An ocean swell propagates in deep water where the water depth is $h = 300\ \text{m}$ and the wavelength is $L = 100\ \text{m}$. Assume gravitational acceleration $g = 9.81\ \text{m/s}^{2}$.
Determine:
Deep-water waves satisfy:
$$ \frac{h}{L} \ge 0.5 $$ $$ \frac{h}{L} = \frac{300}{100} = 3.0 $$Since $3.0 \gg 0.5$, the wave clearly lies in the deep-water regime.
For deep-water waves, the phase speed is given by:
$$ c = \sqrt{\frac{gL}{2\pi}} $$Substituting the values:
$$ c = \sqrt{\frac{(9.81)(100)}{2\pi}} $$ $$ c = \sqrt{156.1} $$ $$ \boxed{c \approx 12.5\ \text{m/s}} $$This confirms the validity of the deep-water approximation.