Section 3 Machinery and engineering systems
Clasification Society 2024 - Version 9.40
Clasifications Register Rules and Regulations - Rules and Regulations for the Classification of Naval Ships, January 2023 - Volume 3 Additional Class Notations - Part 1 Ship Type Capability - Chapter 1 Ice Navigation - First-Year Ice Conditions - Section 3 Machinery and engineering systems

Section 3 Machinery and engineering systems

3.1 General

3.1.1 Where the notation, Ice Class 1AS, 1A, 1B or 1C is desired, the requirements of this Section, in addition to those for open water service, are to be complied with so far as they are applicable.

3.2 Symbols and definitions

3.2.1 The symbols used in this Section are defined as follows:

A WF = area of the waterline of the bow, in m2, as shown in Figure 1.3.1 Definition of angles, areas and length
B = moulded breadth of ship, in metres
D P = diameter of the propeller, in metres
H M = thickness of the brash ice in mid channel, in metres
H F = thickness of the brash layer displaced by the bow, in metres
L BOW = length of bow, in metres, as shown in Figure 1.3.1 Definition of angles, areas and length
L PAR = length of parallel middle body, in metres, as shown in Figure 1.3.1 Definition of angles, areas and length
L WL = length of ship at deep draught waterline, in metres
T ICE = maximum ice class draught amidships, in metres, corresponding to the deep draught waterline
= displacement, in tonnes, on the maximum Ice Class draught amidships on the deep draught waterline, see Vol 3, Pt 1, Ch 1, 2.2 Definitions 2.2.1. This displacement need not be taken as greater than 80 000 tonnes
α = the angle of the waterline at B/4, see Figure 1.3.1 Definition of angles, areas and length
1 = the rake of the stem at the centreline, as shown in Figure 1.3.1 Definition of angles, areas and length
2 = the rake of the bow at B/4, as shown in Figure 1.3.1 Definition of angles, areas and length.

Figure 1.3.1 Definition of angles, areas and length

3.3 Engine output

3.3.1  Definition. The total engine output, P in Vol 3, Pt 1, Ch 1, 3.3 Engine output 3.3.2, is the maximum output the propulsion machinery can continuously deliver to the propulsion system with the propeller(s) operating at the revolutions per minute at the maximum torque for which the system is to be classed. If the output of the machinery is restricted by technical means or by any Regulations applicable to the ship, P, shall be taken as the restricted output.

3.3.2 Required engine output:

  1. For Ice Class 1AS and 1A, the total engine output is not to be less than determined by the following formula:

    P = K E kW

    where K E is as shown in Table 1.3.1 Coefficient of propulsion, K E

    R CH, in N, is the resistance of the ship in a channel with brash ice and a consolidated layer, using the following equation:

    R CH = C 1 + C 2 + 845 (H F + H M)2

    (0,15 cos + sinψ • sinα) + 42L PAR H F 2 + 825K d

    where

    Kd =

    but is not to be taken as more than 20 or less than 5

    H F = 0,26 +
    H M = 1,0 for Ice Classes 1A and 1AS

    C 1 and C 2 take into account a consolidated upper layer of the brash ice and can be taken as zero for Ice Class 1A. For Ice Class 1AS:

    C 1 = 23 + (1 + 0,021)(45,8B + 14,7L BOW + 29BL BOW)
    C 2 = (1 + 0,063)(1530 + 170B) +(400 + 480)
    Ψ = arctan
  2. For Ice Class 1B and 1C, the total engine output is not to be less than that determined by the following formula and in no case less than 740 kW:

    P = f 1 f 2 f 3 ( f 4 ∆ + P o ) kW

    where

    f 1 = 1,0 for a fixed pitch propeller
    = 0,9 for a controllable pitch propeller
    f 2 = + 0,675 but not more than 1,1
    f 2 = 1,1 for a bulbous bow

    The product, f 1 f 2, is not to be taken as less than 0,85.

    f 3 = but not less than 1,0

    f 4 and P 0 are to be taken as shown in Table 1.3.2 Values of f 4 and P 0 :

    ∆ is as defined in Vol 3, Pt 1, Ch 1, 3.2 Symbols and definitions.

Table 1.3.1 Coefficient of propulsion, K E

No. of
propellers
Propeller type
Controllable pitch propeller Fixed pitch propeller
1
2
3
2,03
1,44
1,18
2,26
1,60
1,31

Table 1.3.2 Values of f 4 and P 0

  1B 1C 1B 1C
Δ < 30 000 t Δ ≥ 30,000 t
f 4 0,22 0,18 0,13 0,11
P 0 370 0 3070 2100

3.4 Materials for shafting

3.4.1 All components of the main propulsion system are to be of steel or other approved ductile material.

3.4.2 For screwshafts in ships intended for the notation Ice Class 1AS or 1A and where the connection between the propeller and the screwshaft is by means of a key, Charpy impact tests are to be made in accordance with the requirements of Ch 5, 2.4 Mechanical tests.

3.5 Materials for propellers

3.5.1 Propellers and propeller blades are to be of cast steel or copper alloys.

3.5.2 For steel propellers, the elongation of the material used is to be not less than 19 per cent for a test piece length of 5d. Charpy impact tests are to be carried out in accordance with the requirements of Rules for the Manufacture, Testing and Certification of Materials, July 2022.

3.5.3 Spheroidal cast iron load transmitting components of controllable-pitch mechanisms are to be manufactured, tested and certified in accordance with the requirements of Table 7.3.5 Mechanical properties: special qualities in Ch 7,3 of the Rules for Materials.

3.6 Determination of ice torque

3.6.1 Dimensions of propellers, shafting and gearing are determined by formulae taking into account the impact when a propeller blade hits ice. The ensuing load is hereinafter defined by ice torque, M.

M = m D 2 kN m

where

m = 21,10 for Ice Class 1AS
= 15,69 for Ice Class 1A
= 13,04 for Ice Class 1B
= 11,96 for Ice Class 1C
D = diameter of propeller, in metres.

3.6.2 If the propeller is not fully submerged when the ship is in ballast condition, the ice torque for Ice Class 1A is to be used for Ice Classes 1B and 1C.

3.7 Propeller blade sections

3.7.1 The width, L, and thickness, T, of propeller blade sections are to be determined so that:

  1. at the radius 0,25D/2, for solid propellers

  2. at radius 0,35D/2 for controllable pitch propellers

  3. at the radius 0,6D/2

where

D = diameter of propeller, in metres
L = length of the expanded cylindrical section of the blade, at the radius in question, in mm
N = number of blades
P r = propeller pitch at the radius in question, for solid propellers, in metres
= 0,7 nominal pitch for controllable pitch propellers, in metres
R = propeller speed, in rev/min
T = the corresponding maximum blade thickness, in mm
σu = specified minimum tensile strength of the blade material, in N/mm2.

3.7.2 Where the blade thickness derived from these formulae is less than the blade thickness derived by Vol 2, Pt 4, Ch 1 Propellers, the latter is to apply.

3.8 Propeller blade minimum tip thickness

3.8.1 The blade tip thickness, t, at the radius D/2 is to be determined by the following formulae:

Ice Class 1AS

t = (20 + 2D) mm

Ice Classes 1A, 1B and 1C

t = (15 + 2D) mm

where D and σu are as defined in Vol 3, Pt 1, Ch 1, 3.6 Determination of ice torque and Vol 3, Pt 1, Ch 1, 3.7 Propeller blade sections respectively.

3.9 Intermediate blade sections

3.9.1 The thickness of other sections is to conform to a smooth curve connecting the section thicknesses as determined by Vol 3, Pt 1, Ch 1, 3.7 Propeller blade sections and Vol 3, Pt 1, Ch 1, 3.8 Propeller blade minimum tip thickness.

3.10 Blade edge thickness

3.10.1 The thickness of blade edges is to be not less than 50 per cent of the derived tip thickness, t, measured at 1,25t from edge. For controllable pitch propellers this applies only to the leading edge.

3.11 Mechanisms for controllable pitch propellers

3.11.1 The strength of mechanisms in the boss of a controllable pitch propeller is to be 1,5 times that of the blade when a load is applied at the radius 0,9D/2 in the weakest direction of the blade.

3.12 Keyless propellers

3.12.1 When it is proposed to use keyless propellers, the fit of the propeller boss to the screwshaft will be specially considered.

3.13 Screwshafts

3.13.1 The diameter d s at the aft bearing of the screwshaft fitted in conjunction with a solid propeller is to be not less than:

d s = mm

where

L and T = proposed width and thickness respectively of the propeller blade section at 0,25D/2, in mm
σo = specified minimum yield stress of the material of the screwshaft, in N/mm2
σu = specified minimum tensile strength of the blade material, in N/mm2.

3.13.2 The diameter, d s at the aft bearing of the screwshaft fitted in conjunction with a controllable pitch propeller is to be not less than:

d s = mm

where

L and T = proposed width and thickness respectively of the propeller blade section at 0,35D/2, in mm.

3.13.3 Where the screwshaft diameter as derived by Vol 3, Pt 1, Ch 1, 3.13 Screwshafts 3.13.1 or Vol 3, Pt 1, Ch 1, 3.13 Screwshafts 3.13.2 is less than the diameter derived by Vol 2, Pt 3, Ch 2, 4.4 Screwshafts and tube shafts 4.4.3 or Vol 2, Pt 3, Ch 2, 4.4 Screwshafts and tube shafts 4.4.7 as applicable the latter is to apply.

3.13.4 The shaft may be tapered at the forward end in accordance with Vol 2, Pt 3, Ch 2, 4.4 Screwshafts and tube shafts 4.4.5 or Vol 2, Pt 3, Ch 2, 4.4 Screwshafts and tube shafts 4.4.6 as applicable.

3.14 Intermediate and thrust shafts

3.14.1 The diameters of intermediate shafts and thrust shafts in external bearings are to comply with Vol 2, Pt 3, Ch 2, 4.2 Intermediate shafts 4.2.1 and Vol 2, Pt 3, Ch 2, 4.3 Thrust shafts external to engines 4.3.1 respectively, except for Ice Class 1AS ice strengthening where these diameters are to be increased by 10 per cent.

3.15 Reduction gearing

3.15.1 Where gearing is fitted between the engine and the propeller shafting, the gearing is to be in accordance with Vol 2, Pt 3, Ch 1 Gearing, and is to be designed to transmit a torque, Y i, determined by the following formula:

Y i = Y + kN m

where

u = gear ratio =
h = mass moment of inertia of machinery components rotating at higher speed
l = mass moment of inertia of machinery components rotating at lower speed, including propeller with an addition of 30 per cent of entrained water

( h and l are to be expressed in the same units)

Y = 9,55.

P and R are as defined in Vol 2, Pt 1, Ch 3, 3.3 Calculations and specifications.

3.16 Starting arrangements

3.16.1 In addition to complying with the requirements of Vol 2, Pt 7, Ch 3, 12.11 Dead ship condition starting arrangements,Pt 10, Ch 1, 12.1 General, Vol 2, Pt 7, Ch 3, 12.12 Air receivers, Vol 2, Pt 2, Ch 1, 8.5 Starting air pipe systems and safety fittings and Vol 2, Pt 2, Ch 1, 9.2 Electric starting where applicable, the capacity of the air compressors is to be sufficient for charging the air receivers from atmospheric to full pressure in half an hour for a ship with Ice Class 1AS where the propulsion engine has to be reversed for going astern.

3.17 Sea inlet chests and cooling water systems

3.17.1 The cooling water system is to be designed to ensure a supply of cooling water when navigating in ice. For this purpose at least one cooling water inlet chest is to be arranged as follows:

  1. The sea inlet chest is to be situated near the centreline of the ship and well aft if possible.

  2. As guidance for design the volume of the chest shall be about one cubic metre for every 750 kW engine output of the ship including the output of auxiliary engines necessary for the ship’s service.

  3. The chest shall be of sufficient height to allow ice to accumulate above the inlet pipe.

  4. A recirculating connection from the cooling water overboard discharge line, capable of full capacity discharge, is to be led to the chest.

  5. The net area through the grating at the shell opening is to be not less than four times the sectional area of the inlet pipe.

Where there are difficulties in meeting the requirements of Vol 3, Pt 1, Ch 1, 3.17 Sea inlet chests and cooling water systems 3.17.1.(b) and Vol 3, Pt 1, Ch 1, 3.17 Sea inlet chests and cooling water systems 3.17.1.(c) two smaller chests may be arranged for alternating intake and discharge of cooling water. The arrangement and situation otherwise shall be as above.

3.17.2 Heating coils may be installed in the upper part of the chest or chests.

3.17.3 Arrangements for circulating water from ballast tanks for cooling purposes may be useful as a reserve in ballast conditions but cannot be accepted as a substitute for sea inlet chests as described in Vol 3, Pt 1, Ch 1, 3.17 Sea inlet chests and cooling water systems 3.17.1.

3.18 Fire pumps in motor ships

3.18.1 In motor ships where clearing steam is not available, fire pumps are to be provided with suctions from the cooling water inlet chest referred to in Vol 3, Pt 1, Ch 1, 3.17 Sea inlet chests and cooling water systems.


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