Drag Reduction with a Polymeric Additive in Crude Oil Pipelines

1971 ◽  
Vol 11 (03) ◽  
pp. 229-235 ◽  
Author(s):  
Jaime A. Lescarboura ◽  
John D. Culter ◽  
Harry A. Wahl

Abstract A polymeric drag reducer has been tested in an 8-in. diameter crude oil pipeline. The test segment was 28 miles long. At the normal flow velocity in the 8-in. line of about 6 ft/sec, drag reductions of 16, 21 and 25 percent were obtained at polymer concentrations of 300, 600 and 1,000 volume ppm. A series of tests was run to determine the effect of flow velocity on drag reduction. Drag reduction decreased as the flow velocity decreased. An additional test in a 12-in. pipeline, 32 miles long, supported the results obtained in the 8-in. pipeline. In none of the tests did the polymer appear to degrade or lose effectiveness because of turbulent shear in the lines. Tests were run for the polymer and various polyisobutylenes in a 1-in.-ID laboratory pipe polyisobutylenes in a 1-in.-ID laboratory pipe viscometer. These tests covered a range of concentrations and flow velocities. The results obtained in the 1-in. line showed the same general characteristics as those obtained in the large pipelines. An equation is presented that correlates pipelines. An equation is presented that correlates the 8-in. and 12-in data as a function of flow velocity and polymer concentration. Introduction Drag reduction, as defined by Savins, is the increase in pumpability of a fluid caused by the addition of small amounts of additive to the fluid. The mechanism of drag reduction is not well understood. An extensive discussion on the subject is presented by Patterson et al. Drag reduction occurs only in turbulent flow. Despite this limitation, drag reduction has a wide potential application within the oil industry. At present, however, the only extensive use of drag reducers has been in hydraulic fracturing operations. Water-soluble polymers have been effective in reducing horsepower requirements and/or increasing injection rates during treatments. The drag reduction phenomenon has not been used in the pipelining of large quantities of crude oil and of pipelining of large quantities of crude oil and of petroleum products. Little use has been made of petroleum products. Little use has been made of it in hydraulic fracturing with oil base fluids. One of the main reasons for this situation is that until recently very few materials were available to reduce drag in aliphatic hydrocarbons. Several polymers may be used as drag reducers in aromatic polymers may be used as drag reducers in aromatic or chlorinated solvents. However, drag reduction in aliphatic hydrocarbons has been limited to polyisobutylene and crepe rubber. Another reason polyisobutylene and crepe rubber. Another reason is that there have been discouraging predictions about the performance of drag reducers in large pipes. Ram et al. studied polyisobutylenes in pipes. Ram et al. studied polyisobutylenes in small brass tubes (3.15 to 13.7 mm) and concluded that the critical velocities for onset of drag reduction ranged from 8.5 to 14.2 ft/sec. These velocities were considered usually too high for actual pipeline applications. These researchers also concluded that degradation of long-flexible polymeric chains in turbulent flow was an extremely polymeric chains in turbulent flow was an extremely serious problem. Seyer and Metzner concluded that little or no drag reduction can be expected in large tubes using presently available polymer materials. In this paper we present data on a polymer that gives substantial drag reduction in crude and diesel oils in small and large pipes. Some comparative data obtained with high molecular weight polyisobutylenes are also presented. polyisobutylenes are also presented. EXPERIMENTAL FLOW SYSTEMS Two pipelines, both located in Oklahoma, were used in the testing. One of the pipelines is 8.249-in. ID, 28.3 miles long, running from Kingfisher pump station to Orlando pump station. The line was tapped for pressure measurements at both pump stations and at two intermediate points, thus dividing the line into segments at 7.4, 11.8 and 9.1 miles. The flow rate was measured during the first three tests by gauging tanks at Orlando and by turbine flow meters. For the last twelve tests the system was improved by adding two positive displacement flow meters at Orlando. SPEJ P. 229

1995 ◽  
Vol 302 ◽  
pp. 333-376 ◽  
Author(s):  
D. Goldstein ◽  
R. Handler ◽  
L. Sirovich

An immersed boundary technique is used to model a riblet covered surface on one wall of a channel bounding fully developed turbulent flow. The conjecture that the beneficial drag reduction effect of riblets is a result of the damping of cross-flow velocity fluctuations is then examined. This possibility has been discussed by others but is unverified. The damping effect is explicitly modelled by applying a cross-flow damping force field in elongated streamwise zones with a height and spacing corresponding to the riblet crests. The same trends are observed in the turbulence profiles above both riblet and damped surfaces, thus supporting cross-flow damping as a beneficial mechanism. It is found in the examples presented that the effect of the riblets on the mean flow field quantities (mean velocity profile, velocity fluctuations, Reynolds shear stress, and low–speed sreak spacing) is small. The riblests cause a relatively small drag reduction of about 4%, a figure that is in rough agreement with experiments and other computations. The simulations also suggest a mechanism for the observed displacement of the turbulence quantities away from the wall.The immersed boundary technique used to model the riblets consists of creating an externally imposed spatially localized body force which opposes the flow velocity and creates a riblet-like surface. For unstead viscous flow the calculation of the force is done with a feedback scheme in which the velocity is used to iteratively determine the desired value. In particular, the surface body force is determined by the relation f(xs, t) = α ∫ t0U(xs,t′)dt′ + βU(xs, t) for surface points xs, velocity U time t and negative constants α and β. All simulations are done with a spectral code in a single computational domain without any mapping of the mesh. The combination of the immersed boundary and spectral techniques can potentially be used to solve other problems having complex geometry and flow physics.


2015 ◽  
Vol 9 (1) ◽  
pp. 1 ◽  
Author(s):  
Yanuar Yanuar ◽  
Kurniawan T. Waskito ◽  
Gunawan Gunawan ◽  
Budiarso Budiarso

2020 ◽  
Vol 13 (2) ◽  
pp. 105-109
Author(s):  
E. S. Dremicheva

This paper presents a method of sorption using peat for elimination of emergency spills of crude oil and petroleum products and the possibility of energy use of oil-saturated peat. The results of assessment of the sorbent capacity of peat are presented, with waste motor oil and diesel fuel chosen as petroleum products. Natural peat has been found to possess sorption properties in relation to petroleum products. The sorbent capacity of peat can be observed from the first minutes of contact with motor oil and diesel fuel, and significantly depends on their viscosity. For the evaluation of thermal properties of peat saturated with petroleum products, experimental studies have been conducted on determination of moisture and ash content of as-fired fuel. It is shown that adsorbed oil increases the moisture and ash content of peat in comparison with the initial sample. Therefore, when intended for energy use, peat saturated with petroleum products is to be subjected to additional drying. Simulation of net calorific value has been performed based on the calorific values of peat and petroleum products with different ratios of petroleum product content in peat and for a saturated peat sample. The obtained results are compared with those of experiments conducted in a calorimetric bomb and recalculated for net calorific value. A satisfactory discrepancy is obtained, which amounts to about 12%. Options have been considered providing for combustion of saturated peat as fuel (burnt per se and combined with a solid fuel) and processing it to produce liquid, gaseous and solid fuels. Peat can be used to solve environmental problems of elimination of emergency spills of crude oil and petroleum products and as an additional resource in solving the problem of finding affordable energy.


Author(s):  
Aviral Kumar Tiwari ◽  
Muhammad Tahir Suleman ◽  
Subhan Ullah ◽  
Muhammad Shahbaz
Keyword(s):  

1994 ◽  
Vol 31 (1) ◽  
pp. 93-98 ◽  
Author(s):  
Shen-Min Liang ◽  
Jan-Kuang Fu

2008 ◽  
Vol 18 (1) ◽  
pp. 12421-1-12421-5
Author(s):  
V. Mik ◽  
J. Myska ◽  
Z. Chara ◽  
P. Stern

AbstractEffectiveness of drag reduction by small addition of a surfactant in the turbulent flow of water depends on the structure and concentration of the additive, temperature of the solution and turbulence intensity, possible flow disturbance by a mechanical obstacle and the content of ions in water, but also on the age of the surfactant solution. We show how important aging effects are in connection with total surfactant concentration, in particular how rheological parameters of the drag reducing solution change with time.


2014 ◽  
Vol 747 ◽  
pp. 186-217 ◽  
Author(s):  
S. Türk ◽  
G. Daschiel ◽  
A. Stroh ◽  
Y. Hasegawa ◽  
B. Frohnapfel

AbstractWe investigate the effects of superhydrophobic surfaces (SHS) carrying streamwise grooves on the flow dynamics and the resultant drag reduction in a fully developed turbulent channel flow. The SHS is modelled as a flat boundary with alternating no-slip and free-slip conditions, and a series of direct numerical simulations is performed with systematically changing the spanwise periodicity of the streamwise grooves. In all computations, a constant pressure gradient condition is employed, so that the drag reduction effect is manifested by an increase of the bulk mean velocity. To capture the flow properties that are induced by the non-homogeneous boundary conditions the instantaneous turbulent flow is decomposed into the spatial-mean, coherent and random components. It is observed that the alternating no-slip and free-slip boundary conditions lead to the generation of Prandtl’s second kind of secondary flow characterized by coherent streamwise vortices. A mathematical relationship between the bulk mean velocity and different dynamical contributions, i.e. the effective slip length and additional turbulent losses over slip surfaces, reveals that the increase of the bulk mean velocity is mainly governed by the effective slip length. For a small spanwise periodicity of the streamwise grooves, the effective slip length in a turbulent flow agrees well with the analytical solution for laminar flows. Once the spanwise width of the free-slip area becomes larger than approximately 20 wall units, however, the effective slip length is significantly reduced from the laminar value due to the mixing caused by the underlying turbulence and secondary flow. Based on these results, we develop a simple model that allows estimating the gain due to a SHS in turbulent flows at practically high Reynolds numbers.


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