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*BEAMPRO2
Data format:
An arbitrary number of lines with 11 parameters each, as follows:
IPRO ITRUETENS AIRIN WT OD DBUOY XJ63 XJ36 DENDCAP CL DCONT
...
Status:
Optional
Purpose:
To define geometrical properties of a set of beam elements previously defined by global stiffnesses (*BEAMPRO)
Details :
Parameter | Description |
---|---|
IPRO | Identification number referring to a keyword *BEAMPRO previously defined. |
ITRUETENS | A flag to select whether the axial behavior of the line is defined with respect to the effective tension or to the true wall tension. ITRUETENS = 0 (default): The axial behavior of the riser is given with respect to the effective tension; ITRUETENS = 1 : The axial behavior of the riser is given with respect to its true tension; |
AIRIN | Internal cross section of the riser (m2); |
WT | Wall thickness of the riser (m); |
OD | Outer diameter of the riser (m) |
DBUOY | Buoyancy diameter (m) |
XJ63 | = 0 (obsolete) |
XJ36 | = 0 (obsolete) |
DENDCAP | End cap diameter (m) |
CL | Lift coefficient (used if contact and *LIFTOPTION is defined) |
DCONT | Contact diameter (m) |
Note
Classically, the presence of a fluid inside and outside the riser is accounted for resorting to the effective tension concept. The true tension is linked to the effective tension by the following relationship :
T_{true} = T_eff - P_e S_e + P_i S_i
Where: - P_e is the external pressure due to sea water hydrostatic pressure, - P_i is the internal fluid pressure, - S_e is the external section of the pipe calculated from the hydraulic diameter : S_e = \pi * D_h^2/4 - S_i is the internal cross section (AIRIN hereabove).
The same relation exists between the stresses. The true axial stress
\rho_{real} is deduced from the effective stress \rho_{eff} :
\rho_{real} = \rho_{eff} + \rho_{p} with \rho_p = \frac{P_i S_i - P_e S_e}{S_e - S_i}
The total apparent weight of the global system riser + fluid is used in the
calculations and the resulting effort is then the effective tension. A special
attention must be paid to the link between the axial strain of the riser and
the effective tension :
- When a multi-linear axial stiffness is defined, it is important to distinguish the effective tension from the true tension. When ITRUETENS=1, the axial behaviour is expressed in terms of the true tension;
- On the other hand, due to the Poissons coefficient, the fluid pressures change the axial strain. When ITRUETENS=1,the axial strain is corrected the pressures effect.