Section 1 Calculation procedure
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Clasifications Register Guidance Information - Guidance Notes for the Classification of Special Service Craft – Calculation Procedures for Composite Construction, July 2013 - Chapter 3 Design of Single Skin Hull Laminates - Section 1 Calculation procedure

Section 1 Calculation procedure

1.1 The stress in individual plies of a laminate is calculated in accordance with Pt 8, Ch 3, Pt 8, Ch 3, 1 General of the Rules and Regulations for the Classification of Special Service Craft (hereinafter referred to as the Rules for Special Service Craft), based on bending moment (see Ch 3, 1 Calculation procedure 1.9) and the laminate stiffness of a 1 cm wide elemental strip of material.

1.2 Considering the model shown in Figure 3.1.1 Single skin example model and Figure 3.1.2 'Top-hat' stiffener used in model of a typical single skin hull laminate. Assume a pressure of 33 kN/m2 and that there is no significant panel curvature.

Figure 3.1.1 Single skin example model

Figure 3.1.2 'Top-hat' stiffener used in model

1.3 In this example the maximum bending moment is determined from Pt 8, Ch 3, Pt 8, Ch 3, 1 General of the Rules for Special Service Craft and occurs under the web at the base of the stiffener. It should be noted that no reduction in the bending moment, M b, due to aspect ratio effect is given since the panel aspect ratio, i.e. panel length/panel breadth is greater than 2. See Pt 8, Ch 3, Pt 8, Ch 3, 1 General of the Rules for Special Service Craft.

1.4 The laminate section modulus calculation is shown in Table 3.1.1 Tabulation of single skin laminiate calculations at the end of this Section. From Figure 3.1.3 Regions of tension (T) and compression (C) in example model it will be noted that there will be positions where tension and compression considerations will apply. Such calculations are ideally suited to computer based investigation.

Table 3.1.1 Tabulation of single skin laminiate calculations

  Ply No. Discription Gc Weight t lever @ E E.t E.t.x I @ EI @
(g/m2) (mm) base, x (mm) (N/mm2)     base base
Dry
see note
1 CSM 0,33 600 1,250 10,149 7200 9000 91341 1289,2 9281917
  2 CSM 0,33 600 1,250 8,899 7200 9000 80091 991,5 7139017
  3 CSM 0,33 600 1,250 7,649 7200 9000 68841 733,0 5277367
  4 CSM 0,33 600 1,250 6,399 7200 9000 57591 513,5 3696967
  5 WR 0,5 600 0,734 5,407 14000 10276 55562 214,9 3008869
  6 CSM 0,33 600 1,250 4,415 6950 8688 38355 245,3 1704699
  7 CSM 0,33 600 1,250 3,165 6950 8688 27496 126,8 881558
  8 WR 0,5 600 0,734 2,173 14500 10643 23127 35,0 507333
  9 CSM 0,33 600 1,250 1,181 6950 8688 10260 19,1 132482
  10 CSM 0,268 225 0,556 0,278 6290 3497 972 0,6 3604
Totals         10,774     86479 453637   31633812

Note 'Dry' indicates the inner surface or the hull and 'wet' the outside of the shell laminate

1.5 In order to apply a more detailed investigation it is necessary to establish the position of the neutral axis. However, in relatively balanced laminates this may be assumed to be at mid-depth. The procedure is simply to carry out the calculations assuming compressive properties on one face and tensile properties on the other face. Subsequently, the properties should be reversed and the layer stress calculations repeated. The calculated values should then be compared with the appropriate ultimate properties, i.e. dependent upon whether tension or compression considerations apply.

1.6 In the example the moments were evaluated about the base, which was taken to be the outer (wet) surface. The stiffness, EI, per 1 cm width, about the neutral axis, is determined using the parallel axis theorem:

In general:

I na = I xxAy 2
EI sect = ΣEI base – (ΣEt) x 10 x y 2

where

y = distance of neutral axis above the base (mm)

1.7 A factor of 10 (width in mm) is introduced to correct the value of area used in the parallel axis theorem, since a 1 cm wide strip of material is considered in the calculations.

From the tabulation:

EI sect = 31633812 – (86479 x 10 x 5,2462)
= 7837614 Nmm4/mm2
= 783,8 Ncm4/mm2.

1.8 From Pt 8, Ch 3, Pt 8, Ch 3, 1 General of the Rules for Special Service Craft the individual layer stresses (tensile consideration) are determined from:

1.9 More generally, the calculation of the stresses in individual layers becomes:

where

E i = E ti or E ci for the ply relative to its position above or below the neutral axis
y i = distance from the neutral axis to the outer extremity of an individual ply, i, in mm.

1.10 Consider the following typical arrangement and the associated stresses for a single shell panel outside of the slamming zone:

Consider the outer (wet) surface:

Consider the 225g/m2 chopped strand mat reinforcement in tension:

σti = 693 x 10-6 x E i y i
= 693 x 10-6 x 6290 x 5,246
= 22,9 N/mm2.

1.11 From Pt 8, Ch 3, Pt 8, Ch 3, 3.1 General 3.1.1 of the SSC Rules.

σult tension= 82,2 N/mm2 for CSM at G c =0,286

Hence, stress fraction = 22,9/82,2 = 0,278.

Figure 3.1.3 Regions of tension (T) and compression (C) in example model

1.12 From Table 7.3.1 Limiting stress criteria for local loading in Pt 8, Ch 7 of the Rules for Special Service Craft, the limiting tensile stress fraction is 0,33 for the side shell outside of the slamming zone. Hence, the calculated stress fraction is lower than the limiting stress factor and is therefore acceptable.

1.13 Similarly, consider the 600g/m2 woven roving reinforcement in tension:

σti = 693 x 10-6 x E i y i
= 693 x 10-6 x 14500 x (5,246 – 0,556 – 1,25)
= 34,6 N/mm2
σult tention = 190 N/mm2 for woven roving at G c = 0,5

Stress fraction = 34,6/190 = 0,182

Hence acceptable.

1.14 Consider the inner (dry) surface:

The 600 g/m2 chopped strand mat reinforcements at the inner surface in compression:

σci = 693 x 10-6 x E i y i
= 693 x 10-6 x 7200 x (10,744 – 5,246)
= 27,6 N/mm2
σult comp = 122 N/mm2 for CSM at G c = 0,33

Stress fraction = 27,6/122 = 0,226

Hence acceptable.


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