표 3. | Table. 3. I_in가 주어져 있으며, l ≠ 0일 때, 각 전원들의 수식 | Source equations I_in when is given with l ≠ 0.

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