™ π‘Ÿ Plane of Incidence 𝐸 βŠ₯ 𝑑 = 𝐸 0βŠ₯ 𝑑 𝑒 βˆ’π‘— 𝛽 𝑑 βˆ™ π‘Ÿ 0°≀ πœƒ 𝑖 , πœƒ π‘Ÿ , πœƒ 𝑑 ≀90Β° 𝐸 || 𝑑 = 𝐸 0|| 𝑑 𝑒 βˆ’π‘— 𝛽 𝑑 βˆ™ π‘Ÿ

2 Propagation Directions and Magnitude Relations
𝐸 0βŠ₯ π‘Ÿ 𝐸 0βŠ₯ 𝑖 = πœ‚ 𝑑 cos πœƒ 𝑖 βˆ’ πœ‚ 𝑖 cos πœƒ 𝑑 πœ‚ 𝑑 cos πœƒ 𝑖 + πœ‚ 𝑖 cos πœƒ 𝑑 𝐸 0βŠ₯ 𝑑 𝐸 0βŠ₯ 𝑖 = 2 πœ‚ 𝑑 cos πœƒ 𝑖 πœ‚ 𝑑 cos πœƒ 𝑖 + πœ‚ 𝑖 cos πœƒ 𝑑 𝐸 0|| π‘Ÿ 𝐸 0|| 𝑖 = πœ‚ 𝑖 cos πœƒ 𝑖 βˆ’ πœ‚ 𝑑 cos πœƒ 𝑑 πœ‚ 𝑖 cos πœƒ 𝑖 + πœ‚ 𝑑 cos πœƒ 𝑑 𝐸 0|| 𝑑 𝐸 0|| 𝑖 = 2 πœ‚ 𝑑 cos πœƒ 𝑖 πœ‚ 𝑖 cos πœƒ 𝑖 + πœ‚ 𝑑 cos πœƒ 𝑑 πœƒ 𝑖 = πœƒ π‘Ÿ 𝑛= πœ€ π‘Ÿ 𝑛: index of refraction πœ€ 𝑖 πœ‡ 𝑖 sin πœƒ 𝑖 = πœ€ 𝑑 πœ‡ 𝑑 sin πœƒ 𝑑 πœ€ π‘Ÿ : relative permittivity 𝑛 𝑖 sin πœƒ 𝑖 = 𝑛 𝑑 sin πœƒ 𝑑

3 Reflection and Transmission Coefficients
Ξ“ || =βˆ’ 𝐸 0|| π‘Ÿ 𝐸 0|| 𝑖 Ξ“ βŠ₯ = 𝐸 0βŠ₯ π‘Ÿ 𝐸 0βŠ₯ 𝑖 𝑇 || = 𝐸 0|| 𝑑 𝐸 0|| 𝑖 𝑇 βŠ₯ = 𝐸 0βŠ₯ 𝑑 𝐸 0βŠ₯ 𝑖

4 Reflection and Transmission Coefficients
Ξ“ βŠ₯ = 𝐸 0βŠ₯ π‘Ÿ 𝐸 0βŠ₯ 𝑖 = πœ‚ 𝑑 cos πœƒ 𝑖 βˆ’ πœ‚ 𝑖 cos πœƒ 𝑑 πœ‚ 𝑑 cos πœƒ 𝑖 + πœ‚ 𝑖 cos πœƒ 𝑑 Ξ“ || =βˆ’ 𝐸 0|| π‘Ÿ 𝐸 0|| 𝑖 =βˆ’ πœ‚ 𝑖 cos πœƒ 𝑖 βˆ’ πœ‚ 𝑑 cos πœƒ 𝑑 πœ‚ 𝑖 cos πœƒ 𝑖 + πœ‚ 𝑑 cos πœƒ 𝑑 𝑇 βŠ₯ = 𝐸 0βŠ₯ 𝑑 𝐸 0βŠ₯ 𝑖 = 2 πœ‚ 𝑑 cos πœƒ 𝑖 πœ‚ 𝑑 cos πœƒ 𝑖 + πœ‚ 𝑖 cos πœƒ 𝑑 𝑇 || = 𝐸 0|| 𝑑 𝐸 0|| 𝑖 = 2 πœ‚ 𝑑 cos πœƒ 𝑖 πœ‚ 𝑖 cos πœƒ 𝑖 + πœ‚ 𝑑 cos πœƒ 𝑑

5 Reflection and Transmission Coefficients
Ξ“ βŠ₯ = 𝐸 0βŠ₯ π‘Ÿ 𝐸 0βŠ₯ 𝑖 = 𝑛 𝑖 cos πœƒ 𝑖 βˆ’ 𝑛 𝑑 cos πœƒ 𝑑 𝑛 𝑖 cos πœƒ 𝑖 + 𝑛 𝑑 cos πœƒ 𝑑 Ξ“ || =βˆ’ 𝐸 0|| π‘Ÿ 𝐸 0|| 𝑖 =βˆ’ 𝑛 𝑑 cos πœƒ 𝑖 βˆ’ 𝑛 𝑖 cos πœƒ 𝑑 𝑛 𝑑 cos πœƒ 𝑖 + 𝑛 𝑖 cos πœƒ 𝑑 𝑇 βŠ₯ = 𝐸 0βŠ₯ 𝑑 𝐸 0βŠ₯ 𝑖 = 2 𝑛 𝑖 cos πœƒ 𝑖 𝑛 𝑖 cos πœƒ 𝑖 + 𝑛 𝑑 cos πœƒ 𝑑 𝑇 || = 𝐸 0|| 𝑑 𝐸 0|| 𝑖 = 2 𝑛 𝑖 cos πœƒ 𝑖 𝑛 𝑑 cos πœƒ 𝑖 + 𝑛 𝑖 cos πœƒ 𝑑

6 Reflection and Transmission Coefficients
Example 1: air to water 𝑛 𝑖 =1, 𝑛 𝑑 =4/3 Brewster angle πœƒ 𝐡

7 Reflection and Transmission Coefficients
Example 2: water to air 𝑛 𝑖 =4/3, 𝑛 𝑑 =1 πœƒ 𝑖 > πœƒ 𝑐 πœƒ 𝑐 πœƒ 𝐡 Brewster angle Critical angle

8 Total (Internal) Reflection: Critical Angle
Ξ“ βŠ₯ = 𝐸 0βŠ₯ π‘Ÿ 𝐸 0βŠ₯ 𝑖 = 𝑛 𝑖 cos πœƒ 𝑖 βˆ’ 𝑛 𝑑 cos πœƒ 𝑑 𝑛 𝑖 cos πœƒ 𝑖 + 𝑛 𝑑 cos πœƒ 𝑑 Ξ“ || =βˆ’ 𝐸 0|| π‘Ÿ 𝐸 0|| 𝑖 =βˆ’ 𝑛 𝑑 cos πœƒ 𝑖 βˆ’ 𝑛 𝑖 cos πœƒ 𝑑 𝑛 𝑑 cos πœƒ 𝑖 + 𝑛 𝑖 cos πœƒ 𝑑 πœƒ 𝑖 = πœƒ 𝑐 Critical angle πœƒ 𝑑 =90Β° Ξ“ βŠ₯ =1 Ξ“ || =βˆ’1 𝑛 𝑖 sin πœƒ 𝑖 = 𝑛 𝑑 sin πœƒ 𝑑 sin πœƒ 𝑐 = 𝑛 𝑑 / 𝑛 𝑖 𝑛 𝑖 > 𝑛 𝑑

9 Total Transmission: Brewster Angle
Ξ“ βŠ₯ = 𝐸 0βŠ₯ π‘Ÿ 𝐸 0βŠ₯ 𝑖 = 𝑛 𝑖 cos πœƒ 𝑖 βˆ’ 𝑛 𝑑 cos πœƒ 𝑑 𝑛 𝑖 cos πœƒ 𝑖 + 𝑛 𝑑 cos πœƒ 𝑑 Ξ“ || =βˆ’ 𝐸 0|| π‘Ÿ 𝐸 0|| 𝑖 =βˆ’ 𝑛 𝑑 cos πœƒ 𝑖 βˆ’ 𝑛 𝑖 cos πœƒ 𝑑 𝑛 𝑑 cos πœƒ 𝑖 + 𝑛 𝑖 cos πœƒ 𝑑 πœƒ 𝑖 = πœƒ 𝐡 Brewster angle (Polarization angle) πœƒ 𝐡 + πœƒ 𝑑 =90Β° Ξ“ βŠ₯ β‰ 0 Ξ“ || =0 Parallel component only 𝑛 𝑖 sin πœƒ 𝑖 = 𝑛 𝑑 sin πœƒ 𝑑 tan πœƒ 𝐡 = 𝑛 𝑑 / 𝑛 𝑖 𝑛 𝑖 sin πœƒ 𝐡 = 𝑛 𝑑 cos πœƒ 𝐡

10 Total Reflection/Transmission: Water
𝑛 π‘€π‘Žπ‘‘π‘’π‘Ÿ = πœ€ π‘€π‘Žπ‘‘π‘’π‘Ÿ π‘Ÿπ‘’π‘™ β‰ˆ 4 3 tan πœƒ 𝐡 = 𝑛 𝑑 𝑛 𝑖 𝑛 π‘Žπ‘–π‘Ÿ = πœ€ π‘Žπ‘–π‘Ÿ π‘Ÿπ‘’π‘™ β‰ˆ1 sin πœƒ 𝑐 = 𝑛 𝑑 𝑛 𝑖 Ray travels from Air to water Water to air πœƒ 𝑐 N/A 48.59Β° πœƒ 𝐡 53.13Β° 36.87Β°


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