LATERAL DISPLACEMENT RESPONSE OF PILES INSTALLED IN NEAR SURFACE IMPROVED COARSE-GRAINED SOILS
|
|
- Silvia Morrison
- 5 years ago
- Views:
Transcription
1 ateral Displacement Respnse f Piles Installe in near Surface Imprve Carse-Graine Sils IGC 9, Guntur, INDIA ATERA DISPACEMENT RESPONSE OF PIES INSTAED IN NEAR SURFACE IMPROVED COARSE-GRAINED SOIS V. Pamavathi Assistant Prfessr, JNTUH Cllege f Engineering, Hyeraba, Inia. vpama7@gmail.cm M.R. Mahav Emeritus Prfessr, JNTUH Cllege f Engineering, Hyeraba, Inia. mahavmr@gmail.cm E. Saibaba Rey Registrar & Prfessr in Civil Engineering, JNTUH, Hyeraba, Inia. sbrey@yah.c.in ABSTRACT: Piles especially fr near-shre an ffshre funatins freuently penetrate thrugh lse sil epsits which are prne t excess isplacement at grun level uner lateral las. Pamavathi et al. (7) presente analysis f single rigi free hea pile in chesinless sils base n kinematics an subgrae reactin apprach. In this paper, the effect f increase in stiffness by ensificatin f the surficial chesinless sil n the behaviur f rigi pile base n kinematics an nn-linear subgrae respnse with hyperblic mel has been stuie. The reuctin in the isplacement f the pile at the surface ue t increase in the stiffness f the near surface sil as a cnseuence f ensificatin is uantifie.. INTRODUCTION Piles are cmmnly selecte as an ptin fr the supprt f high-rise structures, highway an infrastructure. These structural members are ften subjecte t cnsierable lateral frces such as ue t win las in hurricane prne areas, earthuake las in areas f seismic activity, an wave las in ffshre envirnments. Hansen (96), Brms (964a), Meyerhf et al. (98), Prasa & Chari (999), Zhang et al. (5), etc., prpse theries fr the estimatin f ultimate capacities f piles, piers an ples in chesinless sils uner varius pile-hea an base cnitins. Pamavathi et al. (7) presente analysis f single rigi free hea pile in chesinless sils base n kinematics an subgrae reactin apprach. With the same cnsieratins as mentine abve, the effect f increase in stiffness f the surficial sil ue t ensificatin n the behaviur f rigi pile using hyperblic apprach has been stuie. In this analysis, bth subgrae mulus an ultimate sil pressure vary linearly with epth. Anther imprtant cnsieratin in this analysis is that the sil es nt mbilie any pressure clse t the pint f rtatin because the isplacement there is er.. PROBEM DEFINITION A rigi pile f length,, an iameter,, is installe in a carse graine sil. A lateral frce, H, is acting at an eccentricity, e, which creating a mment, M (= e.h), at the grun level (Fig. ). The pile is unrestraine an rtates thrugh an angle, θ, abut a pint, O at epth,, frm the grun surface. The isplacement at grun line is ue t the rtatin f the pile. Mulus f hrintal subgrae reactin, k s, ultimate lateral sil pressure, max, unit weight, γ, angle f internal frictin, φ are the relevant prperties f the sil. The isplacements at grun level may be t high frm structural cnsieratins in many f the cases. The near surface sil can be ensifie s that the sil mulus increases in that prtin an the isplacements get reuce. The mulus an maximum sil pressure fr the imprve sil ver the epth,, frm grun level are cnsiere as k s an max respectively (Fig. b). The prblem is euivalent t that f laterally lae pile in ense san verlying lse san. H e G θ k s γ φ O se San H e Densifie GGrun θ k s γ φ Fig. : Original Grun Imprve Sil ayer near the Grun Surface O k s γ φ se San 79
2 ateral Displacement Respnse f Piles Installe in near Surface Imprve Carse-Graine Sils. Variatins f Stiffness an Strength f the Sil The isplacements vary linearly with epth. The respnse f the sil n t the pile is represente by nn-linear Winkler type respnse with mulus f hrintal subgrae reactin, k s, an ultimate lateral sil pressure, max. The lateral stress,, is relate (Fig. ) t the lateral isplacement,, as = k s /(+ k s / max ) () where is the isplacement f the pile at epth,, frm grun surface. Bth k s an max are assume t increase linearly with epth as shwn in Figures & respectively. k s = α k / () an max = α / () where α k an α are the rates f increase f the mulus f hrintal subgrae reactin an the maximum lateral sil pressure with epth respectively. The epth t the pint f rtatin,, an the angle f rtatin, θ, f the pile are the tw unknwns. Fr euilibrium, the applie lateral frce, H, is euate t the ttal respnse frm the sil as, H = k (4) s k + s + max max Taking mments abut the pint f applicatin f the la M = He = + max + max Where = ( ) tanθ an = ( ) tan θ are isplacements abve an belw the pint f rtatin at epth. an θ can be btaine by slving Es. (4) an (5). ateral Displacement, Fig. : Nn-inear Hyperblic Respnse f the Sil k s ateral Stress, k s max Fig. : Variatin f Parameters with Depth, Hrintal Subgrae Mulus Ultimate ateral Resistance max α k α (5) The imprve sil cnsists f subgrae mulus, k s, an maximum sil pressure, max. The variatins f subgrae mulus an maximum sil pressure alng the length f the pile are as shwn in Figures 4 & respectively. Base n these variatins the frce euatin becme ks H = + k k s s k + s + + max max/ max/ (6) The nrmalie euatins fr frce an mment are H H = = α an M + r k r ( ) tan θ + + μ ( ) tan θ M He = = α α k r (αk / αk ) ( ) tan θ + μ ( ) tan θ (αk / αk ) ( ) tan θ + μ ( ) tan θ k r ( ) tan θ + μ ( ) tan θ k s α k α k G Fig. 4: Variatin f Hrintal Subgrae Muli an Ultimate ateral Sil Pressure with Depth, (αk / αk ) ( ) tan θ + μ ( ) tan θ = (8) (αk / αk ) ( ) tan θ + μ ( ) tan θ where = / the nrmalie epth, = / nrmalie epth f pint f rtatin, r = / an nrmalie la, H = H αk The parameters µ an µ, an the rati, α kr are efine as μ = k s / max = α k /α ; μ = k s / max = α k /α an α kr = α k /α k. Ieally, the epth f rtatin,, an the rtatin, θ, are t be estimate fr given lateral frce, H, an mment, M. Hwever, it wul be an iterative prcess an very teius. Fr given values f μ, μ, α kr an θ, an H can be btaine by slving Es. (7) an (8). Knwing an θ, the nrmalie eflectin at grun level, = tan θ, is evaluate crrespning t the nrmalie applie la, H.. DISCUSSIONS The variatins f nrmalie la, H, with nrmalie isplacement at grun level,, are evaluate base n the prpse mel fr ifferent cmbinatins f μ an μ max α α (7) 74
3 ateral Displacement Respnse f Piles Installe in near Surface Imprve Carse-Graine Sils values ranging frm t 7 with intermeiate values f, 5,,, 5,, an 5; stiffness ratis, α kr f 5, 5,, 5, an, nrmalise thickness f imprve sil frm grun level, r varying frm t.7 an nrmalise la eccentricity, e/ values spanning ver,.,.4,.6,.8,, an 4. Figure 5 shws the la versus isplacement at grun level, respnse curves fr the pile fr μ =, μ =, α kr = 5 an θ =.. Stiffness rati f the sils is 5, which crrespns t the stiffness f the imprve grun being five times mre than the riginal ne. The nrmalie la increases with increase in the epth f the imprve sil. Nrmalise a, H The nrmalise la fr a pile fr epth f imprvement.5, is abut % cmpare t that prir t the imprvement f the sil. Nrmalise a, H.E-4 5.E-5.5E-4.5E-4 μ = r =.4.8 Nrmalise Displacement, Fig. 5: Nrmalie a, H vs Nrmalie Displacement, at Grun evel fr μ =, μ = an α kr = 5 Effect f r,,7,.4.8 Nrmalise Displacement at G, Fig. 6: Nrmalie a, H vs Nrmalie Displacement, at Grun evel fr μ =,, r =.4, e/ = an α kr = 5 Effect f μ Figure 6 presents the variatin f nrmalise la with nrmalise isplacement f the pile fr ifferent values f μ fr μ =,, r =.4, e/=, α kr = 5 an θ =.. The nrmalise las are.4 4, an t.5 5 an crrespn t nrmalise isplacements f.6,.4 an.78 fr μ = 5, 5 an 7, respectively an θ =.. The isplacement increases by abut times fr μ increasing frm 5 t 7, an rtatin.. The initial slpes f the la-isplacement curves fr stiff sils (lwer μ values) are high an reuce fr sft sils (higher μ values). The variatins f nrmalise isplacements at the tp with nrmalise imprve sil thickness an fr ifferent stiffness ratis, α kr = t is illustrate in Figure 7 fr μ =,, μ =,, θ =., e/ =. The isplacements f the piles at the grun line ecrease with increase in r, fr the case f stiffer upper surface. The isplacement ecreases frm.77 t.5 fr r increasing frm t.5, fr α kr =. The minimum value f isplacement f the pile tp epens n α kr. Fr example, the nrmalise isplacement is minimum near r values f.5,.6,.67 an.7 fr α kr =, 5, an respectively. The percentage ecrease in isplacement is maximum at r =.5 fr α kr =. The maximum ecrease in isplacement ccurs fr r between.5 an.7 fr α kr in the range t. The maximum ecrease in isplacement is abut % fr α kr = 5. Nrmalise Displacement, r Fig. 7: Variatins f Nrmalise Displacements with r, fr μ =,, μ =, an θ =.-Effect f α kr Figure 8 presents the nrmalise sil pressure istributins alng the length f the pile, fr ifferent values f μ r μ, μ = μ, r =.4, α kr = 5 an θ =.. The nrmalise sil pressure belw the epth f imprve sil ( r ) is significantly less because it is 5 times weaker than the imprve sil. The ifference in nrmalise sil pressures between the curves fr tw values f μ is mre in stiffene sil, while it is less in riginal sil. The variatins f rati f ultimate lateral capacity the pile in imprve sil t that in riginal grun (H u /H u ) is als stuie with respect t r, α kr an presente in Figure 9 fr μ =,, μ =,, / = 4 an e/ =. The increase in nrmalise ultimate pile capacity is high fr values f r between an.5. The ultimate lateral capacity rati H u /H u remains nearly cnstant fr r between.5 an.7 except fr α kr =. 5 α kr = 74
4 ateral Displacement Respnse f Piles Installe in near Surface Imprve Carse-Graine Sils Nrmalise Sil Pressure,.E- 5.E-4 5.E-4.E- 6. Nrmalise Depth, / 7,.5, 5 α kr = μ =5 µ =5 7,, 5 Fig. 8: Variatins f Nrmalise Pressures alng the ength f the Pile, fr r =.4, μ = μ, e/ = an α kr = 5 stiffness f the near surface sil. The maximum ecrease in pile tp isplacement ccurs fr r between.5 an.7. The ecrease in isplacement is abut % fr stiffness rati f.. The preicte la-isplacement plts cmpare well with the measure values reprte by Meyerhf et al. (98) fr piles in tw-layere sils. Nt nly isplacement, but the ultimate carrying capacity f the pile in ensifie grun is als imprve. ateral a, kn.4. exp. Prpse H u /H u Fig. 9: Variatin f Rati f Ultimate ateral Capacity f Pile after an Prir t Imprvement f the Sil, H u an H u with r fr µ =,, µ =,, / = 4 - Effect f α kr Meyerhf et al. (98) cnucte tests n piles installe in tw-layere sils. The ense an the lse sans have the fllwing prperties an cnitins. Unit weights, γ, are 5. an 4 kn/m an angles f internal frictin, φ, are 5 an 5 respectively. ength f the pile,, is. mm, iameter f the pile,, is.5 mm, eccentricity f la (e/ = ) an r =.5 an.75 fr ense san verlying lse san. This ata is applicable fr the present prblem an facilitates cmparisn f the present analysis with experimental results. Figure shws the cmparisn f measure an prpse la-isplacement curves fr the pile respnse, fr ense san verlying lse san fr r =.5. The preicte values agree clsely with the measure nes. 4. CONCUSIONS Present thery preicts the ultimate las as well as the la -isplacement respnses at wrking las f piles installe in ensifie grun. The isplacements at grun line get reuce significantly as can be expecte with increase in the r 5 Displacement at G, mm Fig. : Cmparisn f Preicte an Measure (Meyerhf et al. 98) a-displacement Curves fr Pile in Tw-ayere San: Dense San ver se San, r =.5 REFERENCES Brms, B.B. (964b). ateral Resistance f Piles in Chesinless Sils, Jl. Sil Mech. Fun. Div., ASCE, 9(): 56. Hansen, J.B. (96). The Ultimate Resistance f Rigi Piles against Transversal Frces, Bulletin N., Danish Getechnical Institute, Cpenhagen, Denmark, pp Meyerhf, G.G., Mathur, S.K. an Valsangkar, A.J. (98). ateral Resistance an Deflectin f Rigi Wall an Piles in ayere Sils, Canaian Getechnical Jurnal, Vl. 8(): Pamavathi, V., Saibaba Rey, E. an Mahav, M.R. (7). Analysis f aterally ae Rigi Piles in Sans base n Kinematics an Nn-linear Sub-grae Respnse, Inian Getechnical Jurnal, Vl. 7(): 9 9. Prasa, Y.V.S.N. (997). Stanar Penetratin Tests an Pile Behaviur uner ateral as in Clay, Inian Getechnical Jurnal, Vl. 7():. Zhang,., Silva, F. an Grismala, R. (5). Ultimate ateral Resistance t Piles in Chesinless Sils, Jl. Getechnical & Geenvirnmental Engrg., ASCE, Vl. ():
5 ateral Displacement Respnse f Piles Installe in near Surface Imprve Carse-Graine Sils 74
L 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 informationPhysical Nature of the Covalent Bond Appendix H + H > H 2 ( ) ( )
Physical Nature f the Cvalent Bn Appeni his stuy f the nature f the H cvalent bn frms a mlecular rbital as a linear cmbinatin f scale hyrgenic rbitals, LCAO-MO. he quantum mechanical integrals necessary
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 informationSEISMIC STABILITY ANALYSIS OF FOOTING ADJACENT TO SLOPES BY SLIP LINE METHOD
The 4 th Wrld Cnference n Earthquake Engineering Octber -7, 008, Beijing, China SEISMIC STABILITY ANALYSIS OF FOOTING ADJACENT TO SLOPES BY SLIP LINE METHOD ABSTRACT : M. Jahanandish and M.R. Arvin Assciate
More informationEnergy considerations Energy considerations
Energy cnsieratins 99.0.8 DRFT. Energy cnsieratins The wrk reuire t assemble tw charges, an is fun by first bringing frm infinity t its esire psitin (which reuires n wrk) an then bringing frm infinity
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 information, which yields. where z1. and z2
The Gaussian r Nrmal PDF, Page 1 The Gaussian r Nrmal Prbability Density Functin Authr: Jhn M Cimbala, Penn State University Latest revisin: 11 September 13 The Gaussian r Nrmal Prbability Density Functin
More informationBED FORM DEFORMATION DUE TO UPSTREAM GROUP PILES
BED FORM DEFORMATION DUE TO UPSTREAM GROUP PILES TAE HOON YOON Prfessr Emeritus Deartment f Civil Engineering Hanyang University, Seul, Krea E-mail: taehyn@htmail.cm Abstract Defrmatin f be frms by assing
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 informationModelling of Clock Behaviour. Don Percival. Applied Physics Laboratory University of Washington Seattle, Washington, USA
Mdelling f Clck Behaviur Dn Percival Applied Physics Labratry University f Washingtn Seattle, Washingtn, USA verheads and paper fr talk available at http://faculty.washingtn.edu/dbp/talks.html 1 Overview
More informationDynamic strain softening of concrete in compression under rapid loading K. Fujikake*-, J. Mizuno*, A. Suzuki*, T. Ohno" & T.
Transactins n the Built Envirnment vl 2, 1998 WIT Press, www.witpress.cm, ISSN 174-59 Dynamic strain sftening f cncrete in cmpressin under rapid lading K. Fujikake*-, J. Mizun*, A. Suzuki*, T. hn" & T.
More informationExercise 3 Identification of parameters of the vibrating system with one degree of freedom
Exercise 3 Identificatin f parameters f the vibrating system with ne degree f freedm Gal T determine the value f the damping cefficient, the stiffness cefficient and the amplitude f the vibratin excitatin
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 informationWYSE Academic Challenge Sectional Physics 2007 Solution Set
WYSE caemic Challenge Sectinal Physics 7 Slutin Set. Crrect answer: E. Energy has imensins f frce times istance. Since respnse e. has imensins f frce ivie by istance, it clearly es nt represent energy.
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 information3D 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 informationStudy Group Report: Plate-fin Heat Exchangers: AEA Technology
Study Grup Reprt: Plate-fin Heat Exchangers: AEA Technlgy The prblem under study cncerned the apparent discrepancy between a series f experiments using a plate fin heat exchanger and the classical thery
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 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 informationOF SIMPLY SUPPORTED PLYWOOD PLATES UNDER COMBINED EDGEWISE BENDING AND COMPRESSION
U. S. FOREST SERVICE RESEARCH PAPER FPL 50 DECEMBER U. S. DEPARTMENT OF AGRICULTURE FOREST SERVICE FOREST PRODUCTS LABORATORY OF SIMPLY SUPPORTED PLYWOOD PLATES UNDER COMBINED EDGEWISE BENDING AND COMPRESSION
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 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 informationReactor Pressure Vessel Head Loaded by a Corium Slug Impact Confirmation of the Results
Reactr Pressure Vessel Hea Lae by a Crium Slug Impact Cnfirmatin f the Results B. Dlensky, B. G11er, T. Jran, R. Krieg, M. Lux, G. Messemer, H. Rieger, M. Sir Frschungszentrum Karlsruhe GmbH, Pstfach 364,
More information5.60 Thermodynamics & Kinetics Spring 2008
MIT OpenCurseWare http://cw.mit.edu 5.60 Thermdynamics & Kinetics Spring 2008 Fr infrmatin abut citing these materials r ur Terms f Use, visit: http://cw.mit.edu/terms. 5.60 Spring 2008 Lecture #17 page
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 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 informationChapter 2 GAUSS LAW Recommended Problems:
Chapter GAUSS LAW Recmmended Prblems: 1,4,5,6,7,9,11,13,15,18,19,1,7,9,31,35,37,39,41,43,45,47,49,51,55,57,61,6,69. LCTRIC FLUX lectric flux is a measure f the number f electric filed lines penetrating
More informationCHAPTER 17 COMPOSITES
CHAPTER 17 COMPOSITES EXERCISE 64, Page 373 1. Calculate the stiffness matrix (Q) and derive the (A), (B) and (D) matrices fr a sheet f aluminium 1 mm thick. The fllwing material prperties can be assumed:
More informationGeneral Chemistry II, Unit I: Study Guide (part I)
1 General Chemistry II, Unit I: Study Guide (part I) CDS Chapter 14: Physical Prperties f Gases Observatin 1: Pressure- Vlume Measurements n Gases The spring f air is measured as pressure, defined as the
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 information7.0 Heat Transfer in an External Laminar Boundary Layer
7.0 Heat ransfer in an Eternal Laminar Bundary Layer 7. Intrductin In this chapter, we will assume: ) hat the fluid prperties are cnstant and unaffected by temperature variatins. ) he thermal & mmentum
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 informationDisplacement and Deflection Sensitivity of Gas-coupled Laser Acoustic. Detector
1st Internatinal Sympsium n Laser Ultrasnics: Science, echnlgy and Applicatins July 16-18 008, Mntreal, Canada Displacement and Deflectin Sensitivity f Gas-cupled Laser Acustic Detectin James N. CARON
More informationSupporting information
Electrnic Supplementary Material (ESI) fr Physical Chemistry Chemical Physics This jurnal is The wner Scieties 01 ydrgen perxide electrchemistry n platinum: twards understanding the xygen reductin reactin
More informationLeast Squares Optimal Filtering with Multirate Observations
Prc. 36th Asilmar Cnf. n Signals, Systems, and Cmputers, Pacific Grve, CA, Nvember 2002 Least Squares Optimal Filtering with Multirate Observatins Charles W. herrien and Anthny H. Hawes Department f Electrical
More informationENGI 4430 Parametric Vector Functions Page 2-01
ENGI 4430 Parametric Vectr Functins Page -01. Parametric Vectr Functins (cntinued) Any nn-zer vectr r can be decmpsed int its magnitude r and its directin: r rrˆ, where r r 0 Tangent Vectr: dx dy dz dr
More informationPHYSICS LAB Experiment 10 Fall 2004 ROTATIONAL DYNAMICS VARIABLE I, FIXED
ROTATIONAL DYNAMICS VARIABLE I, FIXED In this experiment we will test Newtn s Secnd Law r rtatinal mtin and examine hw the mment inertia depends n the prperties a rtating bject. THE THEORY There is a crrespndence
More informationBiplots in Practice MICHAEL GREENACRE. Professor of Statistics at the Pompeu Fabra University. Chapter 13 Offprint
Biplts in Practice MICHAEL GREENACRE Prfessr f Statistics at the Pmpeu Fabra University Chapter 13 Offprint CASE STUDY BIOMEDICINE Cmparing Cancer Types Accrding t Gene Epressin Arrays First published:
More informationNumerical Simulation of the Thermal Resposne Test Within the Comsol Multiphysics Environment
Presented at the COMSOL Cnference 2008 Hannver University f Parma Department f Industrial Engineering Numerical Simulatin f the Thermal Respsne Test Within the Cmsl Multiphysics Envirnment Authr : C. Crradi,
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 informationCS 477/677 Analysis of Algorithms Fall 2007 Dr. George Bebis Course Project Due Date: 11/29/2007
CS 477/677 Analysis f Algrithms Fall 2007 Dr. Gerge Bebis Curse Prject Due Date: 11/29/2007 Part1: Cmparisn f Srting Algrithms (70% f the prject grade) The bjective f the first part f the assignment is
More informationAQA GCSE Physics. Topic 7: Magnetism and Electromagnetism. Notes. (Content in bold is for Higher Tier only)
AQA GCSE Physics Tpic 7: Magnetism and Electrmagnetism Ntes (Cntent in bld is fr Higher Tier nly) Magnets - Nrth and Suth Ples - Same Ples repel - Oppsite ples attract Permanent Magnets - Always magnetic,
More informationOn Boussinesq's problem
Internatinal Jurnal f Engineering Science 39 (2001) 317±322 www.elsevier.cm/lcate/ijengsci On Bussinesq's prblem A.P.S. Selvadurai * Department f Civil Engineering and Applied Mechanics, McGill University,
More informationOn the Commutation Process of Capacitor Commutated Converter (CCC)
On the Cmmutatin Prcess f Capacitr Cmmutate Cnverter (CCC Angel J. J. Rezek*; Ariana A. s Sants zir*; Jcéli Suza e Sá** NFE/EE/DET Feeral niversity f tajubá / Electrical Engineering nstitute(* Av. BPS,
More informationANALYTICAL SOLUTIONS TO THE PROBLEM OF EDDY CURRENT PROBES
ANALYTICAL SOLUTIONS TO THE PROBLEM OF EDDY CURRENT PROBES CONSISTING OF LONG PARALLEL CONDUCTORS B. de Halleux, O. Lesage, C. Mertes and A. Ptchelintsev Mechanical Engineering Department Cathlic University
More informationChapter 9 Vector Differential Calculus, Grad, Div, Curl
Chapter 9 Vectr Differential Calculus, Grad, Div, Curl 9.1 Vectrs in 2-Space and 3-Space 9.2 Inner Prduct (Dt Prduct) 9.3 Vectr Prduct (Crss Prduct, Outer Prduct) 9.4 Vectr and Scalar Functins and Fields
More informationYeu-Sheng Paul Shiue, Ph.D 薛宇盛 Professor and Chair Mechanical Engineering Department Christian Brothers University 650 East Parkway South Memphis, TN
Yeu-Sheng Paul Shiue, Ph.D 薛宇盛 Prfessr and Chair Mechanical Engineering Department Christian Brthers University 650 East Parkway Suth Memphis, TN 38104 Office: (901) 321-3424 Rm: N-110 Fax : (901) 321-3402
More informationFinding the Earth s magnetic field
Labratry #6 Name: Phys 1402 - Dr. Cristian Bahrim Finding the Earth s magnetic field The thery accepted tday fr the rigin f the Earth s magnetic field is based n the mtin f the plasma (a miture f electrns
More informationStress and Strain. Stresses are three types such as normal (tensile or compressive), shearing (direct or torsional), and bearing stress.
Stress and Strain Stress Stress is defined as frce per unit area. It has the same units as pressure, and in fact pressure is ne special variety f stress. When a bdy is subjected t a set f frces and is
More information" E ds = 0 becomes " E ds = 0 # d$ B. ! Not only charges produce E-field. ! a changing B-field also produces an E-field.
Faraay s aw & EM waves This ecture Displacement currents Mawell s equatins EM Waves MTE2 results Sme peple that ha the alternate will have a minr grae change talk t me after lecture Ave= 72/15 = 68% Frm
More informationThermodynamics and Equilibrium
Thermdynamics and Equilibrium Thermdynamics Thermdynamics is the study f the relatinship between heat and ther frms f energy in a chemical r physical prcess. We intrduced the thermdynamic prperty f enthalpy,
More informationCONSTRUCTING STATECHART DIAGRAMS
CONSTRUCTING STATECHART DIAGRAMS The fllwing checklist shws the necessary steps fr cnstructing the statechart diagrams f a class. Subsequently, we will explain the individual steps further. Checklist 4.6
More informationDesign and Analysis of Gas Turbine Blade by Potential Flow Approach
V. Vijaya kumar et al Int. Jurnal f Engineering Research and Applicatins RESEARCH ARTICLE OPEN ACCESS Design and Analysis f Gas Turbine Blade by Ptential Flw Apprach V. Vijaya Kumar 1, R. Lalitha Narayana
More informationChemistry 20 Lesson 11 Electronegativity, Polarity and Shapes
Chemistry 20 Lessn 11 Electrnegativity, Plarity and Shapes In ur previus wrk we learned why atms frm cvalent bnds and hw t draw the resulting rganizatin f atms. In this lessn we will learn (a) hw the cmbinatin
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 informationDr M. BROUARD. 5. Thermodynamic formulation of Transition State Theory Entropy of activation. Thermochemical kinetics. CHEMICAL REACTION RATES
CHEMICAL REACTION RATES Dr M. BROUARD Trinity Term 2003 A. Bimlecular Reactins 5 Lectures 1. Intrductin Simple cllisin thery. Ptential energy curves and surfaces. The reactin crdinate and barriers t reactin.
More informationEquilibrium of Stress
Equilibrium f Stress Cnsider tw perpendicular planes passing thrugh a pint p. The stress cmpnents acting n these planes are as shwn in ig. 3.4.1a. These stresses are usuall shwn tgether acting n a small
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 informationAccelerated Chemistry POGIL: Half-life
Name: Date: Perid: Accelerated Chemistry POGIL: Half-life Why? Every radiistpe has a characteristic rate f decay measured by its half-life. Half-lives can be as shrt as a fractin f a secnd r as lng as
More informationDrained Behaviour of Suction Caisson Foundations on Very Dense Sand B.W. Byrne and G.T. Houlsby, The University of Oxford
OTC 1994 Drained Behaviur f Suctin Caissn Fundatins n ery Dense Sand B.W. Byrne and G.T. Hulsby, The University f Oxfrd Cpyright 1999, Offshre Technlgy Cnference This paper was prepared fr presentatin
More informationSOLUTION OF THREE-CONSTRAINT ENTROPY-BASED VELOCITY DISTRIBUTION
SOLUTION OF THREECONSTRAINT ENTROPYBASED VELOCITY DISTRIBUTION By D. E. Barbe,' J. F. Cruise, 2 and V. P. Singh, 3 Members, ASCE ABSTRACT: A twdimensinal velcity prfile based upn the principle f maximum
More informationNUMERICAL SIMULATION OF CHLORIDE DIFFUSION IN REINFORCED CONCRETE STRUCTURES WITH CRACKS
VIII Internatinal Cnference n Fracture Mechanics f Cnete and Cnete Structures FraMCS-8 J.G.M. Van Mier, G. Ruiz, C. Andrade, R.C. Yu and X.X. Zhang (Eds) NUMERICAL SIMULATION OF CHLORIDE DIFFUSION IN REINFORCED
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 informationCOASTAL ENGINEERING Chapter 2
CASTAL ENGINEERING Chapter 2 GENERALIZED WAVE DIFFRACTIN DIAGRAMS J. W. Jhnsn Assciate Prfessr f Mechanical Engineering University f Califrnia Berkeley, Califrnia INTRDUCTIN Wave diffractin is the phenmenn
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 informationDrought damaged area
ESTIMATE OF THE AMOUNT OF GRAVEL CO~TENT IN THE SOIL BY A I R B O'RN EMS S D A T A Y. GOMI, H. YAMAMOTO, AND S. SATO ASIA AIR SURVEY CO., l d. KANAGAWA,JAPAN S.ISHIGURO HOKKAIDO TOKACHI UBPREFECTRAl OffICE
More information( ) kt. Solution. From kinetic theory (visualized in Figure 1Q9-1), 1 2 rms = 2. = 1368 m/s
.9 Kinetic Mlecular Thery Calculate the effective (rms) speeds f the He and Ne atms in the He-Ne gas laser tube at rm temperature (300 K). Slutin T find the rt mean square velcity (v rms ) f He atms at
More informationCHAPTER Read Chapter 17, sections 1,2,3. End of Chapter problems: 25
CHAPTER 17 1. Read Chapter 17, sectins 1,2,3. End f Chapter prblems: 25 2. Suppse yu are playing a game that uses tw dice. If yu cunt the dts n the dice, yu culd have anywhere frm 2 t 12. The ways f prducing
More informationSolar Characteristics
Slar Characteristics 8/8/03 1:55 Slar Characteristics Much f the structure f this sectin is base upn Chapter 7 f [Rahman 1999]. Here yu will be intruce t the characteristics f the energy we receive frm
More informationTypes of Gear Pg xxx. Spur Gear Teeth is parallel to axis of rotation Can transmit power between parallel shaft The simplest form for gear
[Pg / 2] Gears Objectives. 2. 3. 4. 5. Cmpute the frces exerted n gear teeth as they rtate and transmit pwer. Use apprpriate stress analyses t determine the relatinships amng the applied frces, the gemetry
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 informationBASD HIGH SCHOOL FORMAL LAB REPORT
BASD HIGH SCHOOL FORMAL LAB REPORT *WARNING: After an explanatin f what t include in each sectin, there is an example f hw the sectin might lk using a sample experiment Keep in mind, the sample lab used
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 informationChapter 16. Capacitance. Capacitance, cont. Parallel-Plate Capacitor, Example 1/20/2011. Electric Energy and Capacitance
summary C = ε A / d = πε L / ln( b / a ) ab C = 4πε 4πε a b a b >> a Chapter 16 Electric Energy and Capacitance Capacitance Q=CV Parallel plates, caxial cables, Earth Series and parallel 1 1 1 = + +..
More information2-D Momentum Conservation
-D Mmentum Cnseratin Saleback Cllege Physics Department Purpse: T cnirm that linear mmentum is cnsere in tw-imensinal cllisins. T shw that kinetic energy is nearly cnsere in tw-imensinal near-elastic cllisins.
More informationDifferentiation Applications 1: Related Rates
Differentiatin Applicatins 1: Related Rates 151 Differentiatin Applicatins 1: Related Rates Mdel 1: Sliding Ladder 10 ladder y 10 ladder 10 ladder A 10 ft ladder is leaning against a wall when the bttm
More informationChapter 5: Force and Motion I-a
Chapter 5: rce and Mtin I-a rce is the interactin between bjects is a vectr causes acceleratin Net frce: vectr sum f all the frces n an bject. v v N v v v v v ttal net = i = + + 3 + 4 i= Envirnment respnse
More informationo o IMPORTANT REMINDERS Reports will be graded largely on their ability to clearly communicate results and important conclusions.
BASD High Schl Frmal Lab Reprt GENERAL INFORMATION 12 pt Times New Rman fnt Duble-spaced, if required by yur teacher 1 inch margins n all sides (tp, bttm, left, and right) Always write in third persn (avid
More informationNAME TEMPERATURE AND HUMIDITY. I. Introduction
NAME TEMPERATURE AND HUMIDITY I. Intrductin Temperature is the single mst imprtant factr in determining atmspheric cnditins because it greatly influences: 1. The amunt f water vapr in the air 2. The pssibility
More informationChapters 29 and 35 Thermochemistry and Chemical Thermodynamics
Chapters 9 and 35 Thermchemistry and Chemical Thermdynamics 1 Cpyright (c) 011 by Michael A. Janusa, PhD. All rights reserved. Thermchemistry Thermchemistry is the study f the energy effects that accmpany
More informationSimple Models of Foundation-Soil Interactions
IACSIT Internatinal Jurnal f Engineering and Technlgy, Vl. 5, N. 5, Octber 013 Simple Mdels f Fundatin-Sil Interactins Shi-Shuenn Chen and Jun-Yang Shi Abstract This study aims t develp a series f simplified
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 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 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 informationMECHANICS OF SOLIDS TORSION TUTORIAL 2 TORSION OF THIN WALLED SECTIONS AND THIN STRIPS
MECHANICS OF SOLIDS ORSION UORIAL ORSION OF HIN WALLED SECIONS AND HIN SRIPS Yu shuld judge yur prgress by cmpleting the self assessment exercises. On cmpletin f this tutrial yu shuld be able t d the fllwing.
More informationEnhancing Performance of MLP/RBF Neural Classifiers via an Multivariate Data Distribution Scheme
Enhancing Perfrmance f / Neural Classifiers via an Multivariate Data Distributin Scheme Halis Altun, Gökhan Gelen Nigde University, Electrical and Electrnics Engineering Department Nigde, Turkey haltun@nigde.edu.tr
More informationON THE COMPUTATIONAL DESIGN METHODS FOR IMPROOVING THE GEAR TRANSMISSION PERFORMANCES
ON THE COMPUTATIONAL DESIGN METHODS FOR IMPROOVING THE GEAR TRANSMISSION PERFORMANCES Flavia Chira 1, Mihai Banica 1, Dinu Sticvici 1 1 Assc.Prf., PhD. Eng., Nrth University f Baia Mare, e-mail: Flavia.Chira@ubm.r
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 informationCLASS XI SET A PHYSICS
PHYSIS. If the acceleratin f wedge in the shwn arrangement is a twards left then at this instant acceleratin f the blck wuld be, (assume all surfaces t be frictinless) a () ( cs )a () a () cs a If the
More informationand the Doppler frequency rate f R , can be related to the coefficients of this polynomial. The relationships are:
Algrithm fr Estimating R and R - (David Sandwell, SIO, August 4, 2006) Azimith cmpressin invlves the alignment f successive eches t be fcused n a pint target Let s be the slw time alng the satellite track
More informationES201 - Examination 2 Winter Adams and Richards NAME BOX NUMBER
ES201 - Examinatin 2 Winter 2003-2004 Adams and Richards NAME BOX NUMBER Please Circle One : Richards (Perid 4) ES201-01 Adams (Perid 4) ES201-02 Adams (Perid 6) ES201-03 Prblem 1 ( 12 ) Prblem 2 ( 24
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 informationSOIL PROPERTIES STUDY NOTES
SOIL PROPERTIES STUDY NOTES UNIT I SOIL PROPERTIES Objectives and Values f Getechnical Engineering Physical prperties f sil Phase relatins, Grain size distributin, Atterberg Limits, Sil descriptin and
More informationCHAPTER 3 INEQUALITIES. Copyright -The Institute of Chartered Accountants of India
CHAPTER 3 INEQUALITIES Cpyright -The Institute f Chartered Accuntants f India INEQUALITIES LEARNING OBJECTIVES One f the widely used decisin making prblems, nwadays, is t decide n the ptimal mix f scarce
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 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 informationTHE FLUXOID QUANTUM AND ELECTROGRAVITATIONAL DYNAMICS. Chapter 8. This work extends chapter 6 titled, "Field Mass Generation and Control", while
133 THE FLUXOID QUANTUM AND ELECTROGRAVITATIONAL DYNAMICS Chapter 8 This wrk extends chapter 6 titled, "Field Mass Generatin and Cntrl", while als develping a new cnceptual apprach t mass-field vehicle
More informationAnalysis of Curved Bridges Crossing Fault Rupture Zones
Analysis f Curved Bridges Crssing Fault Rupture Znes R.K.Gel, B.Qu & O.Rdriguez Dept. f Civil and Envirnmental Engineering, Califrnia Plytechnic State University, San Luis Obisp, CA 93407, USA SUMMARY:
More informationRelationship Between Amplifier Settling Time and Pole-Zero Placements for Second-Order Systems *
Relatinship Between Amplifier Settling Time and Ple-Zer Placements fr Secnd-Order Systems * Mark E. Schlarmann and Randall L. Geiger Iwa State University Electrical and Cmputer Engineering Department Ames,
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 information