Effect of Pressure on the Crystallization of Crude Oil Waxes. I. Selection of Test Conditions by Microcalorimetry†

2010 ◽  
Vol 24 (4) ◽  
pp. 2208-2212 ◽  
Author(s):  
Lenise C. Vieira ◽  
Maria B. Buchuid ◽  
Elizabete F. Lucas
2019 ◽  
Vol 66 (3) ◽  
pp. 363-388
Author(s):  
Serkan Aras ◽  
Manel Hamdi

When the literature regarding applications of neural networks is investigated, it appears that a substantial issue is what size the training data should be when modelling a time series through neural networks. The aim of this paper is to determine the size of training data to be used to construct a forecasting model via a multiple-breakpoint test and compare its performance with two general methods, namely, using all available data and using just two years of data. Furthermore, the importance of the selection of the final neural network model is investigated in detail. The results obtained from daily crude oil prices indicate that the data from the last structural change lead to simpler architectures of neural networks and have an advantage in reaching more accurate forecasts in terms of MAE value. In addition, the statistical tests show that there is a statistically significant interaction between data size and stopping rule.


Author(s):  
E. Grant Jones ◽  
Walter J. Balster ◽  
James M. Pickard

Surface fouling in aircraft fuel lines that results from autoxidation of aviation fuel remains a serious and very complicated problem. This area has been studied using two Jet-A fuels, POSF-2827 and POSF-2980. The results of a series of dynamic experiments conducted in a single-pass, tubular heat exchanger operated at very slow flow rates under near-isothermal conditions are reported herein. Such studies, by minimizing complications resulting from fluid dynamics and heat flow, constitute a simpler global approach to the chemistry of fouling. The basis for the selection of experimental test conditions is discussed, and data from measurements of dissolved oxygen and surface deposition as a function of fuel stress duration are presented. The effects of parameters such as reaction temperature, tube diameter, experimental test time, and fuel dopants are considered.


1975 ◽  
Vol 10 (1) ◽  
pp. 132-141 ◽  
Author(s):  
P.J. Leinonen ◽  
D. Mackay

Abstract Mathematical models are presented which quantify the processes of evaporation and dissolution of components of crude oil in three situations: a spill on water, a spill on ice, and a spill under ice cover in which the oil lies between the water and ice phases. Constant spill area is assumed. The evaporation flux is calculated using a mass transfer coefficient based on windspeed and spill dimensions. The dissolution flux can be calculated from two models, a mass transfer coefficient approach and an eddy diffusivity approach involving the integration of a set of partial differential equations in depth and time. The selection of model parameters is discussed. For the three physical situations, using a synthetic crude oil, results are presented giving the relative rates of evaporation and dissolution and the aqueous phase concentration of selected hydrocarbons. The implications of the results for clean-up technology and aquatic toxicity are discussed, particularly with regard to spills under ice.


1984 ◽  
Vol 24 (06) ◽  
pp. 593-596 ◽  
Author(s):  
T.M. Doscher ◽  
R.O. Oyekan ◽  
M. El Arabi

Abstract Physical model studies of the displacement of residual oil Physical model studies of the displacement of residual oil by CO2 have led to the conclusion that the driving mechanism for the process is that of a gas drive of the swollen crude. In this final phase of the study, the fluid/fluid displacement process was gravity-stabilized; mixing of the CO2 with the residual crude oil was minimized. As a result, the performance of CO2 was only marginally better than that of relatively insoluble nitrogen. Introduction The work described herein concludes the scaled physical model study of the displacement of residual crude by CO2 that had been sponsored by the U.S. DOE and the U. of Southern California. The overall goal of the work was to elucidate the mechanism of the process and to gain insight into its ultimate efficiency in recovering the crude oil remaining in a reservoir after completing an efficient water flood. The conclusions drawn from the work are limited to the displacement and recovery of residual, nonmobile crude oil. The general applicability of these conclusions to the recovery of higher saturations of mobile crude oil by CO2 is still moot. In the first phase of this work the role of CO2 was simulated by using fluids that were both liquid and completely miscible with the residual crude oil in scaled models of a linear reservoir. The results were consistent with expectations based on the basic laws for fluid flow in porous media.1. After a water flood, the water is the first phase to be displaced by the injected oil-miscible fluid. This can be accounted for readily by the water being the only mobile phase in the reservoir after water flooding has been concluded.2. The first appearance of the injected oil-miscible fluid in the effluent and the volumetric efficiency of the fluid displacement process are functions of the density and viscosity of the injected oil-miscible fluid. These observations can be related to the injected oil-miscible fluids being less dense and less viscous than the continuous, mobile water: therefore the injected fluids both segregate as a result of gravitational instability and finger through the water as a result of viscous instability.3. The residual crude oil was found to be produced along with the injected oil-miscible fluid. It was then inferred that the mechanism of the recovery of the residual crude required solution of the CO2 in the crude, swelling (saturation increase), and, ultimately, displacement of the swollen crude by the injected fluid. The scaled model studies, in which the role of CO2 was simulated by low-viscosity miscible fluids, was followed by high-pressure studies in which CO2 itself was used. However, the geometry was still restricted to that of a linear low-permeability reservoir having a circular cross section. The low permeability of the prototype, 25 md, was chosen since the earlier work already prototype, 25 md, was chosen since the earlier work already had indicated the highly pernicious effect of gravity segregation on the performance of CO2 in displacing and recovering residual crude oil. The circularity and linearity of the reservoir were dictated by the cost of a more realistic three-dimensional model. However, it was easy to show that the linearity and circularity of the prototype led to, if anything, a more optimistic performance being deduced for the recovery process. The results of the high-pressure study duplicated those in which the role of CO2 had been simulated. In addition, however, specific effects of pressure, temperature, and slug size were revealed.1. The efficiency of the displacement process in terms of oil produced per 1,000 scf of CO2 injected (bbl/10 scf) increases rapidly with pressure, but the effect of pressure becomes smaller and smaller as the pressure pressure becomes smaller and smaller as the pressure approaches 1,000 to 1,200 psi [6895 to 8274 kPa] (at temperatures in the range of 100 to 150 degrees F 138 to 66 degrees C]). The reduced effect of pressure on efficiency occurs when the density also becomes less sensitive to further increases in pressure-i.e., when the behavior of the density suggests the CO2 is liquid rather than gaseous.2. Increasing temperature reduces the efficiency of the process and the experiments showed that the negative process and the experiments showed that the negative effect of temperature could be offset by an increase in pressure. The efficiency of the CO2 was the same as long pressure. The efficiency of the CO2 was the same as long as the pressure and temperature of the experiment resulted in an identical density of the CO2.3. The efficiency increases with residual oil saturation (ROS). SPEJ P. 593


1984 ◽  
Vol 2 (5) ◽  
pp. 328-347 ◽  
Author(s):  
Clayton Huggett

A number of procedures have been described in the literature for investigation of the inhalation toxicity of combustion products. There is need for agreement on test methods and test conditions to facilitate communication, allow the ex change of data, and provide a basis for control of hazards due to combustion products in fires. Combustion systems and animal exposure systems which have been employed are classified according to their basic attributes. Simple con siderations of limiting stoichiometry in the combustion module can guide the selection of conditions which simulate real fire environments. The dynamics of the exposure system will determine the procedural dose received by the test animal and can be related to real fire exposure. Many past investigations have failed to take adequate account of these fundamental principles.


Author(s):  
Anita Bausman ◽  
Jerry Waterland ◽  
Dan Reid

Abstract The ASME B16.20 Metallic Gaskets for Pipe Flanges standard was extensively revised in 2017 [1]. One of the significant changes is the introduction of maximum permissible leakage rate. This marks a landmark introduction of an actual leakage performance criterion into ASME B16.20, a most welcome advance. A common maximum permissible leakage rate of 0.0137 mg/s-m (7.67E−10 lb/s-in) is specified for all sizes and pressure classes of finished spiral wound gaskets, that is, including the windings and any or no gauge rings for that particular gasket. Test conditions are defined — ambient temperature and calibration gas with a known methane concentration and flow rate of 1 L/min. The test pressure is defined by the pressure class: 20 bar (290 psi) for Class 150 and 40 bar (580 psi) for Class 300 and above. The qualification parameters listed in B16.20-2017 include prescribed gasket seating stress targets which also vary by pressure class. These gasket seating stress requirements are defined as 35 MPa (5,000 psi) for Class 150, 56 MPa (8,000 psi) for Class 300 and Class 400, and 70 MPa (10,000 psi) for Class 600 and above. Three questions will be explored in this paper. First, to what tightness does the new B16.20 spiral wound gasket leakage rate criterion correspond? Second, do current generation spiral wound gaskets meet this criterion? Several commercially available spiral wound gaskets will be analyzed and compared to the new B16.20 requirements. Leak rates and tightness at the new B16.20 performance qualification test conditions can be determined using publicly available, published Room Temperature Tightness (ROTT) test constants for these gaskets. Finally, an exploration of Assembly Tightness compared to Operating Tightness for a selection of spiral wound gaskets will be presented and compared to the new B16.20 Performance Testing requirements. This exploration of the new maximum leakage performance criterion in ASME B16.20-2017 will help to familiarize the end user with a valuable new aspect of this gasket standard as well as how the current generation of spiral wound gaskets meets that criterion using publicly available ROTT performance data.


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