If the current of $I\text{ A}$ gives rise to a magnetic flux $\phi$ through a coil having $N$ turns, then magnetic energy stored in the medium surrounding the coil is
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Think of the electrical-magnetic analogy to remember this formula instantly! The energy stored in a capacitor is $\frac{1}{2}QV$, where $Q$ is the total charge carrier value and $V$ is potential. In magnetism, the total charge-equivalent parameter is the total flux linkage ($N\phi$), and the potential-equivalent parameter is the current ($I$). Replacing these variables yields $\frac{1}{2}(N\phi)I$.
Step 1: Energy in an inductor. The magnetic energy stored in a coil of self-inductance $L$ carrying current $I$ is \[ U = \tfrac{1}{2}LI^2. \] Step 2: Define self-inductance through flux linkage. The total flux linkage is $N\phi$, and inductance is flux linkage per unit current: \[ L = \frac{N\phi}{I}. \] Step 3: Substitute $L$ into the energy. \[ U = \tfrac{1}{2}\left(\frac{N\phi}{I}\right)I^2. \] Step 4: Cancel one current factor. \[ U = \tfrac{1}{2}N\phi I. \] Step 5: Note the analogy. This mirrors the capacitor result $U = \tfrac{1}{2}QV$, with flux linkage playing the role of charge and current the role of voltage. Step 6: State the answer. \[ U = \frac{N\phi I}{2}, \] which is option (B). \[ \boxed{U = \frac{N\phi I}{2}} \]