A vessel with a displacement hull moving at even moderate speeds in shallow water will experience vertical sinkage, or ``squat,'' as a result of a pressure drop beneath its hull [4].
A number of empirical formulas have been devised to model the squatting problem:
Barrass [1]: | S = | 1/30 · Cb · (As / [Ac - As] )2/3 · Vk2.08 |
Millward [3]: | S = | (L/100) · ([15 · Cb · (B/L) - 0.55] · Fnh2 ) / (1 - 0.9 · Fnh ) |
Norrbin [4]: | S = | (L/100) · ([100 / (L/h)] · [As / Ac] · Fnh2 ) / |
(1 - [As / Ac] - [(h · W0) / Ac] · Fnh2 ) | ||
Tuck [5]: | S = | L · Cs · Fnh2 / (1 - Fnh2 )1/2 |
For all models, the ship clearance is equal to the channel depth minus the ship draft minus the ship squat:
Clearance: | c = h - T - S |
Look at some examples of the numeric and graphical output from the squat models.
Evaluate the squat models.
Plot (univariate) the squat models.
Plot (bivariate) the squat models.
Plot (trivariate) the squat models.
Ac | : | cross-sectional area of channel (m2) | As | : | immersed cross-sectional area of ship (m2) |
B | : | ship beam (m) | c | : | ship clearance, h-T-S (m) |
Cb | : | ship block coefficient | Cs | : | Tuck's ship form factor |
Fnh | : | Froude number of depth, V/(gh)1/2 | g | : | gravitational acceleration, 9.81 (m/sec2) |
h | : | channel water depth (m) | L | : | ship waterline length (m) |
S | : | ship squat (m) | T | : | ship draft (m) |
V | : | ship speed (m/sec) | Vk | : | ship speed (knots, i.e. nautical miles per hour) |
Wo | : | channel waterline width (m) |
C. B. Barrass, ``The Phenomena of Ship Squat,'' International Shipbuilding Progress, 26:44-47, 1979.
This service is a result of the project Formulation of a Model for Ship Transit Risk funded by the U.S. Department of Commerce, U.S. Army Corps of Engineers, and U.S Coast Guard (PIs: N. M. Patrikalakis, MIT, and H. L. Kite-Powell, WHOI).