School of Mechanical Engineering and Automation Harbin Institute of Technology Shenzhen Graduate School Shenzhen, Guangdong Province, China
|
|
- Elwin Damon Bryan
- 5 years ago
- Views:
Transcription
1 2016 International Conference on Mechanics Design, Manufacturing and Automation (MDM 2016) ISBN: A New Decoupling Measurement Method of Five-axis Machine ools Geometric Errors Based on Cross Grid Encoder and DBB Zong-Peng WANG 1,a, Jian-Gang LI 2,b,* 1 School of Mechanical Engineering and Automation Harbin Institute of echnolog Shenzhen Graduate School Shenzhen, Guangdong Province, China 2 School of Mechanical Engineering and Automation, Harbin Institute of echnolog, Shenzhen Graduate School, Shenzhen KeLab for AMC&MAE a wang201438@126.com, b jiangang_lee@163.com *Corresponding author Kewords: Cross grid encoder, Double ball bar, Homogeneous coordinate transformation, Position-independent errors, Position-dependent errors. Abstract. In order to obtain all the geometric errors of five-axis CNC machine tool, a measuring strateg with cross grid encoder and double ball-bar (DBB) is proposed. According to the theor of multi-bod sstems, b using the homogeneous coordinate transformation method the model of geometric errors is established. he cross grid encoder is used to detect the translation geometric errors and the DBB is used to measure the rotation ones. Based on the kinematic chain and the properties of geometric errors, the translation geometric errors are measured before the rotation ones. For each axis, both PIGEs (position-independent errors) and PDGEs (position-dependent errors) are under consideration. hen a complete compensated model can be established. Introduction Except for the thermal error, the geometric errors are the most important factors affecting the machining accurac. About the measurement of geometric errors, man researches have been carried out. Most modeling methods are based on multi-bod sstem [1], different kinds of geometric errors can be modeled as matrices and are eas to analsis. In 1992, Soons et al using the modeling method based on rigid bod hpothesis established the comprehensive model including the rotation axes [2]. Kiridena et al established the quasi static errors model of the multi-axis machine tool based on the homogeneous coordinate transformation matrices [3]. Jianguo Yang et al applied the homogeneous coordinate transformation theor to the turning center to analsis the geometric and thermal errors [4]. sutsumi et al designed an deviations identifing methods with three kinds of simultaneous three-axis control motions for each rotar axis [5]. In 2007, Shengi Li summarized the modeling and measurement schemes of translation axes, but the method he used has some unfavorable factors that affecting the error identification [6]. Zargarbashi proposed a method to assess the axis motion errors of a trunnion-tpe A-axis using the magnetic double ball bar (DBB) as the measuring instrument. he method consisted of five DBB tests with a single setup for all of the tests and the exclusive motion of the trunnion axis during data acquisition [7]. Lee designed a series of measurement paths to increase the sensitivit of the geometric errors, and make a clear expiation that the position-dependent and position-independent errors could be modeled as nth-order polnomials and constants [8]. sutsumi et al analzed the measurement using a clindrical coordinate sstem and Cartesian coordinate sstem respectivel, and pointed out the advantages and disadvantages of the two methods [9]. In 2013, Lee et al studied the
2 position-independent geometric errors including the offset errors and squareness errors of rotar axes of a five axis machine tool with double ball bar [10]. And in the same ear, Lee proposed a robust and simple method using double ball-bar to measure position-independent geometric errors of a rotar axis involving single axis control during the measurement [11]. Above all, decoupling is main problem during the identification of the geometric errors. In this stud, a complete measuring strateg is proposed. For each axis, the PIGEs are alwas measured before the PDGEs. According to the kinematic chain, the translation geometric errors are detected and then the rotar ones. he Mathematical Model of Geometric Errors he research object is a five-axis machine tool with RR structural configuration as shown in Fig.1. Figure 1. Five-axis machine tool with a tilting table with two controlled axes. he machine tool can be divided into the cutter chain and the workpiece chain according the kinematic structure. Onl the Z-axis is in the cutter chain, the Y-axis, X-axis, B-axis and C-axis are in the workpiece chain. O X Z Y Z O W X C Z Y O C Y D B X Z O R X Y Figure 2. he coordinate frames of machine tool. Initiall, the coordinate sstem established as shown in Fig.2 below. he reference coordinate frame titled with R, the Y-axis coordinate frame Y, the X-axis one X, the Z-axis one Z and the B-axis one B, and the origins are the position coincides with the ideal intersection of B-axis and C-axis. he origins of C-axis coordinate located on the intersection of C-axis and the turntable, and the distance between the origins of reference coordinate frame is D. he x, and z direction of all coordinate sstems are the ideal direction of X-axis, Y-axis and Y-axis.
3 he ranslation Parts he PIGEs of translations axes are the squareness errors of the three translation axes. And the PDGEs of each axis are the deviations of six degrees of freedom when the axis is moving. he PIGEs are listed in Fig.3, and the X-axis PDGEs are shown as an example in the same figure. z x x d e dz x x ez x ex x d x x x _real _ideal z_ideal z_ideal x z_real xz z_real z x x Figure 3. he PIGEs and PDGEs of translation axes. In Fig.3(1) the dx(x) is the position error, the d(x) and dz(x) are the radial errors, and the ex(x), e(x) and ez(x) are angular errors. he are all depending on the moving distance of X-axis. In Fig.3(2), the three angles express the squareness error of each two translation axes. For the X-axis, Y-axis and Z-axis, the ideal homogeneous transformation matrices are written as Eq.(1). he x, and z means ideal movement distance of X-axis, Y-axis and Z-axis respectivel. he matrix ab_ideal describes the coordinates based on the a-coordinate frame transform to the b-coordinate frame, the subscript x,, z and r corresponding to each coordinate sstem r _ ideal = x = , x _ ideal = z , zr _ ideal (1) As for the PIGEs of translation axes, the transformation matrices are written in Eq.(2). 1 - x 0 0 x r _ PIGE = , 1 0 z xz 0 zr _ PIGE = z xz (2) he matrices express the PDGEs of translation axes are written in Eq.(3). Where, the ex(x) means the angular error around the X-axis when X-axis moving and the dx(x) means the position error in the X-axis direction. According the above principle, the meaning of the other terms can be understood easil.
4 1 -e z() e () d x() e () 1 e () d () z x r _ PDGE =, e () e x() 1 d z() e z(z) e (z) d x(z) e(z) z 1 e(z) z d(z) zr _ PDGE = e (z) e x(z) 1 d z(z) e z(x) e (x) d x(x) e z(x) 1 e z(x) d (x) x _ PDGE = e (x) e x(x) 1 d z(x) (3) he Rotation Parts he PIGEs of one rotar axis consist of two offset errors and two parallelism errors. he PDGEs of rotar axes just like the translation ones. aking C-axis as an example to show the PDGEs in Fig.4(1) and the PIGEs in Fig.4(2). Figure 4. PDGEs and PIGEs of C-axis. he PIGEs can be described in Eq.(4) and the PDGEs in Eq.(5). 1 b 0 xb 1 0 b b bx _ PIGE =, 0 b 1 z b c xc 0 1 c c cb _ PIGE = c c (4) 1 -e z(b) e (b) d x(b) 1 -e z(c) e (c) d x(c) e e z(c) 1 e z(c) d (c) z(b) 1 e z(b) d (b) cb _ PDGE = bx _ PDGE =, e e (c) e x(c) 1 d z(c) (b) e x(b) 1 d z(b) (5) And the ideal motion of B-axis and C-axis can be written as Eq.(6).
5 cos b 0 sin b bx _ ideal = sin b 0 cos b cos c sin c 0 0 sin c cos c 0 0 = , cb _ ideal (6) he Complete Model In the cutter chain of machine tool, the coordinate of the center of cutter in cutter coordinate sstem can be transformed to reference coordinate sstem with Eq.(7). tr zr _ PDGE zr _ PIGE zr _ ideal tz In the workpiece chain of machine tool, the coordinate in the workpiece coordinate sstem can be transformed to reference coordinate sstem with Eq.(8). wr r _ PDGE r _ PIGE r _ ideal x _ PDGE x _ idealbx _ PDGE bx _ PIGE bx _ idealcb _PDGEcb_PIGEcb_idealwc (7) hen, the relationship of the two chains is established under the consideration of all geometric errors. he Measuring Strateg For each axis, PIGEs are alwas having more remarkable influence than PDGEs, so the PIGEs are measured before the PDGEs. Measurement of Geometric Errors of ranslation Axes he cross grid encoder is used during the measurement of translation axes errors. According to the nature of the error and the feature of the instrument, the PIGEs can be measured with the method in Fig.5. he figure describes the squareness error between X-axis and Y-axis, in which the x_ideal and _ideal represent the ideal direction of X-axis and Y-axis, the x_real and the _real represent the real directions. he direction of the real axis is the directions of measuring data since the influence of PDGEs. (8) Figure 5. Measurement of PIGEs in x-plane.
6 Appling the same method in z-plane and the zx-plane the other two PDGE can be obtained. For the PIGEs of each translation axis, the methods are similar. So onl the measurement of X-axis will be described in detail. he PDGEs measurement strateg of X-axis is shown in Fig.6. Choosing three lines in the working space, onl moving the X-axis and measuring the deviation in the x, and z direction through different installation positon. Figure 6. Measurement of the PDGEs of X-axis. he Eq.(9) can be deduced. he deviation in each direction not onl has relationship with PDGEs but also the PIGEs. Now the PIGEs have been detected, so the can be considered to be constants. x d (x) e (x) e (x) z 1 x z 1 1 d (x) e (x) z e (x) x x 1 x 1 z 1 x 1 z d (x) e (x) x e (x) x 1 z 1 x 1 xz 1 x d (x) e (x) e (x) z 2 x z 2 2 d (x) e (x) z e (x) x x 2 x 2 z 2 x 2 z d (x) e (x) x e (x) x 2 z 2 x 2 xz 2 x d (x) e (x) e (x) z 3 x z 3 3 d (x) e (x) z e (x) x x 3 x 3 z 3 x 3 z d (x) e (x) x e (x) x 3 z 3 x 3 xz 3 Since there are onl six PDGEs in each axis, six equations are enough to solve the answer. After integration the Eq.(10) can be obtained. hen in ever position, the PDGEs can be calculated b using Eq.(10). (9) x z1 1d x (x) z1 0 x 1 d(x) x x 1 z x 0 d(x) x z xz 1 x e x(x) x 2 e(x) xx 2 x e(x) z 0 (10)
7 For the translation axes, the decoupling onl reflects in that the PIGEs should be measured before the PDGEs. hen all the geometric errors can be obtained successfull. Measurement of Geometric Errors of Rotar Axes During the measurement of rotar axes, all geometric errors of translation axes have been obtained. So in the equations of rotar axes, the translation errors have been compensated before and been neglected for simplifing. According the order of kinematic chain, the PIGEs of B-axis are measured in the first place. And before the presentation of measurement strateg, some constants should be introduced. First one Dz is the distance between the center of workpiece-ball and the intersection of B-axis with C-axis in the z-direction. he second one D1 is the distance between the center of workpiece-ball and the intersection of C-axis with worktable in the z-direction too. And the last one D=Dz-D1. In this paper, the measurement of B-axis PIGEs designed as shown in Fig.7. For each mode in the measurement strateg, the motion of B-axis should be associated with two translation axes because the structure of the rotar table. he mode (1), (2) and (3) are axial, tangential and radial direction measurement respectivel. (1) (2) (3) Figure 7. Measurement of B-axis PIGEs. B using the kinematic relation between the cutter ball and the workpiece ball, the Eq.(11) can be deduced which establish the relation between the variation of the DBB s length and the PIGEs, in the equation the PDGEs of B-axis are not taken into account but the PIGEs of C-axis are under consideration. he two and above error terms have been neglected in the equations. R (D D ) (D D ) cosb (D D ) sin b 1 c z c z b z b hen for other two modes, the Eq.(12) and Eq.(13) can be derived. R x (D D x ) cosbdsinb 2 b z 1 c c (11) (12) R z ( x D ) sinbdcosb 3 b c 1 c B observing these three equations, the PIGEs of B-axis and C-axis are coupled and reflect in the DBB s length. But b using the least square method, the PIGEs of C-axis do not impact (13)
8 the identification of PIGEs of B-axis. So the four PIGE of B-axis can be identified b the data of DBB. Secondl, the PIGEs of C-axis should be measured. he measurement of C-axis PIGEs is different from the B-axis because onl C-axis motion can be achieved. As shown in Fig.8, during the measurement of C-axis PIGEs the C-axis is controlled to do a circular motion in the different plane with difference in the z-direction. (1) (2) Figure 8. Measurement of C-axis PIGEs. hrough the kinematic relation between the cutter ball and the workpiece ball, the Eq.(14) and Eq.(15) can be derived. In this case, the PIGEs of B-axis influence the identification of C-axis. So b the designed order, the PIGEs of B-axis are detected before and can be regard as constants. R ( x x ) coscsinc 1 c b c R ( x x L ) cosc [ L ( )] sinc 2 c b c c b c he Eq.(14) can identif the two offset errors and the Eq.(15) can obtain the angular error b the least square method. Lastl, the PDGEs should be measured. he measurement of B-axis and C-axis are ver similar, so onl the measurement of C-axis PDGEs will be illustrated. he measurement strateg are designed as shown in Fig.9 (14) (15) (1) (2) (3) Figure 9. Measurement of C-axis PDGEs. According to the kinematic relationship between the two balls, the Eq.(16), (17) and (18) can be deduced, the equations express the relationship between DBB s length and geometric
9 errors in x, and z direction. In the measurement of PDGEs, the PIGEs should be taken into account as the equations shown. R ( x x D ) dcxd ec x b c z c z R [D ( ) ] dc D ecx z b c c z R z dcz z b here are six PDGEs of C-axis, so six equations are needed. hough observation, the Unique coefficient in the equations is just about the fixed position of balls in the z-direction. So just like the measurement strateg in Fig.8, the balls should be raised in the z-direction. As for the limitation of the method, the angle positioning error cannot be obtained. he other five PDGEs can be calculated b the Eq.(19). (16) (17) (18) R x D d(c) z1 x C11 R D d(c) z1 0 C 21 R d(c) z z C 31 R D e(c) C x2 z2 x 12 R D e(c) 2 z2 0 C 22 (19) Where, C 11 ( xb xc D z1c ) C 21 [D z1( b c) c] C31 zb C 12 ( xb xc D z2c ) C 22 [D z2( b c) c]. he last column vector in the Eq. (19) is consists of PIGEs of B-axis and C-axis, the PDGEs and PIGEs are coupled. Since the PIGEs of two rotar axes are measured before, the vector can be regard as constant vector and the PDGEs of C-axis in different angle of rotation can be calculated. hen all the geometric errors of machine tool have been measured in the strateg before except for the angle position error of rotar axis. As the rotar table adapts the absolute encoder, the neglected error in fact also can be ignored. he Simulation and Experiment In this section, the simulation is mainl carried out in the identification of B-axis PIGEs and C-axis PIGEs. he other errors calculated b equations are not simulated. he ab.1 lists some simulation parameters.
10 able 1. he simulation parameters of PIGEs. PIGEs Given value PIGEs Given value b rad x b mm b rad zb mm c rad x c mm c rad c mm In the simulation, the noise of measurement is under consideration. he noise is presumed among ±0.002mm. hrough the simulation of B-axis axial mode b Matlab as shown in Fig.10, the b can be identified as and the b can be identified as he deviation ratios are 6% and 1%. he magnified part can reveal the deviation between ideal path and simulation path clearl. Figure 10. he simulation of axial mode of B-axis PIGEs. Similarl, the measurement of C-axis PIGEs are simulated as shown if Fig.11. Figure 11. he measurement simulation of C-axis PIGEs. he identified value of and are and he deviation are small enough to show that the identification c methods c are effective both B-axis and C-axis. he next part is some of the experimental results. he Fig.12 and Fig.13 show the measured data of translation axes. Figure12. he measurement of squareness between X-axis and Z-axis.
11 In the Fig.12, the (1) shows the measurement of z-direction and the (2) shows the measurement of x-direction. he Fig.13 shows the three lines measurement of X-axis PDGEs. he data sampling interval is chosen 5mm because the screw pitch is 5mm. he PDGEs in ever 5mm can be calculated b using the measuring data and Eq.10. (1) Line1 measurement in x and direction (2) Line1 measurement in z direction (3) Line2 measurement in x and direction (4) Line3 measurement in x direction Figure 13. Measurement of X-axis PDGEs. Conclusion B using the measuring strateg proposed in the paper, not onl the PIGEs but also the PDGEs of ever axis can be measured in the specified measurement order. And most of all, the coupling among the geometric errors of machine tool can be measured in the separated methods. his strateg can be applied to the CNC machine tool in an structure onl making a corresponding change in the kinematic chain. From the simulation as well as the experimental results, the validit of the proposed method was clarified. Acknowledgements his work is financial supported b Shenzhen science and technolog plan projects, Shenzhen Basic research plan (No. JCYJ ).
12 References [1] R.L. Houston, Youwu Liu. Multi-bod sstem dnamics [M]. ianjin: ianjin Universit press,1991. [2] J.A. Soons, F.C.heuws, P.H.Schellenkens. Modeling the errors of muti-axis machine:a generel methodolog [J]. Precision Engineering, 1992, 14(1): [3] V.S.B. Kiridena, P.M. Ferreira. Kinematic modeling of qusistatic errors of three-axis machining centers [J]. International Journal of Machine ools and Manufacture, 1994, 34(1): [4] Jianguo Yang, Zhihong Pan, Binguan Xue. Kinematic modeling of geometric and thermol errors of NC machine tools [J]. Mechanical design and manufacturing. 1998, (5): [5] M. sutsumi, A. Saito. Identification and compensation of sstematic deviations particular to 5-axis machining center [J]. International Journal of Machine ools and Manufacture, 2003, 43(8): [6] Shengi Li. Precision modeling technolog for precision and ultra-precision machine tools. National Unicersit of Defense echnolog press. Beijing, 2007, [7] S.H.H. Zargarbashi, J.R.R. Maer. Assessment of machine tool trunnion axis motion error, using magnetic double ball bar [J]. International Journal of Machine ools and Manufacture, 2006, 46(14): [8] K.I. Lee, D.M. Lee S.H. Yang. Parametric modeling and estimation of geometric errors for a rotar axis using double ball-bar [J]. he International Journal of Advaced Manufacturing echnolog, 2012, 62(5-8): [9] M. sutsumi, S. one, N. Kato et al. Enhancement of geometric accurac of five-axis machining centers based on identification and compensation of geometric deviations [J]. International Journal of Machine ools and Manufacture, 2013, 68: [10] K.I. Lee, S.H. Yang. Measurement and verification of position-independent geometric errors of a five-axis machine tool using a double ball-bar [J]. International Journal of Machine ools and Manufacture, 2013, 70: [11] K.I. Lee, S.H. Yang. Robust measurement method and uncertaint analsis for position independent geometric errors of a rotar axis using a double ball-bar [J]. International Journal of Precision Engineering and Manufacturing, 2013, 14(2):
COIN TOSS MODELING RĂZVAN C. STEFAN, TIBERIUS O. CHECHE
Romanian Reports in Phsics 69, 94 (7) COIN TOSS MODELING RĂZVAN C. STEFAN, TIBERIUS O. CHECHE Universit of Bucharest, Facult of Phsics, P.O.Box MG-, RO-775, Bucharest Măgurele, Romania E-mails: stefan.constantin6@gmail.com;
More informationProgressive wave: a new multisource vibration technique to assist forming processes - kinematic study, simulation results and design proposition
Progressive wave: a new multisource vibration technique to assist forming processes - kinematic stud, simulation results and design proposition A. Khan a, T. H. Nguen a, C. Giraud-Audine a, G. Abba b,
More informationContents. Dynamics and control of mechanical systems. Focuses on
Dnamics and control of mechanical sstems Date Da (/8) Da (3/8) Da 3 (5/8) Da 4 (7/8) Da 5 (9/8) Da 6 (/8) Content Review of the basics of mechanics. Kinematics of rigid bodies - coordinate transformation,
More informationKINEMATIC RELATIONS IN DEFORMATION OF SOLIDS
Chapter 8 KINEMATIC RELATIONS IN DEFORMATION OF SOLIDS Figure 8.1: 195 196 CHAPTER 8. KINEMATIC RELATIONS IN DEFORMATION OF SOLIDS 8.1 Motivation In Chapter 3, the conservation of linear momentum for a
More informationVibration of Plate on Foundation with Four Edges Free by Finite Cosine Integral Transform Method
854 Vibration of Plate on Foundation with Four Edges Free b Finite Cosine Integral Transform Method Abstract The analtical solutions for the natural frequencies and mode shapes of the rectangular plate
More informationVibrational Power Flow Considerations Arising From Multi-Dimensional Isolators. Abstract
Vibrational Power Flow Considerations Arising From Multi-Dimensional Isolators Rajendra Singh and Seungbo Kim The Ohio State Universit Columbus, OH 4321-117, USA Abstract Much of the vibration isolation
More informationGeometric Stiffness Effects in 2D and 3D Frames
Geometric Stiffness Effects in D and 3D Frames CEE 41. Matrix Structural Analsis Department of Civil and Environmental Engineering Duke Universit Henri Gavin Fall, 1 In situations in which deformations
More informationINSTRUCTIONS TO CANDIDATES:
NATIONAL NIVERSITY OF SINGAPORE FINAL EXAMINATION FOR THE DEGREE OF B.ENG ME 444 - DYNAMICS AND CONTROL OF ROBOTIC SYSTEMS October/November 994 - Time Allowed: 3 Hours INSTRCTIONS TO CANDIDATES:. This
More information1 HOMOGENEOUS TRANSFORMATIONS
HOMOGENEOUS TRANSFORMATIONS Purpose: The purpose of this chapter is to introduce ou to the Homogeneous Transformation. This simple 4 4 transformation is used in the geometr engines of CAD sstems and in
More information877. Design and performance analysis of dual vibrating motors self synchronous shaker with balanced elliptical motion
877. Design and performance analsis of dual vibrating motors self snchronous shaker with balanced elliptical motion Weibing Zhu 1, Heshun Wang, Lin Dong 3 School of Mechanical Engineering and Automation,
More informationStability Analysis of Laminated Composite Thin-Walled Beam Structures
Paper 224 Civil-Comp Press, 2012 Proceedings of the Eleventh International Conference on Computational Structures echnolog, B.H.V. opping, (Editor), Civil-Comp Press, Stirlingshire, Scotland Stabilit nalsis
More informationEquilibrium of Rigid Bodies
Equilibrium of Rigid Bodies 1 2 Contents Introduction Free-Bod Diagram Reactions at Supports and Connections for a wo-dimensional Structure Equilibrium of a Rigid Bod in wo Dimensions Staticall Indeterminate
More informationSpace frames. b) R z φ z. R x. Figure 1 Sign convention: a) Displacements; b) Reactions
Lecture notes: Structural Analsis II Space frames I. asic concepts. The design of a building is generall accomplished b considering the structure as an assemblage of planar frames, each of which is designed
More informationStatic and dynamic testing of machine tools
Static and dynamic testing of machine tools Thomas Liebrich, Michael Gebhardt, Stefan Thoma, Hop Nguyen, Sascha Weikert, Wolfgang Knapp, Konrad Wegener Institute for Machine Tools and Manufacturing (IWF),
More informationAlgebra II Practice Semester Exam Specification Sheet
Algebra II Practice Semester Exam Specification Sheet 1. Properties of real numbers. Procedure (write procedure or process) 3. Concept development/linkage. Theorem/factual knowledge (of theorems and rules)
More informationON THE INTERPRETATION OF THE LAGRANGE MULTIPLIERS IN THE CONSTRAINT FORMULATION OF CONTACT PROBLEMS; OR WHY ARE SOME MULTIPLIERS ALWAYS ZERO?
Proceedings of the ASME 214 International Design Engineering Technical Conferences & Computers and Information in Engineering Conference IDETC/CIE 214 August 17-2, 214, Buffalo, New York, USA DETC214-3479
More informationAffine transformations
Reading Required: Affine transformations Brian Curless CSEP 557 Fall 2016 Angel 3.1, 3.7-3.11 Further reading: Angel, the rest of Chapter 3 Fole, et al, Chapter 5.1-5.5. David F. Rogers and J. Alan Adams,
More informationUnit 12 Study Notes 1 Systems of Equations
You should learn to: Unit Stud Notes Sstems of Equations. Solve sstems of equations b substitution.. Solve sstems of equations b graphing (calculator). 3. Solve sstems of equations b elimination. 4. Solve
More informationKinematics. Félix Monasterio-Huelin, Álvaro Gutiérrez & Blanca Larraga. September 5, Contents 1. List of Figures 1.
Kinematics Féli Monasterio-Huelin, Álvaro Gutiérre & Blanca Larraga September 5, 2018 Contents Contents 1 List of Figures 1 List of Tables 2 Acronm list 3 1 Degrees of freedom and kinematic chains of rigid
More informationCOMPENSATE ALGORITHM OF DEFORMATION IN WOOD HIGH-SPEED FIVE-AXIS MACHINING
U.P.B. Sci. Bull., Series D, Vol. 79, Iss. 3, 2017 ISSN 1454-2358 COMPENSATE ALGORITHM OF DEFORMATION IN WOOD HIGH-SPEED FIVE-AXIS MACHINING Zhang Wei *1,2, Wang Shuangyong 1, Zhang Yang 3,Yang Jianhua
More informationVector Analysis 1.1 VECTOR ANALYSIS. A= Aa A. Aa, A direction of the vector A.
1 Vector nalsis 1.1 VECTR NYSIS Introduction In general, electromagnetic field problem involves three space variables, as a result of which the solutions tend to become complex. This can be overcome b
More informationDynamics of multiple pendula without gravity
Chaotic Modeling and Simulation (CMSIM) 1: 57 67, 014 Dnamics of multiple pendula without gravit Wojciech Szumiński Institute of Phsics, Universit of Zielona Góra, Poland (E-mail: uz88szuminski@gmail.com)
More informationCalculus of the Elastic Properties of a Beam Cross-Section
Presented at the COMSOL Conference 2009 Milan Calculus of the Elastic Properties of a Beam Cross-Section Dipartimento di Modellistica per l Ingegneria Università degli Studi della Calabria (Ital) COMSOL
More informationVectors Primer. M.C. Simani. July 7, 2007
Vectors Primer M.. Simani Jul 7, 2007 This note gives a short introduction to the concept of vector and summarizes the basic properties of vectors. Reference textbook: Universit Phsics, Young and Freedman,
More informationStudy on Nonlinear Vibration and Crack Fault of Rotor-bearing-seal Coupling System
Sensors & Transducers 04 b IFSA Publishing S. L. http://www.sensorsportal.com Stud on Nonlinear Vibration and Crack Fault of Rotor-bearing-seal Coupling Sstem Yuegang LUO Songhe ZHANG Bin WU Wanlei WANG
More informationTransformation of kinematical quantities from rotating into static coordinate system
Transformation of kinematical quantities from rotating into static coordinate sstem Dimitar G Stoanov Facult of Engineering and Pedagog in Sliven, Technical Universit of Sofia 59, Bourgasko Shaussee Blvd,
More informationEffects of birefringence on Fizeau interferometry that uses polarization phase shifting technique
Effects of birefringence on Fizeau interferometr that uses polarization phase shifting technique Chunu Zhao, Dongel Kang and James H. Burge College of Optical Sciences, the Universit of Arizona 1630 E.
More informationy R T However, the calculations are easier, when carried out using the polar set of co-ordinates ϕ,r. The relations between the co-ordinates are:
Curved beams. Introduction Curved beams also called arches were invented about ears ago. he purpose was to form such a structure that would transfer loads, mainl the dead weight, to the ground b the elements
More informationSimultaneous Orthogonal Rotations Angle
ELEKTROTEHNIŠKI VESTNIK 8(1-2): -11, 2011 ENGLISH EDITION Simultaneous Orthogonal Rotations Angle Sašo Tomažič 1, Sara Stančin 2 Facult of Electrical Engineering, Universit of Ljubljana 1 E-mail: saso.tomaic@fe.uni-lj.si
More informationSolution 11. Kinetics of rigid body(newton s Second Law)
Solution () urpose and Requirement Solution Kinetics of rigid bod(newton s Second Law) In rob, kinematics stud regarding acceleration of mass center should be done before Newton s second law is used to
More informationCH. 1 FUNDAMENTAL PRINCIPLES OF MECHANICS
446.201 (Solid echanics) Professor Youn, eng Dong CH. 1 FUNDENTL PRINCIPLES OF ECHNICS Ch. 1 Fundamental Principles of echanics 1 / 14 446.201 (Solid echanics) Professor Youn, eng Dong 1.2 Generalied Procedure
More informationAffine transformations
Reading Optional reading: Affine transformations Brian Curless CSE 557 Autumn 207 Angel and Shreiner: 3., 3.7-3. Marschner and Shirle: 2.3, 2.4.-2.4.4, 6..-6..4, 6.2., 6.3 Further reading: Angel, the rest
More informationENGI 9420 Engineering Analysis Solutions to Additional Exercises
ENGI 940 Engineering Analsis Solutions to Additional Exercises 0 Fall [Partial differential equations; Chapter 8] The function ux (, ) satisfies u u u + = 0, subject to the x x u x,0 = u x, =. Classif
More informationBIAS MOMENTUM SATELLITE MAGNETIC ATTITUDE CONTROL BASED ON GENETIC ALGORITHMS. Jianting Lv, Guangfu Ma, Dai Gao
IAS MOMENUM SAELLIE MAGNEIC AIUDE CONROL ASED ON GENEIC ALGORIHMS Jianting Lv, Guangfu Ma, Dai Gao Department of Control Science and Engineering, Harbin Institute of echnolog, Harbin 5 Abstract: o solve
More informationSection 8.5 Parametric Equations
504 Chapter 8 Section 8.5 Parametric Equations Man shapes, even ones as simple as circles, cannot be represented as an equation where is a function of. Consider, for eample, the path a moon follows as
More informationPhysically Based Rendering ( ) Geometry and Transformations
Phsicall Based Rendering (6.657) Geometr and Transformations 3D Point Specifies a location Origin 3D Point Specifies a location Represented b three coordinates Infinitel small class Point3D { public: Coordinate
More informationUsing Two Tri-Axis Accelerometers for Rotational Measurements
Using Two Tri-Axis Accelerometers for Rotational Measurements Introduction In man applications, customers would like to measure rotational motions (angular velocit, angular acceleration) in addition to
More informationThe Theory of a Scroll Profile
Purdue Universit Purdue e-pus International Compressor Engineering Conference School of Mechanical Engineering 006 The Theor of a Scroll Profile Huert Bukac Little Dnamics Follow this and additional works
More informationFirst Order Differential Equations f ( x,
Chapter d dx First Order Differential Equations f ( x, ).1 Linear Equations; Method of Integrating Factors Usuall the general first order linear equations has the form p( t ) g ( t ) (1) where pt () and
More informationIntroduction to Differential Equations. National Chiao Tung University Chun-Jen Tsai 9/14/2011
Introduction to Differential Equations National Chiao Tung Universit Chun-Jen Tsai 9/14/011 Differential Equations Definition: An equation containing the derivatives of one or more dependent variables,
More informationRotational & Rigid-Body Mechanics. Lectures 3+4
Rotational & Rigid-Body Mechanics Lectures 3+4 Rotational Motion So far: point objects moving through a trajectory. Next: moving actual dimensional objects and rotating them. 2 Circular Motion - Definitions
More informationPHYSICS 1 Forces & Newton s Laws
Advanced Placement PHYSICS 1 Forces & Newton s Laws Presenter 2014-2015 Forces & Newton s Laws What I Absolutel Have to Know to Survive the AP* Exam Force is an push or pull. It is a vector. Newton s Second
More informationHomework Solutions Week of November = 1(1) + 0(x 1) + 0(x 1) 2 x = 1(1) + 1(x 1) + 0(x 1) 2 x 2 = 1(1) + 2(x 1) + 1(x 1) 2
Math 34/84: Matrix heor Dr S Cooper Fall 8 Section 63: Homework Solutions Week of November 8 (7) he sets B { x (x ) } C { x x } are both bases for P We need to find [p(x) B Observe that () + (x ) + (x
More informationMAE4700/5700 Finite Element Analysis for Mechanical and Aerospace Design
MAE4700/5700 Finite Element Analsis for Mechanical and Aerospace Design Cornell Universit, Fall 2009 Nicholas Zabaras Materials Process Design and Control Laborator Sible School of Mechanical and Aerospace
More informationSCRUTINIZE THE ABRASION PHENOMENON WITH THE BRUNT FORCES IN THE JOINTS OF THE ROBOTS AND PROPOSED A NEW WAY TO DECREASE THAT
SCRUTINIZE THE ABRASION PHENOMENON WITH THE BRUNT FORCES IN THE JOINTS OF THE ROBOTS AND PROPOSED A NEW WAY TO DECREASE THAT Khashaar Teimoori and Mahdi Pirhaati Department of Mechanical and Aerospace
More information12.1 Systems of Linear equations: Substitution and Elimination
. Sstems of Linear equations: Substitution and Elimination Sstems of two linear equations in two variables A sstem of equations is a collection of two or more equations. A solution of a sstem in two variables
More informationQUADRATIC AND CONVEX MINIMAX CLASSIFICATION PROBLEMS
Journal of the Operations Research Societ of Japan 008, Vol. 51, No., 191-01 QUADRATIC AND CONVEX MINIMAX CLASSIFICATION PROBLEMS Tomonari Kitahara Shinji Mizuno Kazuhide Nakata Toko Institute of Technolog
More informationStability Analysis of Mathematical Model for New Hydraulic Bilateral Rolling Shear
SJ nternational, Vol. 56 (06), SJ nternational, No. Vol. 56 (06), No., pp. 88 9 Stabilit Analsis of Mathematical Model for New Hdraulic Bilateral Rolling Shear QingXue HUANG, ) Jia L, ) HongZhou L, ) HeYong
More information14.1 Systems of Linear Equations in Two Variables
86 Chapter 1 Sstems of Equations and Matrices 1.1 Sstems of Linear Equations in Two Variables Use the method of substitution to solve sstems of equations in two variables. Use the method of elimination
More informationThe Design of Fuzzy Adaptive PID Controller of Two-Wheeled Self-Balancing Robot
The esign of Fuzz Adaptive PI Controller of Two-Wheeled Self-Balancing Robot Conging Qiu and Yibin Huang Abstract A two-wheeled self-balancing robot sstem is developed and the hardware sstem mainl consists
More informationNeatest and Promptest Manner. E d i t u r ami rul)lihher. FOIt THE CIIILDIIES'. Trifles.
» ~ $ ) 7 x X ) / ( 8 2 X 39 ««x» ««! «! / x? \» «({? «» q «(? (?? x! «? 8? ( z x x q? ) «q q q ) x z x 69 7( X X ( 3»«! ( ~«x ««x ) (» «8 4 X «4 «4 «8 X «x «(» X) ()»» «X «97 X X X 4 ( 86) x) ( ) z z
More information3.0 PROBABILITY, RANDOM VARIABLES AND RANDOM PROCESSES
3.0 PROBABILITY, RANDOM VARIABLES AND RANDOM PROCESSES 3.1 Introduction In this chapter we will review the concepts of probabilit, rom variables rom processes. We begin b reviewing some of the definitions
More informationAffine transformations. Brian Curless CSE 557 Fall 2014
Affine transformations Brian Curless CSE 557 Fall 2014 1 Reading Required: Shirle, Sec. 2.4, 2.7 Shirle, Ch. 5.1-5.3 Shirle, Ch. 6 Further reading: Fole, et al, Chapter 5.1-5.5. David F. Rogers and J.
More informationIntegration of the equation of motion with respect to time rather than displacement leads to the equations of impulse and momentum.
Integration of the equation of motion with respect to time rather than displacement leads to the equations of impulse and momentum. These equations greatl facilitate the solution of man problems in which
More informationStrain Transformation and Rosette Gage Theory
Strain Transformation and Rosette Gage Theor It is often desired to measure the full state of strain on the surface of a part, that is to measure not onl the two etensional strains, and, but also the shear
More information2 Ordinary Differential Equations: Initial Value Problems
Ordinar Differential Equations: Initial Value Problems Read sections 9., (9. for information), 9.3, 9.3., 9.3. (up to p. 396), 9.3.6. Review questions 9.3, 9.4, 9.8, 9.9, 9.4 9.6.. Two Examples.. Foxes
More informationA structural design method for five-axis gantry machining center based on stiffness matching
INER-NOISE 016 A structural design method for five-ais gantry machining center based on stiffness matching Cheng ZHANG 1 ; Jian-run ZHANG ; Bei-bei SUN 3 ; Xi LU 4 1,,3,4 School of Mechanical Engineering,
More informationESMF Based Multiple UAVs Active Cooperative Observation Method in Relative Velocity Coordinates
Joint 48th IEEE Conference on Decision and Control and 8th Chinese Control Conference Shanghai, P.R. China, December 6-8, 009 WeCIn5.4 ESMF Based Multiple UAVs Active Cooperative Observation Method in
More informationExperimental Calibration and Head Loss Prediction of Tuned Liquid Column Damper
Tamkang Journal of Science and Engineering, Vol. 8, No 4, pp. 319-35 (005) 319 Experimental Calibration and Head Loss Prediction of Tuned Liquid Column Damper Jong-Cheng Wu Department of Civil Engineering,
More informationRegulation Performance of Regulatable Dry Gas Seal
Regulation Performance of Regulatable Dr Gas Seal SHUANGXI LI, QIAOFENG ZHU, JINING CAI, QIUXIANG ZHANG, ZHAOXU JIN Colleague of Mechanical and Engineering Beijing Universit of Chemical Technolog No.15
More informationFluid Mechanics II. Newton s second law applied to a control volume
Fluid Mechanics II Stead flow momentum equation Newton s second law applied to a control volume Fluids, either in a static or dnamic motion state, impose forces on immersed bodies and confining boundaries.
More informationSubband Coding and Wavelets. National Chiao Tung University Chun-Jen Tsai 12/04/2014
Subband Coding and Wavelets National Chiao Tung Universit Chun-Jen Tsai /4/4 Concept of Subband Coding In transform coding, we use N (or N N) samples as the data transform unit Transform coefficients are
More informationANSYS-Based Birefringence Property Analysis of Side-Hole Fiber Induced by Pressure and Temperature
PHOTONIC SENSORS / Vol. 8, No. 1, 2018: 13 21 ANSYS-Based Birefringence Propert Analsis of Side-Hole Fiber Induced b Pressure and Temperature Xinbang ZHOU 1 and Zhenfeng GONG 2* 1 School of Ocean Science
More informationA New Closed-loop Identification Method of a Hammerstein-type System with a Pure Time Delay
A New Closed-loop Identification Method of a Hammerstein-tpe Sstem with a Pure Time Dela Edin Drljević a, Branislava Peruničić b, Željko Jurić c, Member of IEEE Abstract A procedure for the closed-loop
More informationJournal of Advanced Mechanical Design, Systems, and Manufacturing
Vol., No., 7 Evaluation of Synchronous Motion in Five-axis Machining Centers With a Tilting Rotary Table * Masaomi TSUTSUMI ** Daisuke YUMIZA ** Keizo UTSUMI *** and Ryuta SATO ** **Tokyo University of
More informationClosed form expressions for the gravitational inner multipole moments of homogeneous elementary solids
Closed form epressions for the gravitational inner multipole moments of homogeneous elementar solids Julian Stirling 1,2, and Stephan Schlamminger 1 1 National Institute of Standards and Technolog, 1 Bureau
More information792. Experimental studies of stabilization of boring cutter form building top oscillation
792. Experimental studies of stabilization of boring cutter form building top oscillation M. R. Sikhimbaev 1, K. Т. Sherov 2, О. М. Zharkevich 3, А. K. Sherov 4, Yu. О. Тkachova 5 Karaganda State Technical
More information10. The dimensional formula for c) 6% d) 7%
UNIT. One of the combinations from the fundamental phsical constants is hc G. The unit of this epression is a) kg b) m 3 c) s - d) m. If the error in the measurement of radius is %, then the error in the
More informationMAE 323: Lecture 1. Review
This review is divided into two parts. The first part is a mini-review of statics and solid mechanics. The second part is a review of matrix/vector fundamentals. The first part is given as an refresher
More informationChapter 4 Transport of Pollutants
4- Introduction Phs. 645: Environmental Phsics Phsics Department Yarmouk Universit hapter 4 Transport of Pollutants - e cannot avoid the production of pollutants. hat can we do? - Transform pollutants
More informationResearch Article Two Mathematical Models for Generation of Crowned Tooth Surface
e Scientific World Journal, Article ID 6409, 6 pages http://dx.doi.org/0.55/204/6409 Research Article Two Mathematical Models for Generation of Crowned Tooth Surface Laszlo Kelemen and Jozsef Szente University
More informationGraph the linear system and estimate the solution. Then check the solution algebraically.
(Chapters and ) A. Linear Sstems (pp. 6 0). Solve a Sstem b Graphing Vocabular Solution For a sstem of linear equations in two variables, an ordered pair (x, ) that satisfies each equation. Consistent
More informationThe first change comes in how we associate operators with classical observables. In one dimension, we had. p p ˆ
VI. Angular momentum Up to this point, we have been dealing primaril with one dimensional sstems. In practice, of course, most of the sstems we deal with live in three dimensions and 1D quantum mechanics
More informationIMECE November 11 17, 2011, Denver, Colorado, USA
Proceedings of the AME 11 International Mechanical Engineering Congress & Exposition IMECE11 November 11-17, 11, enver, Colorado, UA Proceedings of the AME 11 International Mechanical Engineering Congress
More informationA comparison of estimation accuracy by the use of KF, EKF & UKF filters
Computational Methods and Eperimental Measurements XIII 779 A comparison of estimation accurac b the use of KF EKF & UKF filters S. Konatowski & A. T. Pieniężn Department of Electronics Militar Universit
More informationUnit 3 Notes Mathematical Methods
Unit 3 Notes Mathematical Methods Foundational Knowledge Created b Triumph Tutoring Copright info Copright Triumph Tutoring 07 Triumph Tutoring Pt Ltd ABN 60 607 0 507 First published in 07 All rights
More informationMeasurement Model and Precision Analysis of Accelerometers for Maglev Vibration Isolation Platforms
Sensors 25, 5, 253-268; doi:.339/s58253 Article OPEN ACCESS sensors ISSN 424-822 www.mdpi.com/journal/sensors Measurement Model and Precision Analsis of Accelerometers for Maglev Vibration Isolation Platforms
More informationReading. 4. Affine transformations. Required: Watt, Section 1.1. Further reading:
Reading Required: Watt, Section.. Further reading: 4. Affine transformations Fole, et al, Chapter 5.-5.5. David F. Rogers and J. Alan Adams, Mathematical Elements for Computer Graphics, 2 nd Ed., McGraw-Hill,
More informationKrylov Integration Factor Method on Sparse Grids for High Spatial Dimension Convection Diffusion Equations
DOI.7/s95-6-6-7 Krlov Integration Factor Method on Sparse Grids for High Spatial Dimension Convection Diffusion Equations Dong Lu Yong-Tao Zhang Received: September 5 / Revised: 9 March 6 / Accepted: 8
More informationGravitational potential energy
Gravitational potential energ m1 Consider a rigid bod of arbitrar shape. We want to obtain a value for its gravitational potential energ. O r1 1 x The gravitational potential energ of an assembl of N point-like
More informationEstimation Of Linearised Fluid Film Coefficients In A Rotor Bearing System Subjected To Random Excitation
Estimation Of Linearised Fluid Film Coefficients In A Rotor Bearing Sstem Subjected To Random Ecitation Arshad. Khan and Ahmad A. Khan Department of Mechanical Engineering Z.. College of Engineering &
More informationSection 3.1. ; X = (0, 1]. (i) f : R R R, f (x, y) = x y
Paul J. Bruillard MATH 0.970 Problem Set 6 An Introduction to Abstract Mathematics R. Bond and W. Keane Section 3.1: 3b,c,e,i, 4bd, 6, 9, 15, 16, 18c,e, 19a, 0, 1b Section 3.: 1f,i, e, 6, 1e,f,h, 13e,
More informationTwo Levels Data Fusion Filtering Algorithms of Multimode Compound Seeker
TELKOMNKA, Vol.11, No.11, November 13, pp. 674~68 e-ssn: 87-78X 674 Two Levels Data Fusion Filtering Algorithms of Multimode Compound Seeker Guodong Zhang*, Zhong Liu, Ke Li College of Electronic Engineering,
More informationMath 181/281. Rumbos Spring 2011 Page 1. Solutions to Assignment #5. Hence, the dynamical system, θ(t, p, q), for (t, p, q) R 3 corresponding = F.
Math 181/281. Rumbos Spring 2011 Page 1 Solutions to Assignment #5 1. For real numbers a and b with a 2 + b 2 = 0, let F : R 2 R 2 be given b ( ) ( ) ( ) x ax b x F =, for all R 2. (1) bx + a (a) Explain
More informationChapter 1 Introduction
Chapter 1 Introduction 1.1 What is phsics? Phsics deals with the behavior and composition of matter and its interactions at the most fundamental level. 1 Classical Phsics Classical phsics: (1600-1900)
More informationDesign of an Adaptive-Neural Network Attitude Controller of a Satellite using Reaction Wheels
Journal of Applied and Computational echanics, Vol., No., (5), 67-73 DOI:.55/jacm.4.757 Design of an Adaptive-Neural Network Attitude Controller of a Satellite using Reaction heels Abbas Ajorkar, Alirea
More informationMath 4381 / 6378 Symmetry Analysis
Math 438 / 6378 Smmetr Analsis Elementar ODE Review First Order Equations Ordinar differential equations of the form = F(x, ( are called first order ordinar differential equations. There are a variet of
More informationRANGE CONTROL MPC APPROACH FOR TWO-DIMENSIONAL SYSTEM 1
RANGE CONTROL MPC APPROACH FOR TWO-DIMENSIONAL SYSTEM Jirka Roubal Vladimír Havlena Department of Control Engineering, Facult of Electrical Engineering, Czech Technical Universit in Prague Karlovo náměstí
More informationAn analytic proof of the theorems of Pappus and Desargues
Note di Matematica 22, n. 1, 2003, 99 106. An analtic proof of the theorems of Pappus and Desargues Erwin Kleinfeld and Tuong Ton-That Department of Mathematics, The Universit of Iowa, Iowa Cit, IA 52242,
More informationOptimization of Gear Design and Manufacture. Vilmos SIMON *
7 International Conference on Mechanical and Mechatronics Engineering (ICMME 7) ISBN: 978--6595-44- timization of Gear Design and Manufacture Vilmos SIMN * Budaest Universit of Technolog and Economics,
More informationCoordinate geometry. + bx + c. Vertical asymptote. Sketch graphs of hyperbolas (including asymptotic behaviour) from the general
A Sketch graphs of = a m b n c where m = or and n = or B Reciprocal graphs C Graphs of circles and ellipses D Graphs of hperbolas E Partial fractions F Sketch graphs using partial fractions Coordinate
More informationPROPERTIES OF PERIFERAL NERVE EXCITATION IN RESPECT OF LOCATION OF COIL FOR MAGNETIC NERVE STIMULATION
PROPERTIES OF PERIFERAL NERVE EXCITATION IN RESPECT OF LOCATION OF COIL FOR MAGNETIC NERVE STIMULATION O. Hiwaki, H. Kuwano Facult of Information Sciences, Hiroshima Cit Universit, Hiroshima, Japan Abstract-
More informationMulti-axis synchronous interpolation feed rate adaptive planning with rotational tool center point function under comprehensive constraints
Special Issue Article Multi-axis synchronous interpolation feed rate adaptive planning with rotational tool center point function under comprehensive constraints Advances in Mechanical Engineering 2017,
More informationMechanical Spring Reliability Assessments Based on FEA Generated Fatigue Stresses and Monte Carlo Simulated Stress/Strength Distributions
Purdue Universit Purdue e-pubs International Compressor Engineering Conference School of Mechanical Engineering 4 Mechanical Spring Reliabilit Assessments Based on FEA Generated Fatigue Stresses and Monte
More informationResearch Article Equivalent Elastic Modulus of Asymmetrical Honeycomb
International Scholarl Research Network ISRN Mechanical Engineering Volume, Article ID 57, pages doi:.5//57 Research Article Equivalent Elastic Modulus of Asmmetrical Honecomb Dai-Heng Chen and Kenichi
More informationSECOND-ORDER DIFFERENTIAL EQUATIONS: CONDITIONS OF COMPLETE INTEGRABILITY 1. from Lectures on Integration of Differential Equations
Applicable Analsis and Discrete Mathematics available online at http://pefmath.etf.bg.ac.u Appl. Anal. Discrete Math. 008, 3 45. doi:0.98/aadm0803e SECOND-ORDER DIFFERENTIAL EQUATIONS: CONDITIONS OF COMPLETE
More informationFor each problem, place the letter choice of your answer in the spaces provided on this page.
Math 6 Final Exam Spring 6 Your name Directions: For each problem, place the letter choice of our answer in the spaces provided on this page...... 6. 7. 8. 9....... 6. 7. 8. 9....... B signing here, I
More informationChapter 1 Coordinates, points and lines
Cambridge Universit Press 978--36-6000-7 Cambridge International AS and A Level Mathematics: Pure Mathematics Coursebook Hugh Neill, Douglas Quadling, Julian Gilbe Ecerpt Chapter Coordinates, points and
More informationSHORT PLANE BEARINGS LUBRICATION APPLIED ON SILENT CHAIN JOINTS
Bulletin of the Transilvania Universit of Braşov Vol. 9 (58) No. - Special Issue 016 Series I: Engineering Sciences SHORT PLANE BEARINGS LUBRICATION APPLIED ON SILENT CHAIN JOINTS L. JURJ 1 R. VELICU Abstract:
More information2010 IEEE. Personal use of this material is permitted. Permission from IEEE must be obtained for all other uses, in any current or future media,
2010 IEEE. Personal use of this material is permitted. Permission from IEEE must be obtained for all other uses, in an current or future media, including reprinting/republishing this material for advertising
More information