Another way to see this is through the Euler buckling load formula, \(P_{cr} = \dfrac{\pi^2 EI}{L_e^2}\), and how it behaves as the column becomes shorter and stockier.
This formula shows that the critical buckling load grows rapidly (inversely with the square of the effective length) as a column gets shorter, meaning very short columns have an extremely high theoretical buckling load — so high that the column crushes (fails by yielding of the material) long before it could ever buckle. In that situation, the column's compressive capacity is governed purely by the material's crushing or yield strength times its cross-sectional area, which is exactly the same basis used to compute its tensile capacity.
Applying Euler's buckling formula shows the compressive capacity converges to the same material-strength basis as tension only when the column is short.
Therefore, the correct answer is short column.