The energy stored in an inductor carrying a steady current is given by \( U = \dfrac{1}{2}LI^2 \), with \(L\) converted into Henries. Here \(L = 32\text{ mH} = 32\times10^{-3}\text{ H}\) and \(I = 3\text{ A}\).
\[ U = \frac{1}{2}(32\times10^{-3})(3)^2 = \frac{1}{2}(32\times10^{-3})(9) = 0.144\text{ J} \]
- 288 J: This value arises if the inductance is mistakenly left in millihenries (32) instead of being converted to henries, and the factor of \(\frac{1}{2}\) is skipped, since \(32\times9=288\).
- 0.288 J: This is close to the correct method but misses the factor of \(\frac{1}{2}\) in the formula, since \((32\times10^{-3})\times9 = 0.288\), leaving the answer exactly double the true value.
- 0.144 J: This is exactly what the formula gives when \(L\) is correctly converted to henries and the \(\frac{1}{2}\) factor is applied properly, as shown in the computation above.
- 0.0 J: This would only be true if the current were zero or the coil had no inductance, but a steady \(3\text{ A}\) through a real \(32\text{ mH}\) inductor definitely stores nonzero magnetic energy.
Applying the formula carefully, with correct unit conversion and the factor of one-half included, gives a clear, unique value.
Therefore, the correct answer is 0.144 J.