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ipt:basics:resonancefrequency [2024/04/04 10:21] – created adminipt:basics:resonancefrequency [2024/04/04 17:07] (current) – [Equivalent circuit] 2a02:1812:40f:9800:b890:7399:f066:e603
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 +====== Coupled coils with series resistance ====== 
 +===== Circuit =====
 +
 +Consider two coils with inductances $L_1$ and $L_2$, coupled by mutual inducance $M$. The inductors have series resistance $R_1$ and $R_2$.
 +
 {{:ipt:basics:coupled_coils_with_series_resistances.png?400|}} {{:ipt:basics:coupled_coils_with_series_resistances.png?400|}}
 +
 +===== Equivalent circuit =====
 +
 +This circuit can be represented by the following equivalent circuit:
 +
 +INSERT FIGURE HERE
 +
 +Other equivalent circuit representations can be found here.
 +
 +===== Description as a two-port network =====
 +
 +==== Impedance matrix ====
 +
 +The impedance matrix of the circuit is given by:
 +
 +\begin{align}
 + Z =
 +        \begin{bmatrix}
 + z_{11}  & z_{12} \\
 + z_{21}  & z_{22} \\
 + \end{bmatrix}=
 + \begin{bmatrix}
 + R_1+j\omega L_1 & j \omega M  \\
 + j \omega M  & R_2+j\omega L_2 \\
 + \end{bmatrix}
 +\end{align}
 +
 +with $\omega$ the angular frequency.
 +
 +==== Admittance matrix ====
 +
 +\begin{align}
 + Y = \frac{1}{det(Z)}
 + \begin{bmatrix}
 + z_{22}  & -z_{12} \\
 + -z_{21}  & z_{11} \\
 + \end{bmatrix}=
 +        \frac{1}{R_1R_2+\omega^2(M^2-L_1L_2)+j\omega (R_1L_2+R_2L_1)}
 + \begin{bmatrix}
 + R_2+j\omega L_2 & -j \omega M  \\
 + -j \omega M  & R_1+j\omega L_1 \\
 + \end{bmatrix}
 +\end{align}
 +
 +with $det(Z)$ the determinant of Z.
ipt/basics/resonancefrequency.1712226081.txt.gz · Last modified: 2024/04/04 10:21 by admin