Adam Cooman

YZSHGABT
Y Y→Z Y→S Y→H Y→G Y→A Y→B Y→T
Z Z→Y Z→S Z→H Z→G Z→A Z→B Z→T
S S→Y S→Z S→H S→G S→A S→B S→T
H H→Y H→Z H→S H→G H→A H→B H→T
G G→Y G→Z G→S G→H G→A G→B G→T
A A→Y A→Z A→S A→H A→G A→B A→T
B B→Y B→Z B→S B→H B→G B→A B→T
T T→Y T→Z T→S T→H T→G T→A T→B

From G-parameters to T-parameters

In matrix form, the formula is

T=([k10k10]+[Z1 k10−Z1 k10] G) ([0−Z2 k20Z2 k2]+[0k20k2] G)−1\mathbf{T} =\left(\begin{bmatrix} k_{1} & 0\\ k_{1} & 0 \end{bmatrix}+\begin{bmatrix} Z_{1}\,k_{1} & 0\\ -Z_{1}\,k_{1} & 0 \end{bmatrix}\,\mathbf{G}\right)\,{\left(\begin{bmatrix} 0 & -Z_{2}\,k_{2}\\ 0 & Z_{2}\,k_{2} \end{bmatrix}+\begin{bmatrix} 0 & k_{2}\\ 0 & k_{2} \end{bmatrix}\,\mathbf{G}\right)}^{-1}

While for each element, we obtain

T11=k1 (G22+Z2+G11 G22 Z1−G12 G21 Z1+G11 Z1 Z2)2 G21 Z2 k2T12=k1 (Z2−G22−G11 G22 Z1+G12 G21 Z1+G11 Z1 Z2)2 G21 Z2 k2T21=k1 (G22+Z2−G11 G22 Z1+G12 G21 Z1−G11 Z1 Z2)2 G21 Z2 k2T22=−k1 (G22−Z2−G11 G22 Z1+G12 G21 Z1+G11 Z1 Z2)2 G21 Z2 k2\begin{align*}T_{11} &=\frac{k_{1}\,\left(G_{22}+Z_{2}+G_{11}\,G_{22}\,Z_{1}-G_{12}\,G_{21}\,Z_{1}+G_{11}\,Z_{1}\,Z_{2}\right)}{2\,G_{21}\,Z_{2}\,k_{2}}\\T_{12} &=\frac{k_{1}\,\left(Z_{2}-G_{22}-G_{11}\,G_{22}\,Z_{1}+G_{12}\,G_{21}\,Z_{1}+G_{11}\,Z_{1}\,Z_{2}\right)}{2\,G_{21}\,Z_{2}\,k_{2}}\\T_{21} &=\frac{k_{1}\,\left(G_{22}+Z_{2}-G_{11}\,G_{22}\,Z_{1}+G_{12}\,G_{21}\,Z_{1}-G_{11}\,Z_{1}\,Z_{2}\right)}{2\,G_{21}\,Z_{2}\,k_{2}}\\T_{22} &=-\frac{k_{1}\,\left(G_{22}-Z_{2}-G_{11}\,G_{22}\,Z_{1}+G_{12}\,G_{21}\,Z_{1}+G_{11}\,Z_{1}\,Z_{2}\right)}{2\,G_{21}\,Z_{2}\,k_{2}}\\\end{align*}

The formulas are obtained with the methods explained here. The MATLAB implementation can be found in circuitconversions on Gitlab.

Definitions

[I1V2]=G[V1I2]\begin{bmatrix}I_1 \\V_2\end{bmatrix} = \mathbf{G}\begin{bmatrix}V_1 \\I_2\end{bmatrix}

[A1B1]=T[B2A2]\begin{bmatrix}A_1 \\B_1\end{bmatrix} = \mathbf{T}\begin{bmatrix}B_2 \\A_2\end{bmatrix}

The incident and reflected waves are defined as

A1=k1 (V1+I1 Z1)B1=k1 (V1−I1 Z1)A2=k2 (V2+I2 Z2)B2=k2 (V2−I2 Z2)\begin{align*}A_1 &= k_{1}\,\left(V_{1}+I_{1}\,Z_{1}\right)\qquad B_1 &= k_{1}\,\left(V_{1}-I_{1}\,Z_{1}\right)\\A_2 &= k_{2}\,\left(V_{2}+I_{2}\,Z_{2}\right)\qquad B_2 &= k_{2}\,\left(V_{2}-I_{2}\,Z_{2}\right)\\\end{align*}

with Z0,iZ_{0,i} the reference impedance for port ii and kik_i defined as

ki=12ℜ(Z0,i)ki=αℜ(Z0,i)2∣Z0,i∣k_i=\frac{1}{2\sqrt{\Re\left( Z_{0,i}\right) }}\qquad k_i=\alpha\frac{\sqrt{\Re\left( Z_{0,i} \right) }}{2\left|Z_{0,i}\right|}

depending on whether you are using power- or pseudowaves.