Step 1: Picture how the column actually bends. A column fixed at the base and completely free at the top (a cantilever column) bends like one quarter of a full sine wave, bulging outward only near the free end. Step 2: Match this shape to an equivalent pin ended column. A pin ended column of length $L_e$ buckles into a full half sine wave. Since a quarter sine wave of the cantilever is the same curve as half of a sine wave twice as long, the cantilever behaves like a pin ended column of length $2L$. Step 3: Read off the effective length. \[ L_e = 2L. \] \[ \boxed{2L} \]