ABSTRACT

In an ideal transmission line, the voltage phasor V ˜ https://s3-euw1-ap-pe-df-pch-content-public-p.s3.eu-west-1.amazonaws.com/9781315272351/41040b79-9956-496a-ac34-683fa4364729/content/eqi6_1.jpg"/> satisfies the ordinary differential equation (2.54): ∂ 2 V ˜ ∂ z 2 + β 2 V ˜ = 0 , https://s3-euw1-ap-pe-df-pch-content-public-p.s3.eu-west-1.amazonaws.com/9781315272351/41040b79-9956-496a-ac34-683fa4364729/content/equ6_1.jpg"/> where β 2 = ω 2 L ′ C ′ = ω 2 v 2 . https://s3-euw1-ap-pe-df-pch-content-public-p.s3.eu-west-1.amazonaws.com/9781315272351/41040b79-9956-496a-ac34-683fa4364729/content/equ6_2.jpg"/>