Hydrostatics

Introduction

For every floating body therefore for all offshore structures the buoyancy and the stability are critical to the feasibility of the design. The first requirement that the platform has sufficient buoyancy to carry the total weight of the structure itself and, in our case, the weight of the topside facilities (2x6 MW wind turbines, accommodation, substation, crane, research centre).

Methodology

Buoyancy is the upward force that the water applies to a body and, depending on the weight of the structure and the force, the body may float, sink or remain neutrally buoyant in the water [1].

The laws of the buoyancy can be summarised as follows:

  • The volume displaced by a floating body is equal in weight with the weight of the body – i.e. Floating Condition

  • The buoyancy force acting on a floating body is equal to the weight of the displaced water [2]

  • The static forces acting on a floating platform in the water are gravity (the total weight of the structure) and buoyancy (the weight of the water displaced by the platform hull).

    Figure 1. Stability reference points

  • K: Keel is the lowest of the floating body point including the thickness of the hull.
  • B: Centre of Buoyancy is the point where all the buoyancy forces are considered to apply in a vertical upward direction. It is the geometric centre of the underwater body of the structure.
  • G: Centre of Gravity is the point where all the gravity forces are considered to apply. It is the centre of mass of the floating structure.
  • M: Metacentre is the point where two lines intersect. The line of comes through the Centre of Buoyancy in equilibrium with the line comes through the moved Centre of Buoyancy as the floating body inclined to one side [3].
  • Figure 2. Metacenter point [2]

    An important quantity in the buoyancy analysis is the metacentric height (GM). The metacentric height is a measurement of the initial static stability of the floating body.

    The equation described the metacentric height is:

    GM=KB+BM-KG [4]

    The above formula represents the available of the floating body GM, where:

  • KB= the vertical distance from the Keel to the Centre of Buoyancy
  • BM= the vertical distance from the Centre of buoyancy to the Metacentre
  • KG= the vertical distance from the Keel to the Centre of Gravity
  • The first thing needs to be calculated is the KB. KB can be calculated from the below equation:

    KB=0.5DWL

    Where DWL is equal to the draft of the structure (the distance from the Keel to the water plane).

    Secondly BM should be calculated. BM is very important in buoyancy analysis and is equal to the moment of inertia around the water plane over the volume of displacement.

    BM=I/V [4]

    The moment of inertia can be calculated assuming rectangle beam from the equation bellow:

    I=1/12 LB3

    Where:

  • L= length of the platform
  • B= breadth of the platform
  • There are three particular stability conditions regarding the numerical value of metacentric height.

  • If the metacentric height is positive (G under M): stable condition
  • If the metacentric height is negative (G over M): neutral equilibrium
  • If the metacentric height is zero (G=M): unstable condition [2]
  • In order a floating body to be stable the numerical value of the metacentric height should be positive. This is the first floating condition. In case the metacentric height is larger that means that the floating body has better initial stability against overturning [2].

    Afterwards and regarding the second floating condition the displaced weight of water should be equal to the total weight of the structure.

    Analysis and Results

    The buoyancy analysis accomplished for the needs of our project focused on the calculation of the metacentric height. The platform was modelled in AutoCad, then imported to MaxSurf to carry out the analysis, at which point some design simplifications were made. It was assumed that the platform was a full concrete box and the curves and slopes of the external cylinders were not included, as this was only a first pass analysis to determine the overall feasibility of the design.

    Figure 3. Design layout in MaxSurf

    As a result, volume of the platform’s concrete was marginally overestimated; however, this assumption will affect the analysis results by less than 2%.

    Moreover, only the total weight of the structure was included in the analysis – the topside facilities total weight was estimated to be 4,000 to 5,000 tons, which is less than 1% of the total weight, therefore the model was simplified to be solely the concrete structure. As the design of the PSP allows the draft to be altered by varying the air volume in the cylinders, the draft was set to 10 m. Due to the solid deck, the centre of gravity was shifted slightly from the midline and assumed to be 20 m.

    The variables imported in the software to run the analysis were the layout of the platform, the height, the density of concrete, the draft and the Centre of Gravity. The MaxSurf results are presented in the following table:

    Displacement332,512tons
    Volume (displaced)324,401m3
    Draft Amidships10m
    Immersed depth10m
    WL Length720m
    Beam max extents on WL1,247m
    Wetted Area36,820m2
    Max sect. area457m2
    Waterpl. Area35,492m2
    Prismatic coeff. (Cp)0.99 
    LCB length360from zero pt. (+ve fwd) m
    LCF length360from zero pt. (+ve fwd) m
    LCB %50from zero pt. (+ve fwd) % Lwl
    LCF %50from zero pt. (+ve fwd) % Lwl
    KB5m
    KG fluid20m
    BMt50.7m
    BML4,595m
    GMt corrected35.7m
    GML4,562m
    KMt55.7m
    KML4,599m
    Immersion (TPc)363tons/cm
    MTc21069tons*m
    RM at 1deg = GMt.Disp.sin(1)104,426tons*m
    Length/Beam (ratio)0.58 
    Beam/Draft (ratio)136.52 
    Length:Vol^0.333 ratio10.48 
    PrecisionMedium58 stations

    Conclusions

    It is clearly seen that the metacentric height, GMt corrected, is positive:

    GM=KB+BM-KG=5.0+50.7-20.0=35.7 m

    As a result, the platform is in stable condition and the first requirement is fulfilled. Moreover, it is obvious that we are far from the neutral equilibrium. When a small angular displacement is applied the platform tends to return to its preliminary position.

    The large metacentric height in this case justifies greater stability. The platform rolls with small roll angles and periods. The structure is considered more “stiff” in roll.

    Less stable floating bodies have smaller metacentric heights and roll slowly with longer roll periods [5].

    Afterwards assuming a full reinforced concrete box, the displaced weight of water is equal to 332,512 tons and fulfils the second requirement of the floating conditions.

    Despite the fact that many assumptions made, the results are reasonable. However, for more accurate results in depth analysis is required.

    Go to Hydrodynamics

    References
  • [1] "fas.org," 6 4 2016. [Online]. Available: http://fas.org/man/dod-101/navy/docs/swos/dca/stg4-01.html.

  • [2] "www.phillyseaperch.org," 7 4 2016. [Online]. Available: http://www.phillyseaperch.org/uploads/9/1/0/6/9106381/_buoyancy_for_hs.pdf.

  • [3] "www.britannica.com," 7 4 2016. [Online]. Available: http://www.britannica.com/science/metacentre.

  • [4] "http://hawaii-marine.com/," 6 4 2016. [Online]. Available: http://hawaii-marine.com/templates/stability_article.htm.

  • [5] M. Mulholland, 4 16 2016. [Online]. Available: http://www.gwpda.org/naval/gmdefn.htm. [Accessed 1999 7 12].