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en/11.3.14.md
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| + | ### Statement | ||
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| + | $11.3.14.$ [Insert the problem statement] | ||
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| + | ### Solution | ||
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| + | For two ideal inductors with self‑inductances$ L_1 $and $L_2$ and mutual inductance coefficient $M = L_{12}$, connected in series | ||
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| + | the total magnetic flux may be reinforced or partially cancelled depending on the relative orientation of the windings. The total inductance of the circuit is: | ||
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| + | $\boxed{L_{\text{total}} = L_1 + L_2 \pm 2L_{12}}$ | ||
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| + | The positive sign is taken when the currents in both coils produce magnetic fields that add (series‑aiding connection, fluxes in the same direction); the negative sign corresponds to fields that oppose each other (series‑opposing connection, fluxes in opposite directions). | ||
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| + | #### Answer | ||
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| + | [Insert a concise answer or boxed result] | ||
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| ### Statement | |||
| $11.3.14.$ [Insert the problem statement] | |||
| ### Solution | |||
| For two ideal inductors with self‑inductances$ L_1 $and $L_2$ and mutual inductance coefficient $M = L_{12}$, connected in series | |||
| the total magnetic flux may be reinforced or partially cancelled depending on the relative orientation of the windings. The total inductance of the circuit is: | |||
| $\boxed{L_{\text{total}} = L_1 + L_2 \pm 2L_{12}}$ | |||
| The positive sign is taken when the currents in both coils produce magnetic fields that add (series‑aiding connection, fluxes in the same direction); the negative sign corresponds to fields that oppose each other (series‑opposing connection, fluxes in opposite directions). | |||
| #### Answer | |||
| [Insert a concise answer or boxed result] | |||