Longitudinal Centre of Flotation (LCF)

Determine the longitudinal position of the waterplane centroid using waterplane moments or sectional half-breadths with Simpson’s rule.

x is measured forward from AP. The entered area and first moment must describe the same waterplane and use the same longitudinal datum.

Result — Waterplane Moment

LCF from AP: m

LCF as % of LPP from AP: %

Enter inputs to compute.
Enter one non-negative half-breadth for each equally spaced station, ordered from AP to FP. The first station is x = 0 and the final station is x = LPP. The calculator mirrors these values across the centreline, so do not enter full breadths. This method assumes a port-starboard symmetric waterplane.
Result — Simpson Integration

LCF from AP: m

LCF as % of LPP from AP: %

Enter inputs to compute.

Longitudinal Centre of Flotation (LCF): Formula, Datum and Simpson Integration

The longitudinal centre of flotation is the fore-and-aft position of the geometric centroid of a ship's waterplane area at a stated draft. It describes where the waterplane area is balanced longitudinally.

LCF is a position, not an area or moment. A reported value must therefore state its longitudinal datum, positive direction, length reference and loading condition.

This calculator uses the aft perpendicular (AP) as its origin. Positive distances are measured forward, with x = 0 at AP and x = LPP at the forward perpendicular (FP).

Longitudinal centre of flotation formula

The coordinate of the waterplane centroid is its first longitudinal moment divided by its total area:

xF = ∫x dA ÷ AWP

On this page, xF is reported as LCF measured forward from AP.

Symbols used in the LCF calculation
Symbol Meaning Usual unit
xF Longitudinal coordinate of the centre of flotation m
x Longitudinal coordinate measured from the selected datum m
dA Element of waterplane area m2
∫x dA First longitudinal moment of waterplane area about the datum m3
AWP Total area of the selected waterplane m2
LPP Length between aft and forward perpendiculars m

Dividing a first moment in m3 by an area in m2 produces a longitudinal distance in metres.

Datum requirement: the area moment and the reported LCF must use the same origin and positive direction. This calculator assumes a moment about AP with positive x measured forward.

Worked example: direct waterplane-moment method

Consider the following waterplane properties:

  • AWP = 2,240 m2
  • First moment about AP ∫x dA = 139,733.333 m3
  • LPP = 120 m

Step 1: Calculate LCF from AP

LCFAP = 139,733.333 ÷ 2,240 = 62.381 m

Step 2: Express the position as a percentage of LPP

LCF = 62.381 ÷ 120 × 100 = 51.984% of LPP from AP

The centre of flotation is therefore 62.381 m forward of AP.

Calculation methods available on this page

Comparison of the two LCF calculation methods
Method Main inputs Suitable use
Waterplane first moment AWP, ∫x dA and LPP Known waterplane hydrostatic properties
Half-breadth integration LPP and equally spaced waterline half-breadths Waterline offsets or preliminary hull geometry

1. Waterplane first-moment method

Use this method when waterplane area and its first longitudinal moment are available from hydrostatic calculations, a hull model or approved vessel particulars.

The two values must refer to the same waterline, draft, trim and datum. A first moment calculated about FP or amidships cannot be entered as though it were taken about AP.

The entered LPP does not alter the centroid obtained from moment divided by area. It is used to express the result as a percentage of the AP–FP length.

2. LCF from waterline half-breadths

For a port-starboard symmetric waterplane, its area can be found from the half-breadth function y(x):

AWP = 2∫y(x) dx

The first longitudinal moment about AP is:

M1 = 2∫xy(x) dx

The centre of flotation is then:

LCF = 2∫xy dx ÷ 2∫y dx = ∫xy dx ÷ ∫y dx

The symmetry factor of two cancels in the centroid ratio. It remains necessary when reporting the complete waterplane area and its full first moment.

Simpson integration used by the calculator

For N equally spaced stations over LPP, the spacing is:

Δx = LPP ÷ (N − 1)

Simpson's one-third rule is applied to the half-breadths:

∫y dx ≈ Δx ÷ 3 × [y0 + yn + 4(y1 + y3 + ... + yn−1) + 2(y2 + y4 + ... + yn−2)]

The same Simpson multipliers are applied to the products xiyi to obtain the half-waterplane first moment.

Station requirement: Simpson's one-third rule requires an even number of intervals and therefore an odd number of equally spaced stations. Values must be entered in order from AP to FP.

Worked example: LCF from half-breadths

Consider seven equally spaced stations:

  • LPP = 120 m
  • N = 7 stations
  • Half-breadths from AP to FP = 0, 6, 12, 15, 14, 8, 0 m

Step 1: Calculate station spacing

Δx = 120 ÷ (7 − 1) = 20 m

Half-breadths and first-moment products
Station x from AP (m) y(x) (m) xy(x) (m²) Simpson multiplier
00001
12061204
240124802
360159004
480141,1202
510088004
6120001

Step 2: Integrate the waterplane area

AWP = 2 × 20 ÷ 3 × [0 + 0 + 4(6 + 15 + 8) + 2(12 + 14)]

AWP = 2,240 m2

Step 3: Integrate the first moment about AP

M1 = 2 × 20 ÷ 3 × [0 + 0 + 4(120 + 900 + 800) + 2(480 + 1,120)]

M1 = 139,733.333 m3

Step 4: Calculate LCF

LCF = 139,733.333 ÷ 2,240 = 62.381 m from AP

LCF = 51.984% of LPP from AP

AP, FP and amidships reporting conventions

The same physical position may be reported from AP, from FP, as a percentage of length or relative to amidships.

Equivalent reporting conventions for the worked example
Convention Calculation Reported value
Forward from AP xF 62.381 m from AP
Aft of FP LPP − xF 57.619 m aft of FP
Percentage from AP xF/LPP × 100 51.984% LPP
Relative to amidships, positive forward xF − LPP/2 2.381 m forward of amidships

Hydrostatic tables may instead use amidships as zero and take aft as positive. The datum and sign convention must be read before values are compared.

Do not compare unsigned values: a value stated as 2.4 m aft of amidships cannot be compared directly with 52% of LPP from AP without converting both to the same convention.

LCF and small changes of trim

LCF is the centroid of the current waterplane. For a sufficiently small change of trim, the change in waterline is commonly represented as a rotation about LCF.

Adding or removing a small weight at LCF produces approximately parallel sinkage or rise because the weight has no longitudinal lever relative to LCF. Adding or removing the same weight away from LCF produces a trimming moment:

Trimming moment = w × d

Here, d is the signed longitudinal distance between the weight and LCF. The corresponding small change of trim requires MCT 1 cm or another equivalent longitudinal stiffness quantity:

Change of trim in centimetres = Trimming moment ÷ MCT 1 cm

Pure moment distinction: a pure trimming couple changes trim regardless of the point at which it is drawn. The no-trim statement applies to adding or removing a small weight at LCF, not to applying a pure moment there.

LCF, LCB and LCG are different positions

Difference between LCF, LCB and LCG
Position Geometric or physical basis Main use
LCF Centroid of waterplane area Small-trim reference and waterplane geometry
LCB Centroid of displaced underwater volume Longitudinal position of buoyancy
LCG Centroid of the vessel's total weight Longitudinal position of gravity

LCB and LCG are used when considering longitudinal equilibrium. LCF is used when distributing small changes of draft caused by trim.

LCB–LCF separation alone does not determine trim tendency. The relevant equilibrium comparison is between LCG and LCB, while LCF and longitudinal waterplane inertia influence the response to a small trimming moment.

Waterplane span and the LPP station method

The station tab integrates half-breadths only over the entered LPP span from AP to FP.

If the actual selected waterline extends appreciably forward of FP or aft of AP, those areas and their moments are omitted by this station method. The resulting centroid then describes the entered AP–FP portion rather than the complete waterplane.

For such a hull, use complete waterplane geometry or direct hydrostatic AWP and first-moment data calculated over the full intended waterplane.

Effect of draft, trim and heel

LCF belongs to a particular waterplane. As draft changes, bow flare, stern geometry, transom immersion and the length of the waterline may alter the area distribution and move the centroid.

A value calculated for an even-keel condition should not automatically be applied to a substantially trimmed condition.

Heel may also alter the waterplane centroid on flared, chined or asymmetric hulls. The station method on this page assumes a symmetric waterplane represented by one set of half-breadths.

Accuracy of Simpson integration

Simpson integration approximates the shape between the supplied ordinates. Accuracy depends on equal spacing and on whether the station series captures rapid changes in the waterline.

Additional geometric detail may be required near:

  • fine bow and stern endings
  • an immersed transom
  • knuckles or chines
  • abrupt flare changes
  • waterline intersections beyond AP or FP

This calculator does not support unequal station spacing, arbitrary coordinates or mixed Simpson multipliers.

What LCF can and cannot show

LCF is useful for hydrostatic reporting, small-trim calculations, checking waterplane geometry and locating the longitudinal waterplane centroid.

LCF alone cannot determine:

  • final forward and aft drafts
  • displacement or TPC
  • MCT 1 cm
  • longitudinal metacentric height
  • LCB or LCG
  • longitudinal equilibrium
  • large changes of trim
  • transverse stability
  • ship resistance or required power

Common input errors

  • Entering a first moment calculated about FP as though it were about AP.
  • Combining waterplane area and first moment from different drafts.
  • Using LWL or LOA when the station series is defined over LPP.
  • Entering full breadths where the calculator expects half-breadths.
  • Entering station values from FP to AP instead of AP to FP.
  • Using an even number of stations.
  • Using unequal station spacing.
  • Entering a different number of ordinates from the stated station count.
  • Entering negative half-breadths.
  • Including invalid text that is silently mistaken for missing data.
  • Assuming the station method includes waterplane area beyond AP and FP.
  • Mixing metres, feet, square metres or cubic metres.
  • Comparing LCF values using different datums or sign conventions.
  • Confusing LCF with LCB or LCG.
  • Treating LCF as constant over a large change of draft or trim.

Result check: the station-integration result should lie within the entered AP–FP span because all half-breadths are non-negative and all coordinates lie between 0 and LPP. An out-of-range result indicates invalid station order, spacing or input data.

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References

The definitions and numerical methods used on this page follow established naval-architecture sources:

  1. United States Naval Academy, Principles of Ship Performance, Chapter 2: Hull Form and Geometry, sections covering waterplane area, centre of flotation and numerical integration: USNA hull form and geometry notes.
  2. Tupper, E. C., Introduction to Naval Architecture, 5th edition, Butterworth-Heinemann, 2013: Introduction to Naval Architecture.
  3. Rawson, K. J. and Tupper, E. C., Basic Ship Theory, Combined Volume, 5th edition, Butterworth-Heinemann, 2001: Basic Ship Theory.

NauticalSolver calculators are intended for preliminary engineering, study and independent checking. Use approved hydrostatic particulars, vessel-specific waterplane geometry and the loading computer for operational, contractual or statutory trim calculations.