MODELLING, SIMULATION AND OPTIMIZATION OF DAMPING

Size: px
Start display at page:

Download "MODELLING, SIMULATION AND OPTIMIZATION OF DAMPING"

Transcription

1 MODELLNG SMULAON AND OPMZAON O DAMPNG Jiří Vondřich Evžen hőnde Departent of Eectric Drives and raction acut of Eectrica Engineering zech echnica Universit in Prague Astract Modeing siuation and optiization of different sstes were an integra part of the design and construction of sstes he diagra docuenting a phenoena infuencing ehaviour of the sste arrangeent a set of dnaic equations and creating a siuation nuerica ode are the prerequisites for creating a functiona and credie siuation ode Viration in sstes has two effects irst the ver high pea acceerations can ean that the effective weight of the viration sstes increases severa-fod and this a cause its destruction Second peope near the sstes fee these acceerations which can e uncofortae or even dangerous A viration ass is used to protect the sstes fro stead-state haronic disturance Depending on the driving frequenc of the origina sste the virating ass needs to e carefu tuned that is to choose adequate vaues of stiffness daping and eventua ass so that otion of the origina ass is a iniu he tuneae viration asorer is advantageous priari in that reduces the apitude of virations in the sstes for eape unaanced rotors cran gear cearances in earings osciation of the oving driven parts transient oading diverging and coasting of driving otors etc he present artice wi discuss the ethod onine optiization of the viration and daping contro for sstes using a viration tuneae ass with daping he anases and Mata -fie for the auto-tuning contro have een used he ai of the paper is to acquaint the reader with the design of the incorporated asorer to the viration sste which aes the suppression of the viration of the sstes to a iniu possie he resuting vertica trajector and acceeration of the car od showed that asorption using a springs and dapers reduces the viration apitude of the car od ar od virations on uneven highwas affect car ifetie passenger cofort and in turn cause daage to the road Asorption sste reduces these negative infuences and considera iproves the driving properties of the car t is possie to change the paraeters of the springs whie driving and thus contro the driving properties and cofort Before the reaization of viration asorption in a echanica arrangeent it is iportant to carr out a nuerica soution he nuerica soution for car od asorption in cooperation with the Mata-Siuin progra is shown on ode of the car Mode of the Sste On the ig is shown the ode of the car with four degrees of freedo 3 4 he car is oving on uneven road dispaceent st s cos Ωt ro the road then acting on the ripe force t s Ω cos Ωt ψ cos Ωt s Ω ψ Ω ψ n the tie t is the force t aiu and then dispaceent ψ he force acting on the ripe fro the road is t cosωt

2 he reations aong the degree of freedo are ig φ 3 4 st igure : Mode of the car with tires oving on uneven road Miniize criterion Equation of otion of this sste is t t 6 We introduce now 7 hen equation of otion is 8

3 Equations of otion 8 are aso possie written in the for B A 9 B A When we introduce Lapace transforation we otain B A p he transfer function Gp then fro equations is B A p Where the transfer function has for A G p p When optiizing the response of an eisting sste it is conventiona to iniize the aiu response he iniize criterion is in a p G 3 he Siuin schee of the soution and optiization is shown on the ig igure :Siuin schee of the daping of the car

4 3 Resuts and concusion On the ig 3 is shown soution of the iniize criterion 3 of the transfer function igure 3: Apitude characteristic of the soution of iniize criterion he paraeters of the ode are g 3 5 g 4 3 g 9 g N - N - 3 Ns - 8 Ns - s Ω565 s - On the ig 4 are shown the dispaceents of four degrees of freedo 3 4 after using the iniize criterion 3 he aiu apitude of the dispaceent of the car od is 65 he aiu apitude of the dispaceent φ of the car od is rad he aiu apitude of the dispaceent 3 of the ae 3 is 35 he aiu apitude of the dispaceent 4 of the ae 4 is 35

5 igure 4: Dispaceents of the car od and dispaceents of the car aes 3 and 4 References [] Author Jiří Vondřich Departent of Eectric Drives and raction acut of Eectrica Engineering zech echnica Universit in Prague echnica 66 7 Prague 6 vondrich@fecvutcz Author Evžen hőnde Departent of Eectric Drives and raction acut of Eectrica Engineering zech echnica Universit in Prague echnica 66 7 Prague 6 thonde@fecvutcz

OSCILLATIONS. dt x = (1) Where = k m

OSCILLATIONS. dt x = (1) Where = k m OSCILLATIONS Periodic Motion. Any otion, which repeats itsef at reguar interva of tie, is caed a periodic otion. Eg: 1) Rotation of earth around sun. 2) Vibrations of a sipe penduu. 3) Rotation of eectron

More information

14 - OSCILLATIONS Page 1

14 - OSCILLATIONS Page 1 14 - OSCILLATIONS Page 1 14.1 Perioic an Osciator otion Motion of a sste at reguar interva of tie on a efinite path about a efinite point is known as a perioic otion, e.g., unifor circuar otion of a partice.

More information

Wave Motion: revision. Professor Guy Wilkinson Trinity Term 2014

Wave Motion: revision. Professor Guy Wilkinson Trinity Term 2014 Wave Motion: revision Professor Gu Wiinson gu.wiinson@phsics.o.a.u Trinit Ter 4 Introduction Two ectures to reind ourseves of what we earned ast ter Wi restrict discussion to the topics on the sabus Wi

More information

Design and System Modeling of a Tri-Axial Microaccelerometer Using Piezoelectric Thin Films

Design and System Modeling of a Tri-Axial Microaccelerometer Using Piezoelectric Thin Films Ferroeectrics, 85:, 69 74, 009 Reprints avaiae directy fro the puisher DOI:.80/00509090888764 URL: http://dx.doi.org/.80/00509090888764 69 Jyh-Cheng Yu et a. 009 Tayor & Francis ISSN: 005-09 print / 56-5

More information

OSCILLATIONS. Syllabus :

OSCILLATIONS. Syllabus : Einstein Casses, Unit No. 0, 0, Vardhan Rin Road Paza, Vias Puri Extn., Outer Rin Road New Dehi 0 08, Ph. : 96905, 857 PO OSCILLATIONS Sabus : Periodic otion period, dispaceent as a function of tie. Period

More information

Part IA Paper 1: Mechanical Engineering MECHANICAL VIBRATIONS Examples paper 3

Part IA Paper 1: Mechanical Engineering MECHANICAL VIBRATIONS Examples paper 3 ENGINEERING Part IA Paper 1: Mechanical Engineering MECHANICAL VIBRATIONS Exaples paper 3 IRST YEAR Straightforward questions are ared with a Tripos standard questions are ared *. Systes with two or ore

More information

University of Alabama Department of Physics and Astronomy. PH 105 LeClair Summer Problem Set 11

University of Alabama Department of Physics and Astronomy. PH 105 LeClair Summer Problem Set 11 University of Aabaa Departent of Physics and Astronoy PH 05 LeCair Suer 0 Instructions: Probe Set. Answer a questions beow. A questions have equa weight.. Due Fri June 0 at the start of ecture, or eectronicay

More information

Chapter 2: Introduction to Damping in Free and Forced Vibrations

Chapter 2: Introduction to Damping in Free and Forced Vibrations Chapter 2: Introduction to Daping in Free and Forced Vibrations This chapter ainly deals with the effect of daping in two conditions like free and forced excitation of echanical systes. Daping plays an

More information

Modeling of vibration systems

Modeling of vibration systems Modeling of vibration systes Atual syste Mae design deision Choose physial paraeters, hange or augent syste if neessary Physial odeling Mae siple approiations based on engineering judgeent Physial odel

More information

CHAPTER 14: Oscillations. Answers to Questions. l. The length, l, is the distance from the center of the tire to the branch.

CHAPTER 14: Oscillations. Answers to Questions. l. The length, l, is the distance from the center of the tire to the branch. CHAPTER 4: Osciations Answers to Questions. Eapes are: a chid s swing (SHM, for sa osciations), stereo speaers (copicated otion, the addition of any SHMs), the bade on a jigsaw (approiatey SHM), the string

More information

EN40: Dynamics and Vibrations. Final Examination Monday May : 2pm-5pm

EN40: Dynamics and Vibrations. Final Examination Monday May : 2pm-5pm EN40: Dynaics and Vibrations Final Exaination Monday May 13 013: p-5p School of Engineering Brown University NAME: General Instructions No collaboration of any kind is peritted on this exaination. You

More information

A STUDY OF THE DESIGN OF A CANTILEVER TYPE MULTI-D.O.F. DYNAMIC VIBRATION ABSORBER FOR MICRO MACHINE TOOLS

A STUDY OF THE DESIGN OF A CANTILEVER TYPE MULTI-D.O.F. DYNAMIC VIBRATION ABSORBER FOR MICRO MACHINE TOOLS ICSV4 Cairns Australia 9- Jul, 7 A STUDY OF THE DESIGN OF A CANTILEVER TYPE MULTI-D.O.F. DYNAMIC VIBRATION ABSORBER FOR MICRO MACHINE TOOLS Sung-Hun Jang, Sung-Min Ki, Shil-Geun Ki,Young-Hu Choi and Jong-Kwon

More information

Physics 201 Lecture 29

Physics 201 Lecture 29 Phsics 1 ecture 9 Goals ecture 9 v Describe oscillator otion in a siple pendulu v Describe oscillator otion with torques v Introduce daping in SHM v Discuss resonance v Final Ea Details l Sunda, Ma 13th

More information

TRACKING CONTROL FOR WHEELED MOBILE ROBOTS USING NEURAL NETWORK MODEL ALGORITHM CONTROL

TRACKING CONTROL FOR WHEELED MOBILE ROBOTS USING NEURAL NETWORK MODEL ALGORITHM CONTROL Journa of Theoretica and Appied Inforation Technoogy 3 st Deceber. Vo. 46 No. 5 - JATIT & LLS. A rights reserved. ISSN: 99-8645 www.jatit.org E-ISSN: 87-395 TRACKING CONTROL FOR WHEELED OBILE ROBOTS USING

More information

EFFECTIVE MODAL MASS & MODAL PARTICIPATION FACTORS Revision I

EFFECTIVE MODAL MASS & MODAL PARTICIPATION FACTORS Revision I EFFECTIVE MODA MASS & MODA PARTICIPATION FACTORS Revision I B To Irvine Eail: to@vibrationdata.co Deceber, 5 Introduction The effective odal ass provides a ethod for judging the significance of a vibration

More information

T m. Fapplied. Thur Oct 29. ω = 2πf f = (ω/2π) T = 1/f. k m. ω =

T m. Fapplied. Thur Oct 29. ω = 2πf f = (ω/2π) T = 1/f. k m. ω = Thur Oct 9 Assignent 10 Mass-Spring Kineatics (x, v, a, t) Dynaics (F,, a) Tie dependence Energy Pendulu Daping and Resonances x Acos( ωt) = v = Aω sin( ωt) a = Aω cos( ωt) ω = spring k f spring = 1 k

More information

Chapter 1: Basics of Vibrations for Simple Mechanical Systems

Chapter 1: Basics of Vibrations for Simple Mechanical Systems Chapter 1: Basics of Vibrations for Siple Mechanical Systes Introduction: The fundaentals of Sound and Vibrations are part of the broader field of echanics, with strong connections to classical echanics,

More information

Simple Harmonic Motion (SHM)

Simple Harmonic Motion (SHM) Phsics Sipe Haronic Motion (SHM) www.testprepart.co abe of Content. Periodic otion.. Osciator or Vibrator otion. 3. Haronic and Non-haronic osciation. 4. Soe iportant definitions. 5. Sipe haronic otion.

More information

Independent Joint Control

Independent Joint Control ME135 ADANCED OBOICS Independent oint Contro ee-hwan yu Schoo of Mechanica Engineering Introduction to Contro Contro: deterining the tie hitory of joint input to do a coanded otion Contro ethod are depend

More information

Join discussion of this test paper at

Join discussion of this test paper at SECTION - 1. This question consists of TWENTY-FIVE sub-questions (1.1 1.5) of ONE ark each. For each of these sub-questions, four possibe aternatives (,, C and D) are given, out of which ONLY ONE is correct.

More information

Simple Harmonic Motion

Simple Harmonic Motion Siple Haronic Motion Physics Enhanceent Prograe for Gifted Students The Hong Kong Acadey for Gifted Education and Departent of Physics, HKBU Departent of Physics Siple haronic otion In echanical physics,

More information

ACCUMULATION OF FLUID FLOW ENERGY BY VIBRATIONS EXCITATION IN SYSTEM WITH TWO DEGREE OF FREEDOM

ACCUMULATION OF FLUID FLOW ENERGY BY VIBRATIONS EXCITATION IN SYSTEM WITH TWO DEGREE OF FREEDOM ENGINEERING FOR RURAL DEVELOPMENT Jelgava, 9.-.5.8. ACCUMULATION OF FLUID FLOW ENERGY BY VIBRATION EXCITATION IN YTEM WITH TWO DEGREE OF FREEDOM Maris Eiduks, Janis Viba, Lauris tals Riga Technical University,

More information

Slovak University of Technology in Bratislava Institute of Information Engineering, Automation, and Mathematics PROCEEDINGS

Slovak University of Technology in Bratislava Institute of Information Engineering, Automation, and Mathematics PROCEEDINGS Slova University of echnology in Bratislava Institute of Inforation Engineering, Autoation, and Matheatics PROCEEINGS of the 8 th International Conference on Process Control Hotel itris, atransá Lonica,

More information

Oscillatory Hydromagnetic Couette Flow in a Rotating System with Induced Magnetic Field *

Oscillatory Hydromagnetic Couette Flow in a Rotating System with Induced Magnetic Field * CHAPTER-4 Oscillator Hdroagnetic Couette Flow in a Rotating Sste with Induced Magnetic Field * 4. Introduction Lainar flow within a channel or duct in the absence of agnetic field is a phenoenon which

More information

Oscillations: Review (Chapter 12)

Oscillations: Review (Chapter 12) Oscillations: Review (Chapter 1) Oscillations: otions that are periodic in tie (i.e. repetitive) o Swinging object (pendulu) o Vibrating object (spring, guitar string, etc.) o Part of ediu (i.e. string,

More information

MATHEMATICAL MODEL OF THE ENERGETIC CONSUMPTION FOR SOIL DIGGING MACHINES IN GREENHOUSES

MATHEMATICAL MODEL OF THE ENERGETIC CONSUMPTION FOR SOIL DIGGING MACHINES IN GREENHOUSES Bulletin of the Transilvania University of Braşov Vol. 3 (5) - 00 Series II: Forestry Wood Industry Agricultural Food Engineering MATHEMATICAL MODEL OF THE ENERGETIC CONSUMPTION FOR SOIL DIGGING MACHINES

More information

PHY 140Y FOUNDATIONS OF PHYSICS Tutorial Questions #9 Solutions November 12/13

PHY 140Y FOUNDATIONS OF PHYSICS Tutorial Questions #9 Solutions November 12/13 PHY 4Y FOUNDAIONS OF PHYSICS - utorial Questions #9 Solutions Noveber /3 Conservation of Ener and Sprins. One end of a assless sprin is placed on a flat surface, with the other end pointin upward, as shown

More information

Multi ultrasonic actuators with some degree of freedom

Multi ultrasonic actuators with some degree of freedom 005 WA Int. Conf. on DYNAMICAL YM and CONROL, enice, Italy, Noveer -4, 005 (pp609-63) Multi ultrasonic actuators with soe degree of freedo G. KULII, D. MAZIKA, I. UMAONIN 3 ilnius Gediinas echnical University

More information

Session : Electrodynamic Tethers

Session : Electrodynamic Tethers Session : Eectrodynaic Tethers Eectrodynaic tethers are ong, thin conductive wires depoyed in space that can be used to generate power by reoving kinetic energy fro their orbita otion, or to produce thrust

More information

SHM stuff the story continues

SHM stuff the story continues SHM stuff the story continues Siple haronic Motion && + ω solution A cos t ( ω + α ) Siple haronic Motion + viscous daping b & + ω & + Viscous daping force A e b t Viscous daped aplitude Viscous daped

More information

In this chapter we will study sound waves and concentrate on the following topics:

In this chapter we will study sound waves and concentrate on the following topics: Chapter 17 Waves II In this chapter we will study sound waves and concentrate on the following topics: Speed of sound waves Relation between displaceent and pressure aplitude Interference of sound waves

More information

A. Mitra 1, N. Benerjee 1, H. A. Khalane 2, M. A. Sonawane 2, D. R. Joshi 2, G.R. Bagul 2

A. Mitra 1, N. Benerjee 1, H. A. Khalane 2, M. A. Sonawane 2, D. R. Joshi 2, G.R. Bagul 2 OSR Journal of Mechanical and ivil Engineering (OSR-JME) SSN(e) : 78-684, SSN(p) : 3 334X, PP : -33 www.iojournals.org Siulation and Analysis of Full ar Model for various Road profile on a analytically

More information

CHAOTIC BEHAVIOR OF MECHANICAL VIBRO IMPACT SYSTEM WITH TWO DEGREES OF FREEDOM AND POSSIBILITIES OF CHAOTIC BEHAVIOR OF QUARTER VEHICLE MODEL

CHAOTIC BEHAVIOR OF MECHANICAL VIBRO IMPACT SYSTEM WITH TWO DEGREES OF FREEDOM AND POSSIBILITIES OF CHAOTIC BEHAVIOR OF QUARTER VEHICLE MODEL REGIONAL WORKSHOP TRANSPORT RESEARCH AND BUSINESS COOPERATION IN SEE 6-7 Deceber 00, Sofia CHAOTIC BEHAVIOR OF MECHANICAL VIBRO IMPACT SYSTEM WITH TWO DEGREES OF FREEDOM AND POSSIBILITIES OF CHAOTIC BEHAVIOR

More information

Forced Mechanical Oscillations

Forced Mechanical Oscillations 9 Carl von Ossietzky University Oldenurg Faculty V - Institute of Physics Module Introductory Laoratory Course Physics Part I Forced Mechanical Oscillations Keywords: HOOKE's law, haronic oscillation,

More information

Physics 2107 Oscillations using Springs Experiment 2

Physics 2107 Oscillations using Springs Experiment 2 PY07 Oscillations using Springs Experient Physics 07 Oscillations using Springs Experient Prelab Read the following bacground/setup and ensure you are failiar with the concepts and theory required for

More information

AN INVESTIGATION ON SEISMIC ANALYSIS OF SHALLOW TUNEELS IN SOIL MEDIUM

AN INVESTIGATION ON SEISMIC ANALYSIS OF SHALLOW TUNEELS IN SOIL MEDIUM The 4 th October -7, 8, Beijing, China AN INVESTIGATION ON SEISMIC ANALYSIS OF SHALLOW TUNEELS IN SOIL MEDIUM J. Boouri Bazaz and V. Besharat Assistant Professor, Dept. of Civi Engineering, Ferdowsi University,

More information

MODELLING OF VIBRATION WITH ABSORBER

MODELLING OF VIBRATION WITH ABSORBER Journal of Machine Engineering, Vol. 10, No.4, 2010 mumerical modelling, Simulink, vibration, machine, absorber Jiří VONDŘICH 1 Evžen THÖNDE 1 Slavomír JIRKŮ 1 MODEING OF VIBRATION WITH ABSORBER Machine

More information

ME Machine Design I. FINAL EXAM. OPEN BOOK AND CLOSED NOTES. Friday, May 8th, 2009

ME Machine Design I. FINAL EXAM. OPEN BOOK AND CLOSED NOTES. Friday, May 8th, 2009 ME 5 - Machine Design I Spring Seester 009 Nae Lab. Div. FINAL EXAM. OPEN BOOK AND LOSED NOTES. Friday, May 8th, 009 Please use the blank paper for your solutions. Write on one side of the paper only.

More information

Seismic Analysis of Structures by TK Dutta, Civil Department, IIT Delhi, New Delhi.

Seismic Analysis of Structures by TK Dutta, Civil Department, IIT Delhi, New Delhi. Seisic Analysis of Structures by K Dutta, Civil Departent, II Delhi, New Delhi. Module 5: Response Spectru Method of Analysis Exercise Probles : 5.8. or the stick odel of a building shear frae shown in

More information

Modeling & Analysis of the International Space Station

Modeling & Analysis of the International Space Station Modeling & Analysis of the International Space Station 1 Physical Syste Solar Alpha Rotary Joints Physical Syste Rotor Stator Gear Train Solar Array Inboard Body Outboard Body +x Solar Array 3 Physical

More information

TOPIC E: OSCILLATIONS SPRING 2018

TOPIC E: OSCILLATIONS SPRING 2018 TOPIC E: OSCILLATIONS SPRING 018 1. Introduction 1.1 Overview 1. Degrees of freedo 1.3 Siple haronic otion. Undaped free oscillation.1 Generalised ass-spring syste: siple haronic otion. Natural frequency

More information

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

On some problems of synthesis of spatial five-bar hinged mechanisms with two degrees of freedom Internationa Journa of Mechanica Engineering and Appications 014 (6): 104-110 Puished onine ecemer 18, 014 (http://www.sciencepuishinggroup.com/j/ijmea) doi: 10.11648/j.ijmea.014006.14 ISSN: 330-03X (Print)

More information

PHYS 1443 Section 003 Lecture #22

PHYS 1443 Section 003 Lecture #22 PHYS 443 Section 003 Lecture # Monda, Nov. 4, 003. Siple Bloc-Spring Sste. Energ of the Siple Haronic Oscillator 3. Pendulu Siple Pendulu Phsical Pendulu orsion Pendulu 4. Siple Haronic Motion and Unifor

More information

AN ANALYTICAL ESTIMATION OF THE CORIOLIS METER'S CHARACTERISTICS BASED ON MODAL SUPERPOSITION. J. Kutin *, I. Bajsić

AN ANALYTICAL ESTIMATION OF THE CORIOLIS METER'S CHARACTERISTICS BASED ON MODAL SUPERPOSITION. J. Kutin *, I. Bajsić Fow Measureent and Instruentation 1 (00) 345 351 doi:10.1016/s0955-5986(0)00006-7 00 Esevier Science Ltd. AN ANALYTICAL ESTIMATION OF THE CORIOLIS METER'S CHARACTERISTICS BASED ON MODAL SUPERPOSITION J.

More information

ACTIVE VIBRATION CONTROL FOR STRUCTURE HAVING NON- LINEAR BEHAVIOR UNDER EARTHQUAKE EXCITATION

ACTIVE VIBRATION CONTROL FOR STRUCTURE HAVING NON- LINEAR BEHAVIOR UNDER EARTHQUAKE EXCITATION International onference on Earthquae Engineering and Disaster itigation, Jaarta, April 14-15, 8 ATIVE VIBRATION ONTROL FOR TRUTURE HAVING NON- LINEAR BEHAVIOR UNDER EARTHQUAE EXITATION Herlien D. etio

More information

Experimental Measurement of Magnetization of a Rectangular Bar-shaped Permanent Magnet Utilizing MFMIM

Experimental Measurement of Magnetization of a Rectangular Bar-shaped Permanent Magnet Utilizing MFMIM ostafa Kair et a. Experienta easureent of agnetization of Origina Artice Experienta easureent of agnetization of a Rectanguar Bar-shaped Peranent agnet Utiizing FI. Kair,. R. ashayehi, S. Aftai 3,. Khodajou-Choai

More information

Design of a Single Input Fuzzy Logic Controller Based SVC for Dynamic Performance Enhancement of Power Systems

Design of a Single Input Fuzzy Logic Controller Based SVC for Dynamic Performance Enhancement of Power Systems Design of a Singe Input Fuzzy Logic Controer Based SC for Dynaic Perforance Enhanceent of Power Systes DR.D. PADMA SUBRAMANIAN PROFESSOR AND DEAN, DEPARTMENT OF ELECTRICAL AND ELECTRONICS ENGINEERING AMET

More information

Part B: Many-Particle Angular Momentum Operators.

Part B: Many-Particle Angular Momentum Operators. Part B: Man-Partice Anguar Moentu Operators. The coutation reations deterine the properties of the anguar oentu and spin operators. The are copete anaogous: L, L = i L, etc. L = L ± il ± L = L L L L =

More information

The Application of Euler Lagrange Method of Optimization for Electromechanical Motion Control

The Application of Euler Lagrange Method of Optimization for Electromechanical Motion Control HE ANNAS OF "DUNAREA DE OS" UNIVERSIY OF GAAI FASCICE III, ISSN -454X EECROECHNICS, EECRONICS, AUOMAIC CONRO, INFORMAICS he Application o Euler agrange Metho o Optiization or Electroechanical Motion Control

More information

Design and Experimental Research of Atomizer Based on Micro Abrasive Ultrasonic Polishing Bang-fu WANG, Yin ZHEN, Juan SONG and A-chun ZHU

Design and Experimental Research of Atomizer Based on Micro Abrasive Ultrasonic Polishing Bang-fu WANG, Yin ZHEN, Juan SONG and A-chun ZHU 217 3rd International Conference on Applied Mechanics and Mechanical Autoation (AMMA 217) ISBN: 978-1-6595-479- Design and Experiental Research of Atoizer Based on Micro Abrasive Ultrasonic Polishing Bang-fu

More information

Convergence P H Y S I C S

Convergence P H Y S I C S +1 Test (Newton s Law of Motion) 1. Inertia is that property of a body by virtue of which the body is (a) Unabe to change by itsef the state of rest (b) Unabe to change by itsef the state of unifor otion

More information

A Simulation Study for Practical Control of a Quadrotor

A Simulation Study for Practical Control of a Quadrotor A Siulation Study for Practical Control of a Quadrotor Jeongho Noh* and Yongkyu Song** *Graduate student, Ph.D. progra, ** Ph.D., Professor Departent of Aerospace and Mechanical Engineering, Korea Aerospace

More information

HO 25 Solutions. = s. = 296 kg s 2. = ( kg) s. = 2π m k and T = 2π ω. kg m = m kg. = 2π. = ω 2 A = 2πf

HO 25 Solutions. = s. = 296 kg s 2. = ( kg) s. = 2π m k and T = 2π ω. kg m = m kg. = 2π. = ω 2 A = 2πf HO 5 Soution 1.) haronic ociator = 0.300 g with an idea pring T = 0.00 T = π T π π o = = ( 0.300 g) 0.00 = 96 g = 96 N.) haronic ociator = 0.00 g and idea pring = 140 N F = x = a = d x dt o the dipaceent

More information

Research on the Nonlinear Governor of Diesel Engine with Variable Structure Control Theory

Research on the Nonlinear Governor of Diesel Engine with Variable Structure Control Theory Research on the Noninear Governor of Diese Engine with Variabe Structure Contro Theory Xiao-Bing Mao schoo of energy and power engineering wuhan university of technoogy Wuhan, China aoxiaobing@.co Kai-Sheng

More information

Dynamic analysis of frames with viscoelastic dampers: a comparison of damper models

Dynamic analysis of frames with viscoelastic dampers: a comparison of damper models Structural Engineering and Mechanics, Vol. 41, No. 1 (2012) 113-137 113 Dynaic analysis of fraes with viscoelastic dapers: a coparison of daper odels R. Lewandowski*, A. Bartkowiak a and H. Maciejewski

More information

dt dt THE AIR TRACK (II)

dt dt THE AIR TRACK (II) THE AIR TRACK (II) References: [] The Air Track (I) - First Year Physics Laoratory Manual (PHY38Y and PHYY) [] Berkeley Physics Laoratory, nd edition, McGraw-Hill Book Copany [3] E. Hecht: Physics: Calculus,

More information

Multi-body Integrated Vehicle-Occupant Models for Collision Mitigation and Vehicle. Safety using Dynamics Control Systems

Multi-body Integrated Vehicle-Occupant Models for Collision Mitigation and Vehicle. Safety using Dynamics Control Systems Muti-body Integrated Vehice-Occupant Modes for Coision Mitigation and Vehice Safety using Dynaics Contro Systes a,b, Mustafa Ekady, c* Ahed Earakbi, c John MacIntyre and c Mohaed Ahariri a Departent of

More information

Unit 14 Harmonic Motion. Your Comments

Unit 14 Harmonic Motion. Your Comments Today s Concepts: Periodic Motion Siple - Mass on spring Daped Forced Resonance Siple - Pendulu Unit 1, Slide 1 Your Coents Please go through the three equations for siple haronic otion and phase angle

More information

CE573 Structural Dynamics [Fall 2008]

CE573 Structural Dynamics [Fall 2008] CE573 Structural Dynaics [Fall 2008] 1) A rigid vehicle weighing 2000 lb, oving horizontally at a velocity of 12 ft/sec, is stopped by a barrier consisting of wire ropes stretched between two rigid anchors

More information

CHECKLIST. r r. Newton s Second Law. natural frequency ω o (rad.s -1 ) (Eq ) a03/p1/waves/waves doc 9:19 AM 29/03/05 1

CHECKLIST. r r. Newton s Second Law. natural frequency ω o (rad.s -1 ) (Eq ) a03/p1/waves/waves doc 9:19 AM 29/03/05 1 PHYS12 Physics 1 FUNDAMENTALS Module 3 OSCILLATIONS & WAVES Text Physics by Hecht Chapter 1 OSCILLATIONS Sections: 1.5 1.6 Exaples: 1.6 1.7 1.8 1.9 CHECKLIST Haronic otion, periodic otion, siple haronic

More information

A REGULARIZED GMRES METHOD FOR INVERSE BLACKBODY RADIATION PROBLEM

A REGULARIZED GMRES METHOD FOR INVERSE BLACKBODY RADIATION PROBLEM Wu, J., Ma. Z.: A Reguarized GMRES Method for Inverse Backbody Radiation Probe THERMAL SCIENCE: Year 3, Vo. 7, No. 3, pp. 847-85 847 A REGULARIZED GMRES METHOD FOR INVERSE BLACKBODY RADIATION PROBLEM by

More information

Chapter 32 Inductance

Chapter 32 Inductance Chapter 3 nductance 3. Sef-nduction and nductance Sef-nductance Φ BA na --> Φ The unit of the inductance is henry (H). Wb T H A A When the current in the circuit is changing, the agnetic fux is aso changing.

More information

Analysis of Impulsive Natural Phenomena through Finite Difference Methods A MATLAB Computational Project-Based Learning

Analysis of Impulsive Natural Phenomena through Finite Difference Methods A MATLAB Computational Project-Based Learning Analysis of Ipulsive Natural Phenoena through Finite Difference Methods A MATLAB Coputational Project-Based Learning Nicholas Kuia, Christopher Chariah, Mechatronics Engineering, Vaughn College of Aeronautics

More information

Lecture 4 Normal Modes

Lecture 4 Normal Modes Lecture 4 Noral Modes Coupled driven oscillators Double pendulu The daped driven pendulu = g/l +k y+fcost y = y gy/l k y d dt + d dt + g + k l k k d dt + d dt + g + k l y = F 0 Re eit y =Re X Y eit CF

More information

= T. Oscillations and Waves. Example of an Oscillating System IB 12 IB 12

= T. Oscillations and Waves. Example of an Oscillating System IB 12 IB 12 Oscillation: the vibration of an object Oscillations and Waves Eaple of an Oscillating Syste A ass oscillates on a horizontal spring without friction as shown below. At each position, analyze its displaceent,

More information

Solution of Multivariable Optimization with Inequality Constraints by Lagrange Multipliers. where, x=[x 1 x 2. x n] T

Solution of Multivariable Optimization with Inequality Constraints by Lagrange Multipliers. where, x=[x 1 x 2. x n] T Solution of Multivariable Optiization with Inequality Constraints by Lagrange Multipliers Consider this proble: Miniize f where, =[. n] T subect to, g,, The g functions are labeled inequality constraints.

More information

APPENDIX B. Some special functions in low-frequency seismology. 2l +1 x j l (B.2) j l = j l 1 l +1 x j l (B.3) j l = l x j l j l+1

APPENDIX B. Some special functions in low-frequency seismology. 2l +1 x j l (B.2) j l = j l 1 l +1 x j l (B.3) j l = l x j l j l+1 APPENDIX B Soe specia functions in ow-frequency seisoogy 1. Spherica Besse functions The functions j and y are usefu in constructing ode soutions in hoogeneous spheres (fig B1). They satisfy d 2 j dr 2

More information

Torsion Experiment. Encoder #3 ( 3 ) Third encoder/disk for Model 205a only. Figure 1: ECP Torsion Experiment

Torsion Experiment. Encoder #3 ( 3 ) Third encoder/disk for Model 205a only. Figure 1: ECP Torsion Experiment Torsion Experient Introduction For the Torsion lab, there are two required experients to perfor and one extra credit assignent at the end. In experient 1, the syste paraeters need to be identified so that

More information

16.30/31 September 24, 2010 Prof. J. P. How and Prof. E. Frazzoli Due: October 15, 2010 T.A. B. Luders /31 Lab #1

16.30/31 September 24, 2010 Prof. J. P. How and Prof. E. Frazzoli Due: October 15, 2010 T.A. B. Luders /31 Lab #1 16.30/31 Septeber 24, 2010 Prof. J. P. How and Prof. E. Frazzoli Due: October 15, 2010 T.A. B. Luders 16.30/31 Lab #1 1 Introduction The Quanser helicopter is a echanical device that eulates the flight

More information

SPEECH RECOGNITION USING LPC AND HMM APPLIED FOR CONTROLLING MOVEMENT OF MOBILE ROBOT

SPEECH RECOGNITION USING LPC AND HMM APPLIED FOR CONTROLLING MOVEMENT OF MOBILE ROBOT Seinar asiona Teknoogi Inforasi 200 SPEECH RECOGITIO USIG LPC AD HMM APPLIED FOR COTROLLIG MOVEMET OF MOBILE ROBOT Thiang ) Wanto ) ) Eectrica Engineering Departent Petra Christian university Siwaankerto

More information

x(t) y(t) c c F(t) F(t) EN40: Dynamics and Vibrations Homework 6: Forced Vibrations Due Friday April 5, 2018

x(t) y(t) c c F(t) F(t) EN40: Dynamics and Vibrations Homework 6: Forced Vibrations Due Friday April 5, 2018 EN40: Dynais and Vibrations Hoewor 6: Fored Vibrations Due Friday April 5, 2018 Shool of Engineering Brown University 1. The vibration isolation syste shown in the figure has =20g, = 19.8 N / = 1.259 Ns

More information

In this chapter we will start the discussion on wave phenomena. We will study the following topics:

In this chapter we will start the discussion on wave phenomena. We will study the following topics: Chapter 16 Waves I In this chapter we will start the discussion on wave phenoena. We will study the following topics: Types of waves Aplitude, phase, frequency, period, propagation speed of a wave Mechanical

More information

Actuators & Mechanisms Actuator sizing

Actuators & Mechanisms Actuator sizing Course Code: MDP 454, Course Nae:, Second Seester 2014 Actuators & Mechaniss Actuator sizing Contents - Modelling of Mechanical Syste - Mechaniss and Drives The study of Mechatronics systes can be divided

More information

Course support: Control Engineering (TBKRT05E)

Course support: Control Engineering (TBKRT05E) Course Support This course support package is offered to you by TBV Lugus, the study association for Industrial Engineering and Manageent. Although this package is coposed with great care, the association

More information

which proves the motion is simple harmonic. Now A = a 2 + b 2 = =

which proves the motion is simple harmonic. Now A = a 2 + b 2 = = Worked out Exaples. The potential energy function for the force between two atos in a diatoic olecules can be expressed as follows: a U(x) = b x / x6 where a and b are positive constants and x is the distance

More information

Development of an Acoustic Instrument for Bubble Size Distribution Measurement

Development of an Acoustic Instrument for Bubble Size Distribution Measurement Deveopent of an Acoustic Instruent for Bubbe Size Distribution Measureent Xiongjun Wu 1* and Georges L. Chahine 1 1 DYNAFLOW, INC. Jessup, Maryand * E-ai: wxj@dynafow-inc.co ABSTRACT Measureent of bubbe

More information

Physics 41 HW Set 1 Chapter 15 Serway 7 th Edition

Physics 41 HW Set 1 Chapter 15 Serway 7 th Edition Physics HW Set Chapter 5 Serway 7 th Edition Conceptual Questions:, 3, 5,, 6, 9 Q53 You can take φ = π, or equally well, φ = π At t= 0, the particle is at its turning point on the negative side of equilibriu,

More information

Simple Harmonic Motion

Simple Harmonic Motion Chapter 3 Sipe Haronic Motion Practice Probe Soutions Student extboo pae 608. Conceptuaize the Probe - he period of a ass that is osciatin on the end of a sprin is reated to its ass and the force constant

More information

FINITE ELEMENT BASED VIBRATION FATIGUE ANALYSIS OF A NEW TWO- STROKE LINEAR GENERATOR ENGINE COMPONENT. M. M. Rahman, A. K. Ariffin, and S.

FINITE ELEMENT BASED VIBRATION FATIGUE ANALYSIS OF A NEW TWO- STROKE LINEAR GENERATOR ENGINE COMPONENT. M. M. Rahman, A. K. Ariffin, and S. International Journal of Mechanical and Materials Engineering (IJMME), Vol. (7), No. 1, 63-74. FINITE ELEMENT BASED VIBRATION FATIGUE ANALYSIS OF A NEW TWO- STROKE LINEAR GENERATOR ENGINE COMPONENT M.

More information

Simple Harmonic Motion

Simple Harmonic Motion Reading: Chapter 15 Siple Haronic Motion Siple Haronic Motion Frequency f Period T T 1. f Siple haronic otion x ( t) x cos( t ). Aplitude x Phase Angular frequency Since the otion returns to its initial

More information

PHYSICS 110A : CLASSICAL MECHANICS MIDTERM EXAM #2

PHYSICS 110A : CLASSICAL MECHANICS MIDTERM EXAM #2 PHYSICS 110A : CLASSICAL MECHANICS MIDTERM EXAM #2 [1] Two blocks connected by a spring of spring constant k are free to slide frictionlessly along a horizontal surface, as shown in Fig. 1. The unstretched

More information

5/09/06 PHYSICS 213 Exam #1 NAME FEYNMAN Please write down your name also on the back side of the last page

5/09/06 PHYSICS 213 Exam #1 NAME FEYNMAN Please write down your name also on the back side of the last page 5/09/06 PHYSICS 13 Exa #1 NAME FEYNMAN Please write down your nae also on the back side of the last page 1 he figure shows a horizontal planks of length =50 c, and ass M= 1 Kg, pivoted at one end. he planks

More information

Reducing Vibration and Providing Robustness with Multi-Input Shapers

Reducing Vibration and Providing Robustness with Multi-Input Shapers 29 Aerican Control Conference Hyatt Regency Riverfront, St. Louis, MO, USA June -2, 29 WeA6.4 Reducing Vibration and Providing Robustness with Multi-Input Shapers Joshua Vaughan and Willia Singhose Abstract

More information

A Simplified Analytical Approach for Efficiency Evaluation of the Weaving Machines with Automatic Filling Repair

A Simplified Analytical Approach for Efficiency Evaluation of the Weaving Machines with Automatic Filling Repair Proceedings of the 6th SEAS International Conference on Siulation, Modelling and Optiization, Lisbon, Portugal, Septeber -4, 006 0 A Siplified Analytical Approach for Efficiency Evaluation of the eaving

More information

CHAPTER 19: Single-Loop IMC Control

CHAPTER 19: Single-Loop IMC Control When I coplete this chapter, I want to be able to do the following. Recognize that other feedback algoriths are possible Understand the IMC structure and how it provides the essential control features

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

821. Study on analysis method for deepwater TTR coupled vibration of parameter vibration and vortex-induced vibration

821. Study on analysis method for deepwater TTR coupled vibration of parameter vibration and vortex-induced vibration 81. Study on analysis ethod for deepwater TTR coupled vibration of paraeter vibration and vortex-induced vibration Wu Xue-Min 1, Huang Wei-Ping Shandong Key aboratory of Ocean Engineering, Ocean University

More information

Nonlinear Control of Full-Vehicle Active Suspensions with Backstepping Design Scheme

Nonlinear Control of Full-Vehicle Active Suspensions with Backstepping Design Scheme Proceedings of the 7th World Congress The International Federation of Autoatic Control Nonlinear Control of Full-Vehicle Active Suspensions with Backstepping Design Schee Jia-Wei Hu Jung-Shan Lin Departent

More information

Damped Harmonic Motion

Damped Harmonic Motion Daped Haronic Motion PY154 Special Topics in Physics PY154 1 Driven Daped Haronic Motion What if we apply a haronic force?: F h Be it The total force is then: dx F Fh kx b dt d x dt Assue a solution of

More information

ANALELE UNIVERSITĂłII EFTIMIE MURGU REŞIłA ANUL XXI, NR. 1, 2014, ISSN Florin Bausic, Alexandru Cosmescu, Filip Gărdăreanu

ANALELE UNIVERSITĂłII EFTIMIE MURGU REŞIłA ANUL XXI, NR. 1, 2014, ISSN Florin Bausic, Alexandru Cosmescu, Filip Gărdăreanu ANALELE UNIVERSITĂłII ETIMIE MURGU REŞIłA ANUL XXI, NR.,, ISSN 5-797 lorin Bausi, Aleandru Cosesu, ilip Gărdăreanu Stability Analysis for Hand-ar-forear Dynai Syste In this paper we propose a odel with

More information

9 HOOKE S LAW AND SIMPLE HARMONIC MOTION

9 HOOKE S LAW AND SIMPLE HARMONIC MOTION Experient 9 HOOKE S LAW AND SIMPLE HARMONIC MOTION Objectives 1. Verify Hoo s law,. Measure the force constant of a spring, and 3. Measure the period of oscillation of a spring-ass syste and copare it

More information

HYBRID CONTROLLER FOR GUST LOAD ALLEVIATION AND RIDE COMFORT IMPROVEMENT USING DIRECT LIFT CONTROL FLAPS

HYBRID CONTROLLER FOR GUST LOAD ALLEVIATION AND RIDE COMFORT IMPROVEMENT USING DIRECT LIFT CONTROL FLAPS 3 rd EUROPEAN CONFERENCE FOR AEROSPACE SCIENCES (EUCASS) HYBRID CONTROLLER FOR GUST LOAD ALLEVIATION AND RIDE COMFORT IMPROVEMENT USING DIRECT LIFT CONTROL FLAPS Andreas Wildschek*, Rudolf Maier*, Martin

More information

COULD A VARIABLE MASS OSCILLATOR EXHIBIT THE LATERAL INSTABILITY?

COULD A VARIABLE MASS OSCILLATOR EXHIBIT THE LATERAL INSTABILITY? Kragujevac J. Sci. 3 (8) 3-44. UDC 53.35 3 COULD A VARIABLE MASS OSCILLATOR EXHIBIT THE LATERAL INSTABILITY? Nebojša Danilović, Milan Kovačević and Vukota Babović Institute of Physics, Faculty of Science,

More information

Sensorless Control of Induction Motor Drive Using SVPWM - MRAS Speed Observer

Sensorless Control of Induction Motor Drive Using SVPWM - MRAS Speed Observer Journal of Eerging Trends in Engineering and Applied Sciences (JETEAS) 2 (3): 509-513 Journal Scholarlink of Eerging Research Trends Institute in Engineering Journals, 2011 and Applied (ISSN: 2141-7016)

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

B l 4 P A 1 DYNAMICS OF RECIPROCATING ENGINES

B l 4 P A 1 DYNAMICS OF RECIPROCATING ENGINES DYNMIS OF REIROTING ENGINES This chapte studies the dnaics of a side cank echaniss in an anatica wa. This is an eape fo the anatica appoach of soution instead of the gaphica acceeations and foce anases.

More information

More Oscillations! (Today: Harmonic Oscillators)

More Oscillations! (Today: Harmonic Oscillators) More Oscillations! (oday: Haronic Oscillators) Movie assignent reinder! Final due HURSDAY April 20 Subit through ecapus Different rubric; reeber to chec it even if you got 00% on your draft: http://sarahspolaor.faculty.wvu.edu/hoe/physics-0

More information

Overview. Main contributions of Multiresolution Probabilistic Nano Mechanics and Materials.

Overview. Main contributions of Multiresolution Probabilistic Nano Mechanics and Materials. Mutiresoution Probabiistic Nano Mechanics and Materias Fro Vaidation to Prediction In particuar for: Reiabiity Prediction in Heterogeneous Materias and Materias Design Fusion with Product Design and Manufacturing

More information

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

+ 1 2 mv 2. Since no forces act on the system in the x-direction, linear momentum in x-direction is conserved: (2) 0 = mv A2. + Rω 2.

+ 1 2 mv 2. Since no forces act on the system in the x-direction, linear momentum in x-direction is conserved: (2) 0 = mv A2. + Rω 2. ME 74 Spring 018 Final Exaination Proble 1 Given: hoogeneous dis of ass and outer radius R is able to roll without slipping on the curved upper surface of a cart. art (of ass ) is able to ove along a sooth,

More information