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In the following circuit, the magnetic energy stored in inductor in steady state is
(1) \( \frac{1}{2} L\left(\frac{V}{R_{1}+R_{2}}\right)^{2} \)
(2) \( \frac{1}{2} L\left(\frac{V}{R_{1}}\right)^{2} \)
(3) \( \frac{1}{2} L\left(\frac{V}{R_{2}}\right)^{2} \)
(4) \( \frac{1}{2} V^{2} L\left(\frac{R_{1}+R_{2}}{R_{1} R_{2}}\right)^{2} \)
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