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25th International Meeting on Organic Geochemistry IMOG 2011

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O-42<br />

Charge history and petroleum geochemistry of dual phase<br />

accumulati<strong>on</strong>s <strong>on</strong> the Norwegian C<strong>on</strong>tinental Shelf using<br />

comparative analysis of the liquid and vapour phase<br />

Linda Schulz 1 , Michael Erdman 2 , Olaf Thießen 3<br />

1 Statoil ASA, Explorati<strong>on</strong>, Drammensveien 264, 0246 OSLO, Norway, 2 Statoil ASA, Explorati<strong>on</strong>,<br />

Sandsliveien 90, 5020 BERGEN, Norway, 3 Statoil ASA, Explorati<strong>on</strong>, Grenseveien 21, 4035 STAVANGER,<br />

Norway (corresp<strong>on</strong>ding author:lksc@statoil.com)<br />

Understanding charge history of dual phase<br />

accumulati<strong>on</strong>s may be challenging due to multiple source<br />

c<strong>on</strong>tributi<strong>on</strong>s and phase separati<strong>on</strong>s. Identical gas data<br />

of the oil associated gas and the n<strong>on</strong>-associated gas<br />

could indicate a single source rock whereas additi<strong>on</strong>al<br />

data from the gasoline and biomarkers fracti<strong>on</strong> results in<br />

a different picture pointing towards multiple sources. The<br />

main objective of this study has been to investigate<br />

comm<strong>on</strong>ly applied geochemical parameters from all<br />

hydrocarb<strong>on</strong> fracti<strong>on</strong>s in dual phase accumulati<strong>on</strong>s.<br />

Additi<strong>on</strong>al PVT data and pyrolysis data from the main<br />

sources have been c<strong>on</strong>sidered to improve the<br />

understanding of the charge history. Case studies from<br />

the Norwegian C<strong>on</strong>tinental Shelf are used.<br />

The first case shows a reservoir accumulati<strong>on</strong> where the<br />

petroleum most likely has been generated by a marine<br />

source at peak to late-oil maturity. The gas isotope<br />

profiles of oil associated gas and the gas-c<strong>on</strong>densate are<br />

identical (Fig.1, case 1). The maturity of the gasoline<br />

fracti<strong>on</strong> in the gas-c<strong>on</strong>densate phase is slightly higher<br />

than in the oil phase. The dual phase state appears best<br />

explained by phase separati<strong>on</strong> due to reduced pressure<br />

and temperature c<strong>on</strong>diti<strong>on</strong>s which is supported by<br />

saturati<strong>on</strong> pressures close to reservoir pressures. The<br />

gas mass fracti<strong>on</strong> of the discovery is about 0.44, while<br />

pyrolysis experiments of marine source rock samples<br />

indicate gas mass fracti<strong>on</strong>s of around 0.15 to 0.22 with<br />

<strong>on</strong>ly minor increase at high maturity. Volumetric<br />

recombinati<strong>on</strong> of both phases in PVTsim shows that the<br />

charge fluid has a high GOR and possibly was an<br />

undersaturated gas/ c<strong>on</strong>densate. The high gas mass<br />

fracti<strong>on</strong> could be explained by liquid loss <strong>on</strong> the migrati<strong>on</strong><br />

pathway. Additi<strong>on</strong>al gas c<strong>on</strong>tributed from sec<strong>on</strong>dary<br />

cracking is excluded from biomarker versus diam<strong>on</strong>doid<br />

c<strong>on</strong>centrati<strong>on</strong>s. Another explanati<strong>on</strong> for the high gas<br />

fracti<strong>on</strong> could be that oil has been migrated up-flanks<br />

whereas the gas has been efficiently trapped.<br />

The sec<strong>on</strong>d case shows accumulati<strong>on</strong>s in two reservoirs<br />

which are separated by a pressure barrier at present day.<br />

The oil associated gas in the lower reservoir shows a<br />

very low gas mass fracti<strong>on</strong>s of about 0.07. The upper<br />

reservoir c<strong>on</strong>tains a gas c<strong>on</strong>densate with a gas mass<br />

fracti<strong>on</strong> of about 0.92. However, even volumetric<br />

recombinati<strong>on</strong> of both phases will not increase the oil/gas<br />

mass fracti<strong>on</strong> above about 0.08 for the whole<br />

accumulati<strong>on</strong>. Thus, significant gas loss best explains the<br />

observed ratios. At the same time the oil associated gas<br />

and the gas-c<strong>on</strong>densate do show similar isotope profiles<br />

(Fig. 1, case 2). Moreover, gasoline and C15+ range<br />

hydrocarb<strong>on</strong>s indicate that the oil has been generated by<br />

a source rock dominated by terrigenous organic matter,<br />

while the gas-c<strong>on</strong>densate has a marine origin. In spite of<br />

partial loss of gas fracti<strong>on</strong>, complex mixing and alterati<strong>on</strong><br />

processes the gas isotope profiles appear similar in both<br />

reservoirs. This observati<strong>on</strong> appears to be ubiquitous,<br />

pointing to homogenizati<strong>on</strong> of compositi<strong>on</strong>al differences<br />

for gas being very fast in geologic time, also across<br />

phase boundaries.<br />

The c<strong>on</strong>clusi<strong>on</strong> is that lack of differences in isotopic<br />

compositi<strong>on</strong> between the oil associated and n<strong>on</strong>associated<br />

gases not necessarily indicates that gas cap<br />

and oil leg have the same origin. C<strong>on</strong>siderati<strong>on</strong> of all<br />

petroleum fracti<strong>on</strong>s in both phases, ideally combined with<br />

mass balance and PVT data, allows for a proper<br />

interpretati<strong>on</strong> of the charge history of dual phase<br />

accumulati<strong>on</strong>s. This can c<strong>on</strong>tribute to a realistic<br />

evaluati<strong>on</strong> of the prospectivity of the areas adjacent to<br />

discoveries.<br />

� 13 C (‰) PDB<br />

-30<br />

-40<br />

-50<br />

Single-phase system<br />

OIL (for comparis<strong>on</strong> <strong>on</strong>ly)<br />

Two-phase systems<br />

1 - GAS_COND (GOR: 1900)<br />

1 - OIL (GOR: 246)<br />

2 - GAS_COND (GOR: 12585)<br />

2 - OIL (GOR: 92)<br />

Methane Ethane Propane i-Butane n-Butane<br />

Fig.1. Compound specific carb<strong>on</strong> isotope profiles of oil-associated and free<br />

gases/gas-c<strong>on</strong>densates of two-phase systems. The grey shaded area represents<br />

the carb<strong>on</strong> isotopic range of the gas generati<strong>on</strong> index (GGI) according to Clayt<strong>on</strong><br />

(1991).<br />

102

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