'HVLJQRID1RYHO&RPSOLDQW'LIIHUHQWLDO6KDSH0HPRU\$OOR\ $FWXDWRU
|
|
- Felicity Jessica Sims
- 5 years ago
- Views:
Transcription
1 2013 IEEE/RSJ Internatinal Cnference n Intelligent Rbts and Systems (IROS) Nvember 3-7, Tky, Japan 'HVLJQRID1RYHO&RPSOLDQW'LIIHUHQWLDO6KDSH0HPRU\$OOR\ $FWXDWRU Zha Gu, Hayng Yu, Member, IEEE, and Liang-Bn Wee, Senir Member, IEEE bstract²this paper presents a nvel cmpliant differential (CD) Shape Memry lly (SM) actuatr with imprved perfrmance cmpared t traditinal SM actuatrs. This actuatr is cmpsed f tw antagnistic SM wires and a mechanical jint cupled with a trsin spring. The trsin spring is emplyed t reduce the ttal stiffness f SM actuatr and imprve the range f mtin. The antagnistic wires increase the respnse time as ne wire can be heated up while the ther wire is still in the cling prcess. Dynamic mdel f this actuatr was established fr cntrl design. Experimental results prved that this new actuatr can prvide larger utput range f mtin and faster respnse speed than traditinal SM actuatrs under the same cnditins. Sine wave tracking with 0.05 Hz, 0.08 Hz and 0.1 Hz were perfrmed and ur results demnstrated that this cmpliant actuatr has gd tracking perfrmance under simple PID cntrl. I. INTRODUCTION Shape Memry lly (SM) is an intelligent material that can remember its riginal shape at lw temperature and return t the pre-defrmed shape by heating abve a threshld temperature. This phenmenn knwn as the Shape Memry Effect (SME) is the result f a phase transfrmatin between martensite and austenite. SM wire, especially the Nitinl (Ni-Ti) wire, which has a strain rate f up t 8%, is the mst cmmnly used SM frms fr actuatr design. Cmpared t cnventinal (electric, hydraulic, and pneumatic) actuatrs r ther advanced (piezelectric and EP) actuatrs, SM actuatrs have the advantages f high pwer t weight rati, bi-cmpatibility, small size, and silence peratin, and these advantages make them suitable fr a wide range f applicatins [1], such as rbtic surgical systems [2] [3], sft rbtics [4], and airfil prfile cntrl [5]. Hwever, SM actuatrs als have the disadvantages f lw energy efficiency, slw respnse rate, nnlinearity, hysteresis and lw strain rate. Special mechanical design and nnlinear cntrl methds are needed t vercme these limitatins. SM wire can nly achieve unidirectinal actuatin, thus it is necessary t prvide a recvery frce via a weight, a spring r anther antagnistic SM wire t achieve bidirectinal mvement. Typically, there are tw classes f SM actuatrs [6]. One is the bias spring (BS) SM actuatr *Research Supprted by MINDEF/NUS/JPP Zha Gu is with Singapre Institute fr Neurtechnlgy (SINPSE), Department f Biengineering, Natinal University f Singapre, 9 Engineering Drive 1, Singapre , ( biegz@nus.edu.sg ). Hayng Yu is with Singapre Institute fr Neurtechnlgy (SINPSE), Department f Biengineering, Natinal University f Singapre, 9 Engineering Drive 1, Singapre , (crrespnding authr, phne: ; fax: ; bieyhy@nus.edu.sg). Liang-Bn Wee is with DSO Natinal Labratries, 20 Science Park Drive, Singapre , ( wliangb@ds.rg.sg). cmpsed f a SM element and a bias spring. This type f actuatr has slw respnse as the respnse speed is limited by the cling prcess. The ther type f actuatr design cnsists f tw antagnistic SM elements, called differential (DI) SM actuatr [7]. This type actuatr has faster speed f respnse than the BS SM actuatr, but it cnsumes mre pwer and the range f mtin is restricted by the antagnistic SM [8]. SM actuatrs with larger wrking range and quicker respnse are desirable in many fields [9][10][11]. T achieve these gals, a series f new SM-based actuatrs r mechanisms have been develped. Fr instance, Zhang and Yin [12] presented a SM-based artificial muscle cmpsed f 16 parallel SM wires and a simple linear spring t imprve the driving frce and mimic the character f human muscle. Grant and Hayward [13] develped a differential SM actuatr cmprised f 12 SM wires in a helical arrangement t prduce larger mvements. Park, et,al [14] prpsed a differential spring-biased SM actuatr fr a bi-mimetic artificial finger. In this design, the spring was directly cnnected t the SM wire, which may absrb the cntractin length f SM wires and reduce the range f mtin f the jint. In the fields f assistive and rehabilitatin rbtics, cmpliant actuatrs have attracted cnsiderable attentin due t their ability f absrbing shcks, interacting with peple safely, string and releasing energy [15]. Many types f cmpliant actuatrs, such as Series Elastic ctuatr [16], Pneumatic rtificial Muscle [17] have been develped. Hwever, the utilizatin f advanced materials such as SM in cmpliant actuatr has nt been well investigated. The mtivatin f this paper is t develp a new cmpliant differential (CD) SM actuatr with a simple structure. trsin spring is emplyed t achieve better perfrmance ver traditinal DI SM and BS SM actuatrs. System mdels include the dynamics and cnstitutin equatins are established fr cntrl design. testing setup was designed t cmpare the prperties f this actuatr t the tw traditinal SM actuatrs. Furthermre, the psitin cntrl f this actuatr in step respnse and sinusidal tracking was investigated. II. COMPLINT DIFFERENTIL SM CTUTOR DESIGN. Cmpliant differential SM actuatr Inspired by the bilgical structure f human jint actuated by antagnistic skeletal muscles, we prpse a new cmpliant differential SM actuatr t mimic the extensin/flexin mtin f the bilgical jint. s shwn in Fig. 1(a), this cmpliant actuatr is cmpsed f tw antagnistic SM wires, a trsin spring and tw cylindrical cuplers. lad is applied n the cupler #1 by threaded cnnectin. Tw /13/$ IEEE 4925
2 antagnistic SM wires, behaving like artificial muscles, prvide the active frce fr bi-directinal mtin cntrl f the cuplers. The trsin spring, used t mimic the tendn, is packaged inside the cuplers. Tw legs f the trsin spring (0 deflectin, left hand wind) are restricted by the slts in the cuplers. The SM wires are directly cnnected t the cupler. The active cntractin frce prduced by the SM wire can be transmitted frm ne cupler t the ther by the trsin spring. The whle structure is simple and easy t implement fr different applicatins. In this design, we chse a trsin spring. Its stiffness is lwer than that f the SM wire. The spring will prvide the recvery frce fr the agnist SM wire and reduce the ttal stiffness f the actuatr. n encder can be assembled n the axis t get the rtatinal angle. respectively. Due t ks k, the rder f the passive stiffness 2 fllws kcd kbs k. DI Fig.1. CD mdel and prttype f the cmpliant differential SM actuatr B. Three types f SM actuatrs T cmpare the perfrmance f this actuatr with the tw traditinal SM actuatrs, we implement three cnfiguratins t represent three types f SM actuatrs using the same mechanical setup. They are (a) BS SM actuatr, (b) DI SM actuatr, (c) CD SM actuatr. Figure 2 includes the CD mdel and its equivalent mechanical mdel f each actuatr. Tw SM wires generate the tensile frce with a variable stiffness k i and a damping rati b (i=1, i 2). The trsin spring between tw SM wires transmits the cntractin frce with a cnstant stiffness k s.the damping between the spring and the mechanical part is b s. m, m 1 2 represents the mass f tw parts f the spring cupler respectively. The lad applied n the cupler #1 is represented as a mass m. Because f the small rtatinal lad speed, the effect f system damping is neglected. We mainly cnsider the stiffness f these actuatrs. The passive stiffness f each actuatr is k k, k ( k k ) / ( k k ) BS S DI 2 k k, 2 2 CD s s Fig.2. CD mdels and equivalent mechanical mdels fr three SM actuatrs: (a) BS SM actuatr; (b) DI SM actuatr; (c) CD SM actuatr. III. MODELING THE COMPLINT DIFFERENTIL SM CTUTOR The mdel f the actuatin system includes the dynamics and kinematics f the actuatr as well as the cnstitutive equatins, transfrmatin equatins and the heat transfer dynamics f the SM wire.. Dynamics and Kinematics simplified mdel f the actuatr is shwn in Fig.3. The cuplers are actuated independently under the functin f SM wires, the rtatinal angle f each cupler is defined as T, 1 2 T, which is relative t the y axis. Fig.3. Schematic diagram f the CD SM actuatr, F 1,F 2 are the active frces f the upper and lwer SM wires respectively, F s is the trsin spring frce, r 1, r 2 represent the mment arm, r s is the radius f trsin spring. The dynamic equatin f each cupler is given by 4926
3 4927
4 fast cntrl n the jint mtin. The rule fr each wire is shwn in Equatin (10) (11). V V 0 heating Upper SM wire: ut ' T t (10) V 0 ' T 0 cling V V 0 heating Lwer SM wire: ut ' T d (11) V 0 ' T! 0 cling IV. EXPERIMENTL SETUP ND RESULTS. Experimental setup n experimental setup has been develped t evaluate the perfrmance f this CD SM actuatr. small irn stick is cnnected t the actuatr as the lad fr testing. Figure 6 shws the schematic diagram f the cntrl hardware and picture f the experimental setup, respectively. Tw antagnistic NiTi SM wires (Dynally, Inc.) are selected in ur actuatr design. Their prperties are summarized in Table I. The diameter f each SM wire d is 250m. ngular psitin is measured by a shaft encder (Omrn E6B2-CWZ1X) with a reslutin f 2500 pulses per turn. NI-PCI-6221 DQ card is used t cllect the data and prvide the analg vltage utputs with a full-scale range f ±10 V t an amplifier. Tw channel analg vltages were augmented by the amplifier with a gain f 3.125V/V and applied n tw SM wires separately. The test was implemented n a Lab VIEW platfrm (Natinal Instruments, Inc.) n a PC. TBLE I. PRMETERS OF THE CD SM CTUTOR Parameter Value Parameter Value E M 28GPa d 250m E 75GPa w U g/cm s f M s 88 C C u 10 m T amb 20 C 10MPa/ K 98 C C m 10MPa/ K 72 C C p M f 62 C w R 20/m r1, r 2 l1, l m V 0 k s N m/ J/kg C 4 m k, k m1, m2 10g r 2 6.8u 10 kg/m 10mm 25MPa 3714~10348N/m 7.5mm B. Perfrmance cmparisn fr three SM actuatrs We cmpare this new SM actuatr with the ther tw SM actuatrs in tw aspects: range f mtin and respnse speed. We apply the same utput vltage (1V) n the upper SM wire f these actuatrs. The current acrss the SM wire is 0.42, and the lwer SM wire wrks as a variable stiffness spring. ccrding t the <RXQJ VPRGXOXV f SM wire in tw transfrmatin phases, the range f its stiffness is linearly changed frm 3714N m t 10384N m.the stiffness f trsin spring is selected as N m/1 ; its equivalent stiffness t extensin spring is 1031N m. The stiffness f trsin spring is lwer than that f the SM wire. Experimental results fr three actuatrs, including the heating and cling phases f the upper SM wire, are shwn in Fig. 7. The results indicate that the CD SM actuatr prvides largest angular range f mtin. The maximum angular mtin f the CD SM actuatr is clse t 30, while BS SM actuatr is limited t 20 and DI SM actuatr prvides nly 13. This limitatin in angular mtin is due mainly t the high stiffness f the antagnist SM wire. 40 BS DI CD 30 Fig.6. (a) Blck diagram cnfiguratin f the psitin cntrl system and (b) experimental setup fr testing. ngle (deg.) Same starting pint f cling Time (s) Fig.7. Experimental angular psitin f three SM actuatrs under the same applied current. The dynamic respnse f the three actuatrs shw a slight psitin versht befre reaching steady-state, see Fig.7. This behavir is explained with the aid f the heat dynamics, equatin (8). During the heating phase, the SM wire 4928
5 underges a phase change that persists till an energy balance between the pwer input and the pwer lss is reached. This energy transfer als crrespnds t the temperature respnse f SM wire. During the cling phase, we bserved that the rate at which the CD SM actuatr returned t the relaxed state is faster than the ther actuatrs. This faster rate f the CD SM actuatr is prvided by stred energy in the trsin spring. The abve results clearly indicate that the CD SM actuatr prvide large wrking range under the same current stimulating cnditin, as well as mre efficient energy utilizatin cmpared t the ther tw actuatrs. C. Step respnse The experimental respnses t a series f step inputs were examined n this new SM actuatr. single channel and tw-channel cntrls were applied fr a cling speed perfrmance cmparisn. In ne channel cntrl, the upper SM wire was actively heated and the antagnistic SM wire was passive. In tw-channel cntrl, when the real psitin was larger than the reference, the antagnistic SM wire wuld be activated t reduce the versht and increase the cling prcess. phase, the average fall time frm 20 t the 10 and frm 10 t 0 is apprximately 6 secnds. The jint angle reduced slwly t the set pint under the recvery frce frm the trsin spring. T reduce the fall time, a secnd PI cntrller was prvided t the lwer SM wire. Figure 8(b) shws the step respnses t the desired steps f 10 and 20. Cmpared t the ne channel cntrl, the rise time reduces t abut 1s. Despite an versht in the heating phase, the psitin angle tends t stable sn due t the integral gain. Meanwhile during the cling phase f upper SM wire, the secnd SM wire wuld be heated t increase the cling speed. The fall time f step input frm 20 t 10, 10 t 0 reduces t abut 2.5 s. These figures clearly shw that the rise and fall times f step respnses have decreased significantly. The respnse speeds bth in the heating and cling phase are increased. This clearly demnstrates that ur prpsed actuatr design and cntrl methd have achieved better perfrmance than the cnventinal SM actuatr. D. Tracking respnse This part presents the tracking respnses f the CD actuatr t a series f sinusidal inputs with frequencies f 0.05 Hz, 0.08Hz and 0.1 Hz using the prpsed cntrl methd. It can be seen that the tracking perfrmance fr 0.05 Hz is better than 0.08Hz and 0.1Hz in Fig. 9 (a) (b) (c).the tracking errr fr 0.05Hz, 0.08Hz and 0.1 Hz is abut-1 ~1, -1 ~1.5, -2.5 ~1.5 respectively. s the frequency f the sine wave increases, the errr increases gradually, the system begins t lag behind the desired respnse due t the slw respnse speed f the actuatr. (a) (b) Fig.8. (a) One channel cntrl fr the CD SM actuatr and (b) tw channels cntrl fr the CD SM actuatr Figure 8(a) shws respnses t desired steps f 10 and 20 in ne channel cntrl. In terms f time-dmain specificatin, during the heating phase, the average rise time t the 10 step input is apprximately 3.5 s. Fr the respnse t a 20, it is slightly lng and requires apprximately 5 secnds. This is expected, as the set pint is further away frm the zer psitin, s it takes a lnger time fr the actuatr t reach the desired set pint. During the cling (a) 0.05 Hz 4929
6 this new actuatr and the tw cnventinal SM actuatrs have been cnducted fr perfrmance cmparisn. Psitin cntrl experiments fr step respnse and sine wave tracking demnstrated that this nvel cmpliant actuatr has faster respnse speed, larger utput range. The respnse speed f SM actuatr can be further increased t faster and mre rbust jint mtin with better cntrl methds. We are currently develping advanced cntrller t imprve the perfrmance f this actuatr and develping applicatins fr rehabilitatin rbtic and surgical rbtic systems. (b) 0.08 Hz (c) 0.1Hz Fig.9. Sine tracking respnse with (a) 0.05 Hz, (b) 0.08 Hz and (c) 0.1Hz. V. CONCLUSION nvel CD SM actuatr using tw antagnistic SM wires and a trsin spring has been prpsed t imprve the perfrmance f traditinal SM actuatrs. Experiments fr REFERENCES [1]. Nespli, S. Besseghini, S. Pittacci, E. Villa, and S. Viscus, ³The high ptential f shape memry allys in develping miniature mechanical devices: review n shape memry ally mini-actuatrs, Sensrs and ctuatrs, vl. 158, pp , Mar [2] P. Sears and P. Dupnt, ³ steerable needle technlgy using curved cncentric tubes, in IEEE/RSJ Int. Cnf. Intell. Rbts Syst., Beijing, China, frm Oct. 9-15, 2006, pp [3] R. Webster,. M. Okamura, and N. J. Cwan, ³Tward active cannulas: Miniature snake-like surgical rbts, in IEEE/RSJ Int. Cnf. Intell. Rbts Syst., Beijing, China, frm Oct. 9-15, 2006, pp [4] S. Kim, E. Hawkes, K. Chy, M. Jldaz, J. Fleyz, and R. Wd, ³Micr artificial muscle fiber using NiTi spring fr sft rbtics, in IEEE/RSJ Int. Cnf. Intell. Rbts Syst., St. Luis, US, frm Oct , 2009, pp [5] F. Peng, X.-X. Jiang, Y.-R. Hu, and. Ng, ³pplicatin f shape memry ally actuatrs in active shape cntrl f inflatable space structures, in Prc. IEEE Cnf. ersp., 2005, pp [6] C. Liang and C. Rgers, ³Design f shape memry ally actuatrs, J. Intell. Mater. Syst. Struct., vl. 8, pp , [7] R. B. Grbet and R.. Russell, ³ nvel differential shape memry ally actuatr fr psitin cntrl, Rbtica, vl. 13, pp , [8] M. Mallem and V. Tabrizi, ³Tracking cntrl f an antagnistic shape memry ally actuatr pair, IEEE Trans. Cntrl Syst. Technl., vl. 17, pp , [9] H. shrafiun, M. Eshraghi, and M. H. Elahinia, ³Psitin cntrl f a three-link shape memry ally actuated rbt, J. Intell. Mater. Syst. Struct., vl. 17, pp , [10] S. Z. Yan, X. J. Liu, F. Xu, and J. H. Wang, ³ gripper actuated by a pair f differential SM springs, J. Intell. Mater. Syst. Struct., vl. 18, pp , May [11] E. T. Esfahani and M. H. Elahinia, ³Stable walking pattern fr an SM-actuated biped, IEEE-SME Trans. Mechatrn., vl. 12, pp , Oct [12] J. J. Zhang and Y. H. Yin, ³SM-based binic integratin design f self-sensr-actuatr-structure fr artificial skeletal muscle, Sensrs and ctuatrs, vl. 181, pp , Jul [13] D. Grant and V. Hayward, ³Variable structure cntrl f shape memry ally actuatrs, IEEE Cntrl Syst. Mag. vl. 17, pp , Jun [14] V. Bundh, E. Haslam, B. Birch, and E. J. Park, ³ shape memry ally-based tendn-driven actuatin system fr bimimetic artificial fingers, part I: design and evaluatin, Rbtica, vl. 27, pp , [15] R. Van Ham, T. G. Sugar, B. Vanderbrght, K. W. Hllander, and D. Lefeber, ³Cmpliant ctuatr Designs, IEEE Rbt. utm. Mag., vl. 16, pp , Sep [16] G.. Pratt and M. M. Williamsn, ³Series elastic actuatrs, in IEEE/RSJ Int. Cnf. Intell. Rbts Syst., Pittsburgh, US, frm ug. 5-9, 1995, pp [17] C. P. Chu and B. Hannafrd, ³Measurement and mdeling f McKibben pneumatic artificial muscles, IEEE Rbt. utm. Mag., vl. 12, pp , Feb [18] C. Liang and C. Rgers, ³One-dimensinal thermmechanical cnstitutive relatins fr shape memry materials, J. Intell. Mater. Syst. Struct., vl. 1, pp , [19]. R. Shahin, P. H. Meckl, J. D. Jnes, and M.. Thrasher, ³Enhanced Cling f Shape-Memry lly Wires Using Semicnductr Heat-Pump Mdules, J. Intell. Mater. Syst. Struct., vl. 5, pp , Jan
3D FE Modeling Simulation of Cold Rotary Forging with Double Symmetry Rolls X. H. Han 1, a, L. Hua 1, b, Y. M. Zhao 1, c
Materials Science Frum Online: 2009-08-31 ISSN: 1662-9752, Vls. 628-629, pp 623-628 di:10.4028/www.scientific.net/msf.628-629.623 2009 Trans Tech Publicatins, Switzerland 3D FE Mdeling Simulatin f Cld
More informationA Study on Pullout Strength of Cast-in-place Anchor bolt in Concrete under High Temperature
Transactins f the 7 th Internatinal Cnference n Structural Mechanics in Reactr Technlgy (SMiRT 7) Prague, Czech Republic, August 7 22, 23 Paper #H-2 A Study n Pullut Strength f Cast-in-place Anchr blt
More informationLevel Control in Horizontal Tank by Fuzzy-PID Cascade Controller
Wrld Academy f Science, Engineering and Technlgy 5 007 Level Cntrl in Hrizntal Tank by Fuzzy-PID Cascade Cntrller Satean Tunyasrirut, and Santi Wangnipparnt Abstract The paper describes the Fuzzy PID cascade
More informationTransduction Based on Changes in the Energy Stored in an Electrical Field
Lecture 6-3 Transductin Based n Changes in the Energy Stred in an Electrical ield Department f Mechanical Engineering Example:Capacitive Pressure Sensr Pressure sensitive capacitive device With separatin
More informationSynchronous Motor V-Curves
Synchrnus Mtr V-Curves 1 Synchrnus Mtr V-Curves Intrductin Synchrnus mtrs are used in applicatins such as textile mills where cnstant speed peratin is critical. Mst small synchrnus mtrs cntain squirrel
More informationUnit code: H/ QCF level: 5 Credit value: 15 OUTCOME 3 - STATIC AND DYNAMIC FLUID SYSTEMS TUTORIAL 3 - VISCOSITY
Unit 43: Plant and Prcess Principles Unit cde: H/601 44 QCF level: 5 Credit value: 15 OUTCOME 3 - STATIC AND DYNAMIC FLUID SYSTEMS TUTORIAL 3 - VISCOSITY 3 Understand static and namic fluid systems with
More informationENGINEERING COUNCIL CERTIFICATE LEVEL THERMODYNAMIC, FLUID AND PROCESS ENGINEERING C106 TUTORIAL 5 THE VISCOUS NATURE OF FLUIDS
ENGINEERING COUNCIL CERTIFICATE LEVEL THERMODYNAMIC, FLUID AND PROCESS ENGINEERING C106 TUTORIAL 5 THE VISCOUS NATURE OF FLUIDS On cmpletin f this tutrial yu shuld be able t d the fllwing. Define viscsity
More informationTHERMAL-VACUUM VERSUS THERMAL- ATMOSPHERIC TESTS OF ELECTRONIC ASSEMBLIES
PREFERRED RELIABILITY PAGE 1 OF 5 PRACTICES PRACTICE NO. PT-TE-1409 THERMAL-VACUUM VERSUS THERMAL- ATMOSPHERIC Practice: Perfrm all thermal envirnmental tests n electrnic spaceflight hardware in a flight-like
More informationFeasibility Testing Report Muscle Optimization Stage I
Feasibility Testing Reprt Muscle Optimizatin Stage I Team: P15001: Active Ankle Ft Orthtic Engineer: Nah Schadt Mechanical Engineer Engineer: Tyler Leichtenberger Mechanical Engineer Test Date: 10/14/2014
More informationInterference is when two (or more) sets of waves meet and combine to produce a new pattern.
Interference Interference is when tw (r mre) sets f waves meet and cmbine t prduce a new pattern. This pattern can vary depending n the riginal wave directin, wavelength, amplitude, etc. The tw mst extreme
More informationKinematic transformation of mechanical behavior Neville Hogan
inematic transfrmatin f mechanical behavir Neville Hgan Generalized crdinates are fundamental If we assume that a linkage may accurately be described as a cllectin f linked rigid bdies, their generalized
More informationLinearization of the Output of a Wheatstone Bridge for Single Active Sensor. Madhu Mohan N., Geetha T., Sankaran P. and Jagadeesh Kumar V.
Linearizatin f the Output f a Wheatstne Bridge fr Single Active Sensr Madhu Mhan N., Geetha T., Sankaran P. and Jagadeesh Kumar V. Dept. f Electrical Engineering, Indian Institute f Technlgy Madras, Chennai
More informationA mathematical model for complete stress-strain curve prediction of permeable concrete
A mathematical mdel fr cmplete stress-strain curve predictin f permeable cncrete M. K. Hussin Y. Zhuge F. Bullen W. P. Lkuge Faculty f Engineering and Surveying, University f Suthern Queensland, Twmba,
More informationBootstrap Method > # Purpose: understand how bootstrap method works > obs=c(11.96, 5.03, 67.40, 16.07, 31.50, 7.73, 11.10, 22.38) > n=length(obs) >
Btstrap Methd > # Purpse: understand hw btstrap methd wrks > bs=c(11.96, 5.03, 67.40, 16.07, 31.50, 7.73, 11.10, 22.38) > n=length(bs) > mean(bs) [1] 21.64625 > # estimate f lambda > lambda = 1/mean(bs);
More informationL a) Calculate the maximum allowable midspan deflection (w o ) critical under which the beam will slide off its support.
ecture 6 Mderately arge Deflectin Thery f Beams Prblem 6-1: Part A: The department f Highways and Public Wrks f the state f Califrnia is in the prcess f imprving the design f bridge verpasses t meet earthquake
More informationAircraft Performance - Drag
Aircraft Perfrmance - Drag Classificatin f Drag Ntes: Drag Frce and Drag Cefficient Drag is the enemy f flight and its cst. One f the primary functins f aerdynamicists and aircraft designers is t reduce
More informationDesign and Simulation of Dc-Dc Voltage Converters Using Matlab/Simulink
American Jurnal f Engineering Research (AJER) 016 American Jurnal f Engineering Research (AJER) e-issn: 30-0847 p-issn : 30-0936 Vlume-5, Issue-, pp-9-36 www.ajer.rg Research Paper Open Access Design and
More informationAnalysis on the Stability of Reservoir Soil Slope Based on Fuzzy Artificial Neural Network
Research Jurnal f Applied Sciences, Engineering and Technlgy 5(2): 465-469, 2013 ISSN: 2040-7459; E-ISSN: 2040-7467 Maxwell Scientific Organizatin, 2013 Submitted: May 08, 2012 Accepted: May 29, 2012 Published:
More informationDerailment Safety Evaluation by Analytic Equations
PAPER Derailment Safety Evaluatin by Analytic Equatins Hideyuki TAKAI General Manager, Track Technlgy Div. Hirnari MURAMATSU Assistant Senir Researcher, Track Gemetry & Maintenance, Track Technlgy Div.
More informationElectric Current and Resistance
Electric Current and Resistance Electric Current Electric current is the rate f flw f charge thrugh sme regin f space The SI unit f current is the ampere (A) 1 A = 1 C / s The symbl fr electric current
More informationModeling the Nonlinear Rheological Behavior of Materials with a Hyper-Exponential Type Function
www.ccsenet.rg/mer Mechanical Engineering Research Vl. 1, N. 1; December 011 Mdeling the Nnlinear Rhelgical Behavir f Materials with a Hyper-Expnential Type Functin Marc Delphin Mnsia Département de Physique,
More information^YawataR&D Laboratory, Nippon Steel Corporation, Tobata, Kitakyushu, Japan
Detectin f fatigue crack initiatin frm a ntch under a randm lad C. Makabe," S. Nishida^C. Urashima,' H. Kaneshir* "Department f Mechanical Systems Engineering, University f the Ryukyus, Nishihara, kinawa,
More informationTOPPER SAMPLE PAPER 2 Class XII- Physics
TOPPER SAMPLE PAPER 2 Class XII- Physics Time: Three Hurs Maximum Marks: 70 General Instructins (a) All questins are cmpulsry. (b) There are 30 questins in ttal. Questins 1 t 8 carry ne mark each, questins
More informationA Novel Isolated Buck-Boost Converter
vel slated uck-st Cnverter S-Sek Kim *,WOO-J JG,JOOG-HO SOG, Ok-K Kang, and Hee-Jn Kim ept. f Electrical Eng., Seul atinal University f Technlgy, Krea Schl f Electrical and Cmputer Eng., Hanyang University,
More informationVerification of Quality Parameters of a Solar Panel and Modification in Formulae of its Series Resistance
Verificatin f Quality Parameters f a Slar Panel and Mdificatin in Frmulae f its Series Resistance Sanika Gawhane Pune-411037-India Onkar Hule Pune-411037- India Chinmy Kulkarni Pune-411037-India Ojas Pandav
More informationAssume that the water in the nozzle is accelerated at a rate such that the frictional effect can be neglected.
1 HW #3: Cnservatin f Linear Mmentum, Cnservatin f Energy, Cnservatin f Angular Mmentum and Turbmachines, Bernulli s Equatin, Dimensinal Analysis, and Pipe Flws Prblem 1. Cnservatins f Mass and Linear
More informationReview of the Roll-Damping, Measurements in the T-38 Wind Tunnel
Internatinal Jurnal f Scientific and Research Publicatins, Vlume 3, Issue 12, December 2013 1 Review f the Rll-Damping, Measurements in the T-38 Wind Tunnel Dušan Regdić *, Marija Samardžić **, Gjk Grubr
More informationKinetics of Particles. Chapter 3
Kinetics f Particles Chapter 3 1 Kinetics f Particles It is the study f the relatins existing between the frces acting n bdy, the mass f the bdy, and the mtin f the bdy. It is the study f the relatin between
More informationDavid HORN and Irit OPHER. School of Physics and Astronomy. Raymond and Beverly Sackler Faculty of Exact Sciences
Cmplex Dynamics f Neurnal Threshlds David HORN and Irit OPHER Schl f Physics and Astrnmy Raymnd and Beverly Sackler Faculty f Exact Sciences Tel Aviv University, Tel Aviv 69978, Israel hrn@neurn.tau.ac.il
More informationA Novel Electro-thermal Simulation Approach to Power IGBT Modules for Automotive Traction Applications
Special Issue Recent R&D Activities f Pwer Devices fr Hybrid Electric Vehicles 27 Research Reprt A Nvel Electr-thermal Simulatin Apprach t Pwer IGBT Mdules fr Autmtive Tractin Applicatins Takashi Kjima,
More informationLower Limb Stiffness Estimation during Running: The Effect of Using Kinematic Constraints in Muscle Force Optimization Algorithms
Lwer Limb Stiffness Estimatin during Running: The Effect f Using Kinematic Cnstraints in Muscle Frce Optimizatin Algrithms Rbert Brtlett 1, Enric Pagell 1, and Davide Pivesan 2 1 Intelligent Autnmus Systems
More informationIDENTIFICATION OF PIEZOELECTRIC ULTRASONIC TRANSDUCERS FOR MACHINING PROCESSES
Prceedings f the 9 th Internatinal Sympsium n Mechatrnics and its Applicatins (ISMA3), Amman, Jrdan, April 9-, 3 IDENTIFICATION OF PIEZOELECTRIC ULTRASONIC TRANSDUCERS FOR MACHINING PROCESSES Tarek Tutunji,
More informationThree charges, all with a charge of 10 C are situated as shown (each grid line is separated by 1 meter).
Three charges, all with a charge f 0 are situated as shwn (each grid line is separated by meter). ) What is the net wrk needed t assemble this charge distributin? a) +0.5 J b) +0.8 J c) 0 J d) -0.8 J e)
More informationModule 4: General Formulation of Electric Circuit Theory
Mdule 4: General Frmulatin f Electric Circuit Thery 4. General Frmulatin f Electric Circuit Thery All electrmagnetic phenmena are described at a fundamental level by Maxwell's equatins and the assciated
More informationIncreasing Heat Transfer in Microchannels with Surface Acoustic Waves*
Increasing Heat Transfer in Micrchannels with Surface Acustic Waves* Shaun Berry 0/9/04 *This wrk was spnsred by the Department f the Air Frce under Air Frce Cntract #FA87-05-C-000. Opinins, interpretatins,
More informationLecture 02 CSE 40547/60547 Computing at the Nanoscale
PN Junctin Ntes: Lecture 02 CSE 40547/60547 Cmputing at the Nanscale Letʼs start with a (very) shrt review f semi-cnducting materials: - N-type material: Obtained by adding impurity with 5 valence elements
More informationANALYTICAL MODEL FOR PREDICTING STRESS-STRAIN BEHAVIOUR OF BACTERIAL CONCRETE
Internatinal Jurnal f Civil Engineering and Technlgy (IJCIET) Vlume 9, Issue 11, Nvember 018, pp. 383 393, Article ID: IJCIET_09_11_38 Available nline at http://www.iaeme.cm/ijciet/issues.asp?jtype=ijciet&vtype=9&itype=11
More informationModelling of NOLM Demultiplexers Employing Optical Soliton Control Pulse
Micwave and Optical Technlgy Letters, Vl. 1, N. 3, 1999. pp. 05-08 Mdelling f NOLM Demultiplexers Emplying Optical Slitn Cntrl Pulse Z. Ghassemly, C. Y. Cheung & A. K. Ray Electrnics Research Grup, Schl
More informationTransactions on Engineering Sciences vol 19, 1998 WIT Press, ISSN
Transactins n Engineering Sciences vl 19, 1998 WIT Press, www.witpress.cm, ISSN 1743-3533 Fatigue life and cyclic elastic-plastic strain behaviur ahead f ntch f ntched specimen under cyclic plane bending
More informationthe results to larger systems due to prop'erties of the projection algorithm. First, the number of hidden nodes must
M.E. Aggune, M.J. Dambrg, M.A. El-Sharkawi, R.J. Marks II and L.E. Atlas, "Dynamic and static security assessment f pwer systems using artificial neural netwrks", Prceedings f the NSF Wrkshp n Applicatins
More informationOTHER USES OF THE ICRH COUPL ING CO IL. November 1975
OTHER USES OF THE ICRH COUPL ING CO IL J. C. Sprtt Nvember 1975 -I,," PLP 663 Plasma Studies University f Wiscnsin These PLP Reprts are infrmal and preliminary and as such may cntain errrs nt yet eliminated.
More informationSections 15.1 to 15.12, 16.1 and 16.2 of the textbook (Robbins-Miller) cover the materials required for this topic.
Tpic : AC Fundamentals, Sinusidal Wavefrm, and Phasrs Sectins 5. t 5., 6. and 6. f the textbk (Rbbins-Miller) cver the materials required fr this tpic.. Wavefrms in electrical systems are current r vltage
More informationCurrent/voltage-mode third order quadrature oscillator employing two multiple outputs CCIIs and grounded capacitors
Indian Jurnal f Pure & Applied Physics Vl. 49 July 20 pp. 494-498 Current/vltage-mde third rder quadrature scillatr emplying tw multiple utputs CCIIs and grunded capacitrs Jiun-Wei Hrng Department f Electrnic
More informationThe Study of Drive Characteristic and Experimental Approach about Planetary Gearing Mechanism
The Study f Drive Characteristic and Experimental Apprach abut Planetary Gearing Mechanism Feng Liu Schl f Mechanical Engineering, Tianjin University f Technlgy and Educatin N.1310, Da Gu Suth Street,
More informationA Self-Acting Radial Bogie with Independently Rotating Wheels
Cpyright c 2008 ICCES ICCES, vl.7, n.3, pp.141-144 A Self-Acting adial Bgie with Independently tating Wheels CHI, Maru 1 ZHANG, Weihua 1 JIANG, Yiping 1 DAI, Huanyun 1 As the independently rtating wheels
More informationNGSS High School Physics Domain Model
NGSS High Schl Physics Dmain Mdel Mtin and Stability: Frces and Interactins HS-PS2-1: Students will be able t analyze data t supprt the claim that Newtn s secnd law f mtin describes the mathematical relatinship
More informationAP Physics Kinematic Wrap Up
AP Physics Kinematic Wrap Up S what d yu need t knw abut this mtin in tw-dimensin stuff t get a gd scre n the ld AP Physics Test? First ff, here are the equatins that yu ll have t wrk with: v v at x x
More informationAerodynamic Separability in Tip Speed Ratio and Separability in Wind Speed- a Comparison
Jurnal f Physics: Cnference Series OPEN ACCESS Aerdynamic Separability in Tip Speed Rati and Separability in Wind Speed- a Cmparisn T cite this article: M L Gala Sants et al 14 J. Phys.: Cnf. Ser. 555
More informationBASIC DIRECT-CURRENT MEASUREMENTS
Brwn University Physics 0040 Intrductin BASIC DIRECT-CURRENT MEASUREMENTS The measurements described here illustrate the peratin f resistrs and capacitrs in electric circuits, and the use f sme standard
More informationPhysics 2010 Motion with Constant Acceleration Experiment 1
. Physics 00 Mtin with Cnstant Acceleratin Experiment In this lab, we will study the mtin f a glider as it accelerates dwnhill n a tilted air track. The glider is supprted ver the air track by a cushin
More informationBiocomputers. [edit]scientific Background
Bicmputers Frm Wikipedia, the free encyclpedia Bicmputers use systems f bilgically derived mlecules, such as DNA and prteins, t perfrm cmputatinal calculatins invlving string, retrieving, and prcessing
More informationFigure 1a. A planar mechanism.
ME 5 - Machine Design I Fall Semester 0 Name f Student Lab Sectin Number EXAM. OPEN BOOK AND CLOSED NOTES. Mnday, September rd, 0 Write n ne side nly f the paper prvided fr yur slutins. Where necessary,
More informationDetermining the Accuracy of Modal Parameter Estimation Methods
Determining the Accuracy f Mdal Parameter Estimatin Methds by Michael Lee Ph.D., P.E. & Mar Richardsn Ph.D. Structural Measurement Systems Milpitas, CA Abstract The mst cmmn type f mdal testing system
More information5.4 Measurement Sampling Rates for Daily Maximum and Minimum Temperatures
5.4 Measurement Sampling Rates fr Daily Maximum and Minimum Temperatures 1 1 2 X. Lin, K. G. Hubbard, and C. B. Baker University f Nebraska, Lincln, Nebraska 2 Natinal Climatic Data Center 1 1. INTRODUCTION
More informationPressure And Entropy Variations Across The Weak Shock Wave Due To Viscosity Effects
Pressure And Entrpy Variatins Acrss The Weak Shck Wave Due T Viscsity Effects OSTAFA A. A. AHOUD Department f athematics Faculty f Science Benha University 13518 Benha EGYPT Abstract:-The nnlinear differential
More informationExaminer: Dr. Mohamed Elsharnoby Time: 180 min. Attempt all the following questions Solve the following five questions, and assume any missing data
Benha University Cllege f Engineering at Banha Department f Mechanical Eng. First Year Mechanical Subject : Fluid Mechanics M111 Date:4/5/016 Questins Fr Final Crrective Examinatin Examiner: Dr. Mhamed
More informationLead/Lag Compensator Frequency Domain Properties and Design Methods
Lectures 6 and 7 Lead/Lag Cmpensatr Frequency Dmain Prperties and Design Methds Definitin Cnsider the cmpensatr (ie cntrller Fr, it is called a lag cmpensatr s K Fr s, it is called a lead cmpensatr Ntatin
More informationIntroductory Thoughts
Flw Similarity By using the Buckingham pi therem, we have reduced the number f independent variables frm five t tw If we wish t run a series f wind-tunnel tests fr a given bdy at a given angle f attack,
More informationBiological Cybernetics 9 Springer-Verlag 1986
Bil. Cybern. 54, 125-132 (1986) Bilgical Cybernetics 9 Springer-Verlag 1986 Cnstraints fr Jint Angle Cntrl f the Human Arm H. Cruse Department f Bilgy, University f Bielefeld, D-48 Bielefeld 1, Federal
More informationGuaranteeing Reliability with Vibration Simulation and Testing. Dr. Nathan Blattau
Guaranteeing Reliability with Vibratin Simulatin and Testing Dr. Nathan Blattau . Nathan Blattau, Ph.D. - Senir Vice President Has been invlved in the packaging and reliability f electrnic equipment fr
More informationFree Vibrations of Catenary Risers with Internal Fluid
Prceeding Series f the Brazilian Sciety f Applied and Cmputatinal Mathematics, Vl. 4, N. 1, 216. Trabalh apresentad n DINCON, Natal - RN, 215. Prceeding Series f the Brazilian Sciety f Cmputatinal and
More informationMINIMIZATION OF ACTUATOR REPOSITIONING USING NEURAL NETWORKS WITH APPLICATION IN NONLINEAR HVAC 1 SYSTEMS
MINIMIZATION OF ACTUATOR REPOSITIONING USING NEURAL NETWORKS WITH APPLICATION IN NONLINEAR HVAC SYSTEMS M. J. Yazdanpanah *, E. Semsar, C. Lucas * yazdan@ut.ac.ir, semsar@chamran.ut.ac.ir, lucas@ipm.ir
More informationDead-beat controller design
J. Hetthéssy, A. Barta, R. Bars: Dead beat cntrller design Nvember, 4 Dead-beat cntrller design In sampled data cntrl systems the cntrller is realised by an intelligent device, typically by a PLC (Prgrammable
More informationA Study on Applicability of Hysteretic Damper to Existing Rail Way Viaduct Structure
Mem. Fac. Eng. Osaka City Univ. Vl. 49 pp. 43-49 (2008) A Study n Applicability f Hysteretic Damper t Existing Rail Way Viaduct Structure Yuki NAKATA * Hajime OHUCH**. and Hlsa TSUNOKAKE*** (Received September
More information1. Transformer A transformer is used to obtain the approximate output voltage of the power supply. The output of the transformer is still AC.
PHYSIS 536 Experiment 4: D Pwer Supply I. Intrductin The prcess f changing A t D is investigated in this experiment. An integrated circuit regulatr makes it easy t cnstruct a high-perfrmance vltage surce
More informationOn Huntsberger Type Shrinkage Estimator for the Mean of Normal Distribution ABSTRACT INTRODUCTION
Malaysian Jurnal f Mathematical Sciences 4(): 7-4 () On Huntsberger Type Shrinkage Estimatr fr the Mean f Nrmal Distributin Department f Mathematical and Physical Sciences, University f Nizwa, Sultanate
More informationRotator PTR-35. Operating instructions
Rtatr PTR-35 Versin 3.01 - January 2012 Page 2 Cntents 1 Safety...4 2 General Infrmatin...5 3 Getting Started...6 4 Operatin f PTR-35...8 5 Specificatins...11 6 Guarantee and service...13 Versin 3.01 -
More informationFlipping Physics Lecture Notes: Simple Harmonic Motion Introduction via a Horizontal Mass-Spring System
Flipping Physics Lecture Ntes: Simple Harmnic Mtin Intrductin via a Hrizntal Mass-Spring System A Hrizntal Mass-Spring System is where a mass is attached t a spring, riented hrizntally, and then placed
More informationTHERMAL TEST LEVELS & DURATIONS
PREFERRED RELIABILITY PAGE 1 OF 7 PRACTICES PRACTICE NO. PT-TE-144 Practice: 1 Perfrm thermal dwell test n prtflight hardware ver the temperature range f +75 C/-2 C (applied at the thermal cntrl/munting
More informationNUROP CONGRESS PAPER CHINESE PINYIN TO CHINESE CHARACTER CONVERSION
NUROP Chinese Pinyin T Chinese Character Cnversin NUROP CONGRESS PAPER CHINESE PINYIN TO CHINESE CHARACTER CONVERSION CHIA LI SHI 1 AND LUA KIM TENG 2 Schl f Cmputing, Natinal University f Singapre 3 Science
More informationLecture 17: Free Energy of Multi-phase Solutions at Equilibrium
Lecture 17: 11.07.05 Free Energy f Multi-phase Slutins at Equilibrium Tday: LAST TIME...2 FREE ENERGY DIAGRAMS OF MULTI-PHASE SOLUTIONS 1...3 The cmmn tangent cnstructin and the lever rule...3 Practical
More informationLecture 5: Equilibrium and Oscillations
Lecture 5: Equilibrium and Oscillatins Energy and Mtin Last time, we fund that fr a system with energy cnserved, v = ± E U m ( ) ( ) One result we see immediately is that there is n slutin fr velcity if
More informationTorsional Elasticity of Human Skin in vivo
Pfliigers Arch. 342, 255--260 (1973) 9 by Springer-Verlag 1973 Trsinal Elasticity f Human Skin in viv 1~. Sanders Develpment Labratries, N.V. Philips'Gleflampenfabrieken, Drachten, The Netherlands Received
More informationChapter 9: Quantization of Light
Chapter 9: Quantizatin Light 9.1 Planck s Quantum Thery 9.1.1 Distinguish between Planck s quantum thery and classical thery energy The undatin the Planck s quantum thery is a thery black bdy radiatin.
More informationCopyright Paul Tobin 63
DT, Kevin t. lectric Circuit Thery DT87/ Tw-Prt netwrk parameters ummary We have seen previusly that a tw-prt netwrk has a pair f input terminals and a pair f utput terminals figure. These circuits were
More informationHeat Management Methodology for Successful UV Processing on Heat Sensitive Substrates
Heat Management Methdlgy fr Successful UV Prcessing n Heat Sensitive Substrates Juliet Midlik Prime UV Systems Abstract: Nw in 2005, UV systems pssess heat management cntrls that fine tune the exthermic
More informationApplying Kirchoff s law on the primary circuit. V = - e1 V+ e1 = 0 V.D. e.m.f. From the secondary circuit e2 = v2. K e. Equivalent circuit :
TRANSFORMERS Definitin : Transfrmers can be defined as a static electric machine which cnverts electric energy frm ne ptential t anther at the same frequency. It can als be defined as cnsists f tw electric
More informationQ1. In figure 1, Q = 60 µc, q = 20 µc, a = 3.0 m, and b = 4.0 m. Calculate the total electric force on q due to the other 2 charges.
Phys10 Secnd Majr-08 Zer Versin Crdinatr: Dr. I. M. Nasser Saturday, May 3, 009 Page: 1 Q1. In figure 1, Q = 60 µc, q = 0 µc, a = 3.0 m, and b = 4.0 m. Calculate the ttal electric frce n q due t the ther
More informationFebruary 28, 2013 COMMENTS ON DIFFUSION, DIFFUSIVITY AND DERIVATION OF HYPERBOLIC EQUATIONS DESCRIBING THE DIFFUSION PHENOMENA
February 28, 2013 COMMENTS ON DIFFUSION, DIFFUSIVITY AND DERIVATION OF HYPERBOLIC EQUATIONS DESCRIBING THE DIFFUSION PHENOMENA Mental Experiment regarding 1D randm walk Cnsider a cntainer f gas in thermal
More informationDepartment of Economics, University of California, Davis Ecn 200C Micro Theory Professor Giacomo Bonanno. Insurance Markets
Department f Ecnmics, University f alifrnia, Davis Ecn 200 Micr Thery Prfessr Giacm Bnann Insurance Markets nsider an individual wh has an initial wealth f. ith sme prbability p he faces a lss f x (0
More informationA Self-Sensing Homopolar Magnetic Bearing: Analysis and Experimental Results
A Self-Sensing Hmplar Magnetic Bearing: Analysis and Experimental Results Perry Tsa Seth R. Sanders Gabriel Risk Department f Electrical Engineering and Cmputer Science University f Califrnia, Berkeley
More informationECE 2100 Circuit Analysis
ECE 00 Circuit Analysis Lessn 6 Chapter 4 Sec 4., 4.5, 4.7 Series LC Circuit C Lw Pass Filter Daniel M. Litynski, Ph.D. http://hmepages.wmich.edu/~dlitynsk/ ECE 00 Circuit Analysis Lessn 5 Chapter 9 &
More informationEffects of piezo-viscous dependency on squeeze film between circular plates: Couple Stress fluid model
Turkish Jurnal f Science & Technlgy Vlume 9(1), 97-103, 014 Effects f piez-viscus dependency n squeeze film between circular plates: Cuple Stress fluid mdel Abstract U. P. SINGH Ansal Technical Campus,
More informationFundamental Concepts in Structural Plasticity
Lecture Fundamental Cncepts in Structural Plasticit Prblem -: Stress ield cnditin Cnsider the plane stress ield cnditin in the principal crdinate sstem, a) Calculate the maximum difference between the
More informationSurface and Contact Stress
Surface and Cntact Stress The cncept f the frce is fundamental t mechanics and many imprtant prblems can be cast in terms f frces nly, fr example the prblems cnsidered in Chapter. Hwever, mre sphisticated
More informationLab 1 The Scientific Method
INTRODUCTION The fllwing labratry exercise is designed t give yu, the student, an pprtunity t explre unknwn systems, r universes, and hypthesize pssible rules which may gvern the behavir within them. Scientific
More informationRevision: August 19, E Main Suite D Pullman, WA (509) Voice and Fax
.7.4: Direct frequency dmain circuit analysis Revisin: August 9, 00 5 E Main Suite D Pullman, WA 9963 (509) 334 6306 ice and Fax Overview n chapter.7., we determined the steadystate respnse f electrical
More informationSolution to HW14 Fall-2002
Slutin t HW14 Fall-2002 CJ5 10.CQ.003. REASONING AND SOLUTION Figures 10.11 and 10.14 shw the velcity and the acceleratin, respectively, the shadw a ball that underges unirm circular mtin. The shadw underges
More information17 IMPACT PROPERTIES OF COMPOSITES
17 IMPACT PROPERTIES OF COMPOSITES 17-1 Impact resistance is the ability f a material t absrb and dissipate energies under impact r shck lading. The respnse t impact lads ranges frm lcalized damage t ttal
More informationChE 471: LECTURE 4 Fall 2003
ChE 47: LECTURE 4 Fall 003 IDEL RECTORS One f the key gals f chemical reactin engineering is t quantify the relatinship between prductin rate, reactr size, reactin kinetics and selected perating cnditins.
More informationCHAPTER 8b Static Equilibrium Units
CHAPTER 8b Static Equilibrium Units The Cnditins fr Equilibrium Slving Statics Prblems Stability and Balance Elasticity; Stress and Strain The Cnditins fr Equilibrium An bject with frces acting n it, but
More informationMethods for Determination of Mean Speckle Size in Simulated Speckle Pattern
0.478/msr-04-004 MEASUREMENT SCENCE REVEW, Vlume 4, N. 3, 04 Methds fr Determinatin f Mean Speckle Size in Simulated Speckle Pattern. Hamarvá, P. Šmíd, P. Hrváth, M. Hrabvský nstitute f Physics f the Academy
More informationPhysics 2B Chapter 23 Notes - Faraday s Law & Inductors Spring 2018
Michael Faraday lived in the Lndn area frm 1791 t 1867. He was 29 years ld when Hand Oersted, in 1820, accidentally discvered that electric current creates magnetic field. Thrugh empirical bservatin and
More information11. DUAL NATURE OF RADIATION AND MATTER
11. DUAL NATURE OF RADIATION AND MATTER Very shrt answer and shrt answer questins 1. Define wrk functin f a metal? The minimum energy required fr an electrn t escape frm the metal surface is called the
More informationAPEX DYNAMICS, INC. Stainless
APE DYNAMICS, INC. HIGH PRECISION PLANETARY GEARBO AB / ABR Series Stainless High precisin planetary gearbx AB / ABR series Apex Dynamics, Inc. is the wrld s mst prductive manufacturer f servmtr drive
More informationModeling and Control of Piezoelectric Actuators
Mdeling and Cntrl f Piezelectric Actuatrs A Thesis Submitted t the Cllege f Graduate Studies and Research In Partial Fulfillment f the Requirements Fr the Degree f Dctr f Philsphy In the Department f Mechanical
More informationFall 2013 Physics 172 Recitation 3 Momentum and Springs
Fall 03 Physics 7 Recitatin 3 Mmentum and Springs Purpse: The purpse f this recitatin is t give yu experience wrking with mmentum and the mmentum update frmula. Readings: Chapter.3-.5 Learning Objectives:.3.
More informationSYNTHESIS OF TWO MECHANISMS WHICH GENERATE LUNULES OVER AN EQUILATERAL TRIANGLE S SIDES
SYNTHESIS OF TWO MECHANISMS WHICH GENERATE LUNULES OVER AN EQUILATERAL TRIANGLE S SIDES Assciate Prfessr PhD Ludmila SASS, University f Craiva, Faculty f Mechanics, ludmila_sass@yah.cm Prfessr Iulian POPESCU,
More informationCompressibility Effects
Definitin f Cmpressibility All real substances are cmpressible t sme greater r lesser extent; that is, when yu squeeze r press n them, their density will change The amunt by which a substance can be cmpressed
More informationChapter 3: Cluster Analysis
Chapter 3: Cluster Analysis } 3.1 Basic Cncepts f Clustering 3.1.1 Cluster Analysis 3.1. Clustering Categries } 3. Partitining Methds 3..1 The principle 3.. K-Means Methd 3..3 K-Medids Methd 3..4 CLARA
More information