phương pháp tìm khoảng phân li nghiệm của phương trình 1 1
Engineering nanomaterials from bottom up with computer simulation
... Comput Phys 11 7 :1- 19 37 Phillips JC, et al (2005) Scalable molecular dynamics with NAMD J Comput Chem 26 :17 81 18 02 | www.vjsonline.org 34 VJS | January 2 015 | Volume | Issue | c 111 4 01 Engineering ... bonding Nature 4 91: 51 55 11 Zhang L, Niu W, Xua G (2 012 ) Synthesis and applications of noble metal nanocrystals with high-energy facets Nano Today, 7:586–505 12 Israelachvili JN (2 011 ) Intermolecular ... (2 011 ) Cubic crystals from cubic colloids Soft Matter7: 413 9– 414 2 Jiang S, et al (2 010 ) Janus particle synthesis and assembly Adv Mater 22 :10 60 10 71 | www.vjsonline.org 33 VJS | January 2 015 |...
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Modelling continuous risk variables: Introduction to fractional polynomial regression
... FP1:Power (1) β0 + 1 X FP1:Power (2) β0 + 1 X FP1:Power (3) β0 + 1 X FP degree with 36 different pairs of powers, taking from {−2, − 1, − 0.5, 0, 0.5, 1, 2, 3} 10 11 12 13 14 15 16 17 18 19 ... + 1 (1/ X2) + β2 (X) β0 + 1 (1/ X2) + β2 (X2) β0 + 1 (1/ X2) + β2 (X3) β0 + 1 (1/ X) + β2 (1/ sqrt(X)) β0 + 1 (1/ X) + β2 (lnX) β0 + 1 (1/ X) + β2 (sqrt(X)) β0 + 1 (1/ X) + β2 (X) β0 + 1 (1/ X) ... {−2, − 1, − 0.5, 0, 0.5, 1, 2, 3} FP1: Power (-2) β0 + 1 (1/ X2) FP1: Power ( -1) β0 + 1 (1/ X) FP1: Power (-0.5) β0 + 1 (1/ sqrt(X)) FP1: Power (0) β0 + 1 (lnX) FP1:Power (0.5) β0 + 1 (sqrt(X))...
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POLYNOMIAL DECAY SOLUTIONS TO FRACTIONAL DIFFERENTIAL INCLUSIONS WITH INFINITE DELAYS
... s) (α 1) p p 1 Lp − p 1 (t−s) e p 1 p ds ∞ ≤ C||k||Lp (R+ ) s (α 1) p p 1 e Lp − p 1 s p 1 p ds p 1 = C||k||Lp (R+ ) Lp = o (1) as L → ∞, αp 1 p Γ αp − p 1 p 1 p thanks to the H¨ older inequality ... t 1 ≤C t t 1 γ t (t − s)α 1 m(s)ds t 1 Then using the H¨ older inequality again, we get γ t I3 (t) ≤ C t t 1 γ t ||m||Lp (R+ ) (t − s) (α 1) p p 1 p 1 p ds t 1 γ p 1 αp − t =C ||m||Lp (R+ ) t 1 ... changed from line to line Using the H¨older inequality, one has p 1 p t I1 (t) ≤ C||m||Lp (R+ ) p − p 1 (t − s) = C||m||Lp (R+ ) (p − 1) p 1 p p 1 − p 1 p t− p Thus tγ I1 (t) ≤ Ctγ− p = O (1) as t...
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An introduction to disk drive modeling
... (milliseconds) • a fixed controller overhead, and r ea lin 30 real 25 20 Table 15 seek distance seek time (ms) 10 < 616 cylinders 3.45 + 0.597√d ≥ 616 cylinders 10 .8 + 0. 012 d 200 400 600 800 10 00 ... sector size 256 bytes 512 bytes cylinders 14 49 19 62 tracks per cylinder 19 data sectors per track 11 3 72 number of zones 1 track skew 34 sectors sectors cylinder skew 43 sectors 18 sectors revolution ... best C2200A model mean 10 15 20 25 30 Time (ms) 35 40 b Adding caching: readahead and immediate reporting demerit mean simulation 17 . 51 0.02ms 11 .7ms 11 2% demerit simulation 10 .92±0.03ms 0.60ms...
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C++ - I/O Streams as an Introduction to Objects and Classes
... Publishing as Pearson Addison-Wesley Slide 6- 10 Stream Variables Like other variables, a stream variable… Must be declared before it can be used Must be initialized before it contains valid ... Education, Inc Publishing as Pearson Addison-Wesley Slide 6- 24 Calling a Member Function Calling a member function requires specifying the object containing the function The calling object is ... in_stream.open("infile.dat"); Calling object Member function Dot operator Copyright © 2007 Pearson Education, Inc Publishing as Pearson Addison-Wesley Slide 6- 25 Member Function Calling Syntax Syntax for calling a...
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Introduction to Digital Signal Processing and Filter Design
... −0 .12 5 −0 .12 5 0.000 0 .12 5 0.375 0.500 0.500 0.250 0 .12 5 0 .12 5 0 .12 5 Binary Number Form 1 1 0 0 0 0 000 010 0 01 0 01 000 0 01 011 10 0 10 0 010 0 01 0 01 0 01 INTRODUCTION 7/8 6/8 5/8 4/8 3/8 2/8 1/ 8 ... response of the TABLE 1. 1 Bit Binary Numbers and their Decimal Equivalents Binary Form 11 1 11 0 10 1 10 0 011 010 0 01 000 Decimal Value = 0.875 = 0.750 = 0.625 = 0.500 = 0.375 = 0.250 = 0 .12 5 0.0 = 0.000 ... 0 .1 n) = cos(2πn) cos(0 .1 n) + sin(2πn) sin(0 .1 n) = cos(0 .1 n) = v0 (n) (1. 20) (1. 21) 18 INTRODUCTION v1 (n) = cos(2 .1 n) = cos(2πn + 0 .1 n) (1. 22) = cos(2πn) cos(0 .1 n) − sin(2πn) sin(0 .1 n)...
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Introduction to Wireless Communications
... it 16 Wireless Local Area Networks (continued) 17 Wireless Local Area Networks (continued) • Institute of Electrical and Electronic Engineers (IEEE) standards – 802 .11 a, 802 .11 b, and 802 .11 g 18 ... station to another • Transmission time is approximately 250 milliseconds 10 Satellite Networks (continued) 11 Satellite Networks (continued) 12 Cellular Networks • Modern cellular telephone network ... Networks (ISDN) – Transmit at 256 Kbps over regular phone lines • T1 lines – Transmit at 1. 544 Mbps • Cable modems and digital subscriber lines (DSL) – Generally only available in residential areas...
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An Introduction to Software Engineering
... Engineering, 7th edition Chapter Slide 21 Issues of professional responsibility Confidentiality • Engineers should normally respect the confidentiality of their employers or clients irrespective of ... for long-lifetime syst 10 00 System testing Development ©Ian Sommerville 2004 75 Iterative development ems 200 30 400 System evolution Software Engineering, 7th edition Chapter Slide 15 Product ... 2004 Software Engineering, 7th edition Chapter Slide 18 What are the attributes of good software? The software should deliver the required functionality and performance to the user and should be...
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A simple introduction to working with LVM
... hda1 Boot Primary Linux ext3 [/] 8000. 01 hda2 Primary Linux swap / Solaris 10 00.20 hda3 Primary Linux 310 07.57 Here I have a 7Gb root partition which contains my Debian GNU/Linux installation ... LVM2: Sat Jun 10 12 :35:57 2006 contents = "Text Format Volume Group" version = description = "Created *before* executing 'lvcreate -n test size 1g skxvg'" creation_host = "lappy" # Linux lappy ... with the name 'test': root@lappy:~# lvcreate -n test size 1g skx-vol Logical volume "test" created This command creates a volume of size 1Gb with the name test hosted on the LVM volume group skx-vol...
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Cambridge.University.Press.An.Introduction.to.Law.and.Regulation.Text.and.Materials.Apr.2007.pdf
... 3.3.2 Politics, legal culture and institutional variety 3.3.3 Discussion questions 3.4 Conclusion 10 2 10 5 11 3 11 3 11 6 13 2 14 6 14 6 Regulatory enforcement and compliance 4 .1 Introduction 4.2 The limits ... questions 4.5 Conclusion 15 1 15 1 15 3 17 5 17 6 18 1 19 3 Regulatory accountability and legitimacy 5 .1 Introduction 5.2 Levels of theorising 5.3 Regulatory accountability 5.3 .1 Discussion questions ... University Press First published in print format 2007 eBook (EBL) ISBN -13 978-0- 511 -28475-5 ISBN -10 0- 511 -28475-6 eBook (EBL) paperback ISBN -13 978-0-5 21- 68565-8 paperback ISBN -10 0-5 21- 68565-6 Cambridge...
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Cambridge.University.Press.An.Introduction.to.the.Philosophy.of.Mind.Jan.2000.pdf
... schemes 69 70 74 79 82 84 89 92 95 99 10 0 10 2 10 3 10 7 11 0 11 2 11 4 11 6 11 9 12 1 12 5 12 6 12 8 13 0 13 1 13 5 13 7 14 3 14 5 14 9 15 5 15 8 16 0 16 2 16 4 16 7 16 9 17 5 17 8 18 3 Contents Knowledge of language: innate ... Street, New York, NY 10 011 -4 211 , USA 477 Williamstown Road, Port Melbourne, VIC 3207, Australia Ruiz de Alarcón 13 , 28 014 Madrid, Spain Dock House, The Waterfront, Cape Town 80 01, South Africa http://www.cambridge.org ... causation Animalism Knowing one’s own mind Moore’s paradox and the nature of conscious belief Externalism and self-knowledge Self-deception Conclusions Bibliography Index ix 18 8 19 1 19 3 19 4 19 6 200...
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Cambridge.University.Press.The.Cambridge.Introduction.to.Modern.British.Fiction.1950-2000.Apr.2002.pdf
... Repression in Gay Fiction 11 3 vi 83 Contents Chapter National Identity 11 8 Reinventing Englishness 11 9 The Colonial Legacy 12 4 The Troubles 13 1 Irishness Extended 14 1 Welsh Resistance 14 4 The ‘Possible ... Victor Michael Head 26 .10 . 31 18 .4. 01 Contents Acknowledgements Introduction page viii Chapter The State and the Novel 13 The Post-War Wilderness 14 The Testing of Liberal Humanism 19 The Sixties and ... Isles? 15 4 Chapter Multicultural Personae 14 7 15 6 Jewish-British Writing 15 8 The Empire Within 16 1 ‘Windrush’ and After: Dislocation Confronted The Quest for a Settlement 17 0 Ethnic Identity and Literary...
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An introduction to franchising
... Freight 1, 776 1, 155 610 11 894 GROSS PROFIT S STS & EXPENSE OPERATING CO Fixed Insurance Rent Salaries Utilities 544 26 10 0 310 42 Variable Advertising Dues Telephone Office Supplies 24 24 14 350 ... abilities Total Current Li ilities – Note Long-Term Liab uity Stockholders’ Eq S AND EQUITY TAL LIABILITIE TO THE IFA EDUCATIONAL FOUNDATION $6,500 1, 200 1, 800 $9,500 $12 ,500 $20,600 $33 ,10 0 ... 200 $19 ,10 0 sets Total Current As Fixed Assets Machinery r Computer/Printe Furniture ts Total Fixed Asse 8,500 1, 000 4,500 $14 ,000 $33 ,10 0 Total Assets D EQUITY LIABILITIES AN s Current Liabilitie...
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Introduction to fluid mechanics - P1
... mechanics Fig 1. 1 Restored arch of Roman aquedud in Compania Plain, Italy materials posed the most important problems In this sense, it is believed that hydraulics was born in the utilisation of ... conduit had to be designed and its Fig 1. 2 Relief of ancient Egyptian ship The beginning of fluid mechanics Fig 1. 3 Ancient Greek ship depicted on old vase inclination or supply pressure had to be ... region Leonardo was the first to find the least resistive ‘streamline’ shape 4 History of fluid mechanics Leonardo da Vinci (14 52 -15 19 ) An all-round genius born in Italy His unceasing zeal for...
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Introduction to fluid mechanics - P2
... x106) 10 20 30 40 17 9.2 13 0.7 10 0.2 79.7 65.3 1. 792 1. 307 1. 004 0.8 01 0.658 1. 724 1. 773 1. 822 1. 869 1. 915 13 .33 14 . 21 15 .12 16 .04 16 .98 Stokes’ equation, to be stated in Section 9.3.3, is utilised ... m*/(s* K) K (OOC, 760 mm H ) g Gas 0 .17 8 1. 293 1. 250 0.089 1. 429 1. 977 0. 717 2078 .1 287 .1 296.9 12 4.8 259.8 18 9.0 518 .7 1. 66 1. 402 1. 400 1. 409 1. 399 1. 3 01 1. 319 Density (kg/m3) = CJC, Let p be ... (kg/m') Water Air 10 999.8 1. 293 999.7 999 .1 998.2 1. 247 1. 226 1. 205 15 20 10 0 40 60 80 992.2 1. 128 983.2 1. 060 9 71. 8 958.4 1. 000 0.9464 Viscosity As shown in Fig 2 .1, suppose that liquid fills the...
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Introduction to fluid mechanics - P3
... (3 .14 ) From eqs (3 .12 )-(3 .14 ) (3 .15 ) From eqn (3 .15 ) (3 .16 ) In aeronautics, it has been agreed to make the combined values of po = 10 1.325 kPa, T, = 288 .15 K and po = 1. 225 kg/m3 the standard atmos- ... (3 .12 ): (3 .13 ) When the absolute temperatures at sea level and at the point of height z are T, and T respectively, the following equation is obtained from eqn (2 .14 ): (3 .14 ) From eqs (3 .12 )-(3 .14 ) ... (3.6), (3 .10 ) Integrating this equation from z = (sea level), (3 .1 1) The relation between the height and the atmospheric pressure develops into the following equation by eqn (3 .1 1): (3 .12 ) Also,...
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Introduction to fluid mechanics - P4
... cylinder, absolute streamlines are observed (Fig 4.2(b)) In addition, the lines which show streams include the streak line and the path line By the streak line is meant the line formed by a series ... Experimental Physik, IV, Teil, Akademische Verlagsgesellschaft (19 32), 12 7 Rotation and spinning of a liquid 47 Osborne Reynolds (18 42 -19 12) Mathematician and physicist of Manchester, England His ... Relative streamlines and absolute streamlines the x and y directions as u and v respectively, the following equation of the streamline is obtained: dx/u = dy/v (4 .1) Whenever streamlines around...
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Introduction to fluid mechanics - P5
... vertically in the solid wall face parallel to the flow As Bernoulli's theorem applies to a flow line, it is also applicable to the flow in a pipe line as shown in Fig 5.6 Assume the pipe line is horizontal, ... = 0 .12 m3/s, obtain Q,, and F Qz Fig 5.30 10 As shown in Fig 5. 31, if water flows out of the tank of head 50cm through the throttle, obtain the pressure at the throat Problems 81 Fig 5. 31 11 Figure ... that the pipe line is horizontal, z1 = 22 v2 - v: - - PI - P2 - 29 P9 From the continuity equation, 01 = V2A2IAl Conservation of energy 63 Giovanni Battista Venturi (17 46 -18 22) Italian physicist...
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Introduction to fluid mechanics - P6
... the latter the main flow I' '* Schlichting, H., Boundary Layer Theory, (19 68), 563, McGraw-Hill, New York Itaya, M, Bulletin o f J S M E , 7-26, (19 41- 2), 11 1-25 10 2 Flow of viscous fluid This ... Navier-Stokes equation (6 .13 ) using cylindrical coordinates Under the same conditions as in the previous section (6.3 .1) , simplify the upper equation in equation (6 .13 ) to give dp d2u l d u = ... Developments in Fluid Dynamics, (19 65), 336, Dover, New York) lo It may also be expressed as P/u, = u', u.y/v = y+ 10 0 Flow of viscous fluid Theodor von Karman (18 81- 1963) Studied at the Royal Polytechnic...
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