Design and Analysis of Landing Gear Mechanic Structure for the Mine Rescue Carrier Robot
|
|
- Gladys Hutchinson
- 5 years ago
- Views:
Transcription
1 Sensors & Transducers 214 by IFSA Publshng, S. L. Desgn and Analyss of Landng Gear Mechanc Structure for the Mne Rescue Carrer Robot We Juan, Wu Ja-Long X an Unversty of Scence and Technology, X an 7154, Chna Tel.: E-mal: wej@xust.edu.cn Receved: 9 Aprl 214 /Accepted: 3 May 214 /Publshed: 3 June 214 Abstract: The landng gear s used as a channel for the secondary detectng robot to leave and return the frst carrer robot n the coal mne rescue robot system. The planar lnkage mechansm, whch s composed of offset rocker-slder mechansm and double-rocker mechansm, s desgned accordng to the functon and workng prncple of the landng gear. It could realze the 12 rotaton of the flap wth a motor drvng the slder. The sze calculaton of the planar lnkage mechansm s completed accordng to ts workspace. The geometrc modelng of the landng gear s made n the SoldWorks, and the basc Knematc analyss s carred out by the smulaton module of Moton. And the movement rule about angular dsplacement and angular velocty of the lnkage mechansm could be obtaned under gven nput condton, whch could verfy the system s feasblty. It provdes a theoretcal bass for the structure desgn and engneerng applcaton of lnkage mechansm and an applyng bass for the coal mne rescue robot. Copyrght 214 IFSA Publshng, S. L. Keywords: Mne rescue robot, Landng gear, Planar lnkage mechansm, SoldWorks moton. 1. Introducton Mne rescue two-stage robot system s used n the status that mne accdents occur n workng faces away from the mne entrance, t adopts two-stage robot structure [1], the frst orbtal-carrer robot and the secondary crawler detectng robot. As the secondary complex-crawler robot moves slowly, whch needs a long tme to drve to the accdent ste, t would mss the golden perod for rescue, so we use the frst-stage carrer robot, drvng on the orbt wth a faster speed, to reduce the drvng tme. After a mne accdent, the frst-stage carrer robot [2] carres the second-stage detectng robot [3] along the underground transport orbt movng fast to the place where the accdent happened. If the frst-stage robot s obstructed, the second-stage would get off and keep on movng to the accdent ste, and t would get back wth ts work done. And the role of the landng gear s to form a road slope for the second-stage robot to get off and on. The basc machne of the carrer robot ncludng the car body, drvng mechansm, travellng mechansm, brakng mechansm, buffer mechansm and landng gear [4], as shown n Fg. 1, ts man functon s to guarantee the safe runnng of the carrer along the orbt. In the desgn of landng gear, the planar lnkage mechansm would be used to complete part of the complex movement accordng to ts advantages and wldly use n engneerng practce, such as usng lower pars, not easy to wear, easy to process wth low cost and could acheve a varety of complex movement curves and movement rules
2 Fg. 1. The structure of secondary carrer robot. 2. Desgn of the Planar Sx Bar Mechansm The planar sx bar mechansm [5, 6] s composed of the offset rocker-slder mechansm and doublerocker mechansm, the functon of the frst part s to transform the lnear moton of the rack to the rotaton moton of a bar, and the functon of the double-rocker mechansm s to amplfy the rotaton angle and to make sure the 12 rotaton moton of the flap. a = mm S = mm, (3) ϕ = ϕ = For the poston 2, the angle between the bar a and b s 32.27, far away from the dead zone, and the operatng requrement could be satsfed The Sze Calculaton of the Offset Rocker Slder Mechansm The offset rocker-slder mechansm s composed of slder, bar a and bar b. ts target s to turn bar b over 6 n a clockwse drecton. The slder s the nput whle the bar b s the output, and the lnear moton of the slder would translated to the rotaton moton of bar b. The extreme postons [7] are shown n Fg. 2 and Fg. 3 respectvely. The equaton for the extreme poston 1: asnϕ + e= bsnψ acosϕ bcosψ = S, (1) Fg. 2. Poston 1 of the offset rocker slder mechansm. The equaton for the extreme poston 2: asnϕ + e= bsnψ, (2) acosϕ bcosψ = S Accordng to the overall structural sze of the landng gear and carrer robot, defne: S = 8 mm, e= 15 mm, b= 5 mm, ψ = 15, ψ = 75. Smultaneous the equaton could obtan: Fg. 3. Poston 2 of the offset rocker slder mechansm. 236
3 2.2. Sze Calculaton of the Double Rocker Mechansm The double rocker mechansm s composed of bar l 1, l 2, l 3 and l 4. It s target s to rotate the bar l 3, the flap, 12 n the clockwse drecton, the rod l 1 s the nput wth a rotaton of 6 degrees and the bar l 3 s the output wth a rotaton of 12. The extreme postons [8] of ths mechansm are shown n Fg. 4 and Fg. 5 respectvely. 2) The equaton for the extreme poston 2: l1snϕ l2snδ = l3snψ, (7) l1cosϕ + l2cosδ = l4 + l3cosψ After the elmnaton of δ, we could obtan: l = ( l snϕ + l sn ψ ) + ( l + l cosψ l cos ψ ), (8) Accordng to the overall structural sze of the landng gear and carrer robot, defne: l3 = 5 mm, l 4 = 58 mm, ψ = 3, ϕ = 25, ϕ = ϕ + 6, Smultaneous the equaton could obtan: l1 = 952 mm l2 = mm, (9) δ = 42.5 δ1 =77.3 Fg. 4. Extreme poston 1 of the double rocker mechansm. For poston 2, the angle between the rod a and b s 17.3 and the operatng requrement could be satsfed. The bar b of offset rocker slder mechansm and the bar l 1 of double rocker mechansm would rotate around the same pont, the angle between them s 5, and the connectng bar s shown n Fg. 6. Fg. 5. Extreme Poston 2 of the double rocker mechansm. Components could be expressed as vectors, and accordng to the closed vector graphcs, the followng vector equaton could be obtaned: l1+ l2 = l3+ l4, (4) Project to the X axs and Y axs, we could obtan: 1) The equaton for the extreme poston 1: l1snϕ l2snδ = l3, (5) l1cosϕ + l2cosδ = l4 After the elmnaton of δ, we could obtan: l = ( l sn ϕ l ) + ( l l cos ϕ ), (6) Fg. 6. Connectng bar The Structural Characterstcs of the Landng Gear All of the structural szes of the combned mechansm could be obtaned accordng to the dmenson value we calculated, ts CAD drawng of the two extreme postons are shown n Fg. 7 and Fg. 8. In poston 1, the rack s on the left sde whle the flap s perpendcular to the ground, and n poston 2, the rack s on the rght wth a lnear moton whle the flap rotates 12 n the clockwse drecton. 237
4 1 Car body, 2 Gear shaft, 3 Prsmatc par, 4 Rack, 5, 6, 7 bar, 8, 1, 11 Rotaton par, 9 flap. Fg. 7. Poston 1 of the landng gear. Fg. 9. The model of landng gear n SoldWorks Moton Smulaton and Analyss In SoldWorks Moton, all components are regarded as the deal rgd body, whch means the deformaton wll not occurred nsde of each bar and between the bars n smulaton process. Connectng formats and constrants accordng to the movement characterstc of the mechansm should be approprate, that s because those elements have a vtal mportance to the vrtual assemble and moton smulaton [9]. Consderng the speed change of the motor at the startng and stoppng moment and n order to avod the collson between the car body and flap, an optmzed velocty curve of the motor s gven as shown n the Fg. 1. Fg. 8. Poston 2 of landng gear. 3. The Knematc Analyss of the Landng Gear By usng vrtual prototype smulaton tools SoldWorks Moton, Knematcs and dynamcs smulaton analyss of complex mechansms can be done, and moton parameters could be obtaned, such as dsplacement, velocty, acceleraton, force and reacton force, etc. It s provded opportuntes to do Knematc analyss work wthout physcal prototype manufactured. Fg. 1. Velocty-tme curve of the rack Constructon of Three-dmensonal Model In SoldWorks, all components of the landng gear should be modeled and assembled accordng to the actual condtons; the assembly model s shown n Fg. 9. The rack s the nput whle the flap 7 s the output, the lnear moton of the rack could be transformed to the rotatonal moton of the flap. In the moton smulaton analyss, set the moton opton as the functons, and the equaton of the velocty s gven as n equaton y = ( x < 2) 2, y = 95 (2 x < 8) 95 y = ( x 6) + 95(6 x 8) 2 (1) 238
5 The speed of the rack, the vce 3, would be ncrease to 95 mm/s from mm/s on a constant acceleraton, and t would be decrease to mm/s on a constant acceleraton after a constant movement of 4 seconds. After the calculaton, the angular dsplacement-tme curve of the flap could be obtaned as shown n Fg. 11, and the angular speed-tme curve of the flap, revolute par 8, could also be obtaned as shown n Fg. 12. The rotaton angle of the flap s 12, and the angular speed would be ncreased from deg/s gradually and reach the maxmum at about 6 s, then t would be decreased gradually and reached deg/s at 8 s. The collson between the car body and the flap at the extreme postons would be avoded and the expected goals could be acheved better under ths speed curve. 24 deg/s whle the maxmum of the bar 5 s 11 deg/s. we could fnd that the expected target could be obtaned well wth the planar sx rod mechansm from those curves. Fg. 13. Angular dsplacement-tme curve of the bar 6. Fg. 11. Angular dsplacement-tme curve of the flap. Fg. 14. Angular velocty-tme curve of the bar Concluson Fg. 12. Angular velocty-tme curve of the flap. The angular dsplacement-tme and angular speed-tme curves of the bar 6, the revolute par 1 and 11, could also be obtaned as shown n Fg. 13 and Fg. 14. The rotaton angle s 6, ts angular speed-tme curve s smlar to the curve of flap wth a dfferent maxmum, and the maxmum of the flap s The role of the landng gear n the carrer s to provde a pass way for the secondary detectng robot to leave and return, t requres not only strong operaton relablty, runnng stablty, a certan carryng ablty but also the smple structure, easy to control and autonomous control. 1) The structure and geometry szes of the landng gear mechansm were determned after the calculaton of extreme postons of the offset slder rocker mechansm and double rocker mechansm under the suffcent analyss of the functonal requrements of the landng gear. 2) Moton Smulaton of the landng gear were carred out by usng vrtual prototype smulaton tools, SoldWorks Moton, the angular dsplacementtme and angular velocty-tme curves of the man components were obtaned and the feasblty of the mechansm were verfed. In order to avod the 239
6 collsons between the flap and car body n extreme postons, the optmzed nput velocty curve were offered. Acknowledgements The project s supported by the Natural Scence Foundaton of Chna, No and No References [1]. Juan We, Hongwe Ma, Study on mne rescue robot system, n Proceedngs of the 2 nd Internatonal Conference on Intellgent Robotcs and Applcatons, Vol. 2489, December 29, pp [2]. We Juan, Ma Hongwe, Parametrc optmzaton desgn on mne carrer robot, Advanced Materals Research, Vol. 346, 212, pp [3]. We Juan, Ma Hongwe, Knetc characterstcs analyss and smulaton research on carrer robot, Advanced Materals Research, Vol. 346, 212, pp [4]. We Juan, Ja Guangl, Ma Hongwe, Smulaton analyss of the vrtual prototypng of a recue robot, Mechancal Scence and Technology for Aerospace Engneerng, Vol. 27, Issue 11, 28, pp [5]. Yang Yan, Research on knematc smulaton of RRR-RRP planar sx bar mechansm system, Journal of Nanchang Hangkong Unversty (Natural Scences), Vol. 24, No. 4, 21, pp [6]. Qu Xuquan, Dynamc smulaton of planar lnkage based on MATLAB/Smulnk, Harbn Insttute of Technology Press, Harbn, 27. [7]. Hua Danan, Hua Zhhong, Lnkage desgn and applcaton nnovaton, Chna Machne Press, 28. [8]. Zhang Xaolng, Shen Shaohua, Practcal mechansm desgn and analyss, Behang Unversty Press, 21. [9]. L Dale, Dng Tantao, Cheng Janmn, Moton analyss for space swngng nsttuton based on SoldWorks moton, Manufacturng Automaton, Vol. 33, Issue 22, 211, pp Copyrght, Internatonal Frequency Sensor Assocaton (IFSA) Publshng, S. L. All rghts reserved. ( 24
Operating conditions of a mine fan under conditions of variable resistance
Paper No. 11 ISMS 216 Operatng condtons of a mne fan under condtons of varable resstance Zhang Ynghua a, Chen L a, b, Huang Zhan a, *, Gao Yukun a a State Key Laboratory of Hgh-Effcent Mnng and Safety
More informationStudy on Active Micro-vibration Isolation System with Linear Motor Actuator. Gong-yu PAN, Wen-yan GU and Dong LI
2017 2nd Internatonal Conference on Electrcal and Electroncs: echnques and Applcatons (EEA 2017) ISBN: 978-1-60595-416-5 Study on Actve Mcro-vbraton Isolaton System wth Lnear Motor Actuator Gong-yu PAN,
More informationAdvanced Mechanical Elements
May 3, 08 Advanced Mechancal Elements (Lecture 7) Knematc analyss and moton control of underactuated mechansms wth elastc elements - Moton control of underactuated mechansms constraned by elastc elements
More informationTHE EFFECT OF TORSIONAL RIGIDITY BETWEEN ELEMENTS ON FREE VIBRATIONS OF A TELESCOPIC HYDRAULIC CYLINDER SUBJECTED TO EULER S LOAD
Journal of Appled Mathematcs and Computatonal Mechancs 7, 6(3), 7- www.amcm.pcz.pl p-issn 99-9965 DOI:.75/jamcm.7.3. e-issn 353-588 THE EFFECT OF TORSIONAL RIGIDITY BETWEEN ELEMENTS ON FREE VIBRATIONS
More informationCOMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD
COMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD Ákos Jósef Lengyel, István Ecsed Assstant Lecturer, Professor of Mechancs, Insttute of Appled Mechancs, Unversty of Mskolc, Mskolc-Egyetemváros,
More informationAir Age Equation Parameterized by Ventilation Grouped Time WU Wen-zhong
Appled Mechancs and Materals Submtted: 2014-05-07 ISSN: 1662-7482, Vols. 587-589, pp 449-452 Accepted: 2014-05-10 do:10.4028/www.scentfc.net/amm.587-589.449 Onlne: 2014-07-04 2014 Trans Tech Publcatons,
More informationPhysics 111: Mechanics Lecture 11
Physcs 111: Mechancs Lecture 11 Bn Chen NJIT Physcs Department Textbook Chapter 10: Dynamcs of Rotatonal Moton q 10.1 Torque q 10. Torque and Angular Acceleraton for a Rgd Body q 10.3 Rgd-Body Rotaton
More informationAssessment of Site Amplification Effect from Input Energy Spectra of Strong Ground Motion
Assessment of Ste Amplfcaton Effect from Input Energy Spectra of Strong Ground Moton M.S. Gong & L.L Xe Key Laboratory of Earthquake Engneerng and Engneerng Vbraton,Insttute of Engneerng Mechancs, CEA,
More informationStudy on Non-Linear Dynamic Characteristic of Vehicle. Suspension Rubber Component
Study on Non-Lnear Dynamc Characterstc of Vehcle Suspenson Rubber Component Zhan Wenzhang Ln Y Sh GuobaoJln Unversty of TechnologyChangchun, Chna Wang Lgong (MDI, Chna [Abstract] The dynamc characterstc
More informationIndeterminate pin-jointed frames (trusses)
Indetermnate pn-jonted frames (trusses) Calculaton of member forces usng force method I. Statcal determnacy. The degree of freedom of any truss can be derved as: w= k d a =, where k s the number of all
More informationCHAPTER 6. LAGRANGE S EQUATIONS (Analytical Mechanics)
CHAPTER 6 LAGRANGE S EQUATIONS (Analytcal Mechancs) 1 Ex. 1: Consder a partcle movng on a fxed horzontal surface. r P Let, be the poston and F be the total force on the partcle. The FBD s: -mgk F 1 x O
More informationIrregular vibrations in multi-mass discrete-continuous systems torsionally deformed
(2) 4 48 Irregular vbratons n mult-mass dscrete-contnuous systems torsonally deformed Abstract In the paper rregular vbratons of dscrete-contnuous systems consstng of an arbtrary number rgd bodes connected
More informationSpin-rotation coupling of the angularly accelerated rigid body
Spn-rotaton couplng of the angularly accelerated rgd body Loua Hassan Elzen Basher Khartoum, Sudan. Postal code:11123 E-mal: louaelzen@gmal.com November 1, 2017 All Rghts Reserved. Abstract Ths paper s
More informationThe Study of Teaching-learning-based Optimization Algorithm
Advanced Scence and Technology Letters Vol. (AST 06), pp.05- http://dx.do.org/0.57/astl.06. The Study of Teachng-learnng-based Optmzaton Algorthm u Sun, Yan fu, Lele Kong, Haolang Q,, Helongang Insttute
More information829. An adaptive method for inertia force identification in cantilever under moving mass
89. An adaptve method for nerta force dentfcaton n cantlever under movng mass Qang Chen 1, Mnzhuo Wang, Hao Yan 3, Haonan Ye 4, Guola Yang 5 1,, 3, 4 Department of Control and System Engneerng, Nanng Unversty,
More information= 1.23 m/s 2 [W] Required: t. Solution:!t = = 17 m/s [W]! m/s [W] (two extra digits carried) = 2.1 m/s [W]
Secton 1.3: Acceleraton Tutoral 1 Practce, page 24 1. Gven: 0 m/s; 15.0 m/s [S]; t 12.5 s Requred: Analyss: a av v t v f v t a v av f v t 15.0 m/s [S] 0 m/s 12.5 s 15.0 m/s [S] 12.5 s 1.20 m/s 2 [S] Statement:
More informationA Multi-Axis Force Measurement System for a Space Docking Mechanism
3rd Internatonal Conference on Materal, Mechancal and Manufacturng Engneerng (IC3ME 215) A Mult-Axs orce Measurement System for a Space Dockng Mechansm Gangfeng Lu a*, Changle L b and Zenghu Xe c Buldng
More informationModeling of Dynamic Systems
Modelng of Dynamc Systems Ref: Control System Engneerng Norman Nse : Chapters & 3 Chapter objectves : Revew the Laplace transform Learn how to fnd a mathematcal model, called a transfer functon Learn how
More informationDesign and Optimization of Fuzzy Controller for Inverse Pendulum System Using Genetic Algorithm
Desgn and Optmzaton of Fuzzy Controller for Inverse Pendulum System Usng Genetc Algorthm H. Mehraban A. Ashoor Unversty of Tehran Unversty of Tehran h.mehraban@ece.ut.ac.r a.ashoor@ece.ut.ac.r Abstract:
More informationPhysics 5153 Classical Mechanics. D Alembert s Principle and The Lagrangian-1
P. Guterrez Physcs 5153 Classcal Mechancs D Alembert s Prncple and The Lagrangan 1 Introducton The prncple of vrtual work provdes a method of solvng problems of statc equlbrum wthout havng to consder the
More informationAn Algorithm to Solve the Inverse Kinematics Problem of a Robotic Manipulator Based on Rotation Vectors
An Algorthm to Solve the Inverse Knematcs Problem of a Robotc Manpulator Based on Rotaton Vectors Mohamad Z. Al-az*, Mazn Z. Othman**, and Baker B. Al-Bahr* *AL-Nahran Unversty, Computer Eng. Dep., Baghdad,
More informationWeek3, Chapter 4. Position and Displacement. Motion in Two Dimensions. Instantaneous Velocity. Average Velocity
Week3, Chapter 4 Moton n Two Dmensons Lecture Quz A partcle confned to moton along the x axs moves wth constant acceleraton from x =.0 m to x = 8.0 m durng a 1-s tme nterval. The velocty of the partcle
More informationTensor Smooth Length for SPH Modelling of High Speed Impact
Tensor Smooth Length for SPH Modellng of Hgh Speed Impact Roman Cherepanov and Alexander Gerasmov Insttute of Appled mathematcs and mechancs, Tomsk State Unversty 634050, Lenna av. 36, Tomsk, Russa RCherepanov82@gmal.com,Ger@npmm.tsu.ru
More informationCHAPTER 5 NUMERICAL EVALUATION OF DYNAMIC RESPONSE
CHAPTER 5 NUMERICAL EVALUATION OF DYNAMIC RESPONSE Analytcal soluton s usually not possble when exctaton vares arbtrarly wth tme or f the system s nonlnear. Such problems can be solved by numercal tmesteppng
More informationHigh resolution entropy stable scheme for shallow water equations
Internatonal Symposum on Computers & Informatcs (ISCI 05) Hgh resoluton entropy stable scheme for shallow water equatons Xaohan Cheng,a, Yufeng Ne,b, Department of Appled Mathematcs, Northwestern Polytechncal
More informationStructure and Drive Paul A. Jensen Copyright July 20, 2003
Structure and Drve Paul A. Jensen Copyrght July 20, 2003 A system s made up of several operatons wth flow passng between them. The structure of the system descrbes the flow paths from nputs to outputs.
More informationMEV442 Introduction to Robotics Module 2. Dr. Santhakumar Mohan Assistant Professor Mechanical Engineering National Institute of Technology Calicut
MEV442 Introducton to Robotcs Module 2 Dr. Santhakumar Mohan Assstant Professor Mechancal Engneerng Natonal Insttute of Technology Calcut Jacobans: Veloctes and statc forces Introducton Notaton for tme-varyng
More informationDO NOT DO HOMEWORK UNTIL IT IS ASSIGNED. THE ASSIGNMENTS MAY CHANGE UNTIL ANNOUNCED.
EE 539 Homeworks Sprng 08 Updated: Tuesday, Aprl 7, 08 DO NOT DO HOMEWORK UNTIL IT IS ASSIGNED. THE ASSIGNMENTS MAY CHANGE UNTIL ANNOUNCED. For full credt, show all work. Some problems requre hand calculatons.
More informationAP Physics 1 & 2 Summer Assignment
AP Physcs 1 & 2 Summer Assgnment AP Physcs 1 requres an exceptonal profcency n algebra, trgonometry, and geometry. It was desgned by a select group of college professors and hgh school scence teachers
More informationThe equation of motion of a dynamical system is given by a set of differential equations. That is (1)
Dynamcal Systems Many engneerng and natural systems are dynamcal systems. For example a pendulum s a dynamcal system. State l The state of the dynamcal system specfes t condtons. For a pendulum n the absence
More informationSTUDY OF A THREE-AXIS PIEZORESISTIVE ACCELEROMETER WITH UNIFORM AXIAL SENSITIVITIES
STUDY OF A THREE-AXIS PIEZORESISTIVE ACCELEROMETER WITH UNIFORM AXIAL SENSITIVITIES Abdelkader Benchou, PhD Canddate Nasreddne Benmoussa, PhD Kherreddne Ghaffour, PhD Unversty of Tlemcen/Unt of Materals
More information10/23/2003 PHY Lecture 14R 1
Announcements. Remember -- Tuesday, Oct. 8 th, 9:30 AM Second exam (coverng Chapters 9-4 of HRW) Brng the followng: a) equaton sheet b) Calculator c) Pencl d) Clear head e) Note: If you have kept up wth
More informationPlease initial the statement below to show that you have read it
EN40: Dynamcs and Vbratons Mdterm Examnaton Thursday March 5 009 Dvson of Engneerng rown Unversty NME: Isaac Newton General Instructons No collaboraton of any knd s permtted on ths examnaton. You may brng
More informationLab 2e Thermal System Response and Effective Heat Transfer Coefficient
58:080 Expermental Engneerng 1 OBJECTIVE Lab 2e Thermal System Response and Effectve Heat Transfer Coeffcent Warnng: though the experment has educatonal objectves (to learn about bolng heat transfer, etc.),
More informationTHE CURRENT BALANCE Physics 258/259
DSH 1988, 005 THE CURRENT BALANCE Physcs 58/59 The tme average force between two parallel conductors carryng an alternatng current s measured by balancng ths force aganst the gravtatonal force on a set
More informationENGN 40 Dynamics and Vibrations Homework # 7 Due: Friday, April 15
NGN 40 ynamcs and Vbratons Homework # 7 ue: Frday, Aprl 15 1. Consder a concal hostng drum used n the mnng ndustry to host a mass up/down. A cable of dameter d has the mass connected at one end and s wound/unwound
More informationPERFORMANCE OF HEAVY-DUTY PLANETARY GEARS
THE INTERNATIONAL CONFERENCE OF THE CARPATHIAN EURO-REGION SPECIALISTS IN INDUSTRIAL SYSTEMS 6 th edton PERFORMANCE OF HEAVY-DUTY PLANETARY GEARS Attla Csobán, Mhály Kozma 1, 1 Professor PhD., Eng. Budapest
More information11. Dynamics in Rotating Frames of Reference
Unversty of Rhode Island DgtalCommons@URI Classcal Dynamcs Physcs Course Materals 2015 11. Dynamcs n Rotatng Frames of Reference Gerhard Müller Unversty of Rhode Island, gmuller@ur.edu Creatve Commons
More informationAxial Turbine Analysis
Axal Turbne Analyss From Euler turbomachnery (conservaton) equatons need to Nole understand change n tangental velocty to relate to forces on blades and power m W m rc e rc uc uc e Analye flow n a plane
More informationNumerical Heat and Mass Transfer
Master degree n Mechancal Engneerng Numercal Heat and Mass Transfer 06-Fnte-Dfference Method (One-dmensonal, steady state heat conducton) Fausto Arpno f.arpno@uncas.t Introducton Why we use models and
More informationEffect of loading frequency on the settlement of granular layer
Effect of loadng frequency on the settlement of granular layer Akko KONO Ralway Techncal Research Insttute, Japan Takash Matsushma Tsukuba Unversty, Japan ABSTRACT: Cyclc loadng tests were performed both
More informationCalculation of time complexity (3%)
Problem 1. (30%) Calculaton of tme complexty (3%) Gven n ctes, usng exhaust search to see every result takes O(n!). Calculaton of tme needed to solve the problem (2%) 40 ctes:40! dfferent tours 40 add
More informationA PROBABILITY-DRIVEN SEARCH ALGORITHM FOR SOLVING MULTI-OBJECTIVE OPTIMIZATION PROBLEMS
HCMC Unversty of Pedagogy Thong Nguyen Huu et al. A PROBABILITY-DRIVEN SEARCH ALGORITHM FOR SOLVING MULTI-OBJECTIVE OPTIMIZATION PROBLEMS Thong Nguyen Huu and Hao Tran Van Department of mathematcs-nformaton,
More informationNote 10. Modeling and Simulation of Dynamic Systems
Lecture Notes of ME 475: Introducton to Mechatroncs Note 0 Modelng and Smulaton of Dynamc Systems Department of Mechancal Engneerng, Unversty Of Saskatchewan, 57 Campus Drve, Saskatoon, SK S7N 5A9, Canada
More informationAvailable online at ScienceDirect. Procedia Technology 14 (2014 ) Kailash Chaudhary*, Himanshu Chaudhary
Avalable onlne at www.scencedrect.com ScenceDrect Proceda Technology 4 (4 ) 35 4 nd Internatonal Conference on Innovatons n Automaton and Mechatroncs Engneerng, ICIAME 4 Optmum balancng of slder-crank
More informationPart C Dynamics and Statics of Rigid Body. Chapter 5 Rotation of a Rigid Body About a Fixed Axis
Part C Dynamcs and Statcs of Rgd Body Chapter 5 Rotaton of a Rgd Body About a Fxed Axs 5.. Rotatonal Varables 5.. Rotaton wth Constant Angular Acceleraton 5.3. Knetc Energy of Rotaton, Rotatonal Inerta
More informationComparative Studies of Law of Conservation of Energy. and Law Clusters of Conservation of Generalized Energy
Comparatve Studes of Law of Conservaton of Energy and Law Clusters of Conservaton of Generalzed Energy No.3 of Comparatve Physcs Seres Papers Fu Yuhua (CNOOC Research Insttute, E-mal:fuyh1945@sna.com)
More informationDynamic Similarity Design of Geared Rotor System in Five-Shaft Integrally Centrifugal Compressor
Dynamc Smlarty Desgn of Geared Rotor System n Fve-Shaft Integrally Centrfugal Compressor Hao Zhang 1, Gaoshan We, Xu Chen, Qngka Han 1,* 1. Collaboratve Innovaton Center of Maor Machne Manufacturng n Laonng,
More informationConservation of Angular Momentum = "Spin"
Page 1 of 6 Conservaton of Angular Momentum = "Spn" We can assgn a drecton to the angular velocty: drecton of = drecton of axs + rght hand rule (wth rght hand, curl fngers n drecton of rotaton, thumb ponts
More informationResearch on the Fuzzy Control for Vehicle Semi-active Suspension. Xiaoming Hu 1, a, Wanli Li 1,b
Advanced Materals Research Onlne: 0-0- ISSN: -9, Vol., pp -9 do:0.0/www.scentfc.net/amr.. 0 Trans Tech Publcatons, Swterland Research on the Fuy Control for Vehcle Sem-actve Suspenson Xaomng Hu, a, Wanl
More informationChapter 11: Angular Momentum
Chapter 11: ngular Momentum Statc Equlbrum In Chap. 4 we studed the equlbrum of pontobjects (mass m) wth the applcaton of Newton s aws F 0 F x y, 0 Therefore, no lnear (translatonal) acceleraton, a0 For
More informationWeek 9 Chapter 10 Section 1-5
Week 9 Chapter 10 Secton 1-5 Rotaton Rgd Object A rgd object s one that s nondeformable The relatve locatons of all partcles makng up the object reman constant All real objects are deformable to some extent,
More informationCalculating the Quasi-static Pressures of Confined Explosions Considering Chemical Reactions under the Constant Entropy Assumption
Appled Mechancs and Materals Onlne: 202-04-20 ISS: 662-7482, ol. 64, pp 396-400 do:0.4028/www.scentfc.net/amm.64.396 202 Trans Tech Publcatons, Swtzerland Calculatng the Quas-statc Pressures of Confned
More informationSpeeding up Computation of Scalar Multiplication in Elliptic Curve Cryptosystem
H.K. Pathak et. al. / (IJCSE) Internatonal Journal on Computer Scence and Engneerng Speedng up Computaton of Scalar Multplcaton n Ellptc Curve Cryptosystem H. K. Pathak Manju Sangh S.o.S n Computer scence
More informationThe Order Relation and Trace Inequalities for. Hermitian Operators
Internatonal Mathematcal Forum, Vol 3, 08, no, 507-57 HIKARI Ltd, wwwm-hkarcom https://doorg/0988/mf088055 The Order Relaton and Trace Inequaltes for Hermtan Operators Y Huang School of Informaton Scence
More informationFinite Element Modelling of truss/cable structures
Pet Schreurs Endhoven Unversty of echnology Department of Mechancal Engneerng Materals echnology November 3, 214 Fnte Element Modellng of truss/cable structures 1 Fnte Element Analyss of prestressed structures
More informationcoordinates. Then, the position vectors are described by
Revewng, what we have dscussed so far: Generalzed coordnates Any number of varables (say, n) suffcent to specfy the confguraton of the system at each nstant to tme (need not be the mnmum number). In general,
More informationMoments of Inertia. and reminds us of the analogous equation for linear momentum p= mv, which is of the form. The kinetic energy of the body is.
Moments of Inerta Suppose a body s movng on a crcular path wth constant speed Let s consder two quanttes: the body s angular momentum L about the center of the crcle, and ts knetc energy T How are these
More informationModule 14: THE INTEGRAL Exploring Calculus
Module 14: THE INTEGRAL Explorng Calculus Part I Approxmatons and the Defnte Integral It was known n the 1600s before the calculus was developed that the area of an rregularly shaped regon could be approxmated
More informationPhysics 5153 Classical Mechanics. Principle of Virtual Work-1
P. Guterrez 1 Introducton Physcs 5153 Classcal Mechancs Prncple of Vrtual Work The frst varatonal prncple we encounter n mechancs s the prncple of vrtual work. It establshes the equlbrum condton of a mechancal
More informationThe Analysis of Coriolis Effect on a Robot Manipulator
Internatonal Journal of Innovatons n Engneerng and echnology (IJIE) he Analyss of Corols Effect on a Robot Manpulator Pratap P homas Assstant Professor Department of Mechancal Engneerng K G Reddy college
More informationFirst Law: A body at rest remains at rest, a body in motion continues to move at constant velocity, unless acted upon by an external force.
Secton 1. Dynamcs (Newton s Laws of Moton) Two approaches: 1) Gven all the forces actng on a body, predct the subsequent (changes n) moton. 2) Gven the (changes n) moton of a body, nfer what forces act
More informationParameter Estimation for Dynamic System using Unscented Kalman filter
Parameter Estmaton for Dynamc System usng Unscented Kalman flter Jhoon Seung 1,a, Amr Atya F. 2,b, Alexander G.Parlos 3,c, and Klto Chong 1,4,d* 1 Dvson of Electroncs Engneerng, Chonbuk Natonal Unversty,
More informationIterative General Dynamic Model for Serial-Link Manipulators
EEL6667: Knematcs, Dynamcs and Control of Robot Manpulators 1. Introducton Iteratve General Dynamc Model for Seral-Lnk Manpulators In ths set of notes, we are gong to develop a method for computng a general
More informationAngular Momentum and Fixed Axis Rotation. 8.01t Nov 10, 2004
Angular Momentum and Fxed Axs Rotaton 8.01t Nov 10, 2004 Dynamcs: Translatonal and Rotatonal Moton Translatonal Dynamcs Total Force Torque Angular Momentum about Dynamcs of Rotaton F ext Momentum of a
More information2D Motion of Rigid Bodies: Falling Stick Example, Work-Energy Principle
Example: Fallng Stck 1.003J/1.053J Dynamcs and Control I, Sprng 007 Professor Thomas Peacock 3/1/007 ecture 10 D Moton of Rgd Bodes: Fallng Stck Example, Work-Energy Prncple Example: Fallng Stck Fgure
More informationDynamic Analysis Based On ANSYS of Turning and Grinding Compound Machine Spindle Box Zanhui Shu and Qiushi Han
Advanced Materals Research Onlne: 2012-01-03 ISSN: 1662-8985, Vols. 433-440, pp 524-529 do:10.4028/www.scentfc.net/amr.433-440.524 2012 Trans Tech Publcatons, Swtzerland Dynamc Analyss Based On ANSYS of
More informationMODEL OF HYDROPNEUMATIC THREE POINT HITCH
ENINEERIN FR RUR DEVEPMENT Jelgava, 3.-4.05.03. MDE F YDRPNEUMTI TREE PINT IT Jans acekls-bertmans, Erks Kronbergs atva Unversty of grculture jans.lacekls@llu.lv, erks.kronbergs@llu.lv bstract. Ths paper
More informationCHAPTER 14 GENERAL PERTURBATION THEORY
CHAPTER 4 GENERAL PERTURBATION THEORY 4 Introducton A partcle n orbt around a pont mass or a sphercally symmetrc mass dstrbuton s movng n a gravtatonal potental of the form GM / r In ths potental t moves
More informationLesson 5: Kinematics and Dynamics of Particles
Lesson 5: Knematcs and Dynamcs of Partcles hs set of notes descrbes the basc methodology for formulatng the knematc and knetc equatons for multbody dynamcs. In order to concentrate on the methodology and
More information9.2 Seismic Loads Using ASCE Standard 7-93
CHAPER 9: Wnd and Sesmc Loads on Buldngs 9.2 Sesmc Loads Usng ASCE Standard 7-93 Descrpton A major porton of the Unted States s beleved to be subject to sesmc actvty suffcent to cause sgnfcant structural
More informationMulti-Robot Formation Control Based on Leader-Follower Optimized by the IGA
IOSR Journal of Computer Engneerng (IOSR-JCE e-issn: 2278-0661,p-ISSN: 2278-8727, Volume 19, Issue 1, Ver. III (Jan.-Feb. 2017, PP 08-13 www.osrjournals.org Mult-Robot Formaton Control Based on Leader-Follower
More informationEVALUATION OF THE VISCO-ELASTIC PROPERTIES IN ASPHALT RUBBER AND CONVENTIONAL MIXES
EVALUATION OF THE VISCO-ELASTIC PROPERTIES IN ASPHALT RUBBER AND CONVENTIONAL MIXES Manuel J. C. Mnhoto Polytechnc Insttute of Bragança, Bragança, Portugal E-mal: mnhoto@pb.pt Paulo A. A. Perera and Jorge
More informationSo far: simple (planar) geometries
Physcs 06 ecture 5 Torque and Angular Momentum as Vectors SJ 7thEd.: Chap. to 3 Rotatonal quanttes as vectors Cross product Torque epressed as a vector Angular momentum defned Angular momentum as a vector
More informationMulti degree of freedom measurement of machine tool movements. W. Knapp, S.Weikert Institute for Machine Tools and Manufacturing (IWF), Swiss Federal
Mult degree of freedom measurement of machne tool movements W. Knapp, S.Wekert Insttute for Machne Tools and Manufacturng (IWF), Swss Federal \ ^r Az. ca, we z'tz rf @ z w/: Agpr. graz. ca Abstract The
More informationNUMERICAL RESULTS QUALITY IN DEPENDENCE ON ABAQUS PLANE STRESS ELEMENTS TYPE IN BIG DISPLACEMENTS COMPRESSION TEST
Appled Computer Scence, vol. 13, no. 4, pp. 56 64 do: 10.23743/acs-2017-29 Submtted: 2017-10-30 Revsed: 2017-11-15 Accepted: 2017-12-06 Abaqus Fnte Elements, Plane Stress, Orthotropc Materal Bartosz KAWECKI
More informationEPR Paradox and the Physical Meaning of an Experiment in Quantum Mechanics. Vesselin C. Noninski
EPR Paradox and the Physcal Meanng of an Experment n Quantum Mechancs Vesseln C Nonnsk vesselnnonnsk@verzonnet Abstract It s shown that there s one purely determnstc outcome when measurement s made on
More informationChapter 11 Angular Momentum
Chapter 11 Angular Momentum Analyss Model: Nonsolated System (Angular Momentum) Angular Momentum of a Rotatng Rgd Object Analyss Model: Isolated System (Angular Momentum) Angular Momentum of a Partcle
More informationFour Bar Linkages in Two Dimensions. A link has fixed length and is joined to other links and also possibly to a fixed point.
Four bar lnkages 1 Four Bar Lnkages n Two Dmensons lnk has fed length and s oned to other lnks and also possbly to a fed pont. The relatve velocty of end B wth regard to s gven by V B = ω r y v B B = +y
More informationStatistical Energy Analysis for High Frequency Acoustic Analysis with LS-DYNA
14 th Internatonal Users Conference Sesson: ALE-FSI Statstcal Energy Analyss for Hgh Frequency Acoustc Analyss wth Zhe Cu 1, Yun Huang 1, Mhamed Soul 2, Tayeb Zeguar 3 1 Lvermore Software Technology Corporaton
More informationOptimal algorithm for trajectory plann ing of the robot
13 1 20091 EL ECTR ICMACH IN ESANDCON TROL Vol113 No11 Jan. 2009 ( 150080) : SCARA ADAMS/V ew ADAMS :; ; ; ADAMS : TP242 : A : 1007-449X (2009) 01-0123- 05 Optmal algorthm for trajectory plann ng of the
More informationUnknown input extended Kalman filter-based fault diagnosis for satellite actuator
Internatonal Conference on Computer and Automaton Engneerng (ICCAE ) IPCSI vol 44 () () IACSI Press, Sngapore DOI: 776/IPCSIV44 Unnown nput extended Kalman flter-based fault dagnoss for satellte actuator
More informationELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM
ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM An elastc wave s a deformaton of the body that travels throughout the body n all drectons. We can examne the deformaton over a perod of tme by fxng our look
More informationScroll Generation with Inductorless Chua s Circuit and Wien Bridge Oscillator
Latest Trends on Crcuts, Systems and Sgnals Scroll Generaton wth Inductorless Chua s Crcut and Wen Brdge Oscllator Watcharn Jantanate, Peter A. Chayasena, and Sarawut Sutorn * Abstract An nductorless Chua
More informationOne-sided finite-difference approximations suitable for use with Richardson extrapolation
Journal of Computatonal Physcs 219 (2006) 13 20 Short note One-sded fnte-dfference approxmatons sutable for use wth Rchardson extrapolaton Kumar Rahul, S.N. Bhattacharyya * Department of Mechancal Engneerng,
More informationOn the Multicriteria Integer Network Flow Problem
BULGARIAN ACADEMY OF SCIENCES CYBERNETICS AND INFORMATION TECHNOLOGIES Volume 5, No 2 Sofa 2005 On the Multcrtera Integer Network Flow Problem Vassl Vasslev, Marana Nkolova, Maryana Vassleva Insttute of
More informationDEFORMABLE GROUND CONTACT MODELING: AN OPTIMIZATION APPROACH. Jeff Reinbolt. EML 5595 Mechanics of the Human Locomotor System Final Project Report
DEFORMABLE GROUND CONAC MODELING: AN OPIMIZAION APPROACH Jeff Renbolt EML 9 Mechancs of the Human Locomotor System Fnal Project Report INRODUCION One of the most mportant choces made n creatng a mult-body
More informationUncertainty in measurements of power and energy on power networks
Uncertanty n measurements of power and energy on power networks E. Manov, N. Kolev Department of Measurement and Instrumentaton, Techncal Unversty Sofa, bul. Klment Ohrdsk No8, bl., 000 Sofa, Bulgara Tel./fax:
More informationReport on Image warping
Report on Image warpng Xuan Ne, Dec. 20, 2004 Ths document summarzed the algorthms of our mage warpng soluton for further study, and there s a detaled descrpton about the mplementaton of these algorthms.
More informationChapter 5. Solution of System of Linear Equations. Module No. 6. Solution of Inconsistent and Ill Conditioned Systems
Numercal Analyss by Dr. Anta Pal Assstant Professor Department of Mathematcs Natonal Insttute of Technology Durgapur Durgapur-713209 emal: anta.bue@gmal.com 1 . Chapter 5 Soluton of System of Lnear Equatons
More informationMMA and GCMMA two methods for nonlinear optimization
MMA and GCMMA two methods for nonlnear optmzaton Krster Svanberg Optmzaton and Systems Theory, KTH, Stockholm, Sweden. krlle@math.kth.se Ths note descrbes the algorthms used n the author s 2007 mplementatons
More informationIn this section is given an overview of the common elasticity models.
Secton 4.1 4.1 Elastc Solds In ths secton s gven an overvew of the common elastcty models. 4.1.1 The Lnear Elastc Sold The classcal Lnear Elastc model, or Hooean model, has the followng lnear relatonshp
More informationEN40: Dynamics and Vibrations. Homework 7: Rigid Body Kinematics
N40: ynamcs and Vbratons Homewor 7: Rgd Body Knematcs School of ngneerng Brown Unversty 1. In the fgure below, bar AB rotates counterclocwse at 4 rad/s. What are the angular veloctes of bars BC and C?.
More information10/9/2003 PHY Lecture 11 1
Announcements 1. Physc Colloquum today --The Physcs and Analyss of Non-nvasve Optcal Imagng. Today s lecture Bref revew of momentum & collsons Example HW problems Introducton to rotatons Defnton of angular
More informationAn Application of Fuzzy Hypotheses Testing in Radar Detection
Proceedngs of the th WSES Internatonal Conference on FUZZY SYSEMS n pplcaton of Fuy Hypotheses estng n Radar Detecton.K.ELSHERIF, F.M.BBDY, G.M.BDELHMID Department of Mathematcs Mltary echncal Collage
More informationErrors for Linear Systems
Errors for Lnear Systems When we solve a lnear system Ax b we often do not know A and b exactly, but have only approxmatons  and ˆb avalable. Then the best thng we can do s to solve ˆx ˆb exactly whch
More informationModelling and Analysis of Planar Robotic Arm Dynamics Based on An Improved Transfer Matrix Method for Multi-body Systems
he 4th FoMM World ongress, ape, awan, ctober 5-3, 5 D Number:.6567/FoMM.4H.W.S3.46 Modellng and Analyss of Planar Robotc Arm Dynamcs Based on An mproved ransfer Matrx Method for Mult-body Systems W. hen
More informationApplication to Plane (rigid) frame structure
Advanced Computatonal echancs 18 Chapter 4 Applcaton to Plane rgd frame structure 1. Dscusson on degrees of freedom In case of truss structures, t was enough that the element force equaton provdes onl
More informationCelestial Mechanics. Basic Orbits. Why circles? Tycho Brahe. PHY celestial-mechanics - J. Hedberg
PHY 454 - celestal-mechancs - J. Hedberg - 207 Celestal Mechancs. Basc Orbts. Why crcles? 2. Tycho Brahe 3. Kepler 4. 3 laws of orbtng bodes 2. Newtonan Mechancs 3. Newton's Laws. Law of Gravtaton 2. The
More informationGravitational Acceleration: A case of constant acceleration (approx. 2 hr.) (6/7/11)
Gravtatonal Acceleraton: A case of constant acceleraton (approx. hr.) (6/7/11) Introducton The gravtatonal force s one of the fundamental forces of nature. Under the nfluence of ths force all objects havng
More information