| + | * First, [[seal capacity]] is based on the presence of a single, continuous, high-P<sub>d</sub> layer, not upon an arithmetic average of all P<sub>d</sub> values. The trapping capacity is determined by the highest displacement pressure within a seal, theoretically even if that interval is a layer only one grain thick. A 500-m-thick siltstone may appear incapable of trapping more than [[length::1 m]] of hydrocarbon. The presence of a 1-cm-thick claystone layer, however, may create a seal for thousands of meters of hydrocarbon. Predicting these local seals is difficult and adds a measure of risk to any evaluation of intact top seals using capillary theory. |
| + | * Second, experiments demonstrate that hydrocarbon [[migration]] through a seal does not occur along a broad, uniform front but along narrow fingers reflecting local, tortuous pathways of low displacement pressure.<ref name=ch10r17>Dembecki, H., Jr., Anderson, M., J., 1989, [http://archives.datapages.com/data/bulletns/1988-89/data/pg/0073/0008/1000/1018.htm Secondary migration of oil: experiments supporting efficient movement of separate, buoyant oil phase along limited conduits]: AAPG Bulletin, vol. 73, no. 8, p. 1018–1021.</ref><ref name=ch10r12>CatalanXiaown, L., F., Chatzis, I., Dullien, F., A., L., 1992, [http://archives.datapages.com/data/bulletns/1992-93/data/pg/0076/0005/0000/0638.htm An experimental study of secondary oil migration]: AAPG Bulletin, vol. 76, no. 5, p. 638–650.</ref> |