Material Properties and Impact Insulation Technical Information
|
|
- Douglas Cameron Patterson
- 6 years ago
- Views:
Transcription
1 Material Propertie and Impact Inulation Technical Information Sylodamp an overview Sylodamp i a high-damping polyurethane elatomer that ha been pecially developed to aborb the load caued by impact. Sylodamp can alo be employed a an elatic component in conventional vibration inulation application in which, in addition to permanent elaticity, a high level of damping of the elatomer i required. Typical application can be found in ituation where machinery, building tructure, technical equipment or even people need to be protected. The following beneit have been identiied in the area of impact and vibration inulation: Reduce the load caued by impact Reduce impact-induced tructure-borne noie Reduce reonance phenomena Damping of component or tructure Rapid decay of vibration In mot cae, Sylodamp i employed a a preuried pring, the material propertie of which can be ideally adapted to the application in hand by the careful choice of material type, contact area and elatomer thickne. The Sylodamp range cover the following tatic range of ue: The tatic range of ue i the maximum compreive tre deined for tationary load at which the elatic propertie of an elatomer are permanently retained. The material type refer to the compreive hardne at 0 % deformation. Thi i an individually deined meaure for the load-bearing property of an elatomer, but doe not give any information on the behavior during longterm loading. For example, the compreive hardne of Sylodamp 00 i 00 kn/m. Vibration inulation with Sylodamp Vibration inulation ue the principle of ma force compenation to reduce the propagation of mechanical vibration caued by external force or excitation. The principle area of application of Sylomer and Sylodyn material i in conventional vibration inulation. Uing Sylodamp enable even higher level of vibration inulation to be achieved, epecially when the impulive load or trong reonance phenomena that typically occur when machinery i being tarted up or hut down are preent. In addition to the preence of Sylodamp bedding, a combination of Sylodamp and Sylomer pring can alo be ued in parallel. Vibration damping with Sylodamp Vibration damping i undertood to be the converion of kinetic energy into another form of (renewable) energy that no longer ha any impact on the vibration ytem. Due to it high level of material damping, Sylodamp i a particularly effective way of keeping the reonance phenomena occurring in component or tructure within the required tolerance Speciic load in N/mm Fig. : Sylodamp range
2 Impact inulation with Sylodamp Impact inulation i a pecial type of vibration inulation that i ued to reduce the propagation of the force generated by impact. Here, a brief exciting force with a relatively high peak force i converted into a longer lating ground force with a lower peak value. The material damping feature of Sylodamp reult in the rapid damping of kinetic parameter, reducing the decay time of component and tructure. m v Sylodamp d Example of impact Fig. to 4 illutrate ome example of impact in which a ma m collide with a tructure at a velocity v. The high-damping vibration inulator made from Sylodamp i hown in orange. Fig. 3: Horizontal impact ma moving horizontally d m v Sylodamp m Fig. 4: Oblique impact ma moving at an angle h Sylodamp v d m = Ma of the moving body v = Impact velocity of the moving ma d = Thickne of the elatomer = Maximum deformation of the elatomer h = Free-fall drop height Fig. : Vertical impact free-falling ma
3 Degree of inulation The impact-inulating effect introduced by the ue of elatic bedding can be decribed by the degree of inulation I. Thi i deined a the reduction in the maximum repone loading in an intallation with elatic bedding compared to one without: Material election There are two way of electing the mot uitable material for impact application: Computational model (inite element method) Uing diagram howing the energy aborption of Sylodamp I F max, 0 F max F max, 0 I = Degree of inulation in % F max, 0 = Maximum value of the propagated ground force without elatic bedding F max = Maximum value of the propagated ground force with elatic bedding Finite element method model For traightforward impact application, Getzner ha developed a computational FEM model. The material and impact modelling make ue of drop tet tand invetigation with high-damping Sylodamp material and impactor with impact velocitie of up to 5 m/. An FEM impact imulation allow the mot uitable material deign from the Sylodamp range to be elected for the application. Principle of the conervation of energy The principle of the conervation of energy form the bai for the election of the appropriate material for an impact application. Thi equate the mechanical impact energy E kin (kinetic energy) with the deformation energy E def (energy aborption) of the high-damping Sylodamp material: m v E kin E kin E def 3 E kin = Impact energy (kinetic energy) in J E def = Deformation energy (energy aborption) in J Input parameter for the FEM imulation The following input parameter for the impact imulation mut be known: Ma of the moving body Impact velocity of the body The covering of the elatomer urface to be truck by the impactor Required elatomer thickne Reult of the FEM imulation An FEM impact imulation calculate the following reult: Plot againt time of ground force, elatomer deformation, energy aborption and/or brake delay during the impact Maximum propagated ground force Maximum deformation of the elatomer Maximum brake delay 3
4 Reult of FEM impact imulation Fig. 5 to 8 how the reult of a typical FEM impact imulation with Sylodamp. Force in kn Maximum ground force Fmax Delection in mm Maximum delection max.5 Recovery Delection Time in Fig. 5: Impact imulation plot againt time of ground force Time in Fig. 6: Impact imulation plot againt time of deformation Speed in m/ Impact velocity v Reveral point at max Energy aborption in J Maximum energy aborption -0.5 Recovery Time in Time in Fig. 7: Impact imulation plot againt time of velocity of ma Fig. 8: Impact imulation plot againt time of energy aborption 4
5 Energy aborption of Sylodamp A an alternative to FEM imulation, the choice of the mot uitable Sylodamp material for traightforward impact application can alo be made uing the following diagram (Fig. 9 to ). Speciic energy aborption in mj/mm Speciic energy aborption in mj/mm Linear compreion in % Linear compreion in % Fig. 9: Energy aborption of Sylodamp thickne.5 mm Fig. 0: Energy aborption of Sylodamp thickne 5 mm Speciic energy aborption in mj/mm Speciic energy aborption in mj/mm Linear compreion in % Linear compreion in % Fig. : Energy aborption of Sylodamp thickne 37.5 mm Fig. : Energy aborption of Sylodamp thickne 50 mm The impact energy exerted on the elatomer urface i ued a an input parameter when chooing the mot uitable material deign. The impact velocity ha no igniicant effect on the peciic energy aborption of Sylodamp. The peciic energy capacitie hown in the diagram can be ued for impact velocitie of between 0.5 m/ and 5 m/. 5
6 Ideal deformation range A correponding deformation path mut be provided for the elatomer o that Sylodamp can provide the bet poible aborption of impact load. We recommend the following linear compreion igure when uing Sylodamp in impact application: Material type Ideal deformation range Sylodamp 0 40 % to 60 % Sylodamp % to 60 % Sylodamp % to 55 % Sylodamp % to 50 % Sylodamp % to 45 % Sylodamp % to 40 % Impact force propagation The aim of impact inulation i to diipate the kinetic energy of the impactor with minimum level of force over a long a period a poible. The maximum force propagated during an ideal elatic impact can be determined from the deformation energy E def and the deformation path : 4 F max, 0 E def F max, 0 = Maximum value of propagated ground force in N E def = Deformation energy (energy aborption) in J = Deformation path in m Tab. : Recommended deformation range of Sylodamp under impact loading The peciied deformation range of the individual Sylodamp product reult in the energy aborption hown below for the repective elatomer thickne value: In cae where Sylodamp i being ued a the impactinulating element, the kinetic energy of the impactor i converted not jut by an elatic proce, but by damping (diipation) a well, further reducing the maximum propagated impact force. The maximum propagated force in the above cenario can be etimated a follow: Material type Energy aborption Thickne.5 mm 5 mm 37.5 mm 50 mm Sylodamp to to.8.6 to.9.3 to 3.9 Sylodamp 30.4 to.7.6 to to to Sylodamp to to to 9 4 to 5 Sylodamp to to 30 4 to 40 8 to 46 5 F max, 0,5 E def F max, 0 = Maximum value of propagated ground force with elatic Sylodamp bedding in N E def = Deformation energy (energy aborption) in J = Deformation path in m Sylodamp to to 50 4 to 7 56 to 9 Sylodamp to 4 45 to to 8 0 to 8 Tab. : Recommended peciic energy aborption in mj/mm of Sylodamp 6
7 The elatic portion of the elatomer provide oft cuhioning of the impactor, wherea the diipative portion enure that after the impact the bulk of the energy i no longer available to the ytem a kinetic energy. Due to the high level of material damping provided by Sylodamp, the impactor only rebound very lightly following the impact. The impact reilience of Sylodamp i around 5 %, which mean that 85 % of the kinetic energy of the impactor i diipated on impact. Input parameter Ma m = 80 kg Impact velocity v = m/ Impact area A = 5,65 mm (5 mm 5 mm) Calculation of impact force for an elatic Sylodamp bedding Impact energy E kin = m v = 80 = 60 J Deformation energy E Def = E Kin = 60 J Speciic energy aborption E Def, A = E def A = = 0.4 mj/mm Elatomer Sylodamp 00/5 (a per Fig. 0) Linear compreion ɛ = 50 % (a per Fig. 0) Max. deformation = ɛ Material thickne = 50 % 5 mm =.5 mm Max. impact force with elatic bedding F max, 0.5 E Def = = 9. kn Calculation of impact force without elatic bedding with the aumption of an elatic impact with uboil reilience of 0.5 mm Reilience of uboil/max. deformation = 0.5 mm Max. impact force without elatic bedding F max, 0 = Impact-inulating effect of elatic bedding E Def = 60 = 640 kn Degree of inulation I = F max, 0 F max F max, 0 = = 97 % Tab. 3: Sample calculation for a impact iulation with Sylodamp 7
8 Getzner Werktoffe GmbH Herrenau Bür Autria T F info.buer@getzner.com Getzner Werktoffe GmbH Am Borigturm 3507 Berlin Germany T F info.berlin@getzner.com Getzner Werktoffe GmbH Nördliche Münchner Str. 7a 803 Grünwald Germany T F info.munich@getzner.com Getzner Spring Solution GmbH Gottlob-Grotz-Str. 743 Bietigheim-Biingen Germany T F info.tuttgart@getzner.com Getzner France S.A.S. Bâtiment Quadrille 9 Rue Jacqueline Auriol Lyon France T info.lyon@getzner.com Getzner Werktoffe GmbH Middle Eat Regional Office Abdul - Hameed Sharaf Str. 4 Rimawi Center - Shmeiani P. O. Box 9694 Amman 96, Jordan T F info.amman@getzner.com Getzner India Pvt. Ltd. t Floor, Kaivalya 4 Teja Society, Kothrud Pune 4038, India T F info.pune@getzner.com Nihon Getzner K.K. 6-8 Nihonbahi Odenma-cho Chuo-ku, Tokyo 03-00, Japan T F info.tokyo@getzner.com Getzner Material (Beijing) Co., Ltd. No. 905, Tower D, the Vantone Center No. Jia 6, Chaowai Street, Chaoyang Ditrict 000, Beijing, the P.R.C. T F info.beijing@getzner.com Getzner USA, Inc. 870 Red Oak Boulevard, Suite 400 Charlotte, NC 87, USA T info.charlotte@getzner.com DB WS en Copyright by Getzner Werktoffe GmbH l Subject to change without notice.
Material Properties and Vibration Isolation Technical information
Material Properties and Vibration Isolation Technical inormation General inormation on Sylomer Sylomer is a special PUR elastomer manuactured by Getzner, which eatures a cellular, compact orm and is used
More informationdeflection approx. 7 %** approx. 20 %** approx. 80 %** DIN EN ISO 527-3/5/100* DIN EN ISO 527-3/5/100* DIN 53515* DIN Getzner Werkstoffe
sylomer G Material Colour mixed cellular polyurethane yellow Standard Sylomer range Standard dimensions on stock thickness: with Sylomer G12 with Sylomer G25 rolls: 1.5 m wide, 5.0 m long stripes: max.
More informationSylodyn NB. Material: Colour: Standard Sylodyn range. mixed cellular polyurethane red
NB Material: Colour: mixed cellular polyurethane red Standard Sylodyn range Area of application: compression load deflection (depending on shape factor) Static load limit: up to 75 N/mm 2 approx. 7% Operating
More informationStandard Sylodyn range. Material: Colour: mixed cellular polyurethane green
ND Material: Colour: mixed cellular polyurethane green Standard Sylodyn range Area of application: compression load deflection (depending on shape factor) Static load limit: up to.3 N/mm approx. 1% Operating
More informationMATERIAL PROPERTIES test methods comment
Material: Colour: mixed cellular polyurethane red Standard Sylomer range Area of application: compression load deflection (depending on shape factor) Static : N/mm approx. 9% Operating load range: up to
More informationSylodyn Material Data Sheet
ND Sylodyn Material Data Sheet Material Colour closed cellular polyurethane green Standard Sylodyn range Standard dimensions on stock Thickness:. mm with Sylodyn ND mm with Sylodyn ND Rolls:. m wide,.
More informationSylodyn Material Data Sheet
NF Sylodyn Material Data Sheet Material Colour closed cellular polyurethane violet Standard Sylodyn range Standard dimensions on stock Thickness:. mm with Sylodyn NF mm with Sylodyn NF Rolls:. m wide,.
More informationT V P M L R O G W. Sylomer. Material: Colour: Standard Sylomer range. mixed cellular polyurethane brown
M Material: Colour: mixed cellular polyurethane brown Standard Sylomer range Area of application: compression load deflection (depending on shape factor) Static load limit: up to 0.10 N/mm 2 approx. 7%
More informationSylodyn Material Data Sheet
NB Sylodyn Material Data Sheet Material Colour closed cellular polyurethane red Standard Sylodyn range Standard dimensions on stock Thickness:. mm with Sylodyn NB mm with Sylodyn NB Rolls:. m wide,. m
More informationMaterial properties and vibration isolation Technical information
Material properties and vibration isolation Technical inormation General inormation on Sylomer Sylomer is a special PUR elastomer manuactured by Getzner, which eatures a cellular, compact orm and is used
More informationFluid-structure coupling analysis and simulation of viscosity effect. on Coriolis mass flowmeter
APCOM & ISCM 11-14 th December, 2013, Singapore luid-tructure coupling analyi and imulation of vicoity effect on Corioli ma flowmeter *Luo Rongmo, and Wu Jian National Metrology Centre, A*STAR, 1 Science
More informationUnified Design Method for Flexure and Debonding in FRP Retrofitted RC Beams
Unified Deign Method for Flexure and Debonding in FRP Retrofitted RC Beam G.X. Guan, Ph.D. 1 ; and C.J. Burgoyne 2 Abtract Flexural retrofitting of reinforced concrete (RC) beam uing fibre reinforced polymer
More informationResearch on sound insulation of multiple-layer structure with porous material and air-layer
Reearch on ound inulation o multiple-layer tructure with porou material and air-layer Guoeng Bai 1 ; Pei Zhan; Fuheng Sui; Jun Yang Key Laboratory o Noie and Vibration Reearch Intitute o Acoutic Chinee
More informationAPPLICATION OF THE SINGLE IMPACT MICROINDENTATION FOR NON- DESTRUCTIVE TESTING OF THE FRACTURE TOUGHNESS OF NONMETALLIC AND POLYMERIC MATERIALS
APPLICATION OF THE SINGLE IMPACT MICROINDENTATION FOR NON- DESTRUCTIVE TESTING OF THE FRACTURE TOUGHNESS OF NONMETALLIC AND POLYMERIC MATERIALS REN A. P. INSTITUTE OF APPLIED PHYSICS OF THE NATIONAL ACADEMY
More informationMODELLING OF FRICTIONAL SOIL DAMPING IN FINITE ELEMENT ANALYSIS
MODELLING OF FRICTIONAL SOIL DAMPING IN FINITE ELEMENT ANALYSIS S. VAN BAARS Department of Science, Technology and Communication, Univerity of Luxembourg, Luxembourg ABSTRACT: In oil dynamic, the oil i
More informationThe stabilization interval system of a tethered descent underwater vehicle
IOP Conference Serie: Material Science and Engineering PAPER OPEN ACCESS The tabilization interval ytem of a tethered decent underwater vehicle To cite thi article: S A Gayvoronkiy et al 016 IOP Conf.
More information3pt3pt 3pt3pt0pt 1.5pt3pt3pt Honors Physics Impulse-Momentum Theorem. Name: Answer Key Mr. Leonard
3pt3pt 3pt3pt0pt 1.5pt3pt3pt Honor Phyic Impule-Momentum Theorem Spring, 2017 Intruction: Complete the following workheet. Show all of you work. Name: Anwer Key Mr. Leonard 1. A 0.500 kg ball i dropped
More informationHorizontal Biaxial Loading Tests on Sliding Lead Rubber Bearing System
Horizontal Biaxial Loading Tet on Sliding Lead Rubber Bearing Sytem M. Yamamoto, H. Hamaguchi & N. Kamohita Takenaka Reearch and Development Intitute, Japan. M. Kikuchi & K. Ihii Hokkaido Univerity, Japan.
More informationInteraction Diagram - Tied Reinforced Concrete Column (Using CSA A )
Interaction Diagram - Tied Reinforced Concrete Column (Uing CSA A23.3-14) Interaction Diagram - Tied Reinforced Concrete Column Develop an interaction diagram for the quare tied concrete column hown in
More informationa = f s,max /m = s g. 4. We first analyze the forces on the pig of mass m. The incline angle is.
Chapter 6 1. The greatet deceleration (of magnitude a) i provided by the maximum friction force (Eq. 6-1, with = mg in thi cae). Uing ewton econd law, we find a = f,max /m = g. Eq. -16 then give the hortet
More information303b Reducing the impact (Accelerometer & Light gate)
Senor: Logger: Accelerometer High g, Light gate Any EASYSENSE capable of fat logging Science in Sport Logging time: 1 econd 303b Reducing the impact (Accelerometer & Light gate) Read In many porting activitie
More informationEstimating floor acceleration in nonlinear multi-story moment-resisting frames
Etimating floor acceleration in nonlinear multi-tory moment-reiting frame R. Karami Mohammadi Aitant Profeor, Civil Engineering Department, K.N.Tooi Univerity M. Mohammadi M.Sc. Student, Civil Engineering
More informationLiquid cooling
SKiiPPACK no. 3 4 [ 1- exp (-t/ τ )] + [( P + P )/P ] R [ 1- exp (-t/ τ )] Z tha tot3 = R ν ν tot1 tot tot3 thaa-3 aa 3 ν= 1 3.3.6. Liquid cooling The following table contain the characteritic R ν and
More informationThe Influence of the Load Condition upon the Radial Distribution of Electromagnetic Vibration and Noise in a Three-Phase Squirrel-Cage Induction Motor
The Influence of the Load Condition upon the Radial Ditribution of Electromagnetic Vibration and Noie in a Three-Phae Squirrel-Cage Induction Motor Yuta Sato 1, Iao Hirotuka 1, Kazuo Tuboi 1, Maanori Nakamura
More informationUSING NONLINEAR CONTROL ALGORITHMS TO IMPROVE THE QUALITY OF SHAKING TABLE TESTS
October 12-17, 28, Beijing, China USING NONLINEAR CONTR ALGORITHMS TO IMPROVE THE QUALITY OF SHAKING TABLE TESTS T.Y. Yang 1 and A. Schellenberg 2 1 Pot Doctoral Scholar, Dept. of Civil and Env. Eng.,
More informationModule: 8 Lecture: 1
Moule: 8 Lecture: 1 Energy iipate by amping Uually amping i preent in all ocillatory ytem. It effect i to remove energy from the ytem. Energy in a vibrating ytem i either iipate into heat oun or raiate
More informationinto a discrete time function. Recall that the table of Laplace/z-transforms is constructed by (i) selecting to get
Lecture 25 Introduction to Some Matlab c2d Code in Relation to Sampled Sytem here are many way to convert a continuou time function, { h( t) ; t [0, )} into a dicrete time function { h ( k) ; k {0,,, }}
More informationGain and Phase Margins Based Delay Dependent Stability Analysis of Two- Area LFC System with Communication Delays
Gain and Phae Margin Baed Delay Dependent Stability Analyi of Two- Area LFC Sytem with Communication Delay Şahin Sönmez and Saffet Ayaun Department of Electrical Engineering, Niğde Ömer Halidemir Univerity,
More informationCHAPTER 8 OBSERVER BASED REDUCED ORDER CONTROLLER DESIGN FOR LARGE SCALE LINEAR DISCRETE-TIME CONTROL SYSTEMS
CHAPTER 8 OBSERVER BASED REDUCED ORDER CONTROLLER DESIGN FOR LARGE SCALE LINEAR DISCRETE-TIME CONTROL SYSTEMS 8.1 INTRODUCTION 8.2 REDUCED ORDER MODEL DESIGN FOR LINEAR DISCRETE-TIME CONTROL SYSTEMS 8.3
More informationμ + = σ = D 4 σ = D 3 σ = σ = All units in parts (a) and (b) are in V. (1) x chart: Center = μ = 0.75 UCL =
Our online Tutor are available 4*7 to provide Help with Proce control ytem Homework/Aignment or a long term Graduate/Undergraduate Proce control ytem Project. Our Tutor being experienced and proficient
More informationTHE RATIO OF DISPLACEMENT AMPLIFICATION FACTOR TO FORCE REDUCTION FACTOR
3 th World Conference on Earthquake Engineering Vancouver, B.C., Canada Augut -6, 4 Paper No. 97 THE RATIO OF DISPLACEMENT AMPLIFICATION FACTOR TO FORCE REDUCTION FACTOR Mua MAHMOUDI SUMMARY For Seimic
More informationSkyhook Damper Modification Using Fuzzy Logic Control for Control Effort and NVH Reduction
th International Conference on Control, Automation and Sytem Oct. 6-9, in KINTEX, Gyeonggi-do, Korea Skyhook Damper Modification Uing Fuzzy Logic Control for Control Effort and NVH Reduction Jiwon Oh and
More informationCAPACITY OF STIFFENED STEEL SHEAR PANELS AS A STRUCTURAL CONTROL DAMPER
CAPACITY OF STIFFENED STEEL SHEAR PANELS AS A STRUCTURAL CONTROL DAMPER H.B. Ge 1, K. Kaneko and T. Uami 3 1,3 Profeor, Department of Civil Engineering, Meijo Univerity, Nagoya 458-85, Japan Graduate Student,
More informationDesign spacecraft external surfaces to ensure 95 percent probability of no mission-critical failures from particle impact.
PREFERRED RELIABILITY PAGE 1 OF 6 PRACTICES METEOROIDS & SPACE DEBRIS Practice: Deign pacecraft external urface to enure 95 percent probability of no miion-critical failure from particle impact. Benefit:
More informationCHAPTER 4 DESIGN OF STATE FEEDBACK CONTROLLERS AND STATE OBSERVERS USING REDUCED ORDER MODEL
98 CHAPTER DESIGN OF STATE FEEDBACK CONTROLLERS AND STATE OBSERVERS USING REDUCED ORDER MODEL INTRODUCTION The deign of ytem uing tate pace model for the deign i called a modern control deign and it i
More informationSupplementary Figures
Supplementary Figure Supplementary Figure S1: Extraction of the SOF. The tandard deviation of meaured V xy at aturated tate (between 2.4 ka/m and 12 ka/m), V 2 d Vxy( H, j, hm ) Vxy( H, j, hm ) 2. The
More informationFinite Element Analysis of a Fiber Bragg Grating Accelerometer for Performance Optimization
Finite Element Analyi of a Fiber Bragg Grating Accelerometer for Performance Optimization N. Baumallick*, P. Biwa, K. Dagupta and S. Bandyopadhyay Fiber Optic Laboratory, Central Gla and Ceramic Reearch
More informationTHE EXPERIMENTAL ANALYSIS OF DYNAMIC PARAMETERS TO THE VIBRATING SCREEN WITH FUNCTION IN RESONANCE
THE EXPERIMENTAL ANALYSIS OF DYNAMIC PARAMETERS TO THE VIBRATING SCREEN WITH FUNCTION IN RESONANCE TONT VALENTIN, ait drd ing Univeritatea Dunarea de Jo Galati JÄGER DANIELA LIDIA, prof ing Scoala gimnaziala
More informationTHE EXPERIMENTAL PERFORMANCE OF A NONLINEAR DYNAMIC VIBRATION ABSORBER
Proceeding of IMAC XXXI Conference & Expoition on Structural Dynamic February -4 Garden Grove CA USA THE EXPERIMENTAL PERFORMANCE OF A NONLINEAR DYNAMIC VIBRATION ABSORBER Yung-Sheng Hu Neil S Ferguon
More informationModel Based Decoupling Control for Waste Incineration Plants
Model Baed Decoupling Control for Wate Incineration Plant Martin Kozek and Andrea Voigt Intitute of Mechanic and Mechatronic, Vienna Univerity of Technology, Vienna, Autria Email: kozek@impa.tuwien.ac.at
More informationStudy on the effect of vent on the electroacoustic absorber
INTER-NOISE 016 Study on the effect of vent on the electroacoutic aborber Youngeun Cho 1 ; Semyung Wang 1, Gwangju Intitute of Science and Technology, Republic of Korea ABSTRACT Electroacoutic aborber
More informationSocial Studies 201 Notes for March 18, 2005
1 Social Studie 201 Note for March 18, 2005 Etimation of a mean, mall ample ize Section 8.4, p. 501. When a reearcher ha only a mall ample ize available, the central limit theorem doe not apply to the
More information84 ZHANG Jing-Shang Vol. 39 of which would emit 5 He rather than 3 He. 5 He i untable and eparated into n + pontaneouly, which can alo be treated a if
Commun. Theor. Phy. (Beijing, China) 39 (003) pp. 83{88 c International Academic Publiher Vol. 39, No. 1, January 15, 003 Theoretical Analyi of Neutron Double-Dierential Cro Section of n+ 11 B at 14. MeV
More informationANALYTICAL BEARING MODEL FOR ANALYSIS OF INNER LOAD DISTRIBUTION AND ESTIMATION OF OPERATIONAL LUBRICATION REGIME
58 th ICMD 017 6-8 September 017, Prague, Czech Republic ANALYTICAL BEARING MODEL FOR ANALYSIS OF INNER LOAD DISTRIBUTION AND ESTIMATION OF OPERATIONAL LUBRICATION REGIME Jakub CHMELAŘ 1, Votěch DYNYBYL
More informationSoftware Verification
EXAMPLE 17 Crack Width Analyi The crack width, wk, i calculated uing the methodology decribed in the Eurocode EN 1992-1-1:2004, Section 7.3.4, which make ue of the following expreion: (1) w = ( ),max ε
More informationMolecular Dynamics Simulations of Nonequilibrium Effects Associated with Thermally Activated Exothermic Reactions
Original Paper orma, 5, 9 7, Molecular Dynamic Simulation of Nonequilibrium Effect ociated with Thermally ctivated Exothermic Reaction Jerzy GORECKI and Joanna Natalia GORECK Intitute of Phyical Chemitry,
More informationRobust Decentralized Design of H -based Frequency Stabilizer of SMES
International Energy Journal: Vol. 6, No., Part, June 005-59 Robut Decentralized Deign of H -baed Frequency Stabilizer of SMES www.erd.ait.ac.th/reric C. Vorakulpipat *, M. Leelajindakrirerk *, and I.
More informationA Constraint Propagation Algorithm for Determining the Stability Margin. The paper addresses the stability margin assessment for linear systems
A Contraint Propagation Algorithm for Determining the Stability Margin of Linear Parameter Circuit and Sytem Lubomir Kolev and Simona Filipova-Petrakieva Abtract The paper addree the tability margin aement
More informationRecent progress in fire-structure analysis
EJSE Special Iue: Selected Key Note paper from MDCMS 1 1t International Conference on Modern Deign, Contruction and Maintenance of Structure - Hanoi, Vietnam, December 2007 Recent progre in fire-tructure
More informationLecture 10 Filtering: Applied Concepts
Lecture Filtering: Applied Concept In the previou two lecture, you have learned about finite-impule-repone (FIR) and infinite-impule-repone (IIR) filter. In thee lecture, we introduced the concept of filtering
More information1 Parity. 2 Time reversal. Even. Odd. Symmetry Lecture 9
Even Odd Symmetry Lecture 9 1 Parity The normal mode of a tring have either even or odd ymmetry. Thi alo occur for tationary tate in Quantum Mechanic. The tranformation i called partiy. We previouly found
More informationArmorFlex Design Manual ABRIDGED VERSION Design Manual for ArmorFlex Articulating Concrete Blocks
Armorlex eign Manual ABRIGE VERSION 00 eign Manual for Armorlex Articulating Concrete Block . INTROUCTION Thi document i an abridged verion of the full Armorlex eign Manual, available from Armortec. Thi
More informationControl Issues for Velocity Sourced Series Elastic Actuators
Control Iue for Velocity Sourced Serie Elatic Actuator Gordon Wyeth School of Information Technology and Electrical Engineering Univerity of Queenland wyeth@itee.uq.edu.au Abtract The Serie Elaic Actuator
More informationA Study on Simulating Convolutional Codes and Turbo Codes
A Study on Simulating Convolutional Code and Turbo Code Final Report By Daniel Chang July 27, 2001 Advior: Dr. P. Kinman Executive Summary Thi project include the deign of imulation of everal convolutional
More informationFractional-Order PI Speed Control of a Two-Mass Drive System with Elastic Coupling
Fractional-Order PI Speed Control of a Two-Ma Drive Sytem with Elatic Coupling Mohammad Amin Rahimian, Mohammad Saleh Tavazoei, and Farzad Tahami Electrical Engineering Department, Sharif Univerity of
More informationNumerical Simulations of Coriolis Flow Meters for Low Reynolds Number Flows
MAPAN - Journal Numerical of Metrology Simulation Society of of Corioli India, Vol. Flow 26, Meter No. 3, 2011; for Low pp. Reynold 225-235 Number Flow ORIGINAL ARTICLE Numerical Simulation of Corioli
More informationAnalytical and Numerical Study of Foam-Filled Corrugated Core Sandwich Panels under Low Velocity Impact
Analytical and Numerical Study of Foam-Filled Corrugated Core Sandwich Panel under Low Velocity Impact Mohammad Nouri Damghani, Arah Mohammadzadeh Gonabadi To cite thi verion: Mohammad Nouri Damghani,
More informationCONTROL SYSTEMS, ROBOTICS AND AUTOMATION Vol. VIII Decoupling Control - M. Fikar
DECOUPLING CONTROL M. Fikar Department of Proce Control, Faculty of Chemical and Food Technology, Slovak Univerity of Technology in Bratilava, Radlinkého 9, SK-812 37 Bratilava, Slovakia Keyword: Decoupling:
More informationEffects of soil structure interaction on behavior of reinforced concrete structures
Journal of Structural Engineering & Applied Mechanic 18 Volume 1 Iue 1 Page 8-33 http://doi.org/1.3146/jeam.18.1833 www.goldenlightpublih.com RESEARCH ARTICLE Effect of oil tructure interaction on behavior
More informationStability. ME 344/144L Prof. R.G. Longoria Dynamic Systems and Controls/Lab. Department of Mechanical Engineering The University of Texas at Austin
Stability The tability of a ytem refer to it ability or tendency to eek a condition of tatic equilibrium after it ha been diturbed. If given a mall perturbation from the equilibrium, it i table if it return.
More informationChapter 2 Sampling and Quantization. In order to investigate sampling and quantization, the difference between analog
Chapter Sampling and Quantization.1 Analog and Digital Signal In order to invetigate ampling and quantization, the difference between analog and digital ignal mut be undertood. Analog ignal conit of continuou
More informationASPECTS OF ANALYSIS OF REVERSE FRICTION - CAUSED CONTACT PHENOMENA
ASPECTS OF ANALYSIS OF REVERSE FRICTION - CAUSED CONTACT PHENOMENA Paweł PIEC, Cracow Univerity of Technology, Cracow, Poland Staniław PYTKO, Univerity of Mining and Metallurgy, Cracow, Poland S u m m
More informationStreaming Calculations using the Point-Kernel Code RANKERN
Streaming Calculation uing the Point-Kernel Code RANKERN Steve CHUCAS, Ian CURL AEA Technology, Winfrith Technology Centre, Dorcheter, Doret DT2 8DH, UK RANKERN olve the gamma-ray tranport equation in
More informationISSN: [Basnet* et al., 6(3): March, 2017] Impact Factor: 4.116
IJESR INERNAIONAL JOURNAL OF ENGINEERING SCIENCES & RESEARCH ECHNOLOGY DIREC ORQUE CONROLLED INDUCION MOOR DRIVE FOR ORQUE RIPPLE REDUCION Bigyan Banet Department of Electrical Engineering, ribhuvan Univerity,
More informationBasics of a Quartz Crystal Microbalance
Baic of a Quartz Crytal Microbalance Introduction Thi document provide an introduction to the quartz crytal microbalance (QCM) which i an intrument that allow a uer to monitor mall ma change on an electrode.
More informationSymmetry Lecture 9. 1 Gellmann-Nishijima relation
Symmetry Lecture 9 1 Gellmann-Nihijima relation In the lat lecture we found that the Gell-mann and Nihijima relation related Baryon number, charge, and the third component of iopin. Q = [(1/2)B + T 3 ]
More informationOn the Quantum Theory of Impact Phenomenon for the Conditions of Elastic Deformation of Impacted Body
International Letter of Chemitry, Phyic and Atronomy Online: 013-04-0 ISSN: 99-3843, Vol. 1, pp 45-59 doi:10.1805/www.cipre.com/ilcpa.1.45 013 SciPre Ltd., Switzerland On the Quantum Theory of Impact Phenomenon
More informationChristian Linde Olsen Griffith University, Faculty of Engineering and Information Technology, Gold Coast Campus.
1 Abtract Rubble Mound Breakwater Chritian Linde Olen Griffith Univerity, Faculty of Engineering and Information Technology, Gold Coat Campu. 1. Abtract The paper deal with the deign of a rubble mound
More informationLTV System Modelling
Helinki Univerit of Technolog S-72.333 Potgraduate Coure in Radiocommunication Fall 2000 LTV Stem Modelling Heikki Lorentz Sonera Entrum O heikki.lorentz@onera.fi Januar 23 rd 200 Content. Introduction
More informationHalliday/Resnick/Walker 7e Chapter 6
HRW 7e Chapter 6 Page of Halliday/Renick/Walker 7e Chapter 6 3. We do not conider the poibility that the bureau might tip, and treat thi a a purely horizontal motion problem (with the peron puh F in the
More informationMAXIMUM BENDING MOMENT AND DUCTILITY OF R/HPFRCC BEAMS
MAXIMUM BENDING MOMENT AND DUCTILITY OF R/HPFRCC BEAMS Aleandro P. Fantilli 1, Hirozo Mihahi 2 and Paolo Vallini 1 (1) Politecnico di Torino, Torino, Italy (2) Tohoku Univerity, Sendai, Japan Abtract The
More informationA Simplified Methodology for the Synthesis of Adaptive Flight Control Systems
A Simplified Methodology for the Synthei of Adaptive Flight Control Sytem J.ROUSHANIAN, F.NADJAFI Department of Mechanical Engineering KNT Univerity of Technology 3Mirdamad St. Tehran IRAN Abtract- A implified
More informationDimension Effect on Dynamic Stress Equilibrium in SHPB Tests
International Journal of Material Phyic. ISSN 97-39X Volume 5, Numer 1 (1), pp. 15- International Reearch Pulication Houe http://www.irphoue.com Dimenion Effect on Dynamic Stre Equilirium in SHPB Tet Department
More informationConvective Heat Transfer
Convective Heat Tranfer Example 1. Melt Spinning of Polymer fiber 2. Heat tranfer in a Condener 3. Temperature control of a Re-entry vehicle Fiber pinning The fiber pinning proce preent a unique engineering
More informationHSC PHYSICS ONLINE KINEMATICS EXPERIMENT
HSC PHYSICS ONLINE KINEMATICS EXPERIMENT RECTILINEAR MOTION WITH UNIFORM ACCELERATION Ball rolling down a ramp Aim To perform an experiment and do a detailed analyi of the numerical reult for the rectilinear
More informationSIMULATING THE STRESS AND STRAIN BEHAVIOR OF LOESS VIA SCC MODEL
SIMULATING THE STRESS AND STRAIN BEHAVIOR OF LOESS VIA SCC MODEL M.D. LIU Faculty of Engineering, Univerity of Wollongong, Autralia, martindl@uow.edu.au J. LIU Faculty of Engineering, Univerity of Wollongong,
More informationRupro, breach model used by Cemagref during Impact project
PAQUIER 1 Rupro, breach model ued by Cemagref during Impact project A PAQUIER Cemagref, France andre.paquier@cemagref.fr SUMMARY For embankment dam, piping and overtopping failure are the mot frequent
More informationAMS 212B Perturbation Methods Lecture 20 Part 1 Copyright by Hongyun Wang, UCSC. is the kinematic viscosity and ˆp = p ρ 0
Lecture Part 1 Copyright by Hongyun Wang, UCSC Prandtl boundary layer Navier-Stoke equation: Conervation of ma: ρ t + ( ρ u) = Balance of momentum: u ρ t + u = p+ µδ u + ( λ + µ ) u where µ i the firt
More informationSTRAIN LIMITS FOR PLASTIC HINGE REGIONS OF CONCRETE REINFORCED COLUMNS
13 th World Conerence on Earthquake Engineering Vancouver, B.C., Canada Augut 1-6, 004 Paper No. 589 STRAIN LIMITS FOR PLASTIC HINGE REGIONS OF CONCRETE REINFORCED COLUMNS Rebeccah RUSSELL 1, Adolo MATAMOROS,
More informationImproving the Efficiency of a Digital Filtering Scheme for Diabatic Initialization
1976 MONTHLY WEATHER REVIEW VOLUME 15 Improving the Efficiency of a Digital Filtering Scheme for Diabatic Initialization PETER LYNCH Met Éireann, Dublin, Ireland DOMINIQUE GIARD CNRM/GMAP, Météo-France,
More informationCalculation of the temperature of boundary layer beside wall with time-dependent heat transfer coefficient
Ŕ periodica polytechnica Mechanical Engineering 54/1 21 15 2 doi: 1.3311/pp.me.21-1.3 web: http:// www.pp.bme.hu/ me c Periodica Polytechnica 21 RESERCH RTICLE Calculation of the temperature of boundary
More informationMechanics. Free rotational oscillations. LD Physics Leaflets P Measuring with a hand-held stop-clock. Oscillations Torsion pendulum
Mechanic Ocillation Torion pendulum LD Phyic Leaflet P.5.. Free rotational ocillation Meauring with a hand-held top-clock Object of the experiment g Meauring the amplitude of rotational ocillation a function
More informationSocial Studies 201 Notes for November 14, 2003
1 Social Studie 201 Note for November 14, 2003 Etimation of a mean, mall ample ize Section 8.4, p. 501. When a reearcher ha only a mall ample ize available, the central limit theorem doe not apply to the
More informationEarth Potential Rise (EPR) Computation for a Fault on Transmission Mains Pole
ACN: 32586675 ABN: 8632586675 NATIONAL ELECTRICAL ENGINEERING CONULTANCY Earth otential Rie (ER) Computation for a Fault on Tranmiion Main ole repared by: M. Naereddine ACN: 32586675 ABN: 8632586675 Abtract
More informationTuned vibration absorbers for control of noise radiated by a panel
Proceeding of ACOUSICS 9 3-5 November 9, Adelaide, Autralia uned vibration aborber for control of noie radiated by a panel Swee S. Kuik, Carl Q. Howard, Colin H. Hanen & Anthony C. Zander School of echanical
More information6.447 rad/sec and ln (% OS /100) tan Thus pc. the testing point is s 3.33 j5.519
9. a. 3.33, n T ln(% OS /100) 2 2 ln (% OS /100) 0.517. Thu n 6.7 rad/ec and the teting point i 3.33 j5.519. b. Summation of angle including the compenating zero i -106.691, The compenator pole mut contribute
More informationMULTI-LAYERED LOSSY FINITE LENGTH DIELECTRIC CYLINDIRICAL MODEL OF MAN AT OBLIQUE INCIDENCE
Proceeding 3rd Annual Conference IEEE/EMBS Oct.5-8, 1, Itanbul, TURKEY MULTI-LAYERED LOSSY FINITE LENGTH DIELECTRIC CYLINDIRICAL MODEL OF MAN AT OBLIQUE INCIDENCE S.S. Şeker, B. Yeldiren Boğaziçi Univerity,
More informationRobust Mould Level Control
5 American Control Conference June 8-1, 5. Portland, OR, USA ThA9.4 Robut Mould Level Control J. Schuurman, A. Kamperman, B. Middel, P.F.A van den Boch Abtract In the firt year of production ince, the
More informationSimulation Study on the Shock Properties of the Double-Degree-of-Freedom Cushioning Packaging System
Proceeding of the 7th IAPRI World Conference on Packaging Simulation Study on the Shock Propertie of the Double-Degree-of-Freedom Cuhioning Packaging Sytem Xia Zhu, Qiaoqiao Yan, Xiaoling Yao, Junbin Chen,
More informationDYNAMIC MODELS FOR CONTROLLER DESIGN
DYNAMIC MODELS FOR CONTROLLER DESIGN M.T. Tham (996,999) Dept. of Chemical and Proce Engineering Newcatle upon Tyne, NE 7RU, UK.. INTRODUCTION The problem of deigning a good control ytem i baically that
More informationDesign of Digital Filters
Deign of Digital Filter Paley-Wiener Theorem [ ] ( ) If h n i a caual energy ignal, then ln H e dω< B where B i a finite upper bound. One implication of the Paley-Wiener theorem i that a tranfer function
More informationA FUNCTIONAL BAYESIAN METHOD FOR THE SOLUTION OF INVERSE PROBLEMS WITH SPATIO-TEMPORAL PARAMETERS AUTHORS: CORRESPONDENCE: ABSTRACT
A FUNCTIONAL BAYESIAN METHOD FOR THE SOLUTION OF INVERSE PROBLEMS WITH SPATIO-TEMPORAL PARAMETERS AUTHORS: Zenon Medina-Cetina International Centre for Geohazard / Norwegian Geotechnical Intitute Roger
More informationSMALL-SIGNAL STABILITY ASSESSMENT OF THE EUROPEAN POWER SYSTEM BASED ON ADVANCED NEURAL NETWORK METHOD
SMALL-SIGNAL STABILITY ASSESSMENT OF THE EUROPEAN POWER SYSTEM BASED ON ADVANCED NEURAL NETWORK METHOD S.P. Teeuwen, I. Erlich U. Bachmann Univerity of Duiburg, Germany Department of Electrical Power Sytem
More informationLateral vibration of footbridges under crowd-loading: Continuous crowd modeling approach
ateral vibration of footbridge under crowd-loading: Continuou crowd modeling approach Joanna Bodgi, a, Silvano Erlicher,b and Pierre Argoul,c Intitut NAVIER, ENPC, 6 et 8 av. B. Pacal, Cité Decarte, Champ
More informationTrellis Shaping Techniques for Satellite Telecommunication Systems
> 1 Trelli Technique for Satellite Telecommunication Sytem M. Álvarez-Díaz 1, M. Neri, C. Moquera 1 and G. E. Corazza 1 Dept. Signal Theory and Communication (TSC), Univerity of Vigo Campu Univeritario
More informationCollision Planar Impact Analysis
Colliion Planar Impact Analyi Thi colliion model i baed on the Planar Impact Mechanic Model (PIM) of Raymond M. Brach. The PIM model i a time forward calculation that input linear and angular velocite
More informationSEISMIC STRENGTH REDUCTION FACTOR FOR SINGLE AND MULTI-STOREY SHEAR BUILDINGS CONSIDERING SOIL- STRUCTURE INTERACTION
SEISMIC STRENGTH REDUCTION FACTOR FOR SINGLE AND MULTI-STOREY SHEAR BUILDINGS CONSIDERING SOIL- STRUCTURE INTERACTION Yang LU, Iman HAJIRASOULIHA * and Alec M. MARSHALL ABSTRACT A parametric analyi ha
More informationReal Sources (Secondary Sources) Phantom Source (Primary source) LS P. h rl. h rr. h ll. h lr. h pl. h pr
Ecient frequency domain ltered-x realization of phantom ource iet C.W. ommen, Ronald M. Aart, Alexander W.M. Mathijen, John Gara, Haiyan He Abtract A phantom ound ource i a virtual ound image which can
More informationCumulative Review of Calculus
Cumulative Review of Calculu. Uing the limit definition of the lope of a tangent, determine the lope of the tangent to each curve at the given point. a. f 5,, 5 f,, f, f 5,,,. The poition, in metre, of
More informationChapter 12 Radiation Heat Transfer. Special Topic: Heat Transfer from the Human Body
Chapter 1 Radiation Heat ranfer Special opic: Heat ranfer from the Human Body 1-7C Ye, roughly one-third of the metabolic heat generated by a peron who i reting or doing light work i diipated to the environment
More information