An Introduction to Modeling and Simulation of Particulate Flows Part 10 potx
Introduction to Modeling and Control of Internal Combustion Engine Systems P1 potx
... paper987654321springer.com Introduction to Modeling and Control of Internal Combustion Engine Systems 1.3 Overview of SI Engine Control Problems 9Fig. 1.6. Conversion efficiency of a TWC (after light-off, ... Substructure of a complete vehicle control system.1.2.2 Electronic Engine Control Hardware and SoftwareTypically, an electronic engine control unit (ECU) includes standar d micro-controller ... understanding of basic thermodynamic and fluid dynamics proc e sses in internal combustion engines (ICE). Other prerequisites are knowledge of general ME topics (cal-culus, mechanics, etc.) and...
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Introduction to Modeling and Control of Internal Combustion Engine Systems P2 ppsx
... physical link of the engine to the rest of the powertrain is the load torque, which in this text is assumed to be known.The reciprocating behavior of the engine induces a nother dichotomy in theCOM ... first introduced in [89]. One of the earliestpapers proposing MVM for engine systems is [195]. A good overview of the firstdevelopments in the area of MVM of S I engine systems can be found in [167]. ... labele d by ˙mx and masses by mxwhere x = {a, eg}. Theindex m indicates a variable pertaining to the intake manifold, β to the engine intake, γ to the engine outlet, and ε to the exhaust gas...
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An Introduction to Modeling and Simulation of Particulate Flows Part 2 pot
... areã1ijmiT 2 L(1+1),ã2ijmiT 2 L( 2 +1).In other words,1ijmiT 2 L(1+1)system 1=α1ijmiT 2 L−(β1+1)system 2 (1. 62) and α2ijmiT 2 L−(β 2 +1)system 1=α2ijmiT 2 L−(β 2 +1)system ... Szabo and Babúska [185], and Zienkiewicz and Taylor [20 7].For work specifically focusing on the continuum mechanics of particles, see Zohdi and Wriggers [21 6]. For a detailed numerical analysis of ... 2. Modeling of particulate flowswhere vcm(t) is the mean velocity of the group of particles and δvi(t) is a purely fluctuating(about the mean) part of the velocity. For the entire group of...
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An Introduction to Modeling and Simulation of Particulate Flows Part 3 pdf
... [206],Schrefler [1 73] , Lewis et al. [ 133 ], Doltsinis [52], [ 53] , Piperno [162], Lewis and Schrefler[ 132 ], Armero and Simo [7]–[9], Armero [10], Le Tallec and Mouro [ 131 ], Zohdi [208],[209], and the extensive ... and the extensive works of Farhat and coworkers (Piperno et al. [1 63] , Farhat et al.[65], Lesoinne and Farhat [ 130 ], Farhat and Lesoinne [66], Piperno and Farhat [164], and Farhat et al. [67]).Remark. ... write(S(ttol)p)Kd||L+1,0|| = TOL, (3. 28)where TOL is a tolerance and Kdis the number of desired iterations.19If the error toleranceis not met in the desired number of iterations, the contraction constant ηL+1,Kis...
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An Introduction to Modeling and Simulation of Particulate Flows Part 4 pot
... αmm1αmm2αmtαmo8 45 147 0 .44 270188.87 7355 34. 64 141 859.9916 12 849 7 .49 279918.51 778117.81 80526.8532 111 642 .28 5 642 92.53 872627 .48 7899.69 64 3 943 44. 61 625999.39 9107 34. 12 23961.73128 7670 84. 352 643 80.23 ... 530Z02 4 681012 14 16X0Y0Z02 4 681012 14 16X0Y0Z02 4 681012 14 16X0Y0Z02 4 681012 14 16X0Y0Z02 4 681012 14 16X0Y0Z02 4 681012 14 16X0YFigure6.5. Top to bottomandleft to right,the swarm thengoes throughand slightlyovershoots the target (10, 0, 0), and then undershoots it slightly and starts to concentrateitself ... concern.0Z02 4 681012 14 16X0Y0Z02 4 681012 14 16X0Y0Z02 4 681012 14 16X0Y0Z02 4 681012 14 16X0Y0Z02 4 681012 14 16X0Y0Z02 4 681012 14 16X0YFigure 6.6. Top to bottom and left to right, the swarm starts to oscillate slightlyaround the target and then begins to home in on the target and concentrate...
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An Introduction to Modeling and Simulation of Particulate Flows Part 5 potx
... ENERGY0.40. 45 0 .5 0 .55 0.60. 65 0.70. 75 0 0 .5 1 1 .5 2 2 .5 3 3 .5 4 4 .5 5ENERGY (N-m)TIMETOTAL KINETIC ENERGY0.40. 45 0 .5 0 .55 0.60. 65 0.70. 75 0 0 .5 1 1 .5 2 2 .5 3 3 .5 4 4 .5 5ENERGY (N-m)TIMETOTAL ... 710.40. 45 0 .5 0 .55 0.60. 65 0.70. 75 0 0 .5 1 1 .5 2 2 .5 3 3 .5 4 4 .5 5ENERGY (N-m)TIMETOTAL KINETIC ENERGY0.40. 45 0 .5 0 .55 0.60. 65 0.70. 75 0 0 .5 1 1 .5 2 2 .5 3 3 .5 4 4 .5 5ENERGY (N-m)TIMETOTAL KINETIC ... 732983003023043063083103123143163183200 0 .5 1 1 .5 2 2 .5 3 3 .5 4 4 .5 5TEMPERATURETIMETEMPERATURE3003 05 3103 15 3203 25 3303 35 3400 0 .5 1 1 .5 2 2 .5 3 3 .5 4 4 .5 5TEMPERATURETIMETEMPERATURE300400 50 060070080090010000...
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An Introduction to Modeling and Simulation of Particulate Flows Part 6 pps
... t = min(tlim,t )AND GO TO (0); (6) IF TOLERANCE NOT MET (Etot,K> TOL) AND K = Kd, THEN(a) CONSTRUCT NEW TIME STEP: t = Kt;(b) RESTART AT TIME = t AND GO TO (0).Algorithm 8.1 ... Such particle/fluid systems are strongly coupled due to the mechanicalforces and heat transfer induced by the fluid on the particles and vice versa. Because thecoupling of the various particle and ... Accordingly, we require the time rate of change of the sum of the kineticenergy (K) and stored energy (S) to be equal to the sum of the work rate (power, P) and the net heat supplied (H):ddt(K...
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An Introduction to Modeling and Simulation of Particulate Flows Part 7 docx
... field vectors are (left) perpendicular to the plane of incidence and (right) parallel to the plane of incidence (Zohdi [218]).9.2.4 Reflection and absorption of energyNow we consider a plane harmonic ... very dilute gases and, in the limit, in a vacuum. For generaloverviews pertaining to scattering, see Bohren and Huffman [33] and van de Hulst [195].Remark. An application of particular interest, ... (s)Present 1 176 82 07 6. 978 8.506 ì104Not present 1341 14445 10 .77 2 7. 458 ì 104 to intersect, In other words, the particles can “plow” through the (compressible) fluid and contact one another. This...
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An Introduction to Modeling and Simulation of Particulate Flows Part 8 potx
... 1275 18. 809504.222 489 .635475.0 48 460.46445 .87 3431. 286 416.6 98 402.111 387 .524372.9363 58. 349343.762329.175314. 587 5 18. 809504.222 489 .635475.0 48 460.46445 .87 3431. 286 416.6 98 402.111 387 .524372.9363 58. 349343.762329.175314. 587 5 18. 809504.222 489 .635475.0 48 460.46445 .87 3431. 286 416.6 98 402.111 387 .524372.9363 58. 349343.762329.175314. 587 5 18. 809504.222 489 .635475.0 48 460.46445 .87 3431. 286 416.6 98 402.111 387 .524372.9363 58. 349343.762329.175314. 587 Figure ... 1275 18. 809504.222 489 .635475.0 48 460.46445 .87 3431. 286 416.6 98 402.111 387 .524372.9363 58. 349343.762329.175314. 587 5 18. 809504.222 489 .635475.0 48 460.46445 .87 3431. 286 416.6 98 402.111 387 .524372.9363 58. 349343.762329.175314. 587 5 18. 809504.222 489 .635475.0 48 460.46445 .87 3431. 286 416.6 98 402.111 387 .524372.9363 58. 349343.762329.175314. 587 5 18. 809504.222 489 .635475.0 48 460.46445 .87 3431. 286 416.6 98 402.111 387 .524372.9363 58. 349343.762329.175314. 587 Figure 9.14. Top to bottom ... 1295 18. 809504.222 489 .635475.0 48 460.46445 .87 3431. 286 416.6 98 402.111 387 .524372.9363 58. 349343.762329.175314. 587 5 18. 809504.222 489 .635475.0 48 460.46445 .87 3431. 286 416.6 98 402.111 387 .524372.9363 58. 349343.762329.175314. 587 5 18. 809504.222 489 .635475.0 48 460.46445 .87 3431. 286 416.6 98 402.111 387 .524372.9363 58. 349343.762329.175314. 587 5 18. 809504.222 489 .635475.0 48 460.46445 .87 3431. 286 416.6 98 402.111 387 .524372.9363 58. 349343.762329.175314. 587 Figure9.15....
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An Introduction to Modeling and Simulation of Particulate Flows Part 9 pot
... a newclass of methods, based on simultaneous particle flow and growth, has been developed byTorquato and coworkers (see, for example, Kansaal et al. [1 19] and Donev et al. [55]–[ 59] ).Remark. ... [72], Shah [174], van der Wal and Becker [ 197 ], Chyu and Shah [46], and Libby[134], [135], Libby et al. [136], Libby and Aikawa [137], Richardson et al. [1 69] , Loreeet al. [141], and Davies et al. ... et al. [ 199 ], Beckwith et al. [20], Barge and Sommeria [14], Pollack et al. [166], Lissauer [138], Barranco et al. [15], and Barranco and Marcus [16], [17].In closing, itis important to mention...
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An Introduction to Modeling and Simulation of Particulate Flows Part 10 potx
... hereditary spherocytosis and hereditaryelliptocytosis (Eber and Lux [62] and Gallagher [73], [74]). Changes in membrane and cytosolic proteins may affect the state of hydration of the cell and thereby ... coupling.Journal of Fluid Mechanics, Vol. 429, 23–61.[61] Duran, J. 1997. Sands, Powders and Grains. An Introduction to the Physics of Gran-ular Matter. Springer-Verlag.[62] Eber, S. and Lux, S. ... Savage, S. B., and Nohguchi, Y. 1993. Two-dimensionalspreading of a granular avalanche down an inclined plane. Part I: Theory. Acta Me-chanica, Vol. 100 , 37–68. [100 ] Jaeger, H. M. and Nagel, S....
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An Introduction to Modeling and Simulation of Particulate Flows Part 11 pdf
... 121, 123Stefan–Boltzmann, 61, 62, 85, 91, 122swarm, 47–54transmission, 111 , 114 , 152vectors, 1, 6, 9, 11, 50, 82, 110 , 116 , 129,130volume fraction, 31, 32, 68, 96, 104, 107, 115 , 118 –120, 126, ... Weidenschilling, S. J. and Cuzzi, J. N. 1993. Formation of planetesimals in the solarnebula. In Protostars and Planets III. Levy, E. H. and Lunine, J. I., editors. University of Arizona Press, 1031–1060.[199] ... H. F., Kaazempur-Mofrad, M. R., Chan, R., Chau,A. H., Hinton, D. P., Isasi,A. G., Kim, L. A, and Kamm, R. D. 2004. Hemodynamics and wall mechanics inhuman carotid bifurcation and its consequences...
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