표 1. | Table. 1. V_g가 주어져 있으며, l ≠ 0일 때, 각 전원들의 수식 | Source equations when V_g is given with l ≠ 0.

Vg	Incident wave	Reflected wave	Input wave (total wave)
Voltage @z=−l	V i n c = V + ( z = − l ) = V 0 + e j β l	V r e f l e c t e d   = V − ( z = − l ) = V 0 + Γ L e − j β l	V i n = V + ( z = − l ) + V − ( z = − l ) = V 0 + ( e j β l + Γ L e − j β l )
Current @z=−l	I i n c = I + ( z = − l ) = V i n c Z 0 = V 0 + e j β l Z 0	I r e f l e c t e d   = I − ( z = − l ) = − V r e f l e c t e d   Z 0 = − V 0 + Γ L e − j β l Z 0	I i n = I + ( z = − l ) + I − ( z = − l ) = V 0 + Z 0 ( e j β l − Γ L e − j β l )
Power @z=−l	P i n c = 1 2 R e ( V i n c ⋅ I i n c * ) = 1 2 R e ( V 0 + e j β l ⋅ ( V 0 + ) * Z 0 e − j β l ) = | V 0 + | 2 2 Z 0	P r e f l e c t e d   = 1 2 R e ( V r e f l e c t e d   ⋅ I r e f l e c t e d   * ) = − 1 2 R e ( V 0 + Γ L e − j β l ⋅ ( V 0 + ) * Z 0 Γ L * e j β l ) = − | V 0 + | 2 2 Z 0 | Γ L | 2	P i n = 1 2 R e ( V i n ⋅ I i n * ) = − 1 2 R e ( V 0 + ( e j β l + Γ L e − j β l ) ⋅ ( V 0 + ) * Z 0 ( e − j β l − Γ L * e j β l ) ) = | V 0 + | 2 2 Z 0 ( 1 − | Γ L | 2 )