On some problems of synthesis of spatial five-bar hinged mechanisms with two degrees of freedom

Size: px
Start display at page:

Download "On some problems of synthesis of spatial five-bar hinged mechanisms with two degrees of freedom"

Transcription

1 Internationa Journa of Mechanica Engineering and Appications 014 (6): Puished onine ecemer 18, 014 ( doi: /j.ijmea ISSN: X (Print) ISSN: (Onine) On some proems of synthesis of spatia five-ar hinged mechanisms with two degrees of freedom Nodar avitashvii *, Otar Geashvii epartment of Transport and Mechanica Engineering of Georgian Technica University, Tiisi, Georgia Emai address: (N. avitashvii), (O. Geashvii) To cite this artice: Nodar avitashvii, Otar Geashvii. On Some Proems of Synthesis of Spatia Five-Bar Hinged Mechanisms with Two egrees of Freedom. Internationa Journa of Mechanica Engineering and Appications. Vo., No. 6, 014, pp doi: /j.ijmea Astract: Soution of the proems of synthesis of spatia five-ar hinged mechanisms with two degrees of freedom task considering the ange of transmission and definition of conditions of existence of cranks is given in the paper. A possiiity of movement of the designed mechanism without seizure that is depended on shape and sizes of the mechanism inks is envisaged. At soution of the proem of synthesis first are determined sizes of the mechanism coupes considering the ange of transmission and then are determined the imits of variation of the ange of transmission depending on sizes of the mechanism inks. The conditions are ascertained which must e met y sizes of the spatia five-ar mechanism inks so that the two inks adjoining to the frame are crank (theorem on existence of cranks in the spatia five-ar mechanism). Keywords: Synthesis, Ange of Transmission, Spatia Five-Bar Mechanism, Couper, Conditions of Existence of Crank 1. Introduction Spatia mechanism with two degrees of freedom rank high among numerous hinged mechanisms used in practice, which in contrast to four-ar mechanisms, can reaize more compex aws of motion favouring at the same time rise of the machines efficiency and optimization of the technoogica processes. A distinctive feature of these mechanisms is their capacity for variation of the couper point ocus from the simpe to the more compex form in the course of operation at variation of anguar veocities of the input inks considering directions of motions and their mutua initia inter-ocation at constant engths of the inks. These circumstances are directy reated with seection of ength of the output inks of mechanisms and predetermine necessary conditions for creation of compact, ightweight mechanisms, especiay in the fieds of space and rootics industry, decreasing at this consumption of materias and energy. The spatia five-ar hinged mechanisms with two degrees of freedom are widey used in various devices, rootics systems as we as in industria practice as operating memers [1, ] and so on. The researches into hinged mechanisms with two degrees of freedom started at the end of XIX and eginning of XX centuries y first studying panar five-ar mechanisms with two input inks. Soution of the proem on ocations for the spatia mechanisms with severa degrees of freedom and spherica five-ar mechanisms with two degrees of freedom was first considered y A.G. Ovakimov [3] ony in the 70-ies of the XX century. The proems of kinematica anaysis of the spatia five-ar mechanism of type RCRCR with one degree of freedom were considered in the work of J. uffi and G.I. Hai-Oahi. [4]. The anaytica formuae were derived with the use of spherica trigonometry. The positions of output inks of the mechanism are determined y the forth order equation and in the work of J. uffi [5] for determination of dispacements of the spatia five-ar mechanism were used the dua equations. Much attention was given to the proems of anaysis, synthesis, kinetostatics and dynamics of mechanisms with two degrees of freedom y Georgian scientists having carried out deep anaysis of the mentioned mechanisms. In shoud e noted in this aspect the works [6, 7] of N.S. avitashvii. In the work [6] is given anaysis of infuence of parameters of the five-ar hinged mechanism on trajectories of the coupers points and in the work [7] are studied proems of kinematics and precision of these mechanisms. Besides the mentioned works numerous researches into anaysis, synthesis, dynamics and precision of hinged

2 105 Nodar avitashvii and Otar Geashvii: On Some Proems of Synthesis of Spatia Five-Bar Hinged Mechanisms with Two egrees of Freedom mechanisms with two degrees of freedom are carried out y first author of these artices [8, 9, 10]. In the work [11] of N.S. avitashvii and O. Geashvii is given synthesis of the five-ar spatia mechanism with two degrees of freedom according to the trajectory. In the presented work is carried out synthesis of the spatia five-ar hinged mechanism with two degrees of freedom taking into account the ange of transmission and conditions of existence of two cranks.. Synthesis of the Spatia Five-Bar Mechanism Taking into Account the Ange of Transmission At soution of the proem of synthesis of spatia five-ar mechanisms with two degrees of freedom it is necessary to consider the foowing requirements: correct structure of the mechanism to e designed, kinematica precision of the movement to e performed, possiiity of reaization of the given movement y mechanism to e designed from the standpoint of dynamics, possiiity of movement of the mechanism under action of appied forces with maximum possie efficiency (taking into account the ange of transmission to avoid their seizure) and finay, ensuring existence of cranks and reproduction of the given movement y the sizes of inks of the synthesized mechanism..1. imensioning of Coupers of the Five-Bar Spatia Mechanism Taking into Account the Given Vaue of the Ange of Transmission Let's consider spatia five-ink hinged everage RSSRR type mechanism ABCE (Fig. 1) with two degrees of freedom and determine the dimensions BC= 3 and C= 4 of coupers with taking into account the given vaues of ange of transmission γ (γ min, γ max ). Figure 1. Spatia five-ar mechanism with two degrees of freedom. For soution of this proem are given: dimensions of inks 1,, 5, designated as 1,, and 5 anges α 0 and β 0, specifying the initia position of the input AB 0 and E 0 inks and 5, with respect to the frame 1. The aws of motion of the input inks and 5 are given as: ϕ = ϕ ) and ϕ = ϕ ), (1) ( t 5 5 ( t ϕ = α + α( ) and ϕ = β + β ( ). () 0 t 5 0 t Here α and β are the variae anges characterizing the motion of input inks. The gear ratios from ink 5 to ink is defined as = = = =±, (3) the sign (+) is taken for the case when input inks and 5 are rotating in the same direction, and the sign ( ) when they are rotating in the opposite directions.. It shoud e noted that y giving functions of dispacements of the input inks, gear ratio is aso =. (4) We seect two fixed coordinate systems for the input inks and 5 so that point A is ocated in the pane X 0 EY 0. The system EX 0Y0 is seected for ink 5, and system AX1Y 1Z1 - for ink. Accordingy are given the coordinates of point A ( x0 y0z0 ) in the system EX 0Y0 considering ange ξ etween axis EX 0 and frame 1: x = 1 cos y = 1 sin z 0 = 0. (5) 0 ξ 0 ξ The transformation of system AX1Y 1Z1 in the system EX Y is carried out due the matrix: = 0, (6) 11, 1,., 33 are directing cosines of axes of the system AX 1 Y 1 Z 1 with respect to the EX 0 Y 0 Z 0 system. It is possie at first to set the four vaues of directing cosines, for exampe, 11, 1, 31 and 3 =0, then for 33, 1, 3, 1 we wi have: =1 = = =1. The variae distance etween movae joints B and, the vaue of that is depended on dimensions of frame 1 and input inks ( ) and 5 ( 5 ), initia position of input inks (α 0,β 0 ), gear ratio etween input inks with taking into account directions of their movement can e determined in the system EX0Y0 with the hep of formua for the distance etween two points in space: (7) =! +# #! +$ $!, (8)

3 Internationa Journa of Mechanica Engineering and Appications 014 (6): x 0 ϕ ϕ. (9) B = yb = cos zb = sin x 0 ϕ ϕ. (10) = y = 5 cos 5 z = 5 sin Considering the ocation of point A at the origin of the system,, the coordinates of point B CAN e written in the system EX0Y0 using matrix (6) x y z B B B = = 1 = 33 cosϕ + cosϕ + sinϕ sinϕ + sinϕ + 1 cosζ 1 sinζ 5 (11) Considering vaues (), (10) and (11) expression (8) wi take a form: =% ' (cos, - +, ' cos/+ sin/+sin, - +, ' cos/+ sin/ sin/cos3 - +, ( cos, - +,cos3 - +,+ ' '+ sin, - +, ' sin3- +,4, (1) β=,. Here α is a variae vaue. Anaysis of expression (1) shows that distance depends on,, 5, α 0, β 0,, α and directing cosines. FROM triange BC taking into account the given maxima (γ max ) and minima (γ min ) vaues of the ange of transmission can written: cos7 89: = 89: + (13) 6 6 cos7 8< = 8<, max and min are the extreme vaues of variae distance. It is known that if derivative = =, exists, then function wi have maximum or minimum ony if > > =0. (14) If second derivative =² =,² exists, then function wi have maximum when and minimum at Accordingy we can write > =0, >² <0, (15) > >² > =0, >² >0. (16) > >² > = C (17) > C >² = CCFF GC >² 6 C H= (cos, - +, ' cos/+ sin/+sin, - +,, (18) ' cos/+ sin/ sin/cos3 - +, ( cos, - +,cos3 - +,+ ' '+ sin, - +,sin3 - +, H = (cos, - +, cos/+ sin/ ' ' sin, - +, cos/+ sin/+ +,+ sin/sin3 - +, ( cos, - +, ' cos3 - +, ',+ sin3 - +, ' sin, - +, sin, - +, ' cos3 - +,+ +,+ sin3 - +, ' cos, - +,+ + cos, - +, ' sin3 - +,+ + ',+ cos3 - +, ' sin, - +,. The vaues k'' wi e found y differentiation of k'. In turn = F G. (19) For determining of such vaue of α that gives the extreme vaues of distance it is necessary that condition (14) e met. From the reations (17) we wi have cos,%,+ sin/sin3 - + ' + sin, - +,( cos3 - + ' +,+ sin3 - ',+ cos cos, - +,(,+ sin3 - ' - ' cos3 - ' sin sin,%,+ sin/sin3 - '+ + sin, - +,( cos3 -,+ ' ' sin3 - +,+ sin , - +,(,+ cos3 - '

4 107 Nodar avitashvii and Otar Geashvii: On Some Proems of Synthesis of Spatia Five-Bar Hinged Mechanisms with Two egrees of Freedom sin3 - ' ' cos3-4 (sin, - +, cos/+ sin/ ' + +cos, - +, ' cos/+ sin/=0. (0) On the ase of known formuae of the Moivre cos, and sin, incuded in the equation (0) can e presented as cos,=cos J, K J cos JG,sin²,+ 6 +K J cos JG6,sin 6, (1) sin,= cos J G,sin, K J cos JG,sin³,+ +K J cos JG,sin, () Taking into account vaues (1) and () equation (0) wi take a form: N ±N N =0, (3) N = Ocos J, K J cos JG,sin²,+ ' + ' 6 K J cos JG6,sin 6, P %,+ sin/sin3 - + ' + sin, - +,( cos3 - + ' +,+ sin3 - ',+ cos cos, - +,(,+ sin3 - ' cos3 - ' ' sin3-4 N = cos JG,sin, ' K J cos JG,sin³,+ + ' K J cos JG,sin, P %,+ sin/sin3 - + sin, - +, ' ( cos3 -,+ sin3 - + ' + ',+ cos3 - + cos, - +, (,+ cos3 - ' sin3 - ' ' cos3-4 N = (sin, - +, cos/+ sin/ ' + + ' cos, - +, cos/+ sin/. Binomia coefficients in turn wi have forms K J = 1! and so on K J = 1 3! K J 6 = 1 3 4! K J K J = ! < = 1 3 O U 1P. U! In equations (3) a sign (+) is taken when gear ratios is a positive numer, and sign ( ) when is a negative numer. The series of inomia coefficients is finite when is a positive or negative integer, and infinite when is a positive or negative fractiona numer. By soution of equations (3) are determined the vaues α i (α 1, α,, α n ), with the hep of which we determine extreme vaues max and min of distance accordingy to formua (1). In practice are mainy encountered cases when the input inks are moving with constant anguar veocity ( =const). In such case expressions (17), (18) and equation (3) wi e significanty simpified. Thus knowing vaues max and min, and transforming the system (13) we otain a vaue of couper 4 (C= 4 ) ength: 6 =± VW ±XW G6W W W, Y =4cos7 8< cos7 89: (4) Y =4( 89: cos7 8< cos7 89: + ' + ' cos7 89: 89: 8< cos7 8< cos7 89: Y = 89: 8<. Accordingy a ength of couper 3 (BC= 3 ) wi e determined from system (13): = Z[\ G Z]^. (5) _ `ac Z]^G`ac Z[\.. etermination of Limits of Anges of Transmission epending on imensions of Links of the Spatia Five-Bar Mechanism At soution of this proem a condition is envisaged according to which an ange of transmission at any position of the mechanism must not e ess that certain given minimum vaue ensuring norma functioning of the mechanism. Seection of aowae anges of transmission is determined y dynamica conditions of the mechanism operation and in the first pace y asence of seizure of

5 Internationa Journa of Mechanica Engineering and Appications 014 (6): output inks. Considering a poygon of inks ABCE and triange BC (Fig. 1) for distance we can write: Suppose 7= h = c Z[\Gc Z]^. (31) = (cos, - +, ' cos/+ sin/+ '+sin, - +, cos/+ sin/ sin/cos3 - +, ( cos, - +,cos3 - +,+ ' + sin, - +, ' sin3 - +,= = cos7. (6) From expressions (6) can e determined the ange of transmission γ: cos7= 6 G % + 6 ' (cos, - +, cos/+ sin/ ' + + ' sin, - +, cos/+ sin/+ + sin/cos3 - +,+ + ( cos, - +,cos3 - +, ' + + sin, - +,cos3 - +, + sin, - +, ' sin3 - +,4. (7) If 0<γ<π, then the extreme vaues of ange γ wi e determined from formua (7): cos7 89: = d _ GZ[\, (8) _ cos7 8< = d _ GZ]^. (9) _ An optima vaue γ=π/ wi e otained at vaue of variae ange α determined from equation + 6 (cos, - +, cos/+ sin/+ ' +sin, - +, ' cos/+ sin/+ + sin/cos3 - +,+ + ( 'cos, - +,cos3 - +,+ + sin, 0 +,sino ,P]=0. (30) The otained resuts aow to determine reations etween dimensions of inks of the spatia five-ar mechanism for which optima vaue of the ange of transmission wi e arithmetica mean of its extreme vaues, i.e. 7 89: = h +i NU= 7 8< = h i, (3) δ is a certain ange. Sustituting of these vaues in (8) and (9) we wi have: 6 sini = : 6 sini= + 6 8<. Excuding δ we wi otain (33) + 6 = 89: + 8<. (34) Thus if dimensions of inks of the spatia five-ar mechanism satisfy condition (34), then deviations of the ange of transmission γ from optima vaue 7 = j wi e identica in oth sides..3. Conditions of Existence of Two Cranks in Spatia Five-Bar Mechanisms At soution of numerous proems of synthesis of spatia mechanisms with two degrees of freedom it is very important to seect reations etween engths of the inks aowing one or two inks to reaize fu or partia turning around chosen points. It is known that condition of existence of cranks in panar and spherica four-ar mechanisms was first formuated y F. Grasgof. The simiar proems were studied y N.G. Bruevich, V.V. orovoski, F. Freidenstein, F. uditsa and others. For spatia four-ar mechanisms conditions of existence of one of two cranks was first formuated y.s. Tavkheidze. By numerous researches into various hinged mechanisms y N.S. avitashvii were formuated theorems of existience of cranks in spherica five-ar, six-ar and seven-ar mechanisms. By studies of structure and kinematics of five-ar mechanisms with two degrees of freedom is ascertained that conditions of turning of input inks are significanty infuenced y dimensions of frame 1 and inks and 5 (Fig. 1), gear ratio u 5 etween input inks considering their directions of movement, initia positions of input inks specified y anges α 0 and β 0 and duration of the mechanism movement cyce. For spatia five-ar mechanism (Fig. 1) we have otained formua (1) for cacuation of variae distance etween movae hinges B and, whose extreme vaues max and min are found on the ase of satisfaction of conditions (15), (16). The found extreme vaues max and min of distance aow us to write inequaities defining conditions of existence of cranks and 5according to the kinematica scheme of spatia five-ar mechanism: 89: + 6 8< 6. (35) Thus we can formuate a theorem of existence of two cranks

6 109 Nodar avitashvii and Otar Geashvii: On Some Proems of Synthesis of Spatia Five-Bar Hinged Mechanisms with Two egrees of Freedom in spatia five-ar hinged mechanisms as foows. In spatia five-ar hinged mechanisms two inks, adjoining to the frame, wi e cranks if and ony if at movement of the mechanism maximum distance etween the hinges created y connection of input inks and corresponding coupers is ess or equa to the sum of engths of coupers and minimum distance is more or equa to the difference of these engths. If the assume that α0=β0=0 and 5=0 the spatia five-ar mechanism ABSE (Fig. 1) wi e converted into spatia four-ar mechanism ABC (Fig. ). ( + + cos, + sin, n + 6 ( + + cos, + sin, n Concusion (41) By accompished researches into five-ar mechanisms with two degrees of freedom are marked out some proems of synthesis of the mentioned mechanisms. For the purpose of ensuring operation of the mechanism without seizure with maximum possie efficiency are determined dimensions of the inks firsty considering a given ange of transmission and then depending on the dimensions of inks of the spatia five-ar mechanism are cacuated imits of variation of the ange of transmission. A theorem of existence of two cranks in spatia five-ar hinged mechanisms is formuated. The otained resuts are suitae for designing new mechanisms and soution of practica proems. Figure. On the conditions of existence of cranks in a spatia four-ar mechanism. In this case variae distance according to expression (1) wi e: =% '+ + (cos, cos/+ sin/ ' + '+ ' sin, cos/+ sin/4 n. (36) The equation for finding α wi e written as: (cos, cos/+ sin/ ' ' sin, cos/+ sin/=0. (37) Accordingy vaue of α wi e found y formua cos,, =± X d = cos/+ sin/ = cos/+ sin/., (38) Taking into account the vaues of α 1 and α from expression (36) we wi have: 89: =( + + ' cos, '+ + ' sin, n, (39) 8< =( + + ' cos, '+ + ' sin, n. (40) Accordingy to expressions (35) conditions of existence of cranks in the spatia four-ar mechanism wi e: References [1] G. Eason, B. Noe, and I. N. Sneddon, On certain integras of Lipschitz-Hanke type invoving products of Besse functions, Phi. Trans. Roy. Soc. London, vo. A47, pp , Apri (references) [] J. Cerk Maxwe, A Treatise on Eectricity and Magnetism, 3rd ed., vo.. Oxford: Carendon, 189, pp [3] A. G. Ovakimov, Task on positions of spatia mechanisms with severa degree of freedom and its soution y cosed vector contour method in Mechanics of Machines, issue 9-3, Moscow: Nauka, 1971, pp (In Russian). [4] J. uffy, H.Y. Hai-Oahi, A dispacement anaysis of spatia five-ink BR-C mechanism. 1. On the cousers of the RCRCR mechanism in Journa of Mechanics, vo. 5, 3, 1971, pp [5] J. uffy, A derivation of dua dispacement equations for five-size-and seven-ink spatia mechanism using spherica trigonometry. 3. eviation of dua equations for seven-ink spatia mechanism s Rev. roum. sci. techn. Scr. mech. app. vo. 17, 197,, pp [6] N.S. avitashvii, Infuence of parameters of five-ar hinged mechanism on trajectory of couper s points, Transactions of Academy of Sciences of GSSR, vo. 86, 1977,, pp , (In Russian). [7] N.S. avitashvii, Issues of kinematics and precision of five-ar hinged mechanism Fifth Word congress on Theory of Machines and Mechanisms, vo. 1, 1979, Canada, Motrea, Juy 8-13, pp [8] N.S. avitashvii, Fundamentas of the theory of synthesis, anaysis and precision of inkage-ever mechanisms, Tiisi: Technica University, p. (In Russian). [9] N.S. avitashvii, Theoretica fundamentas of error and precision of hinged mechanisms with two degrees of freedom, Tiisi: Metsnierea, p. (In Russian).

7 Internationa Journa of Mechanica Engineering and Appications 014 (6): [10] N.S. avitashvii, ynamic investigation of pane five-ink hinged mechanism with two degrees of freedom,tiisi: Georgian Committee of IFToMM, p. (In Russian). [11] N. avitashvii, O. Geashvii, Synthesis of a spatia five-ink mechanism with two degrees of freedom according to the given aws of Motion, in Proceedings of EUCOMES 08, the second European Congress on Mechanism Science, Springer, pp

Legendre Polynomials - Lecture 8

Legendre Polynomials - Lecture 8 Legendre Poynomias - Lecture 8 Introduction In spherica coordinates the separation of variabes for the function of the poar ange resuts in Legendre s equation when the soution is independent of the azimutha

More information

Dynamics of Planar Five-Link Hinged RRRRT Type Mechanism with Two Degrees of Freedom

Dynamics of Planar Five-Link Hinged RRRRT Type Mechanism with Two Degrees of Freedom International ournal of Mechanical Engineering and Applications 2017; 5(2): 87-94 http://www.sciencepublishinggroup.com/j/ijmea doi: 10.11648/j.ijmea.20170502.13 ISSN: 2330-023X (Print); ISSN: 2330-0248

More information

DYNAMIC RESPONSE OF CIRCULAR FOOTINGS ON SATURATED POROELASTIC HALFSPACE

DYNAMIC RESPONSE OF CIRCULAR FOOTINGS ON SATURATED POROELASTIC HALFSPACE 3 th Word Conference on Earthquake Engineering Vancouver, B.C., Canada August -6, 4 Paper No. 38 DYNAMIC RESPONSE OF CIRCULAR FOOTINGS ON SATURATED POROELASTIC HALFSPACE Bo JIN SUMMARY The dynamic responses

More information

DISTRIBUTION OF TEMPERATURE IN A SPATIALLY ONE- DIMENSIONAL OBJECT AS A RESULT OF THE ACTIVE POINT SOURCE

DISTRIBUTION OF TEMPERATURE IN A SPATIALLY ONE- DIMENSIONAL OBJECT AS A RESULT OF THE ACTIVE POINT SOURCE DISTRIBUTION OF TEMPERATURE IN A SPATIALLY ONE- DIMENSIONAL OBJECT AS A RESULT OF THE ACTIVE POINT SOURCE Yury Iyushin and Anton Mokeev Saint-Petersburg Mining University, Vasiievsky Isand, 1 st ine, Saint-Petersburg,

More information

Technical Data for Profiles. Groove position, external dimensions and modular dimensions

Technical Data for Profiles. Groove position, external dimensions and modular dimensions Technica Data for Profies Extruded Profie Symbo A Mg Si 0.5 F 25 Materia number.206.72 Status: artificiay aged Mechanica vaues (appy ony in pressing direction) Tensie strength Rm min. 245 N/mm 2 Yied point

More information

Implemental Formulation of Newton Dynamics for Free Insect Flight

Implemental Formulation of Newton Dynamics for Free Insect Flight Impementa Formuation of Neton Dynamics for Free Insect Fight Sheng Xu Department of Mathematics, Southern Methodist University, Daas, TX 75275-156, USA Astract A free-fying insect fies and maneuvers y

More information

International Journal of Mass Spectrometry

International Journal of Mass Spectrometry Internationa Journa of Mass Spectrometry 280 (2009) 179 183 Contents ists avaiabe at ScienceDirect Internationa Journa of Mass Spectrometry journa homepage: www.esevier.com/ocate/ijms Stark mixing by ion-rydberg

More information

Module 22: Simple Harmonic Oscillation and Torque

Module 22: Simple Harmonic Oscillation and Torque Modue : Simpe Harmonic Osciation and Torque.1 Introduction We have aready used Newton s Second Law or Conservation of Energy to anayze systems ike the boc-spring system that osciate. We sha now use torque

More information

Related Topics Maxwell s equations, electrical eddy field, magnetic field of coils, coil, magnetic flux, induced voltage

Related Topics Maxwell s equations, electrical eddy field, magnetic field of coils, coil, magnetic flux, induced voltage Magnetic induction TEP Reated Topics Maxwe s equations, eectrica eddy fied, magnetic fied of cois, coi, magnetic fux, induced votage Principe A magnetic fied of variabe frequency and varying strength is

More information

Nonlinear Analysis of Spatial Trusses

Nonlinear Analysis of Spatial Trusses Noninear Anaysis of Spatia Trusses João Barrigó October 14 Abstract The present work addresses the noninear behavior of space trusses A formuation for geometrica noninear anaysis is presented, which incudes

More information

1. Measurements and error calculus

1. Measurements and error calculus EV 1 Measurements and error cacuus 11 Introduction The goa of this aboratory course is to introduce the notions of carrying out an experiment, acquiring and writing up the data, and finay anayzing the

More information

Solution of Wave Equation by the Method of Separation of Variables Using the Foss Tools Maxima

Solution of Wave Equation by the Method of Separation of Variables Using the Foss Tools Maxima Internationa Journa of Pure and Appied Mathematics Voume 117 No. 14 2017, 167-174 ISSN: 1311-8080 (printed version); ISSN: 1314-3395 (on-ine version) ur: http://www.ijpam.eu Specia Issue ijpam.eu Soution

More information

Vibrations of beams with a variable cross-section fixed on rotational rigid disks

Vibrations of beams with a variable cross-section fixed on rotational rigid disks 1(13) 39 57 Vibrations of beams with a variabe cross-section fixed on rotationa rigid disks Abstract The work is focused on the probem of vibrating beams with a variabe cross-section fixed on a rotationa

More information

Modal analysis of a multi-blade system undergoing rotational motion

Modal analysis of a multi-blade system undergoing rotational motion Journa of Mechanica Science and Technoogy 3 (9) 5~58 Journa of Mechanica Science and Technoogy www.springerin.com/content/738-494x DOI.7/s6-9-43-3 Moda anaysis of a muti-bade system undergoing rotationa

More information

IMA Preprint Series # 2323

IMA Preprint Series # 2323 A MATRIX FORMULATION OF THE NEWTON DYNAMICS FOR THE FREE FLIGHT OF AN INSECT By Sheng Xu IMA Preprint Series # 2323 ( June 21 ) INSTITUTE FOR MATHEMATICS AND ITS APPLICATIONS UNIVERSITY OF MINNESOTA 4

More information

Lobontiu: System Dynamics for Engineering Students Website Chapter 3 1. z b z

Lobontiu: System Dynamics for Engineering Students Website Chapter 3 1. z b z Chapter W3 Mechanica Systems II Introduction This companion website chapter anayzes the foowing topics in connection to the printed-book Chapter 3: Lumped-parameter inertia fractions of basic compiant

More information

Physics 505 Fall 2007 Homework Assignment #5 Solutions. Textbook problems: Ch. 3: 3.13, 3.17, 3.26, 3.27

Physics 505 Fall 2007 Homework Assignment #5 Solutions. Textbook problems: Ch. 3: 3.13, 3.17, 3.26, 3.27 Physics 55 Fa 7 Homework Assignment #5 Soutions Textook proems: Ch. 3: 3.3, 3.7, 3.6, 3.7 3.3 Sove for the potentia in Proem 3., using the appropriate Green function otained in the text, and verify that

More information

THE THREE POINT STEINER PROBLEM ON THE FLAT TORUS: THE MINIMAL LUNE CASE

THE THREE POINT STEINER PROBLEM ON THE FLAT TORUS: THE MINIMAL LUNE CASE THE THREE POINT STEINER PROBLEM ON THE FLAT TORUS: THE MINIMAL LUNE CASE KATIE L. MAY AND MELISSA A. MITCHELL Abstract. We show how to identify the minima path network connecting three fixed points on

More information

Simplified analysis of EXAFS data and determination of bond lengths

Simplified analysis of EXAFS data and determination of bond lengths Indian Journa of Pure & Appied Physics Vo. 49, January 0, pp. 5-9 Simpified anaysis of EXAFS data and determination of bond engths A Mishra, N Parsai & B D Shrivastava * Schoo of Physics, Devi Ahiya University,

More information

Identification of macro and micro parameters in solidification model

Identification of macro and micro parameters in solidification model BULLETIN OF THE POLISH ACADEMY OF SCIENCES TECHNICAL SCIENCES Vo. 55, No. 1, 27 Identification of macro and micro parameters in soidification mode B. MOCHNACKI 1 and E. MAJCHRZAK 2,1 1 Czestochowa University

More information

SEA Subsystem Attribute Correction Based on Stiffness Multipliers

SEA Subsystem Attribute Correction Based on Stiffness Multipliers Internationa Conference on Eectrica, Mechanica and Industria Engineering (ICEMIE 016) SEA Subsystem Attribute Correction Based on Stiffness Mutipiers Jie Gao1,* and Yong Yang 1 Coege of hysics and Information

More information

Gauss Law. 2. Gauss s Law: connects charge and field 3. Applications of Gauss s Law

Gauss Law. 2. Gauss s Law: connects charge and field 3. Applications of Gauss s Law Gauss Law 1. Review on 1) Couomb s Law (charge and force) 2) Eectric Fied (fied and force) 2. Gauss s Law: connects charge and fied 3. Appications of Gauss s Law Couomb s Law and Eectric Fied Couomb s

More information

STABILITY OF A PARAMETRICALLY EXCITED DAMPED INVERTED PENDULUM 1. INTRODUCTION

STABILITY OF A PARAMETRICALLY EXCITED DAMPED INVERTED PENDULUM 1. INTRODUCTION Journa of Sound and Vibration (996) 98(5), 643 65 STABILITY OF A PARAMETRICALLY EXCITED DAMPED INVERTED PENDULUM G. ERDOS AND T. SINGH Department of Mechanica and Aerospace Engineering, SUNY at Buffao,

More information

CFD MODELLING OF DIRECT CONTACT STEAM INJECTION

CFD MODELLING OF DIRECT CONTACT STEAM INJECTION Fifth Internationa Conference on CFD in the Process Industries CSIRO, Meourne, Austraia 13-15 Decemer 006 CFD MODELLING OF DIRECT CONTACT STEAM INJECTION Curtis MARSH 1 and Denis WITHERS 1 CFD Design &

More information

Spring Gravity Compensation Using the Noncircular Pulley and Cable For the Less-Spring Design

Spring Gravity Compensation Using the Noncircular Pulley and Cable For the Less-Spring Design The 14th IFToMM Word Congress, Taipei, Taiwan, October 25-30, 2015 DOI Number: 10.6567/IFToMM.14TH.WC.PS3.010 Spring Gravity Compensation Using the Noncircuar Puey and Cabe For the Less-Spring Design M.C.

More information

Numerical simulation of javelin best throwing angle based on biomechanical model

Numerical simulation of javelin best throwing angle based on biomechanical model ISSN : 0974-7435 Voume 8 Issue 8 Numerica simuation of javein best throwing ange based on biomechanica mode Xia Zeng*, Xiongwei Zuo Department of Physica Education, Changsha Medica University, Changsha

More information

Theory of Generalized k-difference Operator and Its Application in Number Theory

Theory of Generalized k-difference Operator and Its Application in Number Theory Internationa Journa of Mathematica Anaysis Vo. 9, 2015, no. 19, 955-964 HIKARI Ltd, www.m-hiari.com http://dx.doi.org/10.12988/ijma.2015.5389 Theory of Generaized -Difference Operator and Its Appication

More information

Lecture 6: Moderately Large Deflection Theory of Beams

Lecture 6: Moderately Large Deflection Theory of Beams Structura Mechanics 2.8 Lecture 6 Semester Yr Lecture 6: Moderatey Large Defection Theory of Beams 6.1 Genera Formuation Compare to the cassica theory of beams with infinitesima deformation, the moderatey

More information

$, (2.1) n="# #. (2.2)

$, (2.1) n=# #. (2.2) Chapter. Eectrostatic II Notes: Most of the materia presented in this chapter is taken from Jackson, Chap.,, and 4, and Di Bartoo, Chap... Mathematica Considerations.. The Fourier series and the Fourier

More information

The Binary Space Partitioning-Tree Process Supplementary Material

The Binary Space Partitioning-Tree Process Supplementary Material The inary Space Partitioning-Tree Process Suppementary Materia Xuhui Fan in Li Scott. Sisson Schoo of omputer Science Fudan University ibin@fudan.edu.cn Schoo of Mathematics and Statistics University of

More information

RELUCTANCE The resistance of a material to the flow of charge (current) is determined for electric circuits by the equation

RELUCTANCE The resistance of a material to the flow of charge (current) is determined for electric circuits by the equation INTRODUCTION Magnetism pays an integra part in amost every eectrica device used today in industry, research, or the home. Generators, motors, transformers, circuit breakers, teevisions, computers, tape

More information

Physics 235 Chapter 8. Chapter 8 Central-Force Motion

Physics 235 Chapter 8. Chapter 8 Central-Force Motion Physics 35 Chapter 8 Chapter 8 Centra-Force Motion In this Chapter we wi use the theory we have discussed in Chapter 6 and 7 and appy it to very important probems in physics, in which we study the motion

More information

PHYSICS LOCUS / / d dt. ( vi) mass, m moment of inertia, I. ( ix) linear momentum, p Angular momentum, l p mv l I

PHYSICS LOCUS / / d dt. ( vi) mass, m moment of inertia, I. ( ix) linear momentum, p Angular momentum, l p mv l I 6 n terms of moment of inertia, equation (7.8) can be written as The vector form of the above equation is...(7.9 a)...(7.9 b) The anguar acceeration produced is aong the direction of appied externa torque.

More information

12.2. Maxima and Minima. Introduction. Prerequisites. Learning Outcomes

12.2. Maxima and Minima. Introduction. Prerequisites. Learning Outcomes Maima and Minima 1. Introduction In this Section we anayse curves in the oca neighbourhood of a stationary point and, from this anaysis, deduce necessary conditions satisfied by oca maima and oca minima.

More information

Combining reaction kinetics to the multi-phase Gibbs energy calculation

Combining reaction kinetics to the multi-phase Gibbs energy calculation 7 th European Symposium on Computer Aided Process Engineering ESCAPE7 V. Pesu and P.S. Agachi (Editors) 2007 Esevier B.V. A rights reserved. Combining reaction inetics to the muti-phase Gibbs energy cacuation

More information

THE OUT-OF-PLANE BEHAVIOUR OF SPREAD-TOW FABRICS

THE OUT-OF-PLANE BEHAVIOUR OF SPREAD-TOW FABRICS ECCM6-6 TH EUROPEAN CONFERENCE ON COMPOSITE MATERIALS, Sevie, Spain, -6 June 04 THE OUT-OF-PLANE BEHAVIOUR OF SPREAD-TOW FABRICS M. Wysocki a,b*, M. Szpieg a, P. Heström a and F. Ohsson c a Swerea SICOMP

More information

Adjustment of automatic control systems of production facilities at coal processing plants using multivariant physico- mathematical models

Adjustment of automatic control systems of production facilities at coal processing plants using multivariant physico- mathematical models IO Conference Series: Earth and Environmenta Science AER OEN ACCESS Adjustment of automatic contro systems of production faciities at coa processing pants using mutivariant physico- mathematica modes To

More information

High-order approximations to the Mie series for electromagnetic scattering in three dimensions

High-order approximations to the Mie series for electromagnetic scattering in three dimensions Proceedings of the 9th WSEAS Internationa Conference on Appied Mathematics Istanbu Turkey May 27-29 2006 (pp199-204) High-order approximations to the Mie series for eectromagnetic scattering in three dimensions

More information

XI PHYSICS. M. Affan Khan LECTURER PHYSICS, AKHSS, K. https://promotephysics.wordpress.com

XI PHYSICS. M. Affan Khan LECTURER PHYSICS, AKHSS, K. https://promotephysics.wordpress.com XI PHYSICS M. Affan Khan LECTURER PHYSICS, AKHSS, K affan_414@ive.com https://promotephysics.wordpress.com [TORQUE, ANGULAR MOMENTUM & EQUILIBRIUM] CHAPTER NO. 5 Okay here we are going to discuss Rotationa

More information

Mathematical Scheme Comparing of. the Three-Level Economical Systems

Mathematical Scheme Comparing of. the Three-Level Economical Systems Appied Mathematica Sciences, Vo. 11, 2017, no. 15, 703-709 IKAI td, www.m-hikari.com https://doi.org/10.12988/ams.2017.7252 Mathematica Scheme Comparing of the Three-eve Economica Systems S.M. Brykaov

More information

Proceedings of Meetings on Acoustics

Proceedings of Meetings on Acoustics Proceedings of Meetings on Acoustics Voume 9, 23 http://acousticasociety.org/ ICA 23 Montrea Montrea, Canada 2-7 June 23 Architectura Acoustics Session 4pAAa: Room Acoustics Computer Simuation II 4pAAa9.

More information

HYDROGEN ATOM SELECTION RULES TRANSITION RATES

HYDROGEN ATOM SELECTION RULES TRANSITION RATES DOING PHYSICS WITH MATLAB QUANTUM PHYSICS Ian Cooper Schoo of Physics, University of Sydney ian.cooper@sydney.edu.au HYDROGEN ATOM SELECTION RULES TRANSITION RATES DOWNLOAD DIRECTORY FOR MATLAB SCRIPTS

More information

The Mechanical Properties Analysis of Machine Tool Spindle After Remanufacturing Based on Uncertain Constraints

The Mechanical Properties Analysis of Machine Tool Spindle After Remanufacturing Based on Uncertain Constraints Send Orders for Reprints to reprints@benthamscience.ae 150 The Open Mechanica Engineering Journa, 2015, 9, 150-155 Open Access The Mechanica Properties Anaysis of Machine Too Spinde After Remanufacturing

More information

2M2. Fourier Series Prof Bill Lionheart

2M2. Fourier Series Prof Bill Lionheart M. Fourier Series Prof Bi Lionheart 1. The Fourier series of the periodic function f(x) with period has the form f(x) = a 0 + ( a n cos πnx + b n sin πnx ). Here the rea numbers a n, b n are caed the Fourier

More information

The influence of temperature of photovoltaic modules on performance of solar power plant

The influence of temperature of photovoltaic modules on performance of solar power plant IOSR Journa of Engineering (IOSRJEN) ISSN (e): 2250-3021, ISSN (p): 2278-8719 Vo. 05, Issue 04 (Apri. 2015), V1 PP 09-15 www.iosrjen.org The infuence of temperature of photovotaic modues on performance

More information

OSCILLATIONS OF PARTIALLY FILLED TANKER TRUCK AT ITS BRAKING

OSCILLATIONS OF PARTIALLY FILLED TANKER TRUCK AT ITS BRAKING ENGINEERING FOR RURAL DEVELOPMENT Jegava, 5.-7.05.06. OSCILLATIONS OF PARTIALLY FILLED TANKER TRUCK AT ITS BRAKING Aexandr Shimanovsky Bearusian State University of Transport tm.esut@gmai.com Astract.

More information

c 2007 Society for Industrial and Applied Mathematics

c 2007 Society for Industrial and Applied Mathematics SIAM REVIEW Vo. 49,No. 1,pp. 111 1 c 7 Society for Industria and Appied Mathematics Domino Waves C. J. Efthimiou M. D. Johnson Abstract. Motivated by a proposa of Daykin [Probem 71-19*, SIAM Rev., 13 (1971),

More information

Candidate Number. General Certificate of Education Advanced Level Examination January 2012

Candidate Number. General Certificate of Education Advanced Level Examination January 2012 entre Number andidate Number Surname Other Names andidate Signature Genera ertificate of Education dvanced Leve Examination January 212 Physics PHY4/1 Unit 4 Fieds and Further Mechanics Section Tuesday

More information

On a geometrical approach in contact mechanics

On a geometrical approach in contact mechanics Institut für Mechanik On a geometrica approach in contact mechanics Aexander Konyukhov, Kar Schweizerhof Universität Karsruhe, Institut für Mechanik Institut für Mechanik Kaiserstr. 12, Geb. 20.30 76128

More information

General Certificate of Education Advanced Level Examination June 2010

General Certificate of Education Advanced Level Examination June 2010 Genera Certificate of Education Advanced Leve Examination June 2010 Human Bioogy HBI6T/P10/task Unit 6T A2 Investigative Skis Assignment Task Sheet The effect of temperature on the rate of photosynthesis

More information

Published in: Proceedings of the Twenty Second Nordic Seminar on Computational Mechanics

Published in: Proceedings of the Twenty Second Nordic Seminar on Computational Mechanics Aaborg Universitet An Efficient Formuation of the Easto-pastic Constitutive Matrix on Yied Surface Corners Causen, Johan Christian; Andersen, Lars Vabbersgaard; Damkide, Lars Pubished in: Proceedings of

More information

D. Prémel, J.M. Decitre and G. Pichenot. CEA, LIST, F Gif-sur-Yvette, France

D. Prémel, J.M. Decitre and G. Pichenot. CEA, LIST, F Gif-sur-Yvette, France SIMULATION OF EDDY CURRENT INSPECTION INCLUDING MAGNETIC FIELD SENSOR SUCH AS A GIANT MAGNETO-RESISTANCE OVER PLANAR STRATIFIED MEDIA COMPONENTS WITH EMBEDDED FLAWS D. Préme, J.M. Decitre and G. Pichenot

More information

A simple reliability block diagram method for safety integrity verification

A simple reliability block diagram method for safety integrity verification Reiabiity Engineering and System Safety 92 (2007) 1267 1273 www.esevier.com/ocate/ress A simpe reiabiity bock diagram method for safety integrity verification Haitao Guo, Xianhui Yang epartment of Automation,

More information

Research of Data Fusion Method of Multi-Sensor Based on Correlation Coefficient of Confidence Distance

Research of Data Fusion Method of Multi-Sensor Based on Correlation Coefficient of Confidence Distance Send Orders for Reprints to reprints@benthamscience.ae 340 The Open Cybernetics & Systemics Journa, 015, 9, 340-344 Open Access Research of Data Fusion Method of Muti-Sensor Based on Correation Coefficient

More information

The Hydrogen Atomic Model Based on the Electromagnetic Standing Waves and the Periodic Classification of the Elements

The Hydrogen Atomic Model Based on the Electromagnetic Standing Waves and the Periodic Classification of the Elements Appied Physics Research; Vo. 4, No. 3; 0 ISSN 96-9639 -ISSN 96-9647 Pubished by Canadian Center of Science and ducation The Hydrogen Atomic Mode Based on the ectromagnetic Standing Waves and the Periodic

More information

A Simple and Efficient Algorithm of 3-D Single-Source Localization with Uniform Cross Array Bing Xue 1 2 a) * Guangyou Fang 1 2 b and Yicai Ji 1 2 c)

A Simple and Efficient Algorithm of 3-D Single-Source Localization with Uniform Cross Array Bing Xue 1 2 a) * Guangyou Fang 1 2 b and Yicai Ji 1 2 c) A Simpe Efficient Agorithm of 3-D Singe-Source Locaization with Uniform Cross Array Bing Xue a * Guangyou Fang b Yicai Ji c Key Laboratory of Eectromagnetic Radiation Sensing Technoogy, Institute of Eectronics,

More information

Separation of Variables and a Spherical Shell with Surface Charge

Separation of Variables and a Spherical Shell with Surface Charge Separation of Variabes and a Spherica She with Surface Charge In cass we worked out the eectrostatic potentia due to a spherica she of radius R with a surface charge density σθ = σ cos θ. This cacuation

More information

Self Inductance of a Solenoid with a Permanent-Magnet Core

Self Inductance of a Solenoid with a Permanent-Magnet Core 1 Probem Sef Inductance of a Soenoid with a Permanent-Magnet Core Kirk T. McDonad Joseph Henry Laboratories, Princeton University, Princeton, NJ 08544 (March 3, 2013; updated October 19, 2018) Deduce the

More information

First-Order Corrections to Gutzwiller s Trace Formula for Systems with Discrete Symmetries

First-Order Corrections to Gutzwiller s Trace Formula for Systems with Discrete Symmetries c 26 Noninear Phenomena in Compex Systems First-Order Corrections to Gutzwier s Trace Formua for Systems with Discrete Symmetries Hoger Cartarius, Jörg Main, and Günter Wunner Institut für Theoretische

More information

Reliability: Theory & Applications No.3, September 2006

Reliability: Theory & Applications No.3, September 2006 REDUNDANCY AND RENEWAL OF SERVERS IN OPENED QUEUING NETWORKS G. Sh. Tsitsiashvii M.A. Osipova Vadivosto, Russia 1 An opened queuing networ with a redundancy and a renewa of servers is considered. To cacuate

More information

1D Heat Propagation Problems

1D Heat Propagation Problems Chapter 1 1D Heat Propagation Probems If the ambient space of the heat conduction has ony one dimension, the Fourier equation reduces to the foowing for an homogeneous body cρ T t = T λ 2 + Q, 1.1) x2

More information

Work and energy method. Exercise 1 : Beam with a couple. Exercise 1 : Non-linear loaddisplacement. Exercise 2 : Horizontally loaded frame

Work and energy method. Exercise 1 : Beam with a couple. Exercise 1 : Non-linear loaddisplacement. Exercise 2 : Horizontally loaded frame Work and energy method EI EI T x-axis Exercise 1 : Beam with a coupe Determine the rotation at the right support of the construction dispayed on the right, caused by the coupe T using Castigiano s nd theorem.

More information

Approximated MLC shape matrix decomposition with interleaf collision constraint

Approximated MLC shape matrix decomposition with interleaf collision constraint Agorithmic Operations Research Vo.4 (29) 49 57 Approximated MLC shape matrix decomposition with intereaf coision constraint Antje Kiese and Thomas Kainowski Institut für Mathematik, Universität Rostock,

More information

LECTURE 10. The world of pendula

LECTURE 10. The world of pendula LECTURE 0 The word of pendua For the next few ectures we are going to ook at the word of the pane penduum (Figure 0.). In a previous probem set we showed that we coud use the Euer- Lagrange method to derive

More information

Gaussian Curvature in a p-orbital, Hydrogen-like Atoms

Gaussian Curvature in a p-orbital, Hydrogen-like Atoms Advanced Studies in Theoretica Physics Vo. 9, 015, no. 6, 81-85 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.1988/astp.015.5115 Gaussian Curvature in a p-orbita, Hydrogen-ike Atoms Sandro-Jose Berrio-Guzman

More information

Homotopy Perturbation Method for Solving Partial Differential Equations of Fractional Order

Homotopy Perturbation Method for Solving Partial Differential Equations of Fractional Order Int Journa of Math Anaysis, Vo 6, 2012, no 49, 2431-2448 Homotopy Perturbation Method for Soving Partia Differentia Equations of Fractiona Order A A Hemeda Department of Mathematics, Facuty of Science

More information

Path planning with PH G2 splines in R2

Path planning with PH G2 splines in R2 Path panning with PH G2 spines in R2 Laurent Gajny, Richard Béarée, Eric Nyiri, Oivier Gibaru To cite this version: Laurent Gajny, Richard Béarée, Eric Nyiri, Oivier Gibaru. Path panning with PH G2 spines

More information

General Certificate of Education Advanced Level Examination June 2010

General Certificate of Education Advanced Level Examination June 2010 Genera Certificate of Education Advanced Leve Examination June 2010 Human Bioogy HBI6T/Q10/task Unit 6T A2 Investigative Skis Assignment Task Sheet The effect of using one or two eyes on the perception

More information

A Fictitious Time Integration Method for a One-Dimensional Hyperbolic Boundary Value Problem

A Fictitious Time Integration Method for a One-Dimensional Hyperbolic Boundary Value Problem Journa o mathematics and computer science 14 (15) 87-96 A Fictitious ime Integration Method or a One-Dimensiona Hyperboic Boundary Vaue Probem Mir Saad Hashemi 1,*, Maryam Sariri 1 1 Department o Mathematics,

More information

Parallel-Axis Theorem

Parallel-Axis Theorem Parae-Axis Theorem In the previous exampes, the axis of rotation coincided with the axis of symmetry of the object For an arbitrary axis, the paraeaxis theorem often simpifies cacuations The theorem states

More information

Dual Integral Equations and Singular Integral. Equations for Helmholtz Equation

Dual Integral Equations and Singular Integral. Equations for Helmholtz Equation Int.. Contemp. Math. Sciences, Vo. 4, 9, no. 34, 1695-1699 Dua Integra Equations and Singuar Integra Equations for Hemhotz Equation Naser A. Hoshan Department of Mathematics TafiaTechnica University P.O.

More information

Ultrasonic Measurements of Kinematic Viscosity for Analize of Engine Oil Parameters

Ultrasonic Measurements of Kinematic Viscosity for Analize of Engine Oil Parameters th European Conference on Non-Destructive Testing (ECNDT 04), October 6-0, 04, Prague, Czech Repubic More Info at Open Access Database www.ndt.net/?id=6344 Utrasonic Measurements of Kinematic Viscosity

More information

2.1. Cantilever The Hooke's law

2.1. Cantilever The Hooke's law .1. Cantiever.1.1 The Hooke's aw The cantiever is the most common sensor of the force interaction in atomic force microscopy. The atomic force microscope acquires any information about a surface because

More information

MATH 172: MOTIVATION FOR FOURIER SERIES: SEPARATION OF VARIABLES

MATH 172: MOTIVATION FOR FOURIER SERIES: SEPARATION OF VARIABLES MATH 172: MOTIVATION FOR FOURIER SERIES: SEPARATION OF VARIABLES Separation of variabes is a method to sove certain PDEs which have a warped product structure. First, on R n, a inear PDE of order m is

More information

Volume 13, MAIN ARTICLES

Volume 13, MAIN ARTICLES Voume 13, 2009 1 MAIN ARTICLES THE BASIC BVPs OF THE THEORY OF ELASTIC BINARY MIXTURES FOR A HALF-PLANE WITH CURVILINEAR CUTS Bitsadze L. I. Vekua Institute of Appied Mathematics of Iv. Javakhishvii Tbiisi

More information

STABILITY OF THERMOELASTIC LAYERED COMPOSITE IN AXIAL MOVEMENT

STABILITY OF THERMOELASTIC LAYERED COMPOSITE IN AXIAL MOVEMENT 6th European Conference on Computationa Mechanics (ECCM 6) 7th European Conference on Computationa Fuid Dynamics (ECFD 7) 11-15 June 18, Gasgow, UK STABILITY OF THERMOELASTIC LAYERED COMPOSITE IN AXIAL

More information

Science & Technologies COMPARISON OF MASS TRANSFER COEFFICIENTS DETERMINED BY DIFFERENT METHODS IN DISTILLATION COLUMN WITH THREE TRAYS

Science & Technologies COMPARISON OF MASS TRANSFER COEFFICIENTS DETERMINED BY DIFFERENT METHODS IN DISTILLATION COLUMN WITH THREE TRAYS COMPARION OF MA TRANFER COEFFICIENT DETERMINED BY DIFFERENT METHOD IN DITIATION COUMN WITH THREE TRAY Dian Radev, Dorin Georgiev, Desisava Koeva, Mariana Karaivanova Facuty of Technica ciences, Prof. D-r.

More information

FOURIER SERIES ON ANY INTERVAL

FOURIER SERIES ON ANY INTERVAL FOURIER SERIES ON ANY INTERVAL Overview We have spent considerabe time earning how to compute Fourier series for functions that have a period of 2p on the interva (-p,p). We have aso seen how Fourier series

More information

Numerical solution of one dimensional contaminant transport equation with variable coefficient (temporal) by using Haar wavelet

Numerical solution of one dimensional contaminant transport equation with variable coefficient (temporal) by using Haar wavelet Goba Journa of Pure and Appied Mathematics. ISSN 973-1768 Voume 1, Number (16), pp. 183-19 Research India Pubications http://www.ripubication.com Numerica soution of one dimensiona contaminant transport

More information

APPENDIX C FLEXING OF LENGTH BARS

APPENDIX C FLEXING OF LENGTH BARS Fexing of ength bars 83 APPENDIX C FLEXING OF LENGTH BARS C.1 FLEXING OF A LENGTH BAR DUE TO ITS OWN WEIGHT Any object ying in a horizonta pane wi sag under its own weight uness it is infinitey stiff or

More information

CE601-Structura Anaysis I UNIT-IV SOPE-DEFECTION METHOD 1. What are the assumptions made in sope-defection method? (i) Between each pair of the supports the beam section is constant. (ii) The joint in

More information

Experimental Investigation and Numerical Analysis of New Multi-Ribbed Slab Structure

Experimental Investigation and Numerical Analysis of New Multi-Ribbed Slab Structure Experimenta Investigation and Numerica Anaysis of New Muti-Ribbed Sab Structure Jie TIAN Xi an University of Technoogy, China Wei HUANG Xi an University of Architecture & Technoogy, China Junong LU Xi

More information

Function Matching Design of Wide-Band Piezoelectric Ultrasonic Transducer

Function Matching Design of Wide-Band Piezoelectric Ultrasonic Transducer Function Matching Design of Wide-Band Piezoeectric Utrasonic Transducer Yingyuan Fan a, Hongqing An b Weifang Medica University, Weifang, 261053, China a yyfan@126.com, b hongqingan01@126.com Abstract

More information

Two-stage least squares as minimum distance

Two-stage least squares as minimum distance Econometrics Journa (2018), voume 0, pp. 1 9. doi: 10.1111/ectj.12115 Two-stage east squares as minimum distance FRANK WINDMEIJER Department of Economics and IEU, University of Bristo, Priory Road, Bristo,

More information

Forces of Friction. through a viscous medium, there will be a resistance to the motion. and its environment

Forces of Friction. through a viscous medium, there will be a resistance to the motion. and its environment Forces of Friction When an object is in motion on a surface or through a viscous medium, there wi be a resistance to the motion This is due to the interactions between the object and its environment This

More information

An H 2 type Riemannian metric on the space of planar curves

An H 2 type Riemannian metric on the space of planar curves An H 2 type Riemannian metric on the space of panar curves Jayant hah Mathematics Department, Northeastern University, Boston MA emai: shah@neu.edu Abstract An H 2 type metric on the space of panar curves

More information

Explicit Exact Solution of Damage Probability for Multiple Weapons against a Unitary Target

Explicit Exact Solution of Damage Probability for Multiple Weapons against a Unitary Target American Journa of Operations Research, 06, 6, 450-467 http://www.scirp.org/ourna/aor ISSN Onine: 60-8849 ISSN Print: 60-8830 Expicit Exact Soution of Damage Probabiity for utipe Weapons against a Unitary

More information

PHYS 110B - HW #1 Fall 2005, Solutions by David Pace Equations referenced as Eq. # are from Griffiths Problem statements are paraphrased

PHYS 110B - HW #1 Fall 2005, Solutions by David Pace Equations referenced as Eq. # are from Griffiths Problem statements are paraphrased PHYS 110B - HW #1 Fa 2005, Soutions by David Pace Equations referenced as Eq. # are from Griffiths Probem statements are paraphrased [1.] Probem 6.8 from Griffiths A ong cyinder has radius R and a magnetization

More information

Position Control of Rolling Skateboard

Position Control of Rolling Skateboard osition Contro of Roing kateboard Baazs Varszegi enes Takacs Gabor tepan epartment of Appied Mechanics, Budapest University of Technoogy and Economics, Budapest, Hungary (e-mai: varszegi@mm.bme.hu) MTA-BME

More information

Extraction of Astrophysical Cross Sections in the Trojan-Horse Method

Extraction of Astrophysical Cross Sections in the Trojan-Horse Method Few-Body Systems 29, 75±93 (2000) Extraction of Astrophysica Cross Sections in the Trojan-Horse Method S. Type and H. H. Woter Sektion Physik, Universitat Munchen, Am Couomwa 1, D-85748 Garching, Germany

More information

VTU-NPTEL-NMEICT Project

VTU-NPTEL-NMEICT Project MODUE-X -CONTINUOUS SYSTEM : APPROXIMATE METHOD VIBRATION ENGINEERING 14 VTU-NPTE-NMEICT Project Progress Report The Project on Deveopment of Remaining Three Quadrants to NPTE Phase-I under grant in aid

More information

Traffic data collection

Traffic data collection Chapter 32 Traffic data coection 32.1 Overview Unike many other discipines of the engineering, the situations that are interesting to a traffic engineer cannot be reproduced in a aboratory. Even if road

More information

Laboratory Exercise 1: Pendulum Acceleration Measurement and Prediction Laboratory Handout AME 20213: Fundamentals of Measurements and Data Analysis

Laboratory Exercise 1: Pendulum Acceleration Measurement and Prediction Laboratory Handout AME 20213: Fundamentals of Measurements and Data Analysis Laboratory Exercise 1: Penduum Acceeration Measurement and Prediction Laboratory Handout AME 20213: Fundamentas of Measurements and Data Anaysis Prepared by: Danie Van Ness Date exercises to be performed:

More information

Physics 116C Helmholtz s and Laplace s Equations in Spherical Polar Coordinates: Spherical Harmonics and Spherical Bessel Functions

Physics 116C Helmholtz s and Laplace s Equations in Spherical Polar Coordinates: Spherical Harmonics and Spherical Bessel Functions Physics 116C Hemhotz s an Lapace s Equations in Spherica Poar Coorinates: Spherica Harmonics an Spherica Besse Functions Peter Young Date: October 28, 2013) I. HELMHOLTZ S EQUATION As iscusse in cass,

More information

Faculty of Machine Building. Technical University of Cluj Napoca

Faculty of Machine Building. Technical University of Cluj Napoca Facuty of Machine Buiding Technica University of Cuj Napoca CONTRIBUTIONS TO THE CALCULATION AND ANALYSIS OF DYNAMIC ABSORBERS, WITH APPLICATIONS ON BALANCING MECHANICAL SYSTEMS PhD THESIS 11 Scientific

More information

Packet Fragmentation in Wi-Fi Ad Hoc Networks with Correlated Channel Failures

Packet Fragmentation in Wi-Fi Ad Hoc Networks with Correlated Channel Failures Packet Fragmentation in Wi-Fi Ad Hoc Networks with Correated Channe Faiures Andrey Lyakhov Vadimir Vishnevsky Institute for Information Transmission Probems of RAS B. Karetny 19, Moscow, 127994, Russia

More information

Expectation-Maximization for Estimating Parameters for a Mixture of Poissons

Expectation-Maximization for Estimating Parameters for a Mixture of Poissons Expectation-Maximization for Estimating Parameters for a Mixture of Poissons Brandon Maone Department of Computer Science University of Hesini February 18, 2014 Abstract This document derives, in excrutiating

More information

High Efficiency Development of a Reciprocating Compressor by Clarification of Loss Generation in Bearings

High Efficiency Development of a Reciprocating Compressor by Clarification of Loss Generation in Bearings Purdue University Purdue e-pubs Internationa Compressor Engineering Conference Schoo of Mechanica Engineering 2010 High Efficiency Deveopment of a Reciprocating Compressor by Carification of Loss Generation

More information

PhysicsAndMathsTutor.com

PhysicsAndMathsTutor.com . Two points A and B ie on a smooth horizonta tabe with AB = a. One end of a ight eastic spring, of natura ength a and moduus of easticity mg, is attached to A. The other end of the spring is attached

More information

AN INTERACTIVE MODELLING OF WORK CYCLE OF SI GAS ENGINE. Karol Cupiał, Grzegorz Katolik. Technical University of Częstochowa, Poland INTRODUCTION

AN INTERACTIVE MODELLING OF WORK CYCLE OF SI GAS ENGINE. Karol Cupiał, Grzegorz Katolik. Technical University of Częstochowa, Poland INTRODUCTION AN INTERACTIVE MODELLING OF WORK CYCLE OF SI GAS ENGINE Karo Cupiał, Grzegorz Katoik Technica University of Częstochowa, Poand INTRODUCTION Zero-dimensiona mode of heat reease is appied in many modes used

More information