Page 42 - Failure Analysis Case Studies II
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          together  they can carry  1.59MN. The total  load  that corresponds to the  19.5kN/m2 maximum
          pressure applied simultaneously across the whole firewall is 5.77 MN. The clamps are at midheight,
          and can be expected to carry at least half the total load. It follows that the clamps are not strong
          enough to carry the total load on the wall, and that the clamps would break if the the wall had not
          already broken up by failure of the frame bolts.
            The analysis is based on plate theory, which is approximate because the deflection is not necessarily
          small by comparison with the effective thickness of the firewall. The effective thickness of the wall
          was estimated by finding the thickness which gives the same ratio between the fully-plastic membrane
          stress resultant at collapse in pure tension and the fully-plastic membrane stress resultant at collapse
          in pure bending [3], both calculated for the governing mode of frame-bolt failure in tension. The
          efective thickness turns out to be 80mm for one direction of bending and  120mm for the other.
          Moreover, the sides of the wall segments are not rigidly fixed at the top and bottom. It is known [4]
           that small inward movements at the edges of transversely-loaded plates much reduce the stiffening
          effect of membrane action, and an approximate calculation showed that in this instance an inward
          edge movement of the order of  1 mm would be enough to eliminate a significant increase in strength
           because of membrane effects. It was concluded that these effects could be neglected.


                           10.  RESPONSE OF  C/D  AND  A/B  FIREWALLS

            The wall between modules C and D was much stiffer and stronger than the wall between modules
           B and C. The estimated collapse pressure of one of  its triangular  panels under quasi-static slow
           loading is about 12 kN/m* (0.12 bars), compared to the peak pressure of 19.5 kN/m2 at PI in module
           C. The lowest natural frequency of one of its triangular segments is about 410 rad/s, corresponding
           to a period of 15 ms, and its response is not far from quasi-static.
            The control room was in D module to the north of the C/D firewall, and had an additional wall
           of steel plate. Two survivors were in the control room at the time of the explosion. They were blown
           across the room, and saw that equipment near the wall  had been  damaged and that  smoke was
           apparently entering at the top part of the wall. Accordingly, since the C/D wall is stronger than the
           B/C wall, it can  be concluded independently that the  B/C wall  would  have been  more severely
           damaged by an explosion in C module than the C/D wall was.
            The A/B wall was similar to the B/C wall in construction  and arrangement. There is evidence
           from survivors that the A/B wall was not damaged. This supports the conclusion that the initial
           explosion was in C module. If the initial explosion had been in B module, it cannot be explained
           how the explosion leaves A/B intact but breaks down the stronger C/D wall. This is a particularly
           robust conclusion, and is of course independent of the calculations.


                                        I I.  CONCLUSIONS
            The analysis of the B/C firewall is consistent with the conclusion of the public inquiry, that an
           initial explosion in C module was followed by  breakup of the firewall and  projection  of  panel
           fragments into B module.

           AcknowledgementsThe author thanks Elf Aquitaine and Paul1 and Williamsons for permission to publish this paper, and
           records his gratitude to David Allwright, Derek Batchelor. Roger Fenner, Lesley Gray, Colin MacAulay, Alan Mitchison
           and Rod Sylvester-Evans  for helpful discussions.


                                          REFERENCES
           I.  The Honourable Lord Cullen, The Public Inquiry into the Piper Alpha Disaster, HMSO, 1990, Command 1310.
           2.  Bakke, J. R., Gas Explosion Simulation in Piper  Alpha Module C  Using FLACS. Christian Michelsen Institute, 1989,
             Report CM1 no. 25230-1.
           3.  Jones, N., Structural Dynamics, Cambridge University Press, 1989.
           4.  Jones, N.,  International Journal of Mechanical Sciences, 1973, 15, 547-561.
           5.  Gradshteyn, I. S. and Ryzhik, I. M., Table of  Integrals, Series, and Products. Academic Press, 1979.
           6. Mansfield, E. H., Proceedings ofthe Ro-Val Society A, 1957,241,311-338.
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