Given the current density \( j = \alpha r \), the current \( I \) from \( r = 0 \) to \( r = \frac{R}{2} \) is calculated by integrating over the circular cross-section in cylindrical coordinates: \[I = \int_0^{\frac{R}{2}} j \cdot dA = \int_0^{\frac{R}{2}} (\alpha r) \cdot (2\pi r \, dr)\]This simplifies to:\[I = 2\pi \alpha \int_0^{\frac{R}{2}} r^2 \, dr = 2\pi \alpha \left[ \frac{r^3}{3} \right]_0^{\frac{R}{2}} = 2\pi \alpha \cdot \frac{1}{3} \cdot \left( \frac{R}{2} \right)^3\]Further calculation yields:\[I = \frac{2\pi \alpha}{3} \cdot \frac{R^3}{8} = \frac{\pi \alpha R^3}{12}\]Thus, the current is directly proportional to \( R^3 \). Final answer: \( R^3 \)