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Z Transform Rational Z-Transform

Z Transform Rational Z-Transform The inverse of the z-transform Z. Aliyazicioglu Electrical and Computer Engineering Department Cal Poly Pomona ... Nz b z zzz zz Xz z

http://www.cpp.edu/~zaliyazici/ece308/ece308-11.pdf

Date added: August 24, 2016 - Views: 2

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X Y Z XY+YZ+XZ' YZ+XZ' - Computer Science and Engineering

XY+YZ+XZ' equals the logic value of YZ+XZ'. So, XY+YZ+XZ' =YZ+XZ'. (b) ... = YX’ + Y +YZ’ +(XX’)Z +XZY + X(ZZ’) (idempotent law, commutative law,

https://cseweb.ucsd.edu/classes/wi06/cse140/solution1.pdf

Date added: September 21, 2016 - Views: 1

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Parameterized Surfaces and Surface Integrals 1 Problems

Parameterized Surfaces and Surface Integrals 1 Problems 1. Consider the circle in the xz-plane with center at x = 5, z = 0 and radius 3. ... ZZ S ¡ xzi+xj+z2 k ...

http://math.bard.edu/~mbelk/math601/SurfaceIntegrals.pdf

Date added: August 26, 2016 - Views: 1

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: f . . . ,2 ' > *'zç# .1' r , c. .z . . . , 'W.-- c * y

t,zpiv-xz-xaaskzalrk' ,I,- pl.., 'szkl-M rurkerezœ- uz-iltzxr. @a.) otr lo6ase JkQiyo :.16.:e : ... -.k. :-+ ytarkn zz oeyzeapxzelo/iœ k.tAraWokw :m- pI--aty ç+

http://www.ziyaraat.net/books/150QAMaarifatImameZamana.pdf

Date added: August 19, 2016 - Views: 5

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Electromagnetic Waves and Antennas - Rutgers ECE

xxx yy zz yxx yy zz zxx yy zz 2 xx xy y xz z 2 yx x y y y z z 2 zx x z y y z z ... S.J. Orfanidis – Electromagnetic Waves and Antennas Exercises Chapter 1

http://www.ece.rutgers.edu/~orfanidi/ewa/ch1%262-sol.pdf

Date added: August 21, 2016 - Views: 1

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IC E S A T -II L a u n c h : 2 0 1 0 -2 0 1 3 M is s io n S ...

HX^Zc XZ D W _ZXi^kZh/ I ] Z b Vhh W VaVc XZ d [ :Vgi] »h \gZVi ^XZ h] ZZih Vc Y i] Z^g Xd c ig^W j i^d c h id hZV aZkZa VgZ

http://cce.nasa.gov/pdfs/ICESAT-II.pdf

Date added: August 18, 2016 - Views: 16

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CHAPTER 6 CHAPTER 8 Write the 2 –D equations in terms of ...

reducing the three equations of continuity, momentum and ... xx yy zz xy xz yz p x y z v xx xy xz yx yy yz zx zy zz x y z 2 v 2 v 2 v 2 v 2 v 2 v S S vol 2 vol 2 S ...

http://www.eng.buffalo.edu/Courses/mae422/GDyn06ch06.pdf

Date added: August 29, 2016 - Views: 1

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>WY [dZe Y [dY W - rarchivoszona33

¾ <[`Z` e1 ;`i\ZZ` e [\ ;`mlc^XZ` e p ;`]lj` e [\ : ... cXj i\Zfc\ZZ`fe\j p [`jZlk`i cfj _XccXq^fj# \kZ k\iX% <j Zfem\e`\ek\ hl\ cfj gif]\jfi\j Xc`\ek\e cfj

https://rarchivoszona33.files.wordpress.com/2012/09/preescolar2006_experimentos.pdf

Date added: August 18, 2016 - Views: 4

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zz yy Stress & Strain: zx zy yz xy A review

zz Stress & Strain: A review xx yy yz xy xz zx zy yy xx zz

https://www.eoas.ubc.ca/courses/eosc433/lecture-material/StressStrain-Review.pdf

Date added: August 29, 2016 - Views: 1

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Z-transform in Matlab.DOC

ece308-191 1 Z-Transform in Matlab Z-transform is defined as 0 ()()n n Xzxnz ∞ − = = ∑ or X(z)= Z[xn()] The inverse z-transform is denoted by x(n)= Z−1 [Xz()]

http://www.cpp.edu/~zaliyazici/ece308/matlab-2.pdf

Date added: August 18, 2016 - Views: 4

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vv v v v v v v vv vv vv () ( ) - Thomas Jefferson National ...

vv vv vv vv vv vv1111 1 212 3 333ˆˆ ˆˆ ˆˆ ′′ ′′ ′′ee ee e e xx xy zz+++ = + ++xx xz z z rr rr rr LL. Abstracting this idea, a 2‐tensor is any 9 ...

http://casa.jlab.org/publications/viewgraphs/lecture/EMag%20Math%20Supplement.pdf

Date added: August 21, 2016 - Views: 5

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2.4.1: Transformation of Stress

2.4.1: Transformation of Stress • Direction cosines • Orthogonality properties ... XY 1 2 xx 1 2 yy 1 2 zz 1 2 2 1 yz 1 2 2 1 xz 1 2 2 1 x XZ 1 3 xx 1 3 yy 1 3 z

http://www2.mae.ufl.edu/haftka/adv-elast/lectures/Section2-4.pdf

Date added: August 19, 2016 - Views: 1

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z dw ( ) - Iowa State University

xz d Ez dx u u dw GGx ... better than Euler/Bernoulli but still a constant across the cross-section so introduce a form factor κ2 dw dx ψ. 2 0 xx xz yy zz xy yz d ...

http://www.public.iastate.edu/~e_m.424/Beam%20Theory.pdf

Date added: August 21, 2016 - Views: 2

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Stress 1 - West Virginia University

2D Stress Tensor xx xz zx zz Sign Conventions • Compression (+) • Tension (-) • Right Lateral Shear (+) • Left Lateral Shear (-) Resolving stress on a plane ...

http://pages.geo.wvu.edu/~jtoro/structure/ppt/06Stress1.pdf

Date added: November 13, 2016 - Views: 1

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Control Design via Feedback Linearization

Harry G. Kwatny Department of Mechanical Engineering & Mechanics. Drexel University. ... zz x zz yy x x y x y x x y x zz zz zz x. a b a b v av Jv J mv a v v mv d m v ...

http://www.pages.drexel.edu/~hgk22/courses/MEM636_638/Lecture05-FBL.pdf

Date added: September 8, 2016 - Views: 3

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2. Plane Elasticity Problems - Harvard University

2. Plane Elasticity Problems Main Reference: Theory of Elasticity, by S.P. Timoshenko and J.N. Goodier, McGraw-Hill, New York. ... zz xz yz!! +!! =!! +!! =!! #=,",".

http://isites.harvard.edu/fs/docs/icb.topic205126.files/2_Plane_Elasticity_1.pdf

Date added: August 22, 2016 - Views: 1

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Subsurface Pressure and Stress - West Virginia University

Units = Pascals, psi = N/m2 =kg/(m . s2) Force= 50 kg * 9.8 m/s 2 Area = 1 cm2= 0.0001 m2 Stress = 4,900,000 Pascals 686 psi How much is 1 Pascal? ... zz zz xz

http://pages.geo.wvu.edu/~jtoro/Petroleum/07_Pressure.pdf

Date added: August 20, 2016 - Views: 3

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ZZ dA R = 0, = 4. - Page Not Found - Minnesota State ...

ZZ R (y +x)dA, where R is the region bounded by x = 0, y = 0, and 2x+y = 4. −2 −1 −1 ... xz = Z 5 0 Z1 5 (10−2x) 0 Z 10−2x−5y 0 ykydzdydx = 20 3 k M xy ...

http://web.mnstate.edu/jamesju/Fall2011/Content/M323Exam4PracKeyF11.pdf

Date added: August 20, 2016 - Views: 1

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0 !21 13 547698

zZ xZ | m~i { x z@ }z ...

http://db.ucsd.edu/webdb2002/papers/59.pdf

Date added: August 25, 2016 - Views: 1

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Winter 2012 Math 255 - Mathematics

Winter 2012 Math 255 Problem Set 11 Solutions 1) Di erentiate the two quantities with respect to time, use the chain ... ZZ S xydS, where Sis the triangular

http://www.math.lsa.umich.edu/~abloch/255/hw11sol.pdf

Date added: August 18, 2016 - Views: 5

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THE UNIVERSITY OF TEXAS AT EL PASO «» E

zz zz zz zz zz zz zz zz xz zx zxy xz zy y x xx xy zz zz zz zz z x y jj j EE P H H H E E H H H E P HE E P HH H P H P H P P H H H PE H H E E HH H P H P P E E ...

http://emlab.utep.edu/pdfs/Poster_TMM.pdf

Date added: September 8, 2016 - Views: 1

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Unit M4.4 Simple Beam Theory - MIT

Unit M4.4 Simple Beam Theory Readings: CDL 7.1 - 7.5, 8.1, 8.2. ... xz >> σ zz Figure M4.4-2 Illustration of moment equilibrium of “isolated element” of beam L

http://web.mit.edu/16.unified/www/SPRING/materials/Lectures/M4.4-Unified09.pdf

Date added: August 19, 2016 - Views: 1

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IV. - ocw.mit.edu

zz, ε xz may be large and really not close enough to zero to be assumed approximately equal to zero Paul A. Lagace © 2001 Unit 13 - 1 2 . MIT - 16.20 Fall, 2002

https://ocw.mit.edu/courses/aeronautics-and-astronautics/16-20-structural-mechanics-fall-2002/lecture-notes/unit13.pdf

Date added: February 7, 2017 - Views: 1

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Two Phase Flow Rev 02 - North Carolina State University

Two Phase Flow Analysis of two phase flow systems is complicated by the appearance and disappearance of phases, discontinuous ... zz xz zz z iw i ∆ ...

http://www4.ncsu.edu/~doster/NE402/Text/TwoPhaseFlow/TwoPhaseFlow.pdf

Date added: August 24, 2016 - Views: 1

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Comparison of Traditional Agility Metrics to Beck Performance ...

SELECTED AGILITY METRICS zz xz 2 xx zz xz yy xz 2 xx zz xz 2 xz 2 zz zz xx zz xz I(sinτcosαsinβ-cosτsinα)+I (sinτsinαsinβ+cosτcosα)sinτcos ...

http://vscl.tamu.edu/papers/AIAA-00-4313ppt.pdf

Date added: August 30, 2016 - Views: 2

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Problem 1. Spherical tensors - tonic.physics.sunysb.edu

Problem 1. Spherical tensors (a)Consider the rotation by angle ... xz zzyz zz 1 A= 0 @ + xz yx yz xz yz 1 A; (2) so = ( xx+ yy)=2 = zz=2 and = (yy)=2. In terms of ...

http://tonic.physics.sunysb.edu/~dteaney/F13_Phy505/lectures/hw3.pdf

Date added: November 20, 2016 - Views: 1

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Stress and strain - ETH Z

Stress and strain In this chapter we introduce the concepts of stress and strain which are crucial for the understanding of glacier flow. ... xz ˙ xz ˙ zz : (4.7)

http://people.ee.ethz.ch/~luethim/pdf/script/pdg/chapter4.pdf

Date added: August 23, 2016 - Views: 2

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A Viscoelastic Higher-Order Beam Finite Element Computational ...

A Viscoelastic Higher-Order Beam Finite Element A. R. Johnson ... xx zz xz T xx zz xz n T n xx n zz n xz =( ) =( ) ∗ ∗ ∗ ...

http://www.cs.odu.edu/~mln/ltrs-pdfs/NASA-96-tm110260.pdf

Date added: December 26, 2016 - Views: 1

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Figure 1. The Plane Rotation Formula - math.utah.edu

Figure 1. The Plane Rotation Formula The rotation formula depicted above says that under a plane rotation about the origin, ... (xX − zZ) −rZ)2 +y2 = ((xZ + zX)+rX)2.

http://www.math.utah.edu/~palais/AMissingPiece/ConicSectionRotation.pdf

Date added: December 26, 2016 - Views: 1

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Symplectic Structures in Quantum Information

Symplectic Structures in Quantum Information Vlad Gheorghiu Department of Physics ... XxZzXx’Zz’ = !xz’ x’zXx’Zz’XxZz where inner products are taken mod D.

http://quantum.phys.cmu.edu/QIP/symplectic.pdf

Date added: February 7, 2017 - Views: 1

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Stress in 3D - University of Colorado Boulder

Mechanical stress measures intensity level of internal forces in a material (solid or fluid body) idealized as a mathematical continuum. ... xx xy xz yy zz yz

http://www.colorado.edu/engineering/CAS/courses.d/Structures.d/IAST.Lect01.d/IAST.Lect01.Slides.pdf

Date added: August 22, 2016 - Views: 1

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Tutorial 8 - DFT and z-transform - Imperial

zz Xz zz − = −+ (b)** 2 2 (2) ... Microsoft Word - Tutorial 8 - DFT and z-transform.doc Author: peterc Created Date: 3/3/2008 12:17:06 AM ...

http://www.ee.ic.ac.uk/pcheung/teaching/ee2_signals/Tutorial%208%20-%20DFT%20and%20z-transform.pdf

Date added: August 29, 2016 - Views: 1

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An Elasticity Solution for the Global Buckling of Sandwich ...

Global Buckling of Sandwich Beams/Wide Panels With Orthotropic Phases There exist several formulas for the global buckling of sandwich plates, ... zz xz 0 + y yz

http://gkardomateas.gatech.edu/Journal_papers/104_Kardom_JAM.pdf

Date added: August 19, 2016 - Views: 1

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Radial and Axial Tubular Reactor - University of Michigan

Radial and Axial ... Ay xz, F Ax W Ax zy Molar flow rate in Molar flow rate out z Molar flow rate in Molar flow rate zyy+Dz out y Mole Balance xy W Az z xy W Az zz xz ...

http://www.umich.edu/~essen/html/byconcept/cdchap/15chap/ECRE_CD-CH15.pdf

Date added: August 18, 2016 - Views: 4

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yZ zZ zZg ~zZg - ALMUALLIM.ORG

Ðg±ZZ 116 59 Š‹ZŠZ®päxlZÅg$u 118 60 (päxlZÅg$u 121 61 Ðg±ZÆ]ÌÅV- zZg ... à yZ ä xZ ™[ YfÆZgzZx?Z:YmCZV$Zgz z1Q÷w®Ðp qg ÷áGî0 4EG&ŠxEx ...

http://www.almuallim.org/ebook/Muallim%20ul%20Ijra%20Bil%20Hadeeth%20Ebook.pdf

Date added: August 29, 2016 - Views: 1

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Module #9Module #9 - University of Alabama

oxxyy2 zz xy xz yz2 ... zz xyyz xyxz xy yz x x z SSS y xy ...

http://bama.ua.edu/~mweaver/courses/MechBeh/Day09.pdf

Date added: August 20, 2016 - Views: 1

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ZZ h i S H - nd.edu

yz 2+ 2xyz;xz2 + xz;2xyz+ x2y 2z (a) f(x;y;z) = xyz2 + x 2yz 1 2 ... ZZ H hx;y;zi dS = ZZ T hacos sin˚;asin sin˚;acos˚i asin˚hacos sin˚;asin sin˚;acos˚idA= ZZ T

https://www3.nd.edu/~taylor/Math20550/images/OldExams/Exam4A.pdf

Date added: February 5, 2017 - Views: 1

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Solutions - Homework sections 17.7-17 - invariant.org

Solutions - Homework sections 17.7-17.9 ... ZZ D xy p ( 2)2 + ( 1)2 + 1 dA = p ... The projection of Sonto the xz-plane is the disk D= f(x;z) : x2 + z2 4g. ZZ S

http://invariant.org/courses/calc3F09/HW_sols/17.7-17.9.pdf

Date added: August 18, 2016 - Views: 3

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BLUP Best Linear Unbiased Prediction-Estimation

BLUP Best Linear Unbiased Prediction-Estimation References Searle, S.R. 1971 Linear Models, Wiley Schaefer, L.R., Linear Models and Computer ... ZX ZZ G XX XZ ' '

http://nitro.biosci.arizona.edu/Nordicpdf/lecture12.pdf

Date added: August 30, 2016 - Views: 1

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Hengyong Yu, PhD Associate Professor Department of Electrical ...

Xz zz 𝑋(𝑧) has two poles at 1/3 and 1/4 and one zero. ROC: |z|>1/3 11 [ ] [ ] 2 [ ] 43 nn x n u n u n § · § ...

http://faculty.uml.edu/Hengyong_Yu/CourseMaterials/Lecture_Notes_Ch10_2.pdf

Date added: February 7, 2017 - Views: 1

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Elastic Properties of Dislocations Stacking faults

Elastic Properties of Dislocations Stacking faults READING LIST DIETER: Ch. 5, Pages 160-168 Ch. 4, Pages 205-222 in Meyers & Chawla, 1st ed. ... L xz yz zz yz xz x y ...

http://bama.ua.edu/~mweaver/courses/MechBeh/N13.pdf

Date added: January 2, 2017 - Views: 1

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ANALYTICAL AND NUMERICAL RESULTS FOR AN ADHESIVELY BONDED ...

zz, and γ xz denotes the engineering shear strain. The laminate thicknesses for the upper and lower adherends are given by h U and h L, respectively, ...

https://ntrs.nasa.gov/archive/nasa/casi.ntrs.nasa.gov/20060020138.pdf

Date added: February 7, 2017 - Views: 1

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Plane Stress Transformations - University of Colorado Boulder

Plane Stress Transformations ASEN 3112 Lecture 6 – Slide 1. ASEN 3112 - Structures ... xx xy xz yy zz yz zx zy yx There are three (3) principal stresses, identified as

http://www.colorado.edu/engineering/CAS/courses.d/Structures.d/IAST.Lect06.d/IAST.Lect06.Slides.pdf

Date added: August 23, 2016 - Views: 1

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A B C D E F G H I J K L M N O P Q R S T U V W X Y Z AA BB CC ...

ss t t uu v v x yy zz hh ww i kk ee ff gg jj mm dd l n oo pp qq rr cc #8 x 1!/2" fh woodscrew #8 x 1" fh woodscrew first: xxxxxxx xxxxxxxxxxx top view (cross section ...

http://www.shopnotes.com/files/issues/112/hardware-cabinet.pdf

Date added: August 18, 2016 - Views: 13

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6.1 The Linear Elastic Model - Faculty of Engineering

6.1 The Linear Elastic Model 6.1.1 The Linear Elastic Model Repeating some of what was said in Section 5.3: the Linear Elastic model is used to ... zz xz yz zz E xx ...

http://homepages.engineering.auckland.ac.nz/~pkel015/SolidMechanicsBooks/Part_I/BookSM_Part_I/06_LinearElasticity/06_Linear_Elasticity_01_Elastic_Model.pdf

Date added: August 31, 2016 - Views: 1

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A singular Lambert-W Schrödinger potential exactly solvable ...

zz z() 0 be a sixth degree polynomial as the form of the invariant requires, we get m1 1, 3 / 2 or 2. ... zWe zzxz x ...

https://aps.arxiv.org/pdf/1606.06383.pdf

Date added: February 7, 2017 - Views: 1

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Lecture #5 Transfer Matrix Method Using Scattering Matrices

Transfer Matrix Method Using Scattering Matrices ... zz zz zz zz zz zz zz zz x xz zx xz zy y yxy y zz zz zz zz zz x y kk k jk k jk k E k jk j k k E z H

http://emlab.utep.edu/ee5390cem/Lecture%205%20--%20TMM%20Using%20Scattering%20Matrices.pdf

Date added: August 19, 2016 - Views: 1

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MATH 2203 ŒFinal Exam (Version 1) Solutions

ZZ Sxz (y z) dS. Since S xz is the graph of the function y = 0, we have ZZ Sxz (y z) dS = ZZ Sxz (y z) q (y x) 2 +(y z) 2 +1dA = ZZ D (0 z) dA = Z 1 0 Z 1 x 0 zdzdx ...

http://ksuweb.kennesaw.edu/~sellerme/sfehtml/classes/math2203/m2203fa07finalexamver1solutions.pdf

Date added: February 6, 2017 - Views: 1

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Transformation of the Navier-Stokes Equation to the Cauchy ...

w u uu u u u uu uυ xx xz yy yz zz zz xz yz zz

http://file.scirp.org/pdf/AM_2016061614151499.pdf

Date added: February 7, 2017 - Views: 1