A Discussion of the Future Oil Spill Problem in the Arctic

Glaeser, J.L.

doi:10.7901/2169-3358-1971-1-479

Cited by 7 publications

(2 citation statements)

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“…Fv-'ry-v. dh y-v.R/(th) (2) For gravity-viscous spreading at equilibrium, the two forces are equal. That is V. A5/2 'It'/2 Q2 t3 (4) kpg…”

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“…This notion is further reinforced by the observation that the spreading of hot oil on ice must of necessity involve flow of oil over a water film formed from the ice at the interface with the hot oil. Such a complex phenomenon -in particular, the presence of a temperature gradient in the oil, and the presence of a film of water between oil and ice The slick area is, therefore, expressed as a function of the elapsed time, t, as follows A __ (k p g ' It,:12 Q2 t3 ) 2 Because R = (Ahr)v" h = VIA and V = Q t, Equa- (1) and the viscous force per unit volume is…”

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The Continuous Spilling of Hot Oil on Ice

Siu

Phillips

Chen

1977

Journal of Canadian Petroleum Technology

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The continuous spilling of hot Norman Wells crude oil onto an ice surface was investigated with oil temperature, ice temperature and spilling rate as parameters. An equation for spreading of the oil was developed in whick the oil slick area, A, was proportional to t(1,2), where t is the elapsed time. Experimental data showed that A was prow portional to t0.8. Increases in both oil and ice temperatures were found to cause an increase in A, and temperature effects could be taken into account by relating kinematic viscosity to a function of the geometric mean of the ice and oil temperatures. Introduction ALTHOUGH the spreading of hot oil on ice is of interest from the point of view of oil spills in Arctic regions, no controlled quantitative study taking several variables into account has been published. In previous work, Chen et al.(1) studied the instantaneous release of oil under controlled isothermal conditions, and Glaeser(2) and McMinn(3) carried out non-isothermal field tests under a single experimental condition. The present work concerns the continuous spilling of hot crude oil on ice at ice temperatures down to −40 °C and oil temperatures up to 60 °C. Continuous spilling would occur in the event of a pipeline leak. The oil and ice temperatures chosen cover likely pipeline conditions during the Arctic winter. In common with the previous work(1), crude oil from commercial production at Norman Wells, Northwest Territories, Canada, was used. Mackay, Charles and Phillips'" have discussed other aspects of the physical behaviour of crude oil in Arctic environments, with particular reference to Norman Wells crude oil and the Mackenzie Valley of the Northwest Territories. Theoretical Background It has been recognized(1–3, 5–7) that the spreading of a liquid over a solid surface passes through three distinct regions: gravity-inertia, gravity-viscous and surface tension-viscous. However, in continuous spreading, the gravity-viscous region is of primary importance because surface-tension spreading is not likely to occur due to the continuous flow, and the gravity-inertia spreading, which occurs only in the area around the point of deposition, will not be observed. Using the same argument as that used by Chen et al.(1), the gravitational outward pressure force per unit volume is (Equation Available In Full Paper) In application of this model to the non-isothermal case of spreading of hot oil on ice, it should be noted that µ (or υ) must represent an effective viscosity, as there is a temperature gradient across the spreading oil film; any correlation of data in terms of equation (5) will therefore be in terms of such an effective viscosity. This notion is further reinforced by the observation that the spreading of hot oil on ice must of necessity involve flow of oil over a water film formed from the ice at the interface with the hot oil.

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“…Fv-'ry-v. dh y-v.R/(th) (2) For gravity-viscous spreading at equilibrium, the two forces are equal. That is V. A5/2 'It'/2 Q2 t3 (4) kpg…”

mentioning

confidence: 99%

mentioning

confidence: 99%