Section 3 Drag coefficients for pontoons
Clasification Society 2024 - Version 9.40
Clasifications Register Rules and Regulations - Rules and Regulations for the Classification of Linkspans, July 2022 - Part 3 Construction, Design and Test Requirements - Chapter 9 Highway Loads, Section Aerodynamics and Pontoon Drag Coefficients - Section 3 Drag coefficients for pontoons

Section 3 Drag coefficients for pontoons

3.1 General

3.1.1 The nature of the forces on floating bodies is considerably complex and not fully understood. In theory, the forces depend on factors such as speed of flow, area normal to the flow, total wetted area, roughness, detailed form or shape, and the proximity of the seabed or other boundaries and bodies. In practice, simplifications are made when describing forces.

3.2 Wall-sided boxes

3.2.1 Towing tests on wall-sided boxes have also been performed and results are reproduced in Table 9.3.1 Typical current drag coefficients for wall-sided boxes.

Table 9.3.1 Typical current drag coefficients for wall-sided boxes

Shape of model Breadth/draught ration B/D Drag force coefficient C D
Square 8,1 0,72
3,4 0,70
1,6 0,86

Note A drag coefficient of 1,0 should be used unless reliable values can be obtain.

3.3 Pontoons and barges

3.3.2 The coefficients in Figure 9.3.1 Longitudinal drag coefficient for rectangular pontoon in deep water and Figure 9.3.2 Transverse drag coefficient for rectangular pontoon in deep water and Table 9.3.1 Typical current drag coefficients for wall-sided boxes apply when the water is deep (depth/draught ≥ 5). The coefficients in Figure 9.3.3 Longitudinal drag coefficient at various water depths for rectangular pontoon with current head on and Figure 9.3.4 Transverse drag coefficient at various water depths for rectangular pontoon with current beam on apply in shallow water.

The following equations should be used when applying the coefficients given in Figure 9.3.1 Longitudinal drag coefficient for rectangular pontoon in deep water, Figure 9.3.2 Transverse drag coefficient for rectangular pontoon in deep water, Figure 9.3.3 Longitudinal drag coefficient at various water depths for rectangular pontoon with current head on, Figure 9.3.4 Transverse drag coefficient at various water depths for rectangular pontoon with current beam on.

F x = ½ (C xρV 2 A x)
F y = ½ (C yρV 2 A y)
where
F x = the current force along the longitudinal (x) axis (in kN)
F y = the current force along the transverse (y) axis (in kN)
C x = the longitudinal current force drag coefficient
C y = the transverse current force drag coefficient
ρ = the mass density of water (in t/m3)
A x = the effective current area normal to the longitudinal (x) axis (in m)
A y = the effective current area normal to the transverse (y) axis (in m)
V = the incident current velocity (in m/s).

Figure 9.3.1 Longitudinal drag coefficient for rectangular pontoon in deep water

Figure 9.3.2 Transverse drag coefficient for rectangular pontoon in deep water

Figure 9.3.3 Longitudinal drag coefficient at various water depths for rectangular pontoon with current head on

Figure 9.3.4 Transverse drag coefficient at various water depths for rectangular pontoon with current beam on


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