A Study of the Effect of Gas Condensate on the Viscosity and Storage Stability of Omani Heavy Crude Oil

Heavy crude oil (density of 0.9571 g/cm3 at 288 K and kinematic viscosity of 7160 mm2/s at 303 K) and natural gas condensate (density of 0.7848 g/cm3 at 288 K and kinematic viscosity of 0.764 mm2/s at 303 K) were sampled from Omani oil fields. The oil was mixed with condensate (5−50 vol %), and the...

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Veröffentlicht in:Energy & fuels 2006-11, Vol.20 (6), p.2504-2508
Hauptverfasser: Shigemoto, Naoya, Al-Maamari, Rashid S, Jibril, Baba Y, Hirayama, Akihiko
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container_end_page 2508
container_issue 6
container_start_page 2504
container_title Energy & fuels
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creator Shigemoto, Naoya
Al-Maamari, Rashid S
Jibril, Baba Y
Hirayama, Akihiko
description Heavy crude oil (density of 0.9571 g/cm3 at 288 K and kinematic viscosity of 7160 mm2/s at 303 K) and natural gas condensate (density of 0.7848 g/cm3 at 288 K and kinematic viscosity of 0.764 mm2/s at 303 K) were sampled from Omani oil fields. The oil was mixed with condensate (5−50 vol %), and the mixture viscosities were measured at the temperature range of 293−348 K. A drastic decrease in kinematic viscosity was achieved. An addition of about 12 vol % of condensate gave a viscosity of 265 mm2/s at 303 K. This made it easier to transport the heavy oil mixtures. The experimental data for the kinematic viscosity [ν (mm2/s)] as a function of the gas-condensate fraction (φ) and temperature [T (K)] could be described by an equation:  ln(ln(ν)) = (k 1 + k 2·T) + (k 3 + k 4·T)·φ, with a high accuracy. Blends of the heavy oil and the gas condensate were stored to evaluate their stability. Results showed less than 0.05 wt % sludge formation after 2 months.
doi_str_mv 10.1021/ef060074h
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The oil was mixed with condensate (5−50 vol %), and the mixture viscosities were measured at the temperature range of 293−348 K. A drastic decrease in kinematic viscosity was achieved. An addition of about 12 vol % of condensate gave a viscosity of 265 mm2/s at 303 K. This made it easier to transport the heavy oil mixtures. The experimental data for the kinematic viscosity [ν (mm2/s)] as a function of the gas-condensate fraction (φ) and temperature [T (K)] could be described by an equation:  ln(ln(ν)) = (k 1 + k 2·T) + (k 3 + k 4·T)·φ, with a high accuracy. Blends of the heavy oil and the gas condensate were stored to evaluate their stability. 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The oil was mixed with condensate (5−50 vol %), and the mixture viscosities were measured at the temperature range of 293−348 K. A drastic decrease in kinematic viscosity was achieved. An addition of about 12 vol % of condensate gave a viscosity of 265 mm2/s at 303 K. This made it easier to transport the heavy oil mixtures. The experimental data for the kinematic viscosity [ν (mm2/s)] as a function of the gas-condensate fraction (φ) and temperature [T (K)] could be described by an equation:  ln(ln(ν)) = (k 1 + k 2·T) + (k 3 + k 4·T)·φ, with a high accuracy. Blends of the heavy oil and the gas condensate were stored to evaluate their stability. Results showed less than 0.05 wt % sludge formation after 2 months.</description><subject>Applied sciences</subject><subject>Crude oil, natural gas and petroleum products</subject><subject>Energy</subject><subject>Exact sciences and technology</subject><subject>Fuels</subject><subject>Processing of crude oil and oils from shales and tar sands. 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source American Chemical Society Journals
subjects Applied sciences
Crude oil, natural gas and petroleum products
Energy
Exact sciences and technology
Fuels
Processing of crude oil and oils from shales and tar sands. Processes. Equipment. Refinery and treatment units
title A Study of the Effect of Gas Condensate on the Viscosity and Storage Stability of Omani Heavy Crude Oil
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