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Transmission Line Theory

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1 Transmission Line Theory
Shahid Bahonar University of Kerman Faculty of Engineering Electrical Engineering Department Transmission Line Theory By: Kambiz Afrooz

2 𝑉(𝑧)=π‘Ž 𝑒 βˆ’π›Ύπ‘§ +𝑏 𝑒 𝛾𝑧 =π‘Ž 𝑒 βˆ’π›Όπ‘§ 𝑒 βˆ’π‘—π›½π‘§ +𝑏 𝑒 𝛼𝑧 𝑒 𝑗𝛽𝑧
πœ•β€‰π‘‰(𝑧 πœ•β€‰π‘§ =βˆ’(𝑅+π‘—πΏπœ”) 𝐼(𝑧)  πœ•β€‰πΌ(𝑧 πœ•β€‰π‘§ =βˆ’(𝐺+π‘—πΆπœ”) 𝑉(𝑧)  πœ• 2  𝑉(𝑧 πœ•β€‰ 𝑧 2 =βˆ’(𝑅+π‘—πΏπœ”)  πœ•β€‰πΌ(𝑧 πœ•β€‰π‘§ =(𝑅+π‘—πΏπœ”)(𝐺+π‘—πΆπœ”)𝑉(𝑧)  πœ• 2  𝑉(𝑧 πœ•β€‰ 𝑧 2 = 𝛾 2 𝑉(𝑧) 𝛾= 𝑅+π‘—πΏπœ”)(𝐺+π‘—πΆπœ” =𝛼+𝑗𝛽 𝑆 2 = 𝛾 2        ⇒𝑆=±𝛾 𝑉(𝑧)=π‘Žβ€‰ 𝑒 βˆ’π›Ύπ‘§ +𝑏  𝑒 𝛾𝑧 =π‘Žβ€‰ 𝑒 βˆ’π›Όπ‘§ 𝑒 βˆ’π‘—π›½π‘§ +𝑏  𝑒 𝛼𝑧 𝑒 𝑗𝛽𝑧 𝑣(𝑧,𝑑)=π‘Žβ€‰ 𝑒 βˆ’π›Όπ‘§  cos(πœ”π‘‘βˆ’π›½π‘§)+𝑏  𝑒 𝛼𝑧  cos(πœ”π‘‘+𝛽𝑧) 

3 𝑍 𝐿 = 𝑉(0) 𝐼(0) = 𝑍 ∘ 𝑉++π‘‰βˆ’ 𝑉+βˆ’π‘‰βˆ’ π‘‰βˆ’ 𝑉+ = 𝑍 𝐿 βˆ’ 𝑍 ∘ 𝑍 𝐿 + 𝑍 ∘
In lossless case: 𝑉 𝑧 =𝑉+  𝑒 βˆ’π‘—π›½π‘§ +π‘‰βˆ’ 𝑒 𝑗𝛽𝑧 𝐼(𝑧)= 𝑉 + 𝑍 ∘ 𝑒 βˆ’π‘—π›½π‘§ βˆ’ 𝑉 βˆ’ 𝑍 ∘ 𝑒 𝑗𝛽𝑧 𝑉 0 =𝑉++π‘‰βˆ’ 𝑍 𝐿 = 𝑉(0) 𝐼(0) = 𝑍 ∘ 𝑉++π‘‰βˆ’ 𝑉+βˆ’π‘‰βˆ’ π‘‰βˆ’ 𝑉+ = 𝑍 𝐿 βˆ’ 𝑍 ∘ 𝑍 𝐿 + 𝑍 ∘ 𝐼(0)= 𝑉 + 𝑍 ∘ βˆ’ 𝑉 βˆ’ 𝑍 ∘

4 𝐼(𝑧)= 𝑉 + 𝑍 ∘ 𝑒 βˆ’π‘—π›½π‘§ βˆ’ 𝑉+Π“L 𝑍 ∘ 𝑒 𝑗𝛽𝑧 = 𝑉+(z)βˆ’π‘‰βˆ’(z) 𝑍 ∘
𝑍 𝐿 βˆ’ 𝑍 ∘ 𝑍 𝐿 + 𝑍 ∘ =Г𝐿 1+Г𝐿 1βˆ’Π“πΏ = 𝑍 𝐿 𝑍 ∘ =𝑧𝐿 π‘‰βˆ’= 𝑍 𝐿 βˆ’ 𝑍 ∘ 𝑍 𝐿 + 𝑍 ∘ 𝑉+=Г𝐿𝑉+ 𝑉 𝑧 =𝑉+  𝑒 βˆ’π‘—π›½π‘§ +𝑉+Π“L 𝑒 𝑗𝛽𝑧 = 𝑉+(z)+ π‘‰βˆ’(z) V(𝑧+Ξ»)=V(z) 𝐼(𝑧)= 𝑉 + 𝑍 ∘ 𝑒 βˆ’π‘—π›½π‘§ βˆ’ 𝑉+Π“L 𝑍 ∘ 𝑒 𝑗𝛽𝑧 = 𝑉+(z)βˆ’π‘‰βˆ’(z) 𝑍 ∘ I(𝑧+Ξ»)=I(z) Π“(z) = π‘‰βˆ’(z) 𝑉+(z) = 𝑉+Π“L 𝑒 𝑗𝛽𝑧 𝑉+  𝑒 βˆ’π‘—π›½π‘§ = Π“L 𝑒 𝑗2𝛽𝑧 Z(z)= 𝑉(𝑧) 𝐼(𝑧) = 𝑍 ∘ 𝑍 𝐿 βˆ’π‘— 𝑍 ∘ tan⁑(β𝑧) 𝑍 ∘ βˆ’π‘— 𝑍 𝐿 tan⁑(β𝑧)

5 Π“(𝑙) = π‘‰βˆ’(𝑙) 𝑉+(𝑙) = 𝑉+Π“L 𝑒 βˆ’π‘—π›½π‘™ 𝑉+ 𝑒 𝑗𝛽𝑙 = Π“L 𝑒 βˆ’π‘—2𝛽𝑙
𝛀(𝑙)=| 𝛀 𝐿 |  𝑒 π‘—β€‰βˆ β€‰ 𝛀 𝐿   𝑒 βˆ’2𝑗𝛽𝑙 | 𝛀(𝑙 |=| 𝛀 𝐿 |  𝑒 𝑗  πœ‘ 𝐿   𝑒 βˆ’2𝑗𝛽𝑙 βˆ β€‰π›€(𝑙)= πœ‘ 𝐿 βˆ’2𝛽𝑙 Z(𝑙)= 𝑉(𝑙) 𝐼(𝑙) = 𝑍 ∘ 𝑍 𝐿 +𝑗 𝑍 ∘ tan⁑(β𝑙) 𝑍 ∘ +𝑗 𝑍 𝐿 tan⁑(β𝑙) V(𝑙+0.5Ξ»)=βˆ’V(𝑙) Z(𝑙+0.5Ξ»)=Z(𝑙) Π“(𝑙+0.5Ξ»)=Π“(𝑙) I(𝑙+0.5Ξ»)=βˆ’I(𝑙)

6 Smith Chart: 𝛀(𝑧)= 𝑍(𝑧)βˆ’ 𝑍 ∘ 𝑍(𝑧)+ 𝑍 ∘ = 𝑧(𝑧)βˆ’1 𝑧(𝑧)+1 𝑧(𝑧)= 1+𝛀(𝑧 1βˆ’π›€(𝑧 𝑧(𝑧)=π‘Ÿ+𝑗π‘₯,𝛀(𝑧)= 𝛀 π‘Ÿ +𝑗 𝛀 𝑖 π‘Ÿ+𝑗π‘₯= 1+ 𝛀 π‘Ÿ +𝑗 𝛀 𝑖 1βˆ’ 𝛀 π‘Ÿ βˆ’π‘— 𝛀 𝑖 = 1+ 𝛀 π‘Ÿ +𝑗 𝛀 𝑖 1βˆ’ 𝛀 π‘Ÿ +𝑗 𝛀 𝑖 1βˆ’ 𝛀 π‘Ÿ βˆ’π‘— 𝛀 𝑖 1βˆ’ 𝛀 π‘Ÿ +𝑗 𝛀 𝑖 = 1βˆ’ 𝛀 π‘Ÿ 2 βˆ’ 𝛀 𝑖 2 +𝑗2 𝛀 𝑖 1βˆ’ 𝛀 π‘Ÿ 𝛀 𝑖 2 π‘Ÿ= 1βˆ’ 𝛀 π‘Ÿ 2 βˆ’ 𝛀 𝑖 βˆ’ 𝛀 π‘Ÿ 𝛀 𝑖 2 β‡’ 1βˆ’ 𝛀 π‘Ÿ 𝛀 𝑖 2 = 1 π‘Ÿ βˆ’ 𝛀 π‘Ÿ 2 π‘Ÿ βˆ’ 𝛀 𝑖 2 π‘Ÿ β‡’π‘Ÿβˆ’2π‘Ÿ 𝛀 π‘Ÿ +π‘Ÿ 𝛀 π‘Ÿ 2 +π‘Ÿ 𝛀 𝑖 2 =1βˆ’ 𝛀 π‘Ÿ 2 βˆ’ 𝛀 𝑖 π‘Ÿ) 𝛀 π‘Ÿ 2 βˆ’2π‘Ÿ 𝛀 π‘Ÿ +(1+π‘Ÿ) 𝛀 𝑖 2 =1βˆ’π‘Ÿβ‡’ 𝛀 π‘Ÿ 2 βˆ’2 π‘Ÿ π‘Ÿ+1 𝛀 π‘Ÿ + 𝛀 𝑖 2 = 1βˆ’π‘Ÿ 1+π‘Ÿ 𝛀 π‘Ÿ βˆ’ π‘Ÿ π‘Ÿ 𝛀 𝑖 2 = 1βˆ’π‘Ÿ 1+π‘Ÿ + π‘Ÿ π‘Ÿ 2 = π‘Ÿ 2

7 Smith Chart: 𝛀(𝑧)= 𝑍(𝑧)βˆ’ 𝑍 ∘ 𝑍(𝑧)+ 𝑍 ∘ = 𝑧(𝑧)βˆ’1 𝑧(𝑧)+1 𝑧(𝑧)= 1+𝛀(𝑧 1βˆ’π›€(𝑧 𝑧(𝑧)=π‘Ÿ+𝑗π‘₯,𝛀(𝑧)= 𝛀 π‘Ÿ +𝑗 𝛀 𝑖 π‘Ÿ+𝑗π‘₯= 1+ 𝛀 π‘Ÿ +𝑗 𝛀 𝑖 1βˆ’ 𝛀 π‘Ÿ βˆ’π‘— 𝛀 𝑖 = 1+ 𝛀 π‘Ÿ +𝑗 𝛀 𝑖 1βˆ’ 𝛀 π‘Ÿ +𝑗 𝛀 𝑖 1βˆ’ 𝛀 π‘Ÿ βˆ’π‘— 𝛀 𝑖 1βˆ’ 𝛀 π‘Ÿ +𝑗 𝛀 𝑖 = 1βˆ’ 𝛀 π‘Ÿ 2 βˆ’ 𝛀 𝑖 2 +𝑗2 𝛀 𝑖 1βˆ’ 𝛀 π‘Ÿ 𝛀 𝑖 2 π‘₯= 2 𝛀 𝑖 1βˆ’ 𝛀 π‘Ÿ 𝛀 𝑖 βˆ’ 𝛀 π‘Ÿ 𝛀 𝑖 2 = 2 π‘₯ 𝛀 𝑖 1βˆ’ 𝛀 π‘Ÿ 𝛀 𝑖 2 βˆ’ 2 π‘₯ 𝛀 𝑖 =0 1βˆ’ 𝛀 π‘Ÿ 𝛀 𝑖 βˆ’ 1 π‘₯ 2 = 1 π‘₯ 2

8 Z Chart: 𝛀 π‘Ÿ βˆ’ π‘Ÿ π‘Ÿ+1 2 + 𝛀 𝑖 2 = 1βˆ’π‘Ÿ 1+π‘Ÿ + π‘Ÿ 2 1+π‘Ÿ 2 = 1 1+π‘Ÿ 2
𝛀 π‘Ÿ βˆ’ π‘Ÿ π‘Ÿ 𝛀 𝑖 2 = 1βˆ’π‘Ÿ 1+π‘Ÿ + π‘Ÿ π‘Ÿ 2 = π‘Ÿ 2 1βˆ’ 𝛀 π‘Ÿ 𝛀 𝑖 βˆ’ 1 π‘₯ 2 = 1 π‘₯ 2

9 Y Chart: 𝛀(𝑧)= 𝑍(𝑧)βˆ’ 𝑍 ∘ 𝑍(𝑧)+ 𝑍 ∘ = 𝑧(𝑧)βˆ’1 𝑧(𝑧)+1 𝑦(𝑧)= 1βˆ’π›€(𝑧 1+𝛀(𝑧 𝑦(𝑧)=𝑔+𝑗𝑏,𝛀(𝑧)= 𝛀 π‘Ÿ +𝑗 𝛀 𝑖 𝑔+𝑗𝑏= 1βˆ’ 𝛀 π‘Ÿ βˆ’π‘— 𝛀 𝑖 1+ 𝛀 π‘Ÿ +𝑗 𝛀 𝑖 = 1βˆ’ 𝛀 π‘Ÿ βˆ’π‘— 𝛀 𝑖 1+ 𝛀 π‘Ÿ βˆ’π‘— 𝛀 𝑖 𝛀 π‘Ÿ +𝑗 𝛀 𝑖 1+ 𝛀 π‘Ÿ βˆ’π‘— 𝛀 𝑖 = 1βˆ’ 𝛀 π‘Ÿ 2 βˆ’ 𝛀 𝑖 2 βˆ’π‘—2 𝛀 𝑖 𝛀 π‘Ÿ 𝛀 𝑖 2 𝑔= 1βˆ’ 𝛀 π‘Ÿ 2 βˆ’ 𝛀 𝑖 𝛀 π‘Ÿ 𝛀 𝑖 2 β‡’ 1+ 𝛀 π‘Ÿ 𝛀 𝑖 2 = 1 𝑔 βˆ’ 𝛀 π‘Ÿ 2 𝑔 βˆ’ 𝛀 𝑖 2 𝑔 ⇒𝑔+2𝑔 𝛀 π‘Ÿ +𝑔 𝛀 π‘Ÿ 2 +𝑔 𝛀 𝑖 2 =1βˆ’ 𝛀 π‘Ÿ 2 βˆ’ 𝛀 𝑖 𝑔) 𝛀 π‘Ÿ 2 +2𝑔 𝛀 π‘Ÿ +(1+𝑔) 𝛀 𝑖 2 =1βˆ’π‘”β‡’ 𝛀 π‘Ÿ 2 +2𝑔 𝑔 π‘Ÿ+1 𝛀 π‘Ÿ + 𝛀 𝑖 2 = 1βˆ’π‘” 1+𝑔 𝛀 π‘Ÿ + 𝑔 𝑔 𝛀 𝑖 2 = 1βˆ’π‘” 1+𝑔 + 𝑔 𝑔 2 = 𝑔 2

10 Y Chart: 𝛀(𝑧)= 𝑍(𝑧)βˆ’ 𝑍 ∘ 𝑍(𝑧)+ 𝑍 ∘ = 𝑧(𝑧)βˆ’1 𝑧(𝑧)+1 𝑦(𝑧)= 1βˆ’π›€(𝑧 1+𝛀(𝑧 𝑦(𝑧)=𝑔+𝑗𝑏,𝛀(𝑧)= 𝛀 π‘Ÿ +𝑗 𝛀 𝑖 𝑔+𝑗𝑏= 1βˆ’ 𝛀 π‘Ÿ βˆ’π‘— 𝛀 𝑖 1+ 𝛀 π‘Ÿ +𝑗 𝛀 𝑖 = 1βˆ’ 𝛀 π‘Ÿ βˆ’π‘— 𝛀 𝑖 1+ 𝛀 π‘Ÿ βˆ’π‘— 𝛀 𝑖 𝛀 π‘Ÿ +𝑗 𝛀 𝑖 1+ 𝛀 π‘Ÿ βˆ’π‘— 𝛀 𝑖 = 1βˆ’ 𝛀 π‘Ÿ 2 βˆ’ 𝛀 𝑖 2 βˆ’π‘—2 𝛀 𝑖 𝛀 π‘Ÿ 𝛀 𝑖 2 π‘₯= 2 𝛀 𝑖 1βˆ’ 𝛀 π‘Ÿ 𝛀 𝑖 βˆ’ 𝛀 π‘Ÿ 𝛀 𝑖 2 = 2 𝑏 𝛀 𝑖 1βˆ’ 𝛀 π‘Ÿ 𝛀 𝑖 2 βˆ’ 2 𝑏 𝛀 𝑖 =0 1βˆ’ 𝛀 π‘Ÿ 𝛀 𝑖 βˆ’ 1 𝑏 2 = 1 𝑏 2

11 ZY Chart: 𝛀 π‘Ÿ βˆ’ π‘Ÿ π‘Ÿ+1 2 + 𝛀 𝑖 2 = 1βˆ’π‘Ÿ 1+π‘Ÿ + π‘Ÿ 2 1+π‘Ÿ 2 = 1 1+π‘Ÿ 2
𝛀 π‘Ÿ βˆ’ π‘Ÿ π‘Ÿ 𝛀 𝑖 2 = 1βˆ’π‘Ÿ 1+π‘Ÿ + π‘Ÿ π‘Ÿ 2 = π‘Ÿ 2 1βˆ’ 𝛀 π‘Ÿ 𝛀 𝑖 βˆ’ 1 π‘₯ 2 = 1 π‘₯ 2 1βˆ’ 𝛀 π‘Ÿ 𝛀 𝑖 βˆ’ 1 𝑏 2 = 1 𝑏 2 𝛀 π‘Ÿ + 𝑔 𝑔 𝛀 𝑖 2 = 1βˆ’π‘” 1+𝑔 + 𝑔 𝑔 2 = 𝑔 2


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