To convert Z parameters (impedance parameters) to Y parameters (admittance parameters) in electrical engineering, you can use the following relationship. Given a network with impedance parameters \( Z_{11} \), \( Z_{12} \), \( Z_{21} \), and \( Z_{22} \), the corresponding admittance parameters \( Y_{11} \), \( Y_{12} \), \( Y_{21} \), and \( Y_{22} \) can be found using the following formulas:
1. **Find the Admittance Matrix \( Y \):**
The admittance parameters are given by:
\[
Y_{11} = \frac{Z_{22}}{Z_{11}Z_{22} - Z_{12}Z_{21}}
\]
\[
Y_{22} = \frac{Z_{11}}{Z_{11}Z_{22} - Z_{12}Z_{21}}
\]
\[
Y_{12} = -\frac{Z_{12}}{Z_{11}Z_{22} - Z_{12}Z_{21}}
\]
\[
Y_{21} = -\frac{Z_{21}}{Z_{11}Z_{22} - Z_{12}Z_{21}}
\]
2. **Apply the Formulas:**
- **For \( Y_{11} \):**
\[
Y_{11} = \frac{Z_{22}}{Z_{11}Z_{22} - Z_{12}Z_{21}}
\]
- **For \( Y_{22} \):**
\[
Y_{22} = \frac{Z_{11}}{Z_{11}Z_{22} - Z_{12}Z_{21}}
\]
- **For \( Y_{12} \):**
\[
Y_{12} = -\frac{Z_{12}}{Z_{11}Z_{22} - Z_{12}Z_{21}}
\]
- **For \( Y_{21} \):**
\[
Y_{21} = -\frac{Z_{21}}{Z_{11}Z_{22} - Z_{12}Z_{21}}
\]
### Example:
If you have the following Z parameters for a network:
\[
Z = \begin{bmatrix}
Z_{11} & Z_{12} \\
Z_{21} & Z_{22}
\end{bmatrix}
\]
Let's say:
\[
Z_{11} = 2 \, \Omega, \quad Z_{12} = 1 \, \Omega, \quad Z_{21} = 1 \, \Omega, \quad Z_{22} = 3 \, \Omega
\]
You can find \( Y_{11} \), \( Y_{12} \), \( Y_{21} \), and \( Y_{22} \) as follows:
1. Compute the determinant of \( Z \):
\[
\text{det}(Z) = Z_{11}Z_{22} - Z_{12}Z_{21} = 2 \times 3 - 1 \times 1 = 6 - 1 = 5
\]
2. Compute \( Y_{11} \), \( Y_{12} \), \( Y_{21} \), and \( Y_{22} \):
- \( Y_{11} = \frac{Z_{22}}{\text{det}(Z)} = \frac{3}{5} \)
- \( Y_{22} = \frac{Z_{11}}{\text{det}(Z)} = \frac{2}{5} \)
- \( Y_{12} = -\frac{Z_{12}}{\text{det}(Z)} = -\frac{1}{5} \)
- \( Y_{21} = -\frac{Z_{21}}{\text{det}(Z)} = -\frac{1}{5} \)
Thus, the Y parameters matrix is:
\[
Y = \begin{bmatrix}
\frac{3}{5} & -\frac{1}{5} \\
-\frac{1}{5} & \frac{2}{5}
\end{bmatrix}
\]
This conversion allows you to work with admittance parameters, which are sometimes more convenient for circuit analysis, especially in parallel circuits.