Rheological properties of f ull ta ilings slurry in pipeline transportation based on the hydromechanics theory

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1 Journal of University of Science and Technology Beijing Vol. 31 No. 11 Nov ) 1) 2) 1) 1), ), ,, L. :,.,,,. ; ; ; TD ; O 373 Rheological properties of f ull ta ilings slurry in pipeline transportation based on the hydromechanics theory D EN G Dai2qiang 1), GA O Yong2tao 1), YA N G Yao2liang 2), W U S hun2chuan 1) 1) School of Civil and Environmental Engineering, University of Science and Technology Beijing, Beijing , China 2) Changsha Institute of Mining Research, Changsha , China ABSTRACT To study the rheological properties of filling slurry, using the principle of hydrodynamics, a gravity flow test through a L2shaped pipe was carried out and the mechanical properties of slurry flow in the pipe was analyzed. The results indicated that the flow resistance and filling rate were depended on slurry concentration, flow rate and pipe diameter, among which slurry concentration was the predominant influencing factor. Under the condition of reasonable filling rates at which the gravity flow of slurry can be achieved, after determining the flow rate and pipe diameter based on filling ability, the slurry concentration can be adjusted in the fill2 ing station to obtain excellent results in transportation, sedimentation, anti2eduction, dehydration and drainage, concretion and me2 chanical properties. KEY WORDS rheological properties ; pipeline transportation ; Bingham fluids ; shear stress,., [1-3 ] ; [4-6 ], ;, [7-13 ],. [12-15 ],.,.,,,.,.,,,, [7-13 ].,,, : : (1974 ),,; (1962 ),,,,E2mail sina. com

2 11 : 1381,,.,,. 1. [7-13 ],,, = 0 + d v d r (1),, Pa ; 0, Pa ;, Pa s; d v/ d r,s - 1., 1. : d p r 0 = 2 0 d l - 1 = 2 0 i, i, Pa m - 1. (6), :R > r 0, ; R r 0,,. 0,,,,.,,,., : 8 V D = (7) 0 /, : = V (8) D 1 Fig. 1 Force analysis of Bingham fluids in a pipeline d p d l r, : : (1) (3) : ( p + d p)r 2 = pr 2 + 2r d l (2) = d p r 2d l (3) d v d r = 1 d p r - 2d l 0 (4) r,r = R, V = 0, : V = 1 1 d p 4 d l ( R 2 - r 2 ) - 0 ( R - r) (5),d p, MPa ; R, m, V,m s - 1. r :r = 0,,, ; r = R,,,. (4) d v/ d r = 0, r, D, m., : 0 = h 0 D 4 ( h 0 + L ) (3-4 0) D = 24 V (9) (10),,t m - 3 ; V,m s - 1 ; h 0, m ; L, m ; 0, Pa ;, Pa s., : i = D + 32V D 2 (11), H, L, : H = i ( H + L ) + n i = 1 i V g +V 2 g (12), H i ( H + L ) n i = 1 i [ V 2 ( 2 g) - 1 ] V 2 (2 g) - 1., 15 %,:

3 : H = 1115 i ( H + L ) (13) H + L H = 1115 i (14) ( H + L ) / H, ,.,, L. 212.,.,1.. V, 2. V = Q/, Q, m 3 h D2 (15) 1 Table 1 Testing data of full tailings slurry s flowing properties /,,,,, / % mm / (t m - 3 ) h 0 / m V / (m s - 1 ) 0 / Pa / ( Pa s) Table 2 Flow velocity of slurry at different pipe diameters and fluxes / (m 3 h - 1 ) / mm m s , :,, ;,,.,,.. 1,,. : 76 % ; 74 % 40 m 3 h mm 1104 ; 72 %70 %,, 3. 3 :,, ;,,.,,,. :,,,,, ;,.,2 3,,,,.

4 11 : : (a) 70 % ; (b) 72 % ; (c) 74 % ; (d) 76 % Fig. 2 Change of slurry s transportation resistance with pipeline diameter and flux. Its mass fraction is (a) 70 %, (b) 72 %, (c) 74 %, and (d) 76 %, respectively 3. : (a) 70 % ; (b) 72 % Fig. 3 Change of slurry s flow rate with pipeline diameter and flux. Its mass fraction is (a) 70 % and (b) 72 %, respectively 3 (1),.,,,. (2),,. 0,.,,,. (3) i 0 V D,,,. 70 %72 %,,,.. [ 1 ] Xiao S X, Gao Z M, Huang X B. Experimental study and numer2 ical simulation of new a modified Ross static mixer. Chin J Pro2

5 cess Eng, 2006, 6 (1) :6 (,,. Ross., 2006, 6 (1) :6) [ 2 ] Jiang S Q. The study of eccentric annular clearance Reynolds number and laminar flow area equation under Newtonian fluid condition. China Of fshore Oil Gas, 2007,19 (6) :398 (.., 2007,19 (6) :398) [ 3 ] He C C, Zhang C. Flow law on turbulent2power law laminar stratified flow in rotund pipes. Nat Gas Oil, 2008,26 (5) :17 (,. -.,2008,26 (5) :17) [ 4 ] Wang Z Y, Fu X Z, Wang Y, et al. Numerical simulation of sol2 id2liquid flow of Yangtze River water in a semi2annulus reentry tube. J Chongqing U niv, 2008,31 (12) :1410 (,,,.., 2008, 31 (12) :1410) [ 5 ] Ren L Z, Shi J G, Zhang Q, et al. Research on applying solid2 fluid double phase theory to water coal slurry nozzle. M ach, 2006,27 (7) :173 Coal Mine (,,,..,2006,27 (7) :173) [ 6 ] Zhao Z N, Hao R, Wang L. Analyses of physical mechanism and numerical simulation for micro2convection enhancement the solid2 liquid two phase flow. J Eng Thermophys, 2005, 26 (4) :656 (,,.., 2005, 26 (4) :656) [ 7 ] Cheng C J, Li B, Zhao H W. Application and development of rheology. Contem p Chem Ind, 2008, 37 (2) :221 (,,..,2008, 37 (2) :221) [ 8 ] Fei XJ. Transportation Hydraulics of Slurry and Grainy M ate2 rial. Beijing : Tsinghua University Press, 1994 (.. :, 1994) [ 9 ] Boylu F, Dincer H, Atesok G. Effect of coal particle size distribu2 tion, volume fraction and rank on the rheology of coal2water slur2 ries. Fuel Process Technol, 2004, 85 : 241 [ 10 ] Marn J, Ternik P. Laminar flow of shear2thickening fluid in a 90 pipe bend. Fluid Dyn Res, 2006, 38 : 295 [ 11 ] Yang X Z, Wang X H, Lei J S. Study on grouting diffusion ra2 dius of Bingham fluids. J Hydraul Eng, 2004 (6) : 1 (,,..,2004 (6) :1) [ 12 ] Xu Y H, Xu X Q. Rheologic behavior of high2density backfill and reasonable determination of the parameters for it s gravity2 flow transport. Min Metall, 2004 (3) :16 (,. ( )., 2004 (3) :16) [ 13 ] Newman P D, Pine R J, Ross Kevin. The optimization of high density backfill at the Stratoni Operations, Greece Proceedings of the 7 th International Sy m posium on Mining with Backf ill. Washington : Seattle, 2001 :273 [ 14 ] Cai M F, Li C L, Xie M W, et al. Subsidence prediction and surface deformation monitoring and analysis in Beiminghe Iron Mine, China. J U niv Sci Technol Beijing, 2008, 30 (2) :109 (,,,..,2008, 30 (2) :109) [ 15 ] Yang C X, Luo Z Q, Hu G B, et al. Application of a microseis2 mic monitoring system in deep mining. J U niv Sci Technol Bei2 jing, 2007, 14 (1) : 6

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