Read the following statements regarding two port networks. (A) The condition of reciprocity and symmetry for a two-port network with 'g' parameter representation can be deduced from the interrelationship of 'h' and g parameters. (B) The condition of reciprocity for the h parameter representation leads to the condition of reciprocity for 'g' parameters representation as g 12 = −g 21 . (C) The condition of symmetry in h-parameters representation never leads to the condition of symmetry in 'g' parameters representation. (D) The symmetry condition in 'h' and 'g parameter representation can be deduced by putting h 11 = g 11 . Choose the correct answer from the options given below:
(A) and (B) only
Two-port networks are fundamental building blocks in electrical engineering, representing circuits or systems with two pairs of terminals (ports) through which electrical signals can enter or leave. These networks can be characterized by various sets of parameters, such as impedance (Z), admittance (Y), hybrid (h), inverse hybrid (g), and transmission (ABCD) parameters.
Each set of parameters relates the port voltages (\(V_1, V_2\)) and currents (\(I_1, I_2\)) in a specific manner. Understanding the relationships between these parameters and their conditions for network properties like reciprocity and symmetry is crucial for circuit analysis and design.
The hybrid parameters, or h-parameters, define the port variables as follows:
\[ \begin{pmatrix} V_1 \\ I_2 \end{pmatrix} = \begin{pmatrix} h_{11} & h_{12} \\ h_{21} & h_{22} \end{pmatrix} \begin{pmatrix} I_1 \\ V_2 \end{pmatrix} \]This expands to the equations:
For a two-port network described by h-parameters:
The inverse hybrid parameters, or g-parameters, define the port variables as follows:
\[ \begin{pmatrix} I_1 \\ V_2 \end{pmatrix} = \begin{pmatrix} g_{11} & g_{12} \\ g_{21} & g_{22} \end{pmatrix} \begin{pmatrix} V_1 \\ I_2 \end{pmatrix} \]This expands to the equations:
For a two-port network described by g-parameters:
The h and g parameters are inverses of each other in a specific way. The conversion formulas between h and g parameters can be derived by rearranging the defining equations. If the h-parameter matrix is \(\mathbf{H}\) and the g-parameter matrix is \(\mathbf{G}\), the relationships between parameters are:
| G Parameters in terms of H Parameters | H Parameters in terms of G Parameters |
|---|---|
| \(g_{11} = \frac{h_{22}}{\Delta_h}\) | \(h_{11} = \frac{g_{22}}{\Delta_g}\) |
| \(g_{12} = \frac{-h_{12}}{\Delta_h}\) | \(h_{12} = \frac{-g_{12}}{\Delta_g}\) |
| \(g_{21} = \frac{-h_{21}}{\Delta_h}\) | \(h_{21} = \frac{-g_{21}}{\Delta_g}\) |
| \(g_{22} = \frac{h_{11}}{\Delta_h}\) | \(h_{22} = \frac{g_{11}}{\Delta_g}\) |
where \(\Delta_h = h_{11}h_{22} - h_{12}h_{21}\) and \(\Delta_g = g_{11}g_{22} - g_{12}g_{21}\).
Note that \(\Delta_g = \frac{1}{\Delta_h}\) (provided \(\Delta_h \neq 0\)).
Let's evaluate each statement based on the definitions and relationships discussed:
(A) The condition of reciprocity and symmetry for a two-port network with 'g' parameter representation can be deduced from the interrelationship of 'h' and g parameters.
The reciprocity condition for g-parameters is \(g_{12} = -g_{21}\). Using the interrelationships: \(-\frac{h_{12}}{\Delta_h} = -(-\frac{h_{21}}{\Delta_h})\) This simplifies to \(h_{12} = -h_{21}\) (assuming \(\Delta_h \neq 0\)), which is the reciprocity condition for h-parameters. Thus, if we know the interrelationship and the h-parameter reciprocity condition, we can deduce the g-parameter reciprocity condition. The symmetry condition for g-parameters is \(\Delta_g = 1\). Using the interrelationship \(\Delta_g = \frac{1}{\Delta_h}\), the condition \(\Delta_g = 1\) is equivalent to \(\frac{1}{\Delta_h} = 1\), which means \(\Delta_h = 1\). This is the symmetry condition for h-parameters. So, the symmetry condition for g-parameters can also be deduced from the interrelationship and the h-parameter symmetry condition. Therefore, statement (A) is correct.
(B) The condition of reciprocity for the h parameter representation leads to the condition of reciprocity for 'g' parameters representation as \(g_{12} = -g_{21}\).
The reciprocity condition for h-parameters is \(h_{12} = -h_{21}\). Using the interrelationships: \(g_{12} = -\frac{h_{12}}{\Delta_h}\) and \(g_{21} = -\frac{h_{21}}{\Delta_h}\). If \(h_{12} = -h_{21}\), then \(g_{12} = -\frac{-h_{21}}{\Delta_h} = \frac{h_{21}}{\Delta_h}\). Also, \(-g_{21} = -(-\frac{h_{21}}{\Delta_h}) = \frac{h_{21}}{\Delta_h}\). Since \(g_{12} = \frac{h_{21}}{\Delta_h}\) and \(-g_{21} = \frac{h_{21}}{\Delta_h}\), it follows that \(g_{12} = -g_{21}\) (assuming \(\Delta_h \neq 0\)). Thus, the reciprocity condition in h-parameters (\(h_{12} = -h_{21}\)) indeed leads to the reciprocity condition in g-parameters (\(g_{12} = -g_{21}\)). Therefore, statement (B) is correct.
(C) The condition of symmetry in h-parameters representation never leads to the condition of symmetry in 'g' parameters representation.
The symmetry condition in h-parameters is \(\Delta_h = 1\). The relationship between the determinants is \(\Delta_g = \frac{1}{\Delta_h}\). If \(\Delta_h = 1\), then \(\Delta_g = \frac{1}{1} = 1\). The condition of symmetry in g-parameters is \(\Delta_g = 1\). So, the symmetry condition in h-parameters (\(\Delta_h = 1\)) actually leads to the symmetry condition in g-parameters (\(\Delta_g = 1\)). Therefore, statement (C) is incorrect.
(D) The symmetry condition in 'h' and 'g parameter representation can be deduced by putting \(h_{11} = g_{11}\).
The symmetry condition for h-parameters is \(\Delta_h = 1\). The symmetry condition for g-parameters is \(\Delta_g = 1\). The interrelationship states \(g_{11} = \frac{h_{22}}{\Delta_h}\). Setting \(h_{11} = g_{11}\) means \(h_{11} = \frac{h_{22}}{\Delta_h}\). This is one equation relating \(h_{11}\), \(h_{22}\), and \(\Delta_h\). This single equation does not imply that \(\Delta_h = 1\) or \(\Delta_g = 1\). For instance, if \(\Delta_h = 2\), the condition becomes \(h_{11} = h_{22}/2\). This is not equivalent to \(\Delta_h = 1\). Therefore, statement (D) is incorrect.
Based on the analysis of each statement using the definitions and interrelationships of h and g parameters for two-port networks, statements (A) and (B) are correct.
| Parameter Type | Defining Equations | Reciprocity Condition | Symmetry Condition | Determinant |
|---|---|---|---|---|
| Hybrid (h) | \(V_1 = h_{11}I_1 + h_{12}V_2\) \(I_2 = h_{21}I_1 + h_{22}V_2\) |
\(h_{12} = -h_{21}\) | \(\Delta_h = 1\) | \(\Delta_h = h_{11}h_{22} - h_{12}h_{21}\) |
| Inverse Hybrid (g) | \(I_1 = g_{11}V_1 + g_{12}I_2\) \(V_2 = g_{21}V_1 + g_{22}I_2\) |
\(g_{12} = -g_{21}\) | \(\Delta_g = 1\) | \(\Delta_g = g_{11}g_{22} - g_{12}g_{21}\) |
Besides h and g parameters, other common representations for two-port networks include:
Conversions between any two sets of parameters are possible, provided the required determinant is non-zero. For instance, Z parameters are defined only when the network is open-circuited at both ports, and Y parameters when short-circuited at both ports. H and G parameters are suitable for networks that are neither open-circuited nor short-circuited at both ports simultaneously.
A Two - port network is reciprocal if and only if:
A passive 2-port network is in a steady-state. Compared to its input, the steady state output can never offer ________.
The condition for symmetric property of ABCD parameter of two port network is:
A two-port network has scattering parameters given \(\left[ s \right] = \left[ {\begin{array}{*{20}{c}} {{s_{11}}}&{{s_{12}}}\\ {{s_{211}}}&{{s_{22}}} \end{array}} \right]\). If the port 2 of the two-port is short-circuited, the s11 parameter for the resultant one-port network is