Step 1: General formulation of the two-phase network.
The relationship between the phase voltages \( V_p, V_q \) and the sequence voltages \( V_\alpha, V_\beta \) is given by:
\[
\begin{bmatrix}
V_p
V_q
\end{bmatrix} = S \begin{bmatrix}
V_\alpha
V_\beta
\end{bmatrix}.
\]
Here, \( S \) is a transformation matrix that determines how \( V_\alpha \) and \( V_\beta \) are mapped to \( V_p \) and \( V_q \).
Step 2: Testing given options.
To determine the valid forms of \( S \), we need to ensure that \( S \) preserves the linear relationship between \( V_p, V_q \) and \( V_\alpha, V_\beta \) while adhering to the structure of a two-phase network.
1. **Option (A):**
\[
S = \begin{bmatrix}
1 & 1
1 & -1
\end{bmatrix}.
\]
This option is valid because it satisfies the linear transformation requirements for the two-phase network.
2. **Option (B):**
\[
S = \begin{bmatrix}
1 & 1
1 & 1
\end{bmatrix}.
\]
This option is not valid, as the second row \( [1 \, 1] \) does not differentiate between \( V_\alpha \) and \( V_\beta \), which is required for the phase transformation.
3. **Option (C):**
\[
S = \begin{bmatrix}
1 & 1
1 & 0
\end{bmatrix}.
\]
This option is invalid because it does not maintain symmetry or proper mapping between \( V_p, V_q \) and \( V_\alpha, V_\beta \).
4. **Option (D):**
\[
S = \begin{bmatrix}
-1 & 1
1 & 1
\end{bmatrix}.
\]
This option is valid because it also satisfies the linear transformation requirements for the two-phase network.
Step 3: Conclusion.
The possible matrices for \( S \) are:
\[
(A) \, \begin{bmatrix} 1 & 1
1 & -1 \end{bmatrix}, \quad
(D) \, \begin{bmatrix} -1 & 1
1 & 1 \end{bmatrix}.
\]
Thus, the correct options are (A) and (D).