{"id":2526,"date":"2019-09-18T16:32:32","date_gmt":"2019-09-18T23:32:32","guid":{"rendered":"https:\/\/c21-wp.phas.ubc.ca\/?post_type=article&p=2526"},"modified":"2020-01-13T11:26:46","modified_gmt":"2020-01-13T19:26:46","slug":"sea-borne-transportation","status":"publish","type":"article","link":"https:\/\/c21.phas.ubc.ca\/article\/sea-borne-transportation\/","title":{"rendered":"Sea-borne Transportation"},"content":{"rendered":"
Ships encounter three forms of drag:<\/p>\n
The first is handled in the usual way with a shape- and Re-dependent drag coefficient. Note that by convention the wetted area is used rather than the frontal (projected) area or wing area (for aircraft).<\/p>\n
The second depends on a dimensionless quantity, the Froude Number<\/em> $Fr$ which in turn depends on the ship’s length $l$, velocity $v$ and the acceleration due to gravity $g$ (Eqn.1)[note] Richard Fitzpatrick’s fluid mechanics pages, http:\/\/farside.ph.utexas.edu\/teaching\/336L\/Fluidhtml\/node151.html<\/a> [2019-09-18].[\/note]:<\/p>\n $\\begin{equation} Fr = \\dfrac{v}{\\sqrt{gl}} \\tag{1} \\end{equation}$<\/p>\n The complicated way that the wave drag depends on $Fr$ is shown in Fig.1.<\/p>\n