Step 1: Inductor Behavior.
In an RL circuit, the inductor voltage for \( t>0 \) is defined by its natural response: \[v_L(t) = V_0 e^{-\gamma t}\] where \( \gamma = \frac{R}{L} \) represents the time constant.
Step 2: Substitute Values.
Given \( V_0 = 25 \, \text{V} \), the inductor voltage for \( t>0 \) is: \[v = 25e^{-\gamma t} \, \text{V}\]
Final Answer: \[\boxed{(2) \, v = 25e^{-\gamma t} \, \text{V}}\]