A third way is dimensional analysis combined with a limiting-case check: since \(v\) must depend only on \(g\) (dimensions \(LT^{-2}\)) and \(h\) (dimension \(L\)), the only combination with dimensions of velocity (\(LT^{-1}\)) is proportional to \(\sqrt{gh}\); a constant of proportionality must then be fixed by comparing to a known simple case.
Dimensionally, \( v = k\sqrt{gh} \) for some dimensionless constant \(k\). Testing against the well-known result for a fall from a small height (verified independently by direct integration of \(v=\int g\,dt\) alongside \(h=\int v\,dt\), which gives \(v^2=2gh\)) fixes \(k=\sqrt2\), so \( v=\sqrt{2gh} \).
Fixing the dimensionless constant confirms the same formula as the energy and kinematic derivations.
Therefore, the correct answer is \( \sqrt{2gh} \).