search.noResults

search.searching

saml.title
dataCollection.invalidEmail
note.createNoteMessage

search.noResults

search.searching

orderForm.title

orderForm.productCode
orderForm.description
orderForm.quantity
orderForm.itemPrice
orderForm.price
orderForm.totalPrice
orderForm.deliveryDetails.billingAddress
orderForm.deliveryDetails.deliveryAddress
orderForm.noItems
Trans RINA, Vol 161, Part A4, Intl J Maritime Eng, Oct-Dec 2019


As indicated in Figure 5, the simulation model utilises the wind tunnel measurements of turbulence as input to the FLIGHTLAB model in terms of the three axis components of wind speed and gradients of speed experienced at the rotor hub. In this regard, the document states the following:- "This is clearly a simplification of a complicated flow field that will, in reality, vary across the whole rotor disk, but again a degree of qualitative validation was obtained from the test pilots, who stated that the effect of the turbulence on the helicopter felt realistic." An important take-away from this validation exercise indicates that the airwake obtained on the helodeck on the rotor planes in wind tunnel or in CFD can be represented/replaced with single statistical quantities assumed to be acting on the rotor hub. Such quantities can be used in quantitative comparison of competing geometries studied through a parametric investigation spread over a large range of parameters using single representative values for complicated spatial variables such as turbulence.


Holdo (Holdo, 1997) reports modelling helicopter landing conditions onboard offshore structures. The paper presents the CFD modelling of wind interaction with offshore platform and its relevance to the location of the helicopter deck, the CFD modelling of gas turbine exhaust jets for a typical offshore production platform and some comparisons between CFD studies and wind tunnel model tests.


2.2


TURBULENCE INTENSITY AND FLUCTUATING VERTICAL VELOCITY


Silva et al (2010), in their investigation of helodeck of an FPSO, have mentioned the relationship between Turbulence Intensity as obtained in isotropic RANS model and the standard deviation of fluctuating vertical velocity. The CAP 437 guidelines for helodeck design recommends a maximum turbulence level based on the standard deviation of the vertical velocity (CAP 437, 2010). The numerical simulation software generally calculates the turbulence kinetic energy (k) or the turbulence intensity (I). The turbulence kinetic energy is defined by following equation:-


k = 1 2 (u′2̅̅̅̅ + v′2̅̅̅̅+w′2̅̅̅̅̅) (1)


Recalling that the turbulence is assumed as fully developed and isotropic in the RANS models, the velocity fluctuations can be assumed to be equal (Silva, et al, 2010). For the steady state regime, the term w′w′


̅̅̅̅̅̅̅ may be


interpreted as the variance of the vertical velocity w. Using these assumptions in Equation 1, the standard deviation of the vertical velocity Sw may be expressed in terms of the turbulence kinetic energy as follows:-


Sw = √w′2̅̅̅̅̅ = √2 3 k (2)


The turbulence intensity (I) is expressed in terms of turbulent kinetic energy (k) as follows:-


I = Uref


√2 3k


(3)


In view of the above, while analysing results of numerical modelling using RANS, the turbulence intensity (I) or the turbulent kinetic energy (k), hence, can be related to the Turbulence Criteria recommended in CAP 437 for offshore helodecks which places a limit on the standard deviation of the vertical velocity Sw.


2.3


HELODECK ENVIRONMENT FOR HELICOPTER PERFORMANCE


Extensive research undertaken by the British CAA for operation of helicopters on offshore platforms bring out some important understanding of the dynamics involved related to the operations aspect. This is an important feature for research in this field since it closes the loop by linking the behaviour of the helicopter, as experienced by the pilot, with the nature of the environmental disturbance, the origins of which can readily be traced back to the basic design of the ship superstructure.


Also, in order to have a better understanding of the helicopter handling qualities on Naval ships, the Research and Technology Organisation (RTO) of the North Atlantic Treaty Organisation (NATO) has published the AGARDograph 300 (2003) which documents the helicopter/ship qualification test procedures including the preparation, execution and data analysis of helicopter/ship flight testing that should be employed, combined with best safety practices to obtain maximum operational capability. Towards this pursuit, the document brings out the following:- "Basic helicopter flight limitations are usually determined in a land-based environment by the aircraft manufacturer and/or by the procuring agency. The land- based limitations are not valid in the shipboard environment due to the individual factors including ship air wake/turbulence, ship motion, confined landing areas and visual cue limitations and the combined effects of these factors. Future NATO operators and force commanders may require the maximum helicopter/ship operational capability that can be accomplished in any environmental condition."


Figure 6 shows the set-up of helicopter/ ship qualification programme as followed by Netherlands' National Aerospace Laboratory (NLR) at Amsterdam. Prior to embarking on Dynamic Interface Testing (SHOL trials), a candidate helicopter flight envelope is developed based on results of land-based hover trials of the particular helicopter and the ship airwake environment defined through wind tunnel tests. In many developing nations, SHOL trials are undertaken directly, without taking help of modern experimental and numerical tools.


©2019: The Royal Institution of Naval Architects


A-407


Page 1  |  Page 2  |  Page 3  |  Page 4  |  Page 5  |  Page 6  |  Page 7  |  Page 8  |  Page 9  |  Page 10  |  Page 11  |  Page 12  |  Page 13  |  Page 14  |  Page 15  |  Page 16  |  Page 17  |  Page 18  |  Page 19  |  Page 20  |  Page 21  |  Page 22  |  Page 23  |  Page 24  |  Page 25  |  Page 26  |  Page 27  |  Page 28  |  Page 29  |  Page 30  |  Page 31  |  Page 32  |  Page 33  |  Page 34  |  Page 35  |  Page 36  |  Page 37  |  Page 38  |  Page 39  |  Page 40  |  Page 41  |  Page 42  |  Page 43  |  Page 44  |  Page 45  |  Page 46  |  Page 47  |  Page 48  |  Page 49  |  Page 50  |  Page 51  |  Page 52  |  Page 53  |  Page 54  |  Page 55  |  Page 56  |  Page 57  |  Page 58  |  Page 59  |  Page 60  |  Page 61  |  Page 62  |  Page 63  |  Page 64  |  Page 65  |  Page 66  |  Page 67  |  Page 68  |  Page 69  |  Page 70  |  Page 71  |  Page 72  |  Page 73  |  Page 74  |  Page 75  |  Page 76  |  Page 77  |  Page 78  |  Page 79  |  Page 80  |  Page 81  |  Page 82  |  Page 83  |  Page 84  |  Page 85  |  Page 86  |  Page 87  |  Page 88  |  Page 89  |  Page 90  |  Page 91  |  Page 92  |  Page 93  |  Page 94  |  Page 95  |  Page 96  |  Page 97  |  Page 98  |  Page 99  |  Page 100  |  Page 101  |  Page 102  |  Page 103  |  Page 104  |  Page 105  |  Page 106  |  Page 107  |  Page 108  |  Page 109  |  Page 110  |  Page 111  |  Page 112  |  Page 113  |  Page 114  |  Page 115  |  Page 116  |  Page 117  |  Page 118  |  Page 119  |  Page 120  |  Page 121  |  Page 122  |  Page 123  |  Page 124  |  Page 125  |  Page 126  |  Page 127  |  Page 128  |  Page 129  |  Page 130  |  Page 131  |  Page 132  |  Page 133  |  Page 134  |  Page 135  |  Page 136  |  Page 137  |  Page 138  |  Page 139  |  Page 140  |  Page 141  |  Page 142  |  Page 143  |  Page 144  |  Page 145  |  Page 146  |  Page 147  |  Page 148  |  Page 149  |  Page 150  |  Page 151  |  Page 152  |  Page 153  |  Page 154  |  Page 155  |  Page 156  |  Page 157  |  Page 158  |  Page 159  |  Page 160  |  Page 161  |  Page 162  |  Page 163  |  Page 164  |  Page 165  |  Page 166