Journal of System Design and Dynamics

Size: px
Start display at page:

Download "Journal of System Design and Dynamics"

Transcription

1 Vbraton Control of Safe Robot Arm wth MR-Based Passve Complant Jont * Seung-kook YUN**,, Seong-Sk YOON**,, Sungchul KANG**, and Munsang KIM** **Intellgent Robotcs Research Center, Korea Insttute of Scence and echnology, Hawolgok-dong1 39-1, Sungbuk-ku, Seoul , Korea E-mal: yunsk@mt.edu, yoon@cello.korea.ac.kr, {kasch, munsang}@kst.re.kr Mr. Seung-kook Yun s now wth Computer Scence and Artfcal Intellgence Laboratory, Massachusetts Insttute of echnology, Cambrdge, USA. Dr. Seong-sk Yoon s currently wth ACI Devson, Samsung Electro-Mechancs Co., 581, Dong-Myon, Yeong-gun, Chungcheongnam-Do , Korea. Abstract In ths paper, vbraton control of a safe arm wth passve complant jonts and vsco-elastc coverng for a human-frendly servce robot s presented. he passve complant jont (PCJ) s desgned to passvely attenuate the appled force. he rotary sprng gves the arm complant property, and yet t can be a source of vbraton. We use an nput-preshapng method whch s motvated by the nput shapng technque (IS) based on mpulse responses. Experments prove that both of fast moton and force attenuaton of the safe arm can be acheved. Key words: Passve Complant Jont, Magneto-Rheologcal Damper, Vsco-Elastc Coverng, Safety, Input Shapng echnque 1. Introducton *Receved 21 Dec., 27 (No ) [DOI: /jsdd.2.475] Buldng a safe robot manpulator and performng hgh-speed manpulaton s a trade-off when speed and precson are consdered (1)(2)(3). he less stff complance we use n a robot arm, the more dffcult the arm has fast moton. In our prevous work (4), a safe arm of a servce robot was developed. In order to have a safe nteracton n a human-robot envronment, the arm has passve complant jonts composed of a magneto-rheologcal rotary damper and rotary sprngs. Despte of the guaranteed safety, unwanted vbraton can occur because of sprngs ncluded n the PCJ durng fast jont moton. Although the damper of the PCJ partly suppresses vbraton, quck moton cannot be performed wthout vbraton. hs vbraton can cause unstable moton or collson to the envronment, whch degrades safety. In ths paper, we propose a new method to enhance performance of our safe manpulator by vbraton control based on nput preshapng. he Input Shapng echnque(is) (5) based on mpulse responses s consdered to solve a problem of vbraton, because of ts smple structure and hgh effcency. he IS s an excellent soluton to reduce vbraton for a lnear tme nvarant(li) system, however t s not so effectve for a non-lnear or a tme varyng system and the safe arm s a tme varyng system n whch ts nertal propertes change accordng to the arm confguraton. Although t s almost mpossble to fnd the exact tmng of the second mpulse for a tme varyng system, there have been approaches to fnd the sequence. Park proved that a proper IS flter wth two mpulses can elmnate a resdual vbraton of a tme nvarant system (6). Rappole (7) appled a tme varyng nput shapng technque(vis) to a two lnk flexble manpulator, and Park (8) proposed a practcal method of the VIS to reduce vbraton of an ndustral robot. he former used a look-up table whch contaned nformaton on confguraton-dependent frequences, whle the latter had a smple equaton relatng a perod 475

2 of vbraton to a length from the swng axs to the wrst axs. Although these methods reduce vbraton of a tme varyng system, an estmaton of tmng of the second mpulse tme s always ncorrect because of dynamcs of a manpulator. Motvated from the IS based on mpulse responses, we desgn a new algorthm to reduce vbraton at both the start and the end poston. Wth the developed safe arm and the proposed control method, experments for vbraton reducton are performed to verfy that vbraton reducton s successfully acheved. hs paper s composed of fve sectons. In Secton 2, we ntroduce how to desgn the 6-dof safe arm ncludng three PCJs. In Secton 3, the nput preshapng method for vbraton reducton of the PCJ s proposed as a controller for the safe arm. Experments on vbraton control by the proposed nput preshapng method are shown n Secton 4. Fnally, we conclude ths work n Secton Safe Arm Desgn We ntroduce a passve complant jont wth a magneto-rheologcal damper and a sprng. Wth the PCJs and soft cover, we show a 6DOF arm for a servce robot. he detals of the arm are n Ref. (4). (a) (b) Fg.1 (a) Desgn of passve complant jont mechansm. (b) Developed PCJ 2.1 Passve Complant Jont Desgn A schematc desgn and components of a passve complant jont(pcj) s shown n Fg. 1. It conssts of a magneto-rheologcal (MR) rotary damper and a rotary sprng. In the PCJ, a MR rotary damper s ntroduced for dampng effect. he PCJ has a resolver sensor wth 16-bts hgh resoluton to read the relatve poston between the housng and the next lnk due to the sprng dsplacement. he relatve poston s converted nto a relatve velocty sgnal by a numercal dfferentaton and a flterng. hen the velocty s sent to a dampng tuner whch converts Coulomb frcton property of the MR flud nto vscous one whch makes the dynamc system lnear. Note that the damper and sprng are located n parallel between the housng and next lnk Safe Arm Desgn By ntegratng the MR-based passve complant jonts and the vsco-elastc coverng, a new safe arm s developed for servce robot applcatons. A sx-dof safe arm wth 3Kg-payload, 3kg weght and 1m reach has been developed as depcted n Fg. 2. hs arm s used for the PSR-2 (Publc Servce Robot) developed at the KIS (Korea Insttute of Scence and echnology). akng account of the weght ncrease of the arm due to the weght of MR dampers and sprngs, PCJs are adopted only to three jonts n the lower part of the 6-dof servce robot arm. he three PCJs gve the arm complance nto the three 476

3 drectons. Parameters for the PCJs are shown n Fg. 2(c) and able.1. θ, x, y complant y x θ (a) (b) m 4=1.7 m5= m 1=4.7 m 2=8. m 3= payload 13. (c) Fg.2 (a) KIS Safe Arm (b) schematc dagram of the arm (c) lengths of the lnks and estmated weghts of pont masses able 1 Specfcatons of the PCJs Axs number Axs 1 Axs 2 Axs 3 Sprng Constant (Nm/rad) Maxmum dampngorque (Nm) Vscous dampng coeffcent (Nm sec/rad) Controller Desgn: Input Preshapng Method for the Safe Arm Although the PCJ enables passve complance, t also can be a source of unwanted vbraton and deflecton by gravty. hey can cause unstable moton or naccuracy of the jont angle. In partcular, bg amount of resdual vbraton can occur durng fast rotaton of the PCJ. o cope wth ths problem, we desgn a vbraton controller based on the nput shapng technque. 3.1 Estmaton of me Varyng Perod of Vbraton from PCJs As an effectve soluton to reduce ths vbraton, an nput shapng technque(is) based on mpulse response was proposed (5). he IS uses two mpulses to elmnate resdual vbraton. Fgure 3 shows how the IS works wth two mpulse responses. If the second mpulse tme s properly selected, the superposed response wll have no vbraton after the second mpulse. he IS s a smple flter snce two mpulses are convoluted wth a desred trajectory or an open loop control nput. 477

4 Fg.3 Vbraton suppresson va IS For ths tme varyng nput shapng technque(vis), we need to know perods of vbraton n all confguratons that the arm can have n ts workspace. Note that t s proved that a proper IS flter wth two mpulses can elmnate a resdual vbraton of a tme nvarant system (6). A dynamc equaton of the -th PCJ of the safe arm excludng gravty s as follows: J ( θ ) θ + C( θ, θ ) + K ( θ θ ) = τ (1) m where J s a nerta term, C s a Corols and centrfugal term, K s a sprng constant, θ m s a motor angle of -th axs and τ s a control torque. A perod of vbraton for the -th PCJ can be expressed as follows: J = 2 π ( = 1,2,3) (2) K Because the safe arm s a seral manpulator, a perod of vbraton for each jont s functon of the next jont angles assumng a sprng constant s tme-nvarant. We consder the perod of vbraton for the thrd jont as a constant because change of nerta along the wrst confguraton s comparably small. herefore, tme varyng ISs for the frst and second jont are needed. In ths paper, vbraton control of the second jont s only mplemented snce the same method can be appled to the frst jont. perod of vbraton (s) expermental value ftted cosne curve θ 3 (deg) Fg.4 Perod of vbraton at second jont along jont confguratons o determne parameters for VIS, the perods of vbraton at dfferent confguratons 478

5 are expermentally measured. In Fg.4, the perod of vbraton for the second jont accordng to the thrd jont angle s shown. We can expect the perod of vbraton s proportonal to square root of cosθ 3 because nerta s proportonal to the square root of cosθ 3. he curve of perod of vbraton s a functon of cosθ 3 as follows: = α + β cos( θ θ ) (3) perod 3 o where α =.2, β =.22, θ ο = 3. We can make a table of the perod of vbraton along each jont confguraton usng obtaned data. When controllng the PCJ, we can use the table or the equaton. Although ths paper deals wth only the case of no-payload, we can extend the method for any payload condtons by measurng the vbraton perods wth varous payloads and nterpolatng values from the curve equatons. 3.2 Modfed VIS In prevous VISs, a controller estmates the second mpulse tmng by comparng a jont confguraton wth measured perods of vbraton. Even f the estmaton s correct and the measured data are exact, however, there wll be stll a lttle vbraton because of tmng error due to dynamcs of the system. When nerta ncreases, the second mpulse occurs later than the correct tmng as shown n Fg.5. Fg.5 Estmaton error of the second mpulse tmng o compensate ths error, we propose to estmate the second mpulse tme as a mean of the measured parameters at the start and the end. he proposed method gves better result unless dynamcs s faster than a changng rate of the mpulse tmng. We have found the dynamcs of the developed manpulator s not fast enough that our estmaton holds. Furthermore, t wll gve a perfect result f the square root of nerta changes lnearly. For ths, the nerta change of our manpulator shows approxmately lnearly snce tme between the mpulses s very short compared to the jont trajectory. hen the second mpulse tme guessed at the moton-start as follows: half + half _ start half _ VIS = (4) 2 where 479

6 half _ start = π J( θ( t)) K θ = θ ( t= ) start (5) half _ VIS = π J( θ( t)) K θ = θ( t= estmated tme) (6) 35 1 motor angle [deg] lnk angle motor angle PCJ dsplacement [deg] tme [s] tme [s] (a) (b) Fg.6 (a) Motor angle and lnk angle of the second PCJ (b) two modes of vbraton n PCJ dsplacement PCJ dsplacement [deg] 1.5 modfed VIS for 1st fltered orgnal PCJ dsplacement [deg] 1.5 conventonal IS for 2nd tme [s] tme [s] (a) (b) Fg.7 Smulaton results: (a) IS for the frst mode (b) IS for the second mode 3.3 Input Preshapng Method for the safe arm Generally, there are two phases of vbraton durng the moton of a flexble jont. he frst one s excted by start moton, and the second s by end moton. In Fg.6, a smulaton result s shown when the second axs moves by 3 degree durng one second. Lookng at the rght part of the drawng carefully, we can fnd that there are two knd of vbraton; the frst one s started at zero second, and the second s started at one second whch s the begnnng of the steady state. wo vbratons have dfferent frequences snce the safe arm s a tme varyng system. herefore, we need two dfferent IS flters to elmnate both of vbraton. We desgn a proposed VIS flter for the frst vbraton, and a conventonal IS flter for the 2nd vbraton because the system s almost tme nvarant when the jont moton reaches the steady state. Smulaton results are shown In Fg.7. Fgure 7(a) results from a controller wth a 48

7 modfed VIS, and Fgure 7(b) comes from a conventonal IS for the second vbraton. We can see the modfed VIS elmnates the frst vbraton but second vbraton, and the conventonal IS can elmnate only the second vbraton. In case of a lnear tme nvarant system, we can easly elmnate both of vbraton by usng a merged IS flter by convolutng the frst IS flter to second one. However, ths prncple does not work n case of a lnear tme varyng system. Now we propose a new nput-preshapng method for the safe arm. We already have IS parameters of each vbraton that are composed of each magntude of two mpulses and the second mpulse tmng. All parameters we need to know are lsted as follows: A 1 : magntude of 1st mpulse for the modfed VIS A 2 : magntude of 2nd mpulse for the modfed VIS 2A : half perod of 1st vbraton B 1 : magntude of 1st mpulse for the conventonal IS B 2 : magntude of 2nd mpulse for the conventonal IS 2B : half perod of 2nd vbraton Where A + A = B + B = (7) to guarantee the same steady-state value. We set a new trajectory whch s convoluted by the mpulses as follows: θ () t = R [ Aθ () t + Aθ ( t ) u( t )] < t< * d 1 d 2 d 2A 2A f θ () t = R [ Bθ () t + Bθ ( t ) u( t ) + α] < t * d 1 d 2 d 2B 2B f (8) where f s the tme of steady state pont and θ d s a orgnal desred trajectory and R s set to satsfy the followng: θ dt = θ dt (9) + f f 2 B * d d, therefore the total dsplacement of the reference trajectory s the same as that of the shaped one. Note that the fnal dsplacement of the jont s mantaned by R. α = Aθ ( ) + Aθ ( ) Bθ ( ) Bθ ( ) (1) 1 d f 2 d f 2A 1 d f 2 d f 2B, and for t < ut ( ) = 1 for t > (11) whch s a step functon to enable the effect of the mpulses. All calculatons are executed off-lne, not a real-tme estmaton. If a reference trajectory s gven, we can estmate all parameters from the frequency and jont confguraton table. Fgure 8 shows a smulaton result usng proposed nput preshapng method. You can see that smple change of the reference nput make clear response wthout vbraton. he proposed method gves better result than that of both tme nvarant and tme varyng nput shapng flters because ths reflects not only tme varyng property of the system but also the 481

8 dynamc effect durng the control w/ preshaped w/ unshaped 1 w/ preshaped w/ unshaped desred velocty [deg/s] PCJ dsplacement [deg] tme [s] tme [s] Fg.8 Smulaton: proposed nput preshapng method 4. Expermental Results We prove the proposed nput preshapng by experments wth the safe arm. Vbratons of the second and thrd jont are successfully suppressed wth the IS and the proposed controller. As for the set-up, a PC-based UMAC moton controller (9) s used for controllng the sx-dof safe arm, and MR dampers are ndependently controlled. Encoder sgnals are sent to PC va USB and RS-232C port. motor angle3 (deg) command velocty (deg/s) t m e [s] ( a ) t m e [ s] ( b ) w / I S w / o I S w / I S w / o I S PCJ dsplacement (deg) w/ IS w/o IS tme [s] (c) Fg.9 Experment: vbraton reducton for thrd axs: (a) motor angle of the 3rd jont. (b) command velocty of the thrd motor, (c) PCJ dsplacement of 3rd PCJ defned n equaton(5) An experment of rotatng the thrd jont of the safe arm wth the IS s presented n Fg. 9. A desred trajectory s 6 deg/sec durng a second. We have found that the frequency of the vbraton s around 3Hz. he mplemented IS reduces vbraton from the 3rd axs dramatcally. Note that the dfference between the PCJ dsplacement of a startng pont and steady state s caused by gravty of the lnk. As shown n Fg. 9, IS works well even n gravty. A lttle amount of overshoot s stll shown, but ths s due to the nerta of the thrd 482

9 lnk not to the vbraton mode. After the second mpulse tmng, lttle vbraton s shown. 3 Fg.1 Change of jont confguraton durng the experment Wth the proposed VIS controller, an experment of rotatng the 2nd axs wth varyng effectve nerta s performed. he jont moves from 3 degree to zero degree, whle the thrd jont rotates from 3 degree to +3 degree as shown n Fg.1. Wth a gven trajectory and the table of perods of vbraton versus jont confguratons, we can expect that the frequency of vbraton vares from 1.85Hz to 1.55Hz. A trajectory by the proposed algorthm s generated and tested. Fgure 11 shows the preshaped nput and the vbraton of the second PCJ. he controller wth the preshaped nput clearly suppresses both of vbraton ncludng vbraton of startng moton and endng moton. θ 2 (deg) velocty (deg/s) tme [s] (a) w/o preshaped w/ preshaped PCJ dsplacement (deg) w/ unshaped nput w/ preshaped nput tme [s] (b) tme [s] Fg.11 Experment: vbraton reducton for 2nd axs: (a) motor angle of the 2nd jont, (b) command velocty of the 2nd motor, (c) dsplacement of the 2nd PCJ 5. Concluson In ths paper, we propose a new nput preshapng controller for a safe arm that has passve complant jonts wth sprngs and dampers and a soft cover. wo modes of vbraton are caused by startng moton and by endng moton, and a reference trajectory s shaped to reduce the vbraton by the proposed controller. Parameters of mpulse sequences by the 483

10 modfed VIS and a conventonal IS are used for nput preshapng. Expermental results show that proposed method mplemented successfully to the safe arm. In future, we wll explore strateges for contact moton by the safe arm as well as devse lghtweght passve jonts. References (1) M. Znn, O. Khatb, B. Roth, and J. Salsbury, Playng t safe [humanfrendly robots], Robotcs and Automaton Magazne, IEEE, vol. 11(24), pp (2). Morta and S. Sugano, Development and evaluaton of seven dof ma arm, n IEEE Internatonal Conference on Robotcs and Automaton, 1997, pp (3) A. Bcch and G. onett. Fast and Soft Arm actcs: Dealng wth the Safety-Performance rade-off n Robot Arms Control IEEE Robotcs and Automaton Magazne, Vol. 11(24), pp (4) S.-S. Yoon, S. Kang, S.-J. Km, Y.-H. Km, M. Km, and C.-w. Lee, "Safe Arm wth MR-based Passve Complant jonts and Vsco-elastc Coverng for Servce Robot Applcaton, In Proceedngs of the IEEE/RSJ Internatonal Conference on Intellgent Robots and Systems(23), pp (5) N.C. Snger, and W.P. Seerng, Preshapng Command Inputs to Reduce System Vbraton, ASME Journal of Dynamc Systems, Measurement and Control, Vol.112(199), pp (6) J. Park, P.H. Chang, and E. Lee, Can a me Invarant Input Shapng echnque Elmnate Resdual Vbratons of LV Systems, Proc. of the Amercan Control Conference(22), pp (7) B.W. Rappole, Mnmzng Resdual Vbratons n Flexble Systems, Master thess, Department of Mechancal Engneerng (1992), MI. (8) H.Y. Park, P.H. Chang, and J.S. Hur, me-varyng Input Shapng echnque Appled to Vbraton Reducton of An Industral Robot, Proc. of the IEEE/RSJ Internatonal Conference on Intellgent Robots and Systems(1999), pp (9) he Deltaau Corporaton ( 484

Study on Active Micro-vibration Isolation System with Linear Motor Actuator. Gong-yu PAN, Wen-yan GU and Dong LI

Study 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 information

An Algorithm to Solve the Inverse Kinematics Problem of a Robotic Manipulator Based on Rotation Vectors

An 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 information

829. An adaptive method for inertia force identification in cantilever under moving mass

829. 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

Pop-Click Noise Detection Using Inter-Frame Correlation for Improved Portable Auditory Sensing

Pop-Click Noise Detection Using Inter-Frame Correlation for Improved Portable Auditory Sensing Advanced Scence and Technology Letters, pp.164-168 http://dx.do.org/10.14257/astl.2013 Pop-Clc Nose Detecton Usng Inter-Frame Correlaton for Improved Portable Audtory Sensng Dong Yun Lee, Kwang Myung Jeon,

More information

Parameter Estimation for Dynamic System using Unscented Kalman filter

Parameter 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 information

CHAPTER 5 NUMERICAL EVALUATION OF DYNAMIC RESPONSE

CHAPTER 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 information

Effect of loading frequency on the settlement of granular layer

Effect 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 information

Advanced Mechanical Elements

Advanced 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 information

First 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.

First 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 information

11. Dynamics in Rotating Frames of Reference

11. 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 information

Second Order Analysis

Second Order Analysis Second Order Analyss In the prevous classes we looked at a method that determnes the load correspondng to a state of bfurcaton equlbrum of a perfect frame by egenvalye analyss The system was assumed to

More information

NUMERICAL DIFFERENTIATION

NUMERICAL DIFFERENTIATION NUMERICAL DIFFERENTIATION 1 Introducton Dfferentaton s a method to compute the rate at whch a dependent output y changes wth respect to the change n the ndependent nput x. Ths rate of change s called the

More information

Transfer Functions. Convenient representation of a linear, dynamic model. A transfer function (TF) relates one input and one output: ( ) system

Transfer Functions. Convenient representation of a linear, dynamic model. A transfer function (TF) relates one input and one output: ( ) system Transfer Functons Convenent representaton of a lnear, dynamc model. A transfer functon (TF) relates one nput and one output: x t X s y t system Y s The followng termnology s used: x y nput output forcng

More information

THE EFFECT OF TORSIONAL RIGIDITY BETWEEN ELEMENTS ON FREE VIBRATIONS OF A TELESCOPIC HYDRAULIC CYLINDER SUBJECTED TO EULER S LOAD

THE 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 information

Modeling of Dynamic Systems

Modeling 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 information

One-sided finite-difference approximations suitable for use with Richardson extrapolation

One-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 information

Indeterminate pin-jointed frames (trusses)

Indeterminate 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 information

COMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD

COMPOSITE 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 information

Design and Analysis of Landing Gear Mechanic Structure for the Mine Rescue Carrier Robot

Design and Analysis of Landing Gear Mechanic Structure for the Mine Rescue Carrier Robot Sensors & Transducers 214 by IFSA Publshng, S. L. http://www.sensorsportal.com Desgn and Analyss of Landng Gear Mechanc Structure for the Mne Rescue Carrer Robot We Juan, Wu Ja-Long X an Unversty of Scence

More information

EN40: Dynamics and Vibrations. Homework 4: Work, Energy and Linear Momentum Due Friday March 1 st

EN40: Dynamics and Vibrations. Homework 4: Work, Energy and Linear Momentum Due Friday March 1 st EN40: Dynamcs and bratons Homework 4: Work, Energy and Lnear Momentum Due Frday March 1 st School of Engneerng Brown Unversty 1. The fgure (from ths publcaton) shows the energy per unt area requred to

More information

Suppose that there s a measured wndow of data fff k () ; :::; ff k g of a sze w, measured dscretely wth varable dscretzaton step. It s convenent to pl

Suppose that there s a measured wndow of data fff k () ; :::; ff k g of a sze w, measured dscretely wth varable dscretzaton step. It s convenent to pl RECURSIVE SPLINE INTERPOLATION METHOD FOR REAL TIME ENGINE CONTROL APPLICATIONS A. Stotsky Volvo Car Corporaton Engne Desgn and Development Dept. 97542, HA1N, SE- 405 31 Gothenburg Sweden. Emal: astotsky@volvocars.com

More information

Assessment of Site Amplification Effect from Input Energy Spectra of Strong Ground Motion

Assessment 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 information

Note 10. Modeling and Simulation of Dynamic Systems

Note 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 information

Irregular vibrations in multi-mass discrete-continuous systems torsionally deformed

Irregular 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 information

Design and Optimization of Fuzzy Controller for Inverse Pendulum System Using Genetic Algorithm

Design 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 information

Statistical Energy Analysis for High Frequency Acoustic Analysis with LS-DYNA

Statistical 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 information

ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM

ELASTIC 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 information

COEFFICIENT DIAGRAM: A NOVEL TOOL IN POLYNOMIAL CONTROLLER DESIGN

COEFFICIENT DIAGRAM: A NOVEL TOOL IN POLYNOMIAL CONTROLLER DESIGN Int. J. Chem. Sc.: (4), 04, 645654 ISSN 097768X www.sadgurupublcatons.com COEFFICIENT DIAGRAM: A NOVEL TOOL IN POLYNOMIAL CONTROLLER DESIGN R. GOVINDARASU a, R. PARTHIBAN a and P. K. BHABA b* a Department

More information

Research on the Fuzzy Control for Vehicle Semi-active Suspension. Xiaoming Hu 1, a, Wanli Li 1,b

Research 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 information

Chapter 5. Solution of System of Linear Equations. Module No. 6. Solution of Inconsistent and Ill Conditioned Systems

Chapter 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 information

A Multi-Axis Force Measurement System for a Space Docking Mechanism

A 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 information

A particle in a state of uniform motion remain in that state of motion unless acted upon by external force.

A particle in a state of uniform motion remain in that state of motion unless acted upon by external force. The fundamental prncples of classcal mechancs were lad down by Galleo and Newton n the 16th and 17th centures. In 1686, Newton wrote the Prncpa where he gave us three laws of moton, one law of gravty,

More information

Lab 2e Thermal System Response and Effective Heat Transfer Coefficient

Lab 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 information

Department of Electrical & Electronic Engineeing Imperial College London. E4.20 Digital IC Design. Median Filter Project Specification

Department of Electrical & Electronic Engineeing Imperial College London. E4.20 Digital IC Design. Median Filter Project Specification Desgn Project Specfcaton Medan Flter Department of Electrcal & Electronc Engneeng Imperal College London E4.20 Dgtal IC Desgn Medan Flter Project Specfcaton A medan flter s used to remove nose from a sampled

More information

Physics 5153 Classical Mechanics. D Alembert s Principle and The Lagrangian-1

Physics 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 information

Iterative General Dynamic Model for Serial-Link Manipulators

Iterative 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 information

Command Shaping Under Nonsymmetrical Acceleration and Braking Dynamics

Command Shaping Under Nonsymmetrical Acceleration and Braking Dynamics Command Shapng Under Nonsymmetrcal Acceleraton and Brakng Dynamcs homas H. Bradley Jon Danelson Jason Lawrence Wllam Snghose Georga Insttute of echnology, Atlanta, GA 30332-0405 he conventonal unty magntude

More information

Identification of Instantaneous Modal Parameters of A Nonlinear Structure Via Amplitude-Dependent ARX Model

Identification of Instantaneous Modal Parameters of A Nonlinear Structure Via Amplitude-Dependent ARX Model Identfcaton of Instantaneous Modal Parameters of A Nonlnear Structure Va Ampltude-Dependent ARX Model We Chh Su(NCHC), Chung Shann Huang(NCU), Chng Yu Lu(NCU) Outlne INRODUCION MEHODOLOGY NUMERICAL VERIFICAION

More information

MEASUREMENT OF MOMENT OF INERTIA

MEASUREMENT OF MOMENT OF INERTIA 1. measurement MESUREMENT OF MOMENT OF INERTI The am of ths measurement s to determne the moment of nerta of the rotor of an electrc motor. 1. General relatons Rotatng moton and moment of nerta Let us

More information

MEV442 Introduction to Robotics Module 2. Dr. Santhakumar Mohan Assistant Professor Mechanical Engineering National Institute of Technology Calicut

MEV442 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 information

Week 9 Chapter 10 Section 1-5

Week 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 information

VIBRATION FATIGUE DESIGN METHODOLOGY OF A LARGE SCALE HEAVY DUTY ROBOT

VIBRATION FATIGUE DESIGN METHODOLOGY OF A LARGE SCALE HEAVY DUTY ROBOT ICSV14 Carns Australa 9-12 July, 2007 VIBRATION FATIGUE DESIGN METHODOLOGY OF A LARGE SCALE HEAVY DUTY ROBOT Jong Hw Seo 1, Jae Chul Hwang 1, Yong Won Cho 1, Dong Il Km 1, Hong Jae Ym 2 1 Robotcs Technology

More information

1 Derivation of Rate Equations from Single-Cell Conductance (Hodgkin-Huxley-like) Equations

1 Derivation of Rate Equations from Single-Cell Conductance (Hodgkin-Huxley-like) Equations Physcs 171/271 -Davd Klenfeld - Fall 2005 (revsed Wnter 2011) 1 Dervaton of Rate Equatons from Sngle-Cell Conductance (Hodgkn-Huxley-lke) Equatons We consder a network of many neurons, each of whch obeys

More information

Conservation of Angular Momentum = "Spin"

Conservation 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 information

Spin-rotation coupling of the angularly accelerated rigid body

Spin-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 information

Week3, Chapter 4. Position and Displacement. Motion in Two Dimensions. Instantaneous Velocity. Average Velocity

Week3, 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 information

AP Physics 1 & 2 Summer Assignment

AP 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 information

The Analysis of Coriolis Effect on a Robot Manipulator

The 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 information

ONE DIMENSIONAL TRIANGULAR FIN EXPERIMENT. Technical Advisor: Dr. D.C. Look, Jr. Version: 11/03/00

ONE DIMENSIONAL TRIANGULAR FIN EXPERIMENT. Technical Advisor: Dr. D.C. Look, Jr. Version: 11/03/00 ONE IMENSIONAL TRIANGULAR FIN EXPERIMENT Techncal Advsor: r..c. Look, Jr. Verson: /3/ 7. GENERAL OJECTIVES a) To understand a one-dmensonal epermental appromaton. b) To understand the art of epermental

More information

8 Derivation of Network Rate Equations from Single- Cell Conductance Equations

8 Derivation of Network Rate Equations from Single- Cell Conductance Equations Physcs 178/278 - Davd Klenfeld - Wnter 2015 8 Dervaton of Network Rate Equatons from Sngle- Cell Conductance Equatons We consder a network of many neurons, each of whch obeys a set of conductancebased,

More information

Supplemental Material: Causal Entropic Forces

Supplemental Material: Causal Entropic Forces Supplemental Materal: Causal Entropc Forces A. D. Wssner-Gross 1, 2, and C. E. Freer 3 1 Insttute for Appled Computatonal Scence, Harvard Unversty, Cambrdge, Massachusetts 02138, USA 2 The Meda Laboratory,

More information

ECE559VV Project Report

ECE559VV Project Report ECE559VV Project Report (Supplementary Notes Loc Xuan Bu I. MAX SUM-RATE SCHEDULING: THE UPLINK CASE We have seen (n the presentaton that, for downlnk (broadcast channels, the strategy maxmzng the sum-rate

More information

DETERMINATION OF TEMPERATURE DISTRIBUTION FOR ANNULAR FINS WITH TEMPERATURE DEPENDENT THERMAL CONDUCTIVITY BY HPM

DETERMINATION OF TEMPERATURE DISTRIBUTION FOR ANNULAR FINS WITH TEMPERATURE DEPENDENT THERMAL CONDUCTIVITY BY HPM Ganj, Z. Z., et al.: Determnaton of Temperature Dstrbuton for S111 DETERMINATION OF TEMPERATURE DISTRIBUTION FOR ANNULAR FINS WITH TEMPERATURE DEPENDENT THERMAL CONDUCTIVITY BY HPM by Davood Domr GANJI

More information

CHAPTER 4 SPEECH ENHANCEMENT USING MULTI-BAND WIENER FILTER. In real environmental conditions the speech signal may be

CHAPTER 4 SPEECH ENHANCEMENT USING MULTI-BAND WIENER FILTER. In real environmental conditions the speech signal may be 55 CHAPTER 4 SPEECH ENHANCEMENT USING MULTI-BAND WIENER FILTER 4.1 Introducton In real envronmental condtons the speech sgnal may be supermposed by the envronmental nterference. In general, the spectrum

More information

9 Derivation of Rate Equations from Single-Cell Conductance (Hodgkin-Huxley-like) Equations

9 Derivation of Rate Equations from Single-Cell Conductance (Hodgkin-Huxley-like) Equations Physcs 171/271 - Chapter 9R -Davd Klenfeld - Fall 2005 9 Dervaton of Rate Equatons from Sngle-Cell Conductance (Hodgkn-Huxley-lke) Equatons We consder a network of many neurons, each of whch obeys a set

More information

Introduction to Vapor/Liquid Equilibrium, part 2. Raoult s Law:

Introduction to Vapor/Liquid Equilibrium, part 2. Raoult s Law: CE304, Sprng 2004 Lecture 4 Introducton to Vapor/Lqud Equlbrum, part 2 Raoult s Law: The smplest model that allows us do VLE calculatons s obtaned when we assume that the vapor phase s an deal gas, and

More information

System in Weibull Distribution

System in Weibull Distribution Internatonal Matheatcal Foru 4 9 no. 9 94-95 Relablty Equvalence Factors of a Seres-Parallel Syste n Webull Dstrbuton M. A. El-Dacese Matheatcs Departent Faculty of Scence Tanta Unversty Tanta Egypt eldacese@yahoo.co

More information

November 5, 2002 SE 180: Earthquake Engineering SE 180. Final Project

November 5, 2002 SE 180: Earthquake Engineering SE 180. Final Project SE 8 Fnal Project Story Shear Frame u m Gven: u m L L m L L EI ω ω Solve for m Story Bendng Beam u u m L m L Gven: m L L EI ω ω Solve for m 3 3 Story Shear Frame u 3 m 3 Gven: L 3 m m L L L 3 EI ω ω ω

More information

Problem Set 9 Solutions

Problem Set 9 Solutions Desgn and Analyss of Algorthms May 4, 2015 Massachusetts Insttute of Technology 6.046J/18.410J Profs. Erk Demane, Srn Devadas, and Nancy Lynch Problem Set 9 Solutons Problem Set 9 Solutons Ths problem

More information

DO NOT DO HOMEWORK UNTIL IT IS ASSIGNED. THE ASSIGNMENTS MAY CHANGE UNTIL ANNOUNCED.

DO 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 information

Chapter 3. Estimation of Earthquake Load Effects

Chapter 3. Estimation of Earthquake Load Effects Chapter 3. Estmaton of Earthquake Load Effects 3.1 Introducton Sesmc acton on chmneys forms an addtonal source of natural loads on the chmney. Sesmc acton or the earthquake s a short and strong upheaval

More information

Physics 111: Mechanics Lecture 11

Physics 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 information

Global Sensitivity. Tuesday 20 th February, 2018

Global Sensitivity. Tuesday 20 th February, 2018 Global Senstvty Tuesday 2 th February, 28 ) Local Senstvty Most senstvty analyses [] are based on local estmates of senstvty, typcally by expandng the response n a Taylor seres about some specfc values

More information

Physics 181. Particle Systems

Physics 181. Particle Systems Physcs 181 Partcle Systems Overvew In these notes we dscuss the varables approprate to the descrpton of systems of partcles, ther defntons, ther relatons, and ther conservatons laws. We consder a system

More information

Integrals and Invariants of Euler-Lagrange Equations

Integrals and Invariants of Euler-Lagrange Equations Lecture 16 Integrals and Invarants of Euler-Lagrange Equatons ME 256 at the Indan Insttute of Scence, Bengaluru Varatonal Methods and Structural Optmzaton G. K. Ananthasuresh Professor, Mechancal Engneerng,

More information

Problem Points Score Total 100

Problem Points Score Total 100 Physcs 450 Solutons of Sample Exam I Problem Ponts Score 1 8 15 3 17 4 0 5 0 Total 100 All wor must be shown n order to receve full credt. Wor must be legble and comprehensble wth answers clearly ndcated.

More information

JAB Chain. Long-tail claims development. ASTIN - September 2005 B.Verdier A. Klinger

JAB Chain. Long-tail claims development. ASTIN - September 2005 B.Verdier A. Klinger JAB Chan Long-tal clams development ASTIN - September 2005 B.Verder A. Klnger Outlne Chan Ladder : comments A frst soluton: Munch Chan Ladder JAB Chan Chan Ladder: Comments Black lne: average pad to ncurred

More information

COMPARISON OF SOME RELIABILITY CHARACTERISTICS BETWEEN REDUNDANT SYSTEMS REQUIRING SUPPORTING UNITS FOR THEIR OPERATIONS

COMPARISON OF SOME RELIABILITY CHARACTERISTICS BETWEEN REDUNDANT SYSTEMS REQUIRING SUPPORTING UNITS FOR THEIR OPERATIONS Avalable onlne at http://sck.org J. Math. Comput. Sc. 3 (3), No., 6-3 ISSN: 97-537 COMPARISON OF SOME RELIABILITY CHARACTERISTICS BETWEEN REDUNDANT SYSTEMS REQUIRING SUPPORTING UNITS FOR THEIR OPERATIONS

More information

MODAL ANALYSIS AND TESTING OF ROTATING MACHINES FOR PREDICTIVE MAINTENANCE: EFFECT OF GYROSCOPIC FORCES

MODAL ANALYSIS AND TESTING OF ROTATING MACHINES FOR PREDICTIVE MAINTENANCE: EFFECT OF GYROSCOPIC FORCES MODAL ANALYSIS AND TESTING OF ROTATING MACHINES FOR PREDICTIVE MAINTENANCE: EFFECT OF GYROSCOPIC FORCES A. Vansteenkste; M. Loccufer; B. Vervsch; P. De Baets; Ghent Unversty, Belgum Abstract Through the

More information

8.592J: Solutions for Assignment 7 Spring 2005

8.592J: Solutions for Assignment 7 Spring 2005 8.59J: Solutons for Assgnment 7 Sprng 5 Problem 1 (a) A flament of length l can be created by addton of a monomer to one of length l 1 (at rate a) or removal of a monomer from a flament of length l + 1

More information

Lecture 8 Modal Analysis

Lecture 8 Modal Analysis Lecture 8 Modal Analyss 16.0 Release Introducton to ANSYS Mechancal 1 2015 ANSYS, Inc. February 27, 2015 Chapter Overvew In ths chapter free vbraton as well as pre-stressed vbraton analyses n Mechancal

More information

EVALUATION OF THE VISCO-ELASTIC PROPERTIES IN ASPHALT RUBBER AND CONVENTIONAL MIXES

EVALUATION 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 information

9.2 Seismic Loads Using ASCE Standard 7-93

9.2 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 information

Chapter 8. Potential Energy and Conservation of Energy

Chapter 8. Potential Energy and Conservation of Energy Chapter 8 Potental Energy and Conservaton of Energy In ths chapter we wll ntroduce the followng concepts: Potental Energy Conservatve and non-conservatve forces Mechancal Energy Conservaton of Mechancal

More information

A New Design of Multiplier using Modified Booth Algorithm and Reversible Gate Logic

A New Design of Multiplier using Modified Booth Algorithm and Reversible Gate Logic Internatonal Journal of Computer Applcatons Technology and Research A New Desgn of Multpler usng Modfed Booth Algorthm and Reversble Gate Logc K.Nagarjun Department of ECE Vardhaman College of Engneerng,

More information

SIO 224. m(r) =(ρ(r),k s (r),µ(r))

SIO 224. m(r) =(ρ(r),k s (r),µ(r)) SIO 224 1. A bref look at resoluton analyss Here s some background for the Masters and Gubbns resoluton paper. Global Earth models are usually found teratvely by assumng a startng model and fndng small

More information

Please initial the statement below to show that you have read it

Please 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 information

(Online First)A Lattice Boltzmann Scheme for Diffusion Equation in Spherical Coordinate

(Online First)A Lattice Boltzmann Scheme for Diffusion Equation in Spherical Coordinate Internatonal Journal of Mathematcs and Systems Scence (018) Volume 1 do:10.494/jmss.v1.815 (Onlne Frst)A Lattce Boltzmann Scheme for Dffuson Equaton n Sphercal Coordnate Debabrata Datta 1 *, T K Pal 1

More information

Multiple Sound Source Location in 3D Space with a Synchronized Neural System

Multiple Sound Source Location in 3D Space with a Synchronized Neural System Multple Sound Source Locaton n D Space wth a Synchronzed Neural System Yum Takzawa and Atsush Fukasawa Insttute of Statstcal Mathematcs Research Organzaton of Informaton and Systems 0- Mdor-cho, Tachkawa,

More information

MR Damper in Reducing Pounding Effect of Base- Isolated RC Highway Bridges

MR Damper in Reducing Pounding Effect of Base- Isolated RC Highway Bridges Australan Earthquake Engneerng Socety 21 Conference, Perth, Western Australa MR Damper n Reducng Poundng Effect of Base- Isolated RC Hghway Brdges M. Neaz Shekh 1, Jngya Xong 2, and Wehua L 3 1. Senor

More information

Lecture 13 APPROXIMATION OF SECOMD ORDER DERIVATIVES

Lecture 13 APPROXIMATION OF SECOMD ORDER DERIVATIVES COMPUTATIONAL FLUID DYNAMICS: FDM: Appromaton of Second Order Dervatves Lecture APPROXIMATION OF SECOMD ORDER DERIVATIVES. APPROXIMATION OF SECOND ORDER DERIVATIVES Second order dervatves appear n dffusve

More information

Physics 53. Rotational Motion 3. Sir, I have found you an argument, but I am not obliged to find you an understanding.

Physics 53. Rotational Motion 3. Sir, I have found you an argument, but I am not obliged to find you an understanding. Physcs 53 Rotatonal Moton 3 Sr, I have found you an argument, but I am not oblged to fnd you an understandng. Samuel Johnson Angular momentum Wth respect to rotatonal moton of a body, moment of nerta plays

More information

Short Term Load Forecasting using an Artificial Neural Network

Short Term Load Forecasting using an Artificial Neural Network Short Term Load Forecastng usng an Artfcal Neural Network D. Kown 1, M. Km 1, C. Hong 1,, S. Cho 2 1 Department of Computer Scence, Sangmyung Unversty, Seoul, Korea 2 Department of Energy Grd, Sangmyung

More information

CONTRAST ENHANCEMENT FOR MIMIMUM MEAN BRIGHTNESS ERROR FROM HISTOGRAM PARTITIONING INTRODUCTION

CONTRAST ENHANCEMENT FOR MIMIMUM MEAN BRIGHTNESS ERROR FROM HISTOGRAM PARTITIONING INTRODUCTION CONTRAST ENHANCEMENT FOR MIMIMUM MEAN BRIGHTNESS ERROR FROM HISTOGRAM PARTITIONING N. Phanthuna 1,2, F. Cheevasuvt 2 and S. Chtwong 2 1 Department of Electrcal Engneerng, Faculty of Engneerng Rajamangala

More information

A Hybrid Variational Iteration Method for Blasius Equation

A Hybrid Variational Iteration Method for Blasius Equation Avalable at http://pvamu.edu/aam Appl. Appl. Math. ISSN: 1932-9466 Vol. 10, Issue 1 (June 2015), pp. 223-229 Applcatons and Appled Mathematcs: An Internatonal Journal (AAM) A Hybrd Varatonal Iteraton Method

More information

Compilers. Spring term. Alfonso Ortega: Enrique Alfonseca: Chapter 4: Syntactic analysis

Compilers. Spring term. Alfonso Ortega: Enrique Alfonseca: Chapter 4: Syntactic analysis Complers Sprng term Alfonso Ortega: alfonso.ortega@uam.es nrque Alfonseca: enrque.alfonseca@uam.es Chapter : Syntactc analyss. Introducton. Bottom-up Analyss Syntax Analyser Concepts It analyses the context-ndependent

More information

Physics 5153 Classical Mechanics. Principle of Virtual Work-1

Physics 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 information

MAE140 - Linear Circuits - Winter 16 Final, March 16, 2016

MAE140 - Linear Circuits - Winter 16 Final, March 16, 2016 ME140 - Lnear rcuts - Wnter 16 Fnal, March 16, 2016 Instructons () The exam s open book. You may use your class notes and textbook. You may use a hand calculator wth no communcaton capabltes. () You have

More information

Study Guide For Exam Two

Study Guide For Exam Two Study Gude For Exam Two Physcs 2210 Albretsen Updated: 08/02/2018 All Other Prevous Study Gudes Modules 01-06 Module 07 Work Work done by a constant force F over a dstance s : Work done by varyng force

More information

Grover s Algorithm + Quantum Zeno Effect + Vaidman

Grover s Algorithm + Quantum Zeno Effect + Vaidman Grover s Algorthm + Quantum Zeno Effect + Vadman CS 294-2 Bomb 10/12/04 Fall 2004 Lecture 11 Grover s algorthm Recall that Grover s algorthm for searchng over a space of sze wors as follows: consder the

More information

Experimental Study on Ultimate Strength of Flexural-Failure-Type RC Beams under Impact Loading

Experimental Study on Ultimate Strength of Flexural-Failure-Type RC Beams under Impact Loading xpermental Study on Ultmate Strength of Flexural-Falure-Type RC Beams under Impact Loadng N. Ksh 1), O. Nakano 2~, K. G. Matsuoka 1), and T. Ando 1~ 1) Dept. of Cvl ngneerng, Muroran Insttute of Technology,

More information

Power law and dimension of the maximum value for belief distribution with the max Deng entropy

Power law and dimension of the maximum value for belief distribution with the max Deng entropy Power law and dmenson of the maxmum value for belef dstrbuton wth the max Deng entropy Bngy Kang a, a College of Informaton Engneerng, Northwest A&F Unversty, Yanglng, Shaanx, 712100, Chna. Abstract Deng

More information

Adiabatic Sorption of Ammonia-Water System and Depicting in p-t-x Diagram

Adiabatic Sorption of Ammonia-Water System and Depicting in p-t-x Diagram Adabatc Sorpton of Ammona-Water System and Depctng n p-t-x Dagram J. POSPISIL, Z. SKALA Faculty of Mechancal Engneerng Brno Unversty of Technology Techncka 2, Brno 61669 CZECH REPUBLIC Abstract: - Absorpton

More information

CHAPTER 14 GENERAL PERTURBATION THEORY

CHAPTER 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 information

Lecture 12: Discrete Laplacian

Lecture 12: Discrete Laplacian Lecture 12: Dscrete Laplacan Scrbe: Tanye Lu Our goal s to come up wth a dscrete verson of Laplacan operator for trangulated surfaces, so that we can use t n practce to solve related problems We are mostly

More information

Modal Strain Energy Decomposition Method for Damage Detection of an Offshore Structure Using Modal Testing Information

Modal Strain Energy Decomposition Method for Damage Detection of an Offshore Structure Using Modal Testing Information Thrd Chnese-German Jont Symposum on Coastal and Ocean Engneerng Natonal Cheng Kung Unversty, Tanan November 8-16, 2006 Modal Stran Energy Decomposton Method for Damage Detecton of an Offshore Structure

More information

EEE 241: Linear Systems

EEE 241: Linear Systems EEE : Lnear Systems Summary #: Backpropagaton BACKPROPAGATION The perceptron rule as well as the Wdrow Hoff learnng were desgned to tran sngle layer networks. They suffer from the same dsadvantage: they

More information

ORIGIN 1. PTC_CE_BSD_3.2_us_mp.mcdx. Mathcad Enabled Content 2011 Knovel Corp.

ORIGIN 1. PTC_CE_BSD_3.2_us_mp.mcdx. Mathcad Enabled Content 2011 Knovel Corp. Clck to Vew Mathcad Document 2011 Knovel Corp. Buldng Structural Desgn. homas P. Magner, P.E. 2011 Parametrc echnology Corp. Chapter 3: Renforced Concrete Slabs and Beams 3.2 Renforced Concrete Beams -

More information

AGC Introduction

AGC Introduction . Introducton AGC 3 The prmary controller response to a load/generaton mbalance results n generaton adjustment so as to mantan load/generaton balance. However, due to droop, t also results n a non-zero

More information

Electrical double layer: revisit based on boundary conditions

Electrical double layer: revisit based on boundary conditions Electrcal double layer: revst based on boundary condtons Jong U. Km Department of Electrcal and Computer Engneerng, Texas A&M Unversty College Staton, TX 77843-318, USA Abstract The electrcal double layer

More information