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 NOV CTES
 9870 Pozos Lane
 Conroe, TX 77303
 936.521.2200
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 Aberdeen, AB10 6QP
 44 (0) 1224 588788

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 4910 80 Ave SE
 Calgary AB T2C 2X3
 403.203.1581

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 Al Ghaf 4a
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 Dubai U.A.E.
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ZETA Safety System - Riser Monitoring & Safety System

Failure Modes of Well Intervention Stacks

There are basically two ways an intervention stack can fail.

Buckling
Buckling occurs due to instability of the structure. A long slender column will fail when a compressive “buckling load” is applied to the column. The classical method of calculating this buckling load is known as the Euler buckling calculation. There are models in the industry that use Euler buckling calculations to try to determine if an intervention stack is safe. There several problems with this calculation technique:

  • A ”K” factor is required for the Euler calculation, which is dependent upon the end conditions of the column. Real world intervention stacks often have more complicated end conditions than those provided for with theoretical Euler buckling. Often the K factor is misapplied. Fortunately, the K factor error is usually on the side of caution.
  • The Euler models apply to a straight, constant diameter, weightless column. An intervention stack has large BOPs, small lubricator, larger valves, all of which are far from weightless! As a result, the predicted critical buckling loads from the Euler model are higher than the actual buckling loads. This can lead to a catastrophic buckling failure during field operations.
  • These Euler models cannot address the complex loading conditions and supports found in a typical intervention stack. Side loads such as coiled tubing reel back tension, bending moments applied by off-center loads, guy wire or chain supports attached at various locations along the stack, and the bending and dynamics of moving wellheads and platforms (SPARs and TLPs) cannot be considered in these models.

With all of these shortcomings of the Euler approach, why don’t we hear of more catastrophic buckling failures? NOV CTES has analyzed many different intervention stacks as part of this effort. We found that even though accurate modeling had not been previously performed, most stacks had buckling loads greater than the expected working loads. While we’ve focused on catastrophic buckling events to this point, there are other failure modes that can cost significant time and money.

Bending
Bending of a stack component is considered a “failure” in engineering terms, but often doesn’t result in a catastrophic event such as the collapse of the stack or a release of well pressure. Thus, bending failures are often not counted as failures. This type of failure mode may damage equipment and result in operational flat time, but is more likely to be counted as a “near miss”, if it is counted at all. Yet a bending failure is much more common than a buckling failure, and increases the cost associated with the well intervention.

Until this Zeta model was completed, there were no commercially available models which determined the stresses in an intervention stack due to pressure, bending, axial load and dynamic forces. A tall intervention stack may have relatively low combined stresses when it is static, but when it begins to sway dynamically due to reel-back tension surge, wellhead movement and/or platform movement, the stress levels in the stack can increase dramatically.

Results from the Zeta Model have also provided some additional insights that may not be immediately obvious.  For example, bending failure due to wellhead movement may be worse with lower compressive loads than with higher loads. This is counter to the concept of a buckling load, which is worse as the load increases. Often a lifting frame or compensated support structure is used to apply tension to the stack, in an attempt to prevent buckling, when no buckling was eminent! Instead, these additional supports may increase the risk of bending failure. Additional cost and complexity is being added, and the job risk is being increased!

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