STRENGTH AND DEFORMATION CHARACTERISTICS OF SRC FRAMES HAVING WEAK AXIS BENDING COLUMNS
|
|
- Lillian Jones
- 5 years ago
- Views:
Transcription
1 13 th Wold Confeence on Eathquake Engineeing Vancouve, B.C., Canada Augut 1-6, 24 Pape o STREGTH AD DEFORATIO CHARACTERISTICS OF SRC FRAES HAVIG WEAK AXIS BEDIG COLS.Haegawa 1 T.Fujinaga 2, I.itani 3,.chida 4,.aihaa 5, Y.Ohtani 6 and T.Fukuumi 7 SARY An expeimental wok of SRC (Steel encaed Reinfoced Concete) fame with weak axi bending column wa pefomed. Total fou pecimen wee ubjected to contant vetical load and cyclic hoizontal load. A the expeimental paamete, the column length to ection depth atio and axial load atio wee elected. Fom the tet eult, the expeimental tength wa compaed with AIJ (Achitectual Intitute of Japan) deign fomula. In addition, the collape mechanim of pecimen, the hyteei chaacteitic and the defomation capacity wee invetigated and dicued. ITRODCTIO Steel-concete compoite tuctue ae being widely ued fo the building in Japan now. And by the development of the indutial technology in ecent yea, high-tength concete and teel ae ued a a building mateial. Theefoe, a column membe hould become lende. In AIJ deign fomula, the tength of lende teel-concete compoite column i calculated by upepoed method conideed additional bending moment. Howeve, the deign method take no conideation about defomation capacity. To evaluate the defomation capacity, it i neceay to etablih pope hyteei model fo teel-concete compoite membe. Fom the above, an expeimental tudy on SRC fame wa pefomed. The objective of the tudy ae to examine the AIJ deign fomula and to evaluate the defomation capability of the compoite column. 1 Gaduate tudent, Kobe niv., Japan. m-haegawa@juno.ocn.ne.jp 2 Reeach Aociate,.Eng., Kobe niv., Japan. ftaka@kobe-u.ac.jp 3 Pof., D.Eng., Kobe niv., Japan. imitani@kobe-u.ac.jp 4 Pof., D.Eng., Kobe niv., Japan. nuchida@kobe-u.ac.jp 5 Gaduate tudent, Kobe niv., Japan. neitatu@k9.o-net.ne.jp 6 Aoc. Pof., Ph.D., Kobe niv., Japan. ohtani@kobe-u.ac.jp 7 Aoc. Pof.,D.Eng., Kobe niv., Japan. fukuumi@kobe-u.ac.jp
2 TEST PROGRA 1. Specimen Total fou SRC pecimen wee teted to invetigate the elatic-platic behavio of compoite fame. The pecimen wee ubjected to contant vetical load and cyclic hoizontal load. The encaed H-ection column wa weak-axi bending. When pefoming the expeimental tudy, two paamete wee choen. One wa L/D (column Length to ection Depth atio) of 12and 6, the othe wa axial load atio (/BDF c =.1,.5 (: axial load, B: width of a column, F c : compeive tength of concete )). The dimenion and popetie, and the detail of pecimen ae hown in Table 1 and Fig.1. The cleaheight of column i 18mm o 9mm. The column, with quae ection of 15x15mm, ae einfoced with 4-D6 (D: defomed ba, SD295A) longitudinal ba and 4φ hoop (@1mm). The encaed H-ection deigned a H-1x5x5x7 i mild teel and i placed o a to be ubjected to weak axi bending. The aea atio of the teel ection to the ection of the column i about 4.6%. The beam, with ection of 15x16mm, ae einfoced with 8-D1 (SD295A) ba and 4φ tiup (@5mm). The encaed H-ection i placed o a to be ubjected to tong axi bending. The pecimen wee deigned o that the column wee collaped ealie than the beam. Theefoe, the numbe of tiup wa aanged in the beam. The main einfocement wee welded to the end plate. All pecimen ae named uch a SRC-6-1. In thi cae, 6 mean L/D (the column Length to ection Depth atio) and 1 mean vetical load atio. Column 4φ@5 4φ@1 Beam Fig. 1 Detail of pecimen
3 Table 1. Popetie and Size of pecimen b(mm) D(mm) mp(%) p(%) ce(gpa) F c (pa) (k) n n' batch Column SRC A L/D=6 Beam Column SRC B Beam Column SRC A Beam L/D=12 Column SRC B Beam b: width of co ection, D: depth of co ection, m p: einfocement atio ( m A/bD, m A: go aea of eba) p: teel atio ( A/bD, A: aea of H-ection), ce: modulu of elaticity of concete, F c : compeive tength of concete, : applied axial load, n: axial load atio, n': / 2F c bd Specimen: SRC-L/D-n 2. echanical popetie The popetie of concete uch a the modulu of elaticity and the compeive tength ae hown in Table 1. The mechanical popetie of teel obtained fom the coupon tet ae hown in Table 2 and the ize of H-ection i ummaized in Table 3. Table 4 how the mix popotion of concete. The deign tength of concete wa 27Pa. The tength of concete hown in Table 1 wa the eult of compeive tet uing cylinde (1φx2mm) at tet age of the pecimen. The maximum aggegate diamete wa 15mm. Table 2. echanical popetie of teel diamete Young' odulu yield point tenile tength yield tain yield atio elongation φ(mm) E(GPa) σ Y (Pa) σ u (Pa) ε Y ( σ Y / E) σ Y / σ u (%) flange web D1 A B D φ A B Table 3. Size of H-ection height width flange thickne web thickne H (mm) B (mm) t f (mm) t w (mm) Table 4. ix popotion of concete weight pe unit volume (kg/m 3 ) W/C S/a F G AX Slump C W S1(ea) S2(cuhed) G AE agency (%) (%) (Pa) (mm) (cm) F: deign tength of concete, G AX : maximum diamete of coae aggegate, S: S1+S2 A B
4 3. Loading Appaatu toy dift angle(ad.) The loading pogam i hown in Fig.2. The.4 amplitude of toy dift angle of the fame wa inceaed in incement of.5ad..3 The expeimental appaatu i hown in Fig.3..2 Though the Loading beam, the contant vetical load wa applied on the pecimen by hydaulic jack 1, and.1 kept contant duing hoizontal loading poce. The cyclic hoizontal load wa applied to the pecimen by -.1 hydaulic jack 2. And the applied foce wee meaued by load cell. -.2 Fig.4 how the poition of meauement. Hoizontal -.3 diplacement wee meaued uing diplacement tanduce at the cente of the beam. Axi -.4 cycle diplacement wee meaued by diplacement tanduce at the top of the both column and 1.5D (D: Fig. 2 Loading pogam depth of column) below. The tain of concete, encaed H-ection, and main einfocement wee meaued by wie tain gauge placed at D apat fom the face of column and beam. 4 Wie tain gauge Diplacement tanduce Slide Slide Jack 1 Load cell Loading beam D Load cell Specimen Jack 2 D 1.5D H Reaction wall 4 Fig. 3 Loading appaatu Fig. 4 Poition of meauement RESLTS AD DISCCTIO 1. Load-diplacement elation Fig.5 how the Q-R elation of all pecimen, whee Q mean the lateal foce applied to the pecimen and R mean the toy dift angle defined a the elative lateal diplacement between top and bottom of the column divided by height of the column H (See Fig.4). Additionally, the tage obeved flexual cack and bond cack ae hown by mak A and B, epectively. And the tage that main
5 einfocement and H-ection teel eached thei yield tain ae hown by C, D, E and F. In that cae, the occuence of the cack wa judged by eye obevation and yielding of the teel mateial by tain gauge. In Fig.5, the olid line how the expeimental behavio. The chain line how initial igidity of the fame, which i calculated by diegading the igid zone and uing linea-fame model. The dotted line how the igid platic collape mechanim line baed on the fully platic moment of the column co ection, which i calculated by auming that a platic hinge ae fomed at the uface of the beam (the 1 Q(k) 8 Initial igidity A 6 echanim line C B AIJ fomula Q(k) B 8 D 6 A 4 F 2 E E D SRC-6-1 C SRC Q(k) 4 3 C 5 Q(k) 4 3 C D E 2 A A 2 F D -2-3 F -4-5 SRC SRC-12-5 A : flexual cack wee obeved B : bond cack wee obeved C : occuence of main einfocement at top of column yielding D : occuence of main einfocement at bottom of column yielding E : occuence of teel at top of column yielding F : occuence of teel at bottom of column yielding Fig. 5 Hoizontal load - toy dift angle elation
6 top and bottom of the column). The dahed line epeent the tength that i calculated by AIJ fomula fo lende column. In all of the pecimen, the table hyteei popetie wee obeved until thei maximum tength wa obeved. And the yielding of H-ection wa obeved in the final tage of all pecimen. The expeimental tength of all pecimen exceed the tength calculated by AIJ deign fomula. eithe pecimen excluding SRC-12-5 eached the igid platic collape mechanim line. Two pecimen whoe axial load atio i.1 howed thei maximum tength at R=.2ad. On the othe hand, two pecimen whoe axial load atio i.5 howed thei maximum tength (at about R=.1). Afte peak, the tength of all pecimen deteioated lage than the mechanim line. 2. Poce of collape The final cack patten of the tet pecimen ae illutated in Fig.6. The L/D=12 pecimen collaped flexual failue. On the othe hand, the L/D=6 pecimen collaped hea bond failue that wa diffeent fom that aumed in AIJ deign fomula. In cae of the L/D=12 pecimen, flexual cack wee obeved at the top and bottom of the column (R=.5 ad.). Subequently, the numbe of cack inceaed a the defomation wa inceaed. The SRC-12-1 pecimen eached maximum tength at R=.25ad. and the SRC-12-5 pecimen ha aleady eached at R=.1ad. And afte that, cuh of concete ection wa obeved at R=.3ad in both pecimen. bond cack SRC-6-1 SRC-6-5 flexual cack SRC-12-1 SRC-12-5 Fig. 6 Cack patten (final tage)
7 In cae of the L/D=6 pecimen, flexual cack obeved at R=.5ad. At R=.1ad, bond cack between teel and concete wa obeved. Afte that, the cack have pogeed fat. Finally, the cacked cove concete fell off gadually. 3. Compaion of tength between Tet and AIJ fomula In AIJ deign fomula, the tength of lende compoite column i calculated by Equation 1, whee a conventional equation of imple upepoition i modified. The tength of lende compoite column i obtained a lage value of the two upepoed tength. One i pefeable fo bending about the tong axi of teel membe, the othe one i pefeable fo bending about weak axi. pefeable fo bending about the tong axi When o (1 / k ) =, = + 1 k When o (1 / ) k = +, = 1 (1-1) k pefeable fo bending about the weak axi When o (1 / k ) =, = + 1 k When o (1 / ) = +, k = 1 (1-2) k whee : ultimate compeive tength of membe, : ultimate flexual tength of membe, : ultimate compeive tength of RC potion, : ultimate flexual tength of RC potion, : ultimate compeive tength of RC potion ubjected to compeion alone, : ultimate flexual tength of RC potion ubjected to bending alone, : ultimate compeive tength of teel potion ubjected to compeion alone, : ultimate compeive tength of teel potion, : ultimate flexual tength of teel potion, : ultimate flexual tength of teel potion ubjected to bending alone, k : elatic buckling tength of column defined by Equation 2 π E I = 2 c c k + E I 2 lk 5 whee ce and E: modulu of elaticity of concete and teel, epectively, ci and I: moment inetia of concete potion and teel, epectively, l k : buckling length of column (2)
8 The expeimental tength ae compaed with the tength calculated by AIJ deign fomula in tem of moment axial load elation in Fig.7. In Fig.7, thick olid line ae the tength of AIJ SRC Standad deign fomula. The thin olid line ae baed on fully platic moment. The tength of mateial compoing a co ection i ued value hown in Table 1 and 2. And the cicle how the expeimental maximum tength. 14 u(k) 14 u(k) 12 Section Section 4 2 AIJ Standad Tet u(km) SRC Tet 2 AIJ Standad u(km) SRC u(k) 14 u(k) 12 Section Section 6 AIJ Standad 6 AIJ Standad 4 4 Tet 2 Tet u(km) u(km) SRC-12-1 SRC-12-5 Fig. 7 oment-axial load elation
9 The expeimental ultimate flexual moment obtained by tet eult ae compaed with the tength calculated by AIJ deign fomula (See Table 5). AIJ deign fomula etimate the tet eult conevatively and eaonably. Becaue the atio of tet eult to AIJ tength i (L/D=6) and (L/D=12). Table 5. Compaion between meaued tength and AIJ tength ex AX AIJ p ex AX / AIJ (k) (km) (km) (km) SRC L/D=6 SRC SRC L/D=12 SRC : applied axial load, AIJ : calculated ultimate flexual tength, p : fully platic moment ex AX : maximum expeimental tength ( ex Q AX L/4, ex Q AX : maximum meaued tength ) 4. Limit toy dift angle Some of the limit toy dift angle (R AX,R 95, R 9 ) ae hown in Fig.9 and Table 6. They ae defined a hown in Fig.8. i.e. R AX i the toy dift angle at the maximum tength. R 95 and R 9 ae one at 95% and 9% tength afte peak tength, epectively. Datic deceae of the tength i obeved afte peak tength in all pecimen. Theefoe, thee ae few diffeence between R AX and R 9 (See Fig.9). In all the pecimen, the tength deceae moe than 1% of the maximum tength at the next cycle afte eaching maximum tength. Q AX Q 95 Q 9 Q(k) R AX R 95 R 9 Fig. 8 Definition of limit toy dift angle Table 6. Limit toy dift angle.4 R AX R 9 exq AX R AX R 95 R 9 (k) (ad.) (ad.) (ad.) SRC SRC SRC SRC Ru(ad.) SRC-6-1 SRC-12-1 SRC-6-5 SRC-12-5 Fig. 9 Limit toy dift angle
10 5. Equivalent vicou damping atio The loop dawn by the hyteei chaacteitic of tuctue bea impotant ole of the damping pefomance. The equivalent vicou damping atio h eq i defined by Equation 3 and epeent the damping pefomance at each loop (See Fig.1). 1 W h = eq 4π We whee W: aea of one cycle W e : equivalent potential enegy = 1 2 k e a 2 Fig.11 how the tanition of the equivalent vicou damping atio at R=.1 to.2. The equivalent vicou damping atio of all the pecimen i between about The H-ection of all the pecimen yielded at final tage (See Fig.5), theefoe it i thought that the damping pefomance doen t inceaed geatly. (3) Q W W e =k e a 2 / SRC-6-1 SRC-6-5 SRC-12-1 SRC a k e a δ heq Fig.1 Definition of equivalent vicou damping atio Fig.11 Tanition of equivalent vicou damping atio COCLSIOS To examine the AIJ deign fomula and to evaluate the defomation capacity of the compoite column, an expeimental wok of SRC fame with weak-axi bending column wa pefomed. Fom eult, it ha become clea that: 1) In all of the pecimen, the table hyteei popetie wee obeved until thei tength eached thei maximum tength. And afte that, the tength of all pecimen deteioated lage than that of the mechanim line. 2) The atio of the meaued tength to the value by AIJ deign fomula wa (L/D=6) and (L/D=12). The AIJ SRC Standad deign fomula wa conevative compaed to the tet eult.
11 3) In all of the pecimen, the equivalent vicou damping atio (R=.1-.2) wa between about.5-.1 and damping pefomance didn t inceaed geatly. 4) The L/D=12 pecimen collaped flexual failue. The collape mechanim of L/D=6 wa hea bond failue that wa diffeent fom that aumed in AIJ deign fomula. REFERECES 1. Achitectual Intitute of Japan. Standad fo Stuctual Calculation of Steel Reinfoced Concete Stuctue, 21.
Thin-Walled Tube Extension by Rigid Curved Punch
Engineeing,, 3, 45-46 doi:.436/eng..355 Publihed Online May (http://www.scirp.og/jounal/eng) Thin-Walled Tube Extenion by Rigid Cuved Punch Abtact Rotilav I. Nepehin Platic Defomation Sytem Depatment,
More informationMATERIAL SPREADING AND COMPACTION IN POWDER-BASED SOLID FREEFORM FABRICATION METHODS: MATHEMATICAL MODELING
MATERIAL SPREADING AND COMPACTION IN POWDER-BASED SOLID FREEFORM FABRICATION METHODS: MATHEMATICAL MODELING Yae Shanjani and Ehan Toyekani Depatment of Mechanical and Mechatonic Engineeing, Univeity of
More informationGravity. David Barwacz 7778 Thornapple Bayou SE, Grand Rapids, MI David Barwacz 12/03/2003
avity David Bawacz 7778 Thonapple Bayou, and Rapid, MI 495 David Bawacz /3/3 http://membe.titon.net/daveb Uing the concept dicued in the peceding pape ( http://membe.titon.net/daveb ), I will now deive
More informationThe Analysis of the Influence of the Independent Suspension on the Comfort for a Mine Truck
16 3 d Intenational Confeence on Vehicle, Mechanical and Electical Engineeing (ICVMEE 16 ISBN: 978-1-6595-37- The Analyi of the Influence of the Independent Supenion on the Comfot fo a Mine Tuck JINGMING
More informationPassive Pressure on Retaining Wall supporting c-φ Backfill using Horizontal Slices Method
Cloud Publication Intenational Jounal of Advanced Civil Engineeing and Achitectue Reeach 2013, Volume 2, Iue 1, pp. 42-52, Aticle ID Tech-106 Reeach Aticle Open Acce Paive Peue on Retaining Wall uppoting
More informationSupplemental Materials. Advanced Thermoelectrics Governed by Single Parabolic Band Model:
Electonic Supplementay Mateial (ESI) fo Phyical Chemity Chemical Phyic. Thi jounal i The Royal Society of Chemity 04 Supplemental Mateial Advanced Themoelectic Govened by Single Paabolic and Model: Mg
More informationSolutions Practice Test PHYS 211 Exam 2
Solution Pactice Tet PHYS 11 Exam 1A We can plit thi poblem up into two pat, each one dealing with a epaate axi. Fo both the x- and y- axe, we have two foce (one given, one unknown) and we get the following
More informationNew Analysis for The FGM Thick Cylinders Under Combined Pressure and Temperature Loading
Ameican Jounal of Applied Science 5 (7): 85-859, 008 ISSN 546-939 008 Science Publication New Analyi fo The FGM Thick Cylinde Unde Combined Peue and Tempeatue Loading K. Abinia, H. Naee, F. Sadeghi and
More informationTheory. Single Soil Layer. ProShake User s Manual
PoShake Ue Manual Theoy PoShake ue a fequency domain appoach to olve the gound epone poblem. In imple tem, the input motion i epeented a the um of a eie of ine wave of diffeent amplitude, fequencie, and
More informationFracture criterion developed for elastic-plastic Russian materials
ndian Jounal of Engineeing & Mateial Science Vol. 1, Octobe 005, pp. 51-55 Factue citeion developed fo elatic-platic Ruian mateial A Ziliuka Depatment of Mechanic of Solid, Kauna Univeity of Technology,
More informationRE 7.a. RE 7.b Energy Dissipation & Resonance RE 7.c EP7, HW7: Ch 7 Pr s 31, 32, 45, 62 & CP
Wed. Lab Fi. Mon. Tue. 7.-.4 Macocopic Enegy Quiz 6 4pm, hee Math & Phy Reeach L6 Wok and Enegy 7.5-.9 Enegy Tanfe RE 7.a RE 7.b 7.0-. Enegy Diipation & Reonance RE 7.c EP7, HW7: Ch 7 P 3, 3, 45, 6 & CP
More informationTitle. Author(s)Y. IMAI; T. TSUJII; S. MOROOKA; K. NOMURA. Issue Date Doc URL. Type. Note. File Information
Title CALCULATION FORULAS OF DESIGN BENDING OENTS ON TH APPLICATION OF THE SAFETY-ARGIN FRO RC STANDARD TO Autho(s)Y. IAI; T. TSUJII; S. OROOKA; K. NOURA Issue Date 013-09-1 Doc URL http://hdl.handle.net/115/538
More informationPrecision Spectrophotometry
Peciion Spectophotomety Pupoe The pinciple of peciion pectophotomety ae illutated in thi expeiment by the detemination of chomium (III). ppaatu Spectophotomete (B&L Spec 20 D) Cuvette (minimum 2) Pipet:
More informationInference for A One Way Factorial Experiment. By Ed Stanek and Elaine Puleo
Infeence fo A One Way Factoial Expeiment By Ed Stanek and Elaine Puleo. Intoduction We develop etimating equation fo Facto Level mean in a completely andomized one way factoial expeiment. Thi development
More informationSee the solution to Prob Ans. Since. (2E t + 2E c )ch - a. (s max ) t. (s max ) c = 2E c. 2E c. (s max ) c = 3M bh 2E t + 2E c. 2E t. h c.
*6 108. The beam has a ectangula coss section and is subjected to a bending moment. f the mateial fom which it is made has a diffeent modulus of elasticity fo tension and compession as shown, detemine
More informationMECHANICAL ANALYSIS OF REINFORCED PLATE STRUCTURES
Budapet 9-30Ma 008 MECHANICA ANAYSIS OF REINFORCED PATE STRUCTURES Gábo M Vöö Depatment of Applied Mechanic Budapet Univeit of Technolog and Economic H-151 Budapet Hunga E-mail: voo@mmbmehu Abtact: The
More informationone primary direction in which heat transfers (generally the smallest dimension) simple model good representation for solving engineering problems
CHAPTER 3: One-Dimenional Steady-State Conduction one pimay diection in which heat tanfe (geneally the mallet dimenion) imple model good epeentation fo olving engineeing poblem 3. Plane Wall 3.. hot fluid
More informationShrinkage Estimation of Reliability Function for Some Lifetime Distributions
Ameican Jounal of Computational and Applied Mathematic 4, 4(3): 9-96 DOI:.593/j.ajcam.443.4 Shinkage Etimation of eliability Function fo Some Lifetime Ditibution anjita Pandey Depatment of Statitic, niveity
More informationTRAVELING WAVES. Chapter Simple Wave Motion. Waves in which the disturbance is parallel to the direction of propagation are called the
Chapte 15 RAVELING WAVES 15.1 Simple Wave Motion Wave in which the ditubance i pependicula to the diection of popagation ae called the tanvee wave. Wave in which the ditubance i paallel to the diection
More informationASTR 3740 Relativity & Cosmology Spring Answers to Problem Set 4.
ASTR 3740 Relativity & Comology Sping 019. Anwe to Poblem Set 4. 1. Tajectoie of paticle in the Schwazchild geomety The equation of motion fo a maive paticle feely falling in the Schwazchild geomety ae
More informationChapter 19 Webassign Help Problems
Chapte 9 Webaign Help Poblem 4 5 6 7 8 9 0 Poblem 4: The pictue fo thi poblem i a bit mileading. They eally jut give you the pictue fo Pat b. So let fix that. Hee i the pictue fo Pat (a): Pat (a) imply
More informationRotational Kinetic Energy
Add Impotant Rotational Kinetic Enegy Page: 353 NGSS Standad: N/A Rotational Kinetic Enegy MA Cuiculum Famewok (006):.1,.,.3 AP Phyic 1 Leaning Objective: N/A, but olling poblem have appeaed on peviou
More informationStatic Electric Fields. Coulomb s Law Ε = 4πε. Gauss s Law. Electric Potential. Electrical Properties of Materials. Dielectrics. Capacitance E.
Coulomb Law Ε Gau Law Electic Potential E Electical Popetie of Mateial Conducto J σe ielectic Capacitance Rˆ V q 4πε R ρ v 2 Static Electic Field εe E.1 Intoduction Example: Electic field due to a chage
More informationAIRCRAFT ENGINE RESPONSE DUE TO FAN UNBALANCE AND TO THE PRESENCE OF CONSUMED GAPS IN THE ENGINE DURING THE PHASE OF WINDMILLING
ICAS CONGRESS AIRCRAF ENGINE RESPONSE DUE O FAN UNBALANCE AND O HE PRESENCE OF CONSUMED GAPS IN HE ENGINE DURING HE PHASE OF WINDMILLING B. Benay AEROSPAIALE MARA AIRBUS 316 ouloue Cedex 3 Fance Abtact
More informationCurrent Balance Warm Up
PHYSICS EXPERIMENTS 133 Cuent Balance-1 Cuent Balance Wam Up 1. Foce between cuent-caying wies Wie 1 has a length L (whee L is "long") and caies a cuent I 0. What is the magnitude of the magnetic field
More informationSimulation of Spatially Correlated Large-Scale Parameters and Obtaining Model Parameters from Measurements
Simulation of Spatially Coelated Lage-Scale Paamete and Obtaining Model Paamete fom PER ZETTERBERG Stockholm Septembe 8 TRITA EE 8:49 Simulation of Spatially Coelated Lage-Scale Paamete and Obtaining Model
More informationPerforation of 5083-H116 Aluminum Armor Plates with Ogive- Nose Rods and 7.62mm APM2 Bullets
Pefoation of 583-H116 Aluminum Amo Plate with Ogive- Noe Rod and 7.62mm APM2 Bullet T. Bøvik M.J. Foetal T.L. Waen Poceeding of the SEM Annual Confeence June 1-4, 29 Albuqueque New Mexico USA 29 Society
More informationSection 25 Describing Rotational Motion
Section 25 Decibing Rotational Motion What do object do and wh do the do it? We have a ve thoough eplanation in tem of kinematic, foce, eneg and momentum. Thi include Newton thee law of motion and two
More informationGeneral. Eqn. 1. where, F b-bbf = Allowable bending stress at the bottom of the beam bottom flange, ksi.
COMPUERS AND SRUCURES, INC., BERKELEY, CALIORNIA DECEMBER 2001 COMPOSIE BEAM DESIGN AISC-ASD89 echnical Note Allowale Bending Stesses Geneal his echnical Note descies how the pogam detemines the allowale
More informationFormula Formula symbols Units. s = F A. e = x L. E = s ε. k = F δ. G = t γ. e = at. maximum load original cross sectional area. s M E = = N/m.
A Lit of foulae fo ecanical engineeing pinciple Foula Foula ybol Unit Ste Stain applied foce co ectionalaea cange in lengt oiginal lengt F A e x L Young odulu of elaticity te tain Stiffne foce extenion
More information5. Pressure Vessels and
5. Pessue Vessels and Axial Loading Applications 5.1 Intoduction Mechanics of mateials appoach (analysis) - analyze eal stuctual elements as idealized models subjected simplified loadings and estaints.
More informationTHE INFLUENCE OF THE ROTOR ARCHITECTURE OF A ROTATING WORKING MACHINE ON THE DRIVING POWER
U.P.B. Sci. Bull., Seie D, Vol. 77, I. 1, 015 ISSN 1454-358 THE INFLUENCE OF THE ROTOR ARCHITECTURE OF A ROTATING WORKING MACHINE ON THE DRIVING POWER Antonio DETZORTZIS 1, Nicolae BĂRAN, Malik N. HAWAS
More informationModule 7. Limit State of Serviceability. Version 2 CE IIT, Kharagpur
Module 7 Limit State of Seviceability Lesson 17 Limit State of Seviceability nstuction Objectives: At the end of this lesson, the student should be able to: explain the need to check fo the limit state
More informationThe Deformation Analysis of the Curved Box Girder Bridges under Different Radius
The Defomation Analsis of the Cuved Bo Gide Bidges unde Diffeent Radius Liu Fangping (Coesponding autho) School of Civil Engineeing & Achitectue, Chongqing Jiao tong Univesit 66 Xuefu Road, Nan an Distict,
More informationLINEAR AND NONLINEAR ANALYSES OF A WIND-TUNNEL BALANCE
LINEAR AND NONLINEAR ANALYSES O A WIND-TUNNEL INTRODUCTION BALANCE R. Kakehabadi and R. D. Rhew NASA LaRC, Hampton, VA The NASA Langley Reseach Cente (LaRC) has been designing stain-gauge balances fo utilization
More informationDESIGN OF BEAMS FOR MOMENTS
CHAPTER Stuctual Steel Design RFD ethod Thid Edition DESIGN OF BEAS FOR OENTS A. J. Clak School of Engineeing Deatment of Civil and Envionmental Engineeing Pat II Stuctual Steel Design and Analysis 9 FA
More informationBENDING OF BEAM. Compressed layer. Elongated. layer. Un-strained. layer. NA= Neutral Axis. Compression. Unchanged. Elongation. Two Dimensional View
BNDING OF BA Compessed laye N Compession longation Un-stained laye Unchanged longated laye NA Neutal Axis Two Dimensional View A When a beam is loaded unde pue moment, it can be shown that the beam will
More informationEddy Currents in Permanent Magnets of a Multi-pole Direct Drive Motor
Acta Technica Jauineni Vol. 6. No. 1. 2013 Eddy Cuent in Pemanent Magnet of a Multi-pole Diect Dive Moto G. Gotovac 1, G. Lampic 1, D. Miljavec 2 Elaphe Ltd. 1, Univeity of Ljubljana, Faculty of Electical
More information7.2.1 Basic relations for Torsion of Circular Members
Section 7. 7. osion In this section, the geomety to be consideed is that of a long slende cicula ba and the load is one which twists the ba. Such poblems ae impotant in the analysis of twisting components,
More informationAbove Flux Estimation Issues in Induction Generators with Application at Energy Conversion Systems
Acta Polytechnica Hungaica Vol. 3, No. 3, 2006 Above Flux Etimation Iue in Induction Geneato with Application at Enegy Conveion Sytem Ioif Szeidet, Octavian Potean, Ioan Filip, Vaa Citian Depatment of
More informationIncreasing the Strength of Standard Involute Gear Teeth with Novel Circular Root Fillet Design
Ameican Jounal of Applied Science 2 (6): 1058-1064, 2005 ISSN 1546-9239 Science Publication, 2005 Inceaing the Stength of Standad Involute Gea Teeth with Novel Cicula Root Fillet Deign V. Spita, Th. Cotopoulo
More informationConsiderations Regarding the Flux Estimation in Induction Generator with Application at the Control of Unconventional Energetic Conversion Systems
Conideation Regading the Flux Etimation in Induction Geneato with Application at the Contol of Unconventional Enegetic Conveion Sytem Ioif Szeidet, Octavian Potean, Ioan Filip, Vaa Citian Depatment of
More informationAP Physics Electric Potential Energy
AP Physics lectic Potential negy Review of some vital peviously coveed mateial. The impotance of the ealie concepts will be made clea as we poceed. Wok takes place when a foce acts ove a distance. W F
More informationA PHENOMENOLOGICAL DESCRIPTION OF MIXING- SEGREGATION EFFECTS DURING SHEAR
A PHENOMENOLOGICAL DESCRIPTION OF MIXING-SEGREGATION EFFECTS DURING SHEAR DEFORMATION OF PARTICULATE SOLIDS Poceeding of Euopean Conge of Chemical Engineeing (ECCE-6) Copenhagen, 6- Septembe 7 A PHENOMENOLOGICAL
More informationLECTURE 14. m 1 m 2 b) Based on the second law of Newton Figure 1 similarly F21 m2 c) Based on the third law of Newton F 12
CTU 4 ] NWTON W O GVITY -The gavity law i foulated fo two point paticle with ae and at a ditance between the. Hee ae the fou tep that bing to univeal law of gavitation dicoveed by NWTON. a Baed on expeiental
More informationTheorem 2: Proof: Note 1: Proof: Note 2:
A New 3-Dimenional Polynomial Intepolation Method: An Algoithmic Appoach Amitava Chattejee* and Rupak Bhattachayya** A new 3-dimenional intepolation method i intoduced in thi pape. Coeponding to the method
More informationObjectives: After finishing this unit you should be able to:
lectic Field 7 Objectives: Afte finishing this unit you should be able to: Define the electic field and explain what detemines its magnitude and diection. Wite and apply fomulas fo the electic field intensity
More informationTHROUGHPUT OF LARGE WIRELESS NETWORKS ON SQUARE, HEXAGONAL AND TRIANGULAR GRIDS. Kezhu Hong, Yingbo Hua
THROUGHPUT OF LARGE WIRELESS NETWORKS ON SQUARE, HEAGONAL AND TRIANGULAR GRIDS Kezhu Hong, Yingbo Hua Dept. of Electical Engineeing Univeity of Califonia Riveide, CA 9252 {khong,yhua}@ee.uc.edu ABSTRACT
More informationAnalysis of high speed machining center spindle dynamic unit structure performance Yuan guowei
Intenational Confeence on Intelligent Systems Reseach and Mechatonics Engineeing (ISRME 0) Analysis of high speed machining cente spindle dynamic unit stuctue pefomance Yuan guowei Liaoning jidian polytechnic,dan
More information06 - ROTATIONAL MOTION Page 1 ( Answers at the end of all questions )
06 - ROTATIONAL MOTION Page ) A body A of mass M while falling vetically downwads unde gavity beaks into two pats, a body B of mass ( / ) M and a body C of mass ( / ) M. The cente of mass of bodies B and
More informationγ from B D(Kπ)K and B D(KX)K, X=3π or ππ 0
fom and X, X= o 0 Jim Libby, Andew Powell and Guy Wilkinon Univeity of Oxfod 8th Januay 007 Gamma meeting 1 Outline The AS technique to meaue Uing o 0 : intoducing the coheence facto Meauing the coheence
More informationPhysics 2A Chapter 10 - Moment of Inertia Fall 2018
Physics Chapte 0 - oment of netia Fall 08 The moment of inetia of a otating object is a measue of its otational inetia in the same way that the mass of an object is a measue of its inetia fo linea motion.
More informationEFFECTS OF GFRP REINFORCING REBARS ON SHRINKAGE AND THERMAL STRESSES IN CONCRETE
EFFECTS OF GFRP REINFORCING REBARS ON SHRINKAGE AND THERMAL STRESSES IN CONCRETE Roge H. L. Chen 1 and Jeong-Hoon Choi 2 ABSTRACT The use of Glass Fibe Reinfoced Polyme (GFRP) ebas instead of conventional
More informationNatural Frequency Analysis of Composite Skew Plates with Embedded Shape Memory Alloys in Thermal Environment
AUT Jounal of Mechanical ngineeing AUT J. Mech. ng., ( (7 79-9 DOI:.6/mej.7.655.5389 atual Fequenc Anali of Compoite kew Plate with mbedded hape Memo Allo in Themal nvionment. Kamaian, M. hakei * Depatment
More informationPiezoceramics-based Devices for Active Balancing of Flexible Shafts
Piezoceamic-baed Device fo Active Balancing of Flexible Shaft P. J. Sloetje, A. de Boe Univeity of Twente, Faculty of Engineeing Technology, Applied Mechanic Section Dienelolaan 5, 7500 AE, Enchede, The
More informationPrediction of acoustic foam properties by numerical simulation of polyurethane foaming process
Pediction of acoutic foam popetie by numeical imulation of polyuethane foaming poce Hichem Abdealam, Bouad Abbè,a, Yuming Li, Ying-Qiao Guo, Elvi Kwai and Jean-Luc Romain Univeité de Reim Champagne-Adenne,
More informationFI 2201 Electromagnetism
FI Electomagnetim Aleande A. Ikanda, Ph.D. Phyic of Magnetim and Photonic Reeach Goup ecto Analyi CURILINEAR COORDINAES, DIRAC DELA FUNCION AND HEORY OF ECOR FIELDS Cuvilinea Coodinate Sytem Cateian coodinate:
More informationMAGNETIC FIELD INTRODUCTION
MAGNETIC FIELD INTRODUCTION It was found when a magnet suspended fom its cente, it tends to line itself up in a noth-south diection (the compass needle). The noth end is called the Noth Pole (N-pole),
More informationDetermining the Best Linear Unbiased Predictor of PSU Means with the Data. included with the Random Variables. Ed Stanek
Detemining te Bet Linea Unbiaed Pedicto of PSU ean wit te Data included wit te andom Vaiable Ed Stanek Intoduction We develop te equation fo te bet linea unbiaed pedicto of PSU mean in a two tage andom
More informationTest 2 phy a) How is the velocity of a particle defined? b) What is an inertial reference frame? c) Describe friction.
Tet phy 40 1. a) How i the velocity of a paticle defined? b) What i an inetial efeence fae? c) Decibe fiction. phyic dealt otly with falling bodie. d) Copae the acceleation of a paticle in efeence fae
More informationHonors Classical Physics I
Hono Claical Phyic I PHY141 Lectue 9 Newton Law of Gavity Pleae et you Clicke Channel to 1 9/15/014 Lectue 9 1 Newton Law of Gavity Gavitational attaction i the foce that act between object that have a
More informationSafety variations in steel designed using Eurocode 3
JCSS Wokshop on eliability Based Code Calibation Safety vaiations in steel designed using Euocode 3 Mike Byfield Canfield Univesity Swindon, SN6 8LA, UK David Nethecot Impeial College London SW7 2BU, UK
More informationGeometry Contest 2013
eomety ontet 013 1. One pizza ha a diamete twice the diamete of a malle pizza. What i the atio of the aea of the lage pizza to the aea of the malle pizza? ) to 1 ) to 1 ) to 1 ) 1 to ) to 1. In ectangle
More informationWater flows through the voids in a soil which are interconnected. This flow may be called seepage, since the velocities are very small.
Wate movement Wate flows though the voids in a soil which ae inteconnected. This flow may be called seepage, since the velocities ae vey small. Wate flows fom a highe enegy to a lowe enegy and behaves
More informationImpulse and Momentum
Impule and Momentum 1. A ca poee 20,000 unit of momentum. What would be the ca' new momentum if... A. it elocity wee doubled. B. it elocity wee tipled. C. it ma wee doubled (by adding moe paenge and a
More informationComputational Methods of Solid Mechanics. Project report
Computational Methods of Solid Mechanics Poject epot Due on Dec. 6, 25 Pof. Allan F. Bowe Weilin Deng Simulation of adhesive contact with molecula potential Poject desciption In the poject, we will investigate
More informationRigid Body Dynamics 2. CSE169: Computer Animation Instructor: Steve Rotenberg UCSD, Winter 2018
Rigid Body Dynamics 2 CSE169: Compute Animation nstucto: Steve Rotenbeg UCSD, Winte 2018 Coss Poduct & Hat Opeato Deivative of a Rotating Vecto Let s say that vecto is otating aound the oigin, maintaining
More information6.1: Angles and Their Measure
6.1: Angles and Thei Measue Radian Measue Def: An angle that has its vetex at the cente of a cicle and intecepts an ac on the cicle equal in length to the adius of the cicle has a measue of one adian.
More informationUsing DEA and AHP for Multiplicative Aggregation of Hierarchical Indicators
Ameican Jounal of Opeation Reeach, 205, 5, 327-336 Publihed Online Septembe 205 in SciRe. http://www.cip.og/jounal/ajo http://dx.doi.og/0.4236/ajo.205.55026 Uing DEA and AHP fo Multiplicative Aggegation
More informationElectrostatics (Electric Charges and Field) #2 2010
Electic Field: The concept of electic field explains the action at a distance foce between two chaged paticles. Evey chage poduces a field aound it so that any othe chaged paticle expeiences a foce when
More informationMaterials selection The materials index
MME445: Lectue 20 Mateials selection The mateials index A. K. M. B. Rashid Pofesso, Depatment of MME BUET, Dhaka Leaning Objectives Knowledge & Undestanding Elementay knowledge of how to expess design
More informationMotithang Higher Secondary School Thimphu Thromde Mid Term Examination 2016 Subject: Mathematics Full Marks: 100
Motithang Highe Seconday School Thimphu Thomde Mid Tem Examination 016 Subject: Mathematics Full Maks: 100 Class: IX Witing Time: 3 Hous Read the following instuctions caefully In this pape, thee ae thee
More informationINFLUENCE OF DESIGN DATA OF INDUCTION MOTOR ON EFFECTS OF CAGE ASYMMETRY
Pace Nauowe Intytutu Mazyn, Naędów i Pomiaów Eletycznych N 66 Politechnii Wocławiej N 66 Studia i Mateiały N 3 1 Alejando FERNANDEZ GOMEZ* Tadeuz J. SOBCZYK* induction moto, oto cage aymmety, cage moto
More information修士論文 シリコン中における 転位の交差すべり挙動解析 p.1 60 完 平成 20 年 2 月 8 日 提出 指導教員 酒井 信介 教授 杉本 有正
p.1 60 20 2 8 66211 6 1.1 6 1.2 8 1.3 10 1.4 11 12 2.1 12 2.2 13 2.2.1 14 2.2.2 17 2.2.3 18 2.3 20 2.3.1 20 2.3.2 21 23 3.1 23 3.1.1 23 3.1.2 24 3.1.3 25 3.1.5 26 3.2 STI 27 3.2.1 27 3.2.2 29 3.2.2.1 29
More informationContent 5.1 Angular displacement and angular velocity 5.2 Centripetal acceleration 5.3 Centripetal force. 5. Circular motion.
5. Cicula otion By Liew Sau oh Content 5.1 Angula diplaceent and angula elocity 5. Centipetal acceleation 5.3 Centipetal foce Objectie a) expe angula diplaceent in adian b) define angula elocity and peiod
More informationCOMPLEX MODE SUPERPOSITION METHOD CONSIDERING THE EFFECT OF MULTIPLE FOLD EIGENVALUE IN SEISMIC DESIGN
The 4 th Wold Confeence on Eathquae Engineeing Octobe -7, 008, Being, China COMPLEX MODE SUPERPOSITION METHOD CONSIDERING THE EFFECT OF MULTIPLE FOLD EIGENVALUE IN SEISMIC DESIGN Ruifang Yu,, Xiyuan Zhou
More informationGraphs of Sine and Cosine Functions
Gaphs of Sine and Cosine Functions In pevious sections, we defined the tigonometic o cicula functions in tems of the movement of a point aound the cicumfeence of a unit cicle, o the angle fomed by the
More informationNumerical Study on Improving Indoor Thermal Comfort Using a PCM Wall
Numeical Study on Impoving Indoo Themal Comfot Uing a PCM Wall M. Faaji, F. Beoug Abtact A one-dimenional mathematical model wa developed in ode to analyze and optimize the latent heat toage wall. The
More informationCement & Concrete Composites
Cement & Concete Compoite 33 (2011) 171 178 Content lit available at Scienceiect Cement & Concete Compoite jounal homepage: www.elevie.com/locate/cemconcomp Vicoelatic popetie dying te extacted fom concete
More informationEstimation and Confidence Intervals: Additional Topics
Chapte 8 Etimation and Confidence Inteval: Additional Topic Thi chapte imply follow the method in Chapte 7 fo foming confidence inteval The text i a bit dioganized hee o hopefully we can implify Etimation:
More informationUnified Design Method for Flexure and Debonding in FRP Retrofitted RC Beams
Unified Deign Method for Flexure and Debonding in FRP Retrofitted RC Beam G.X. Guan, Ph.D. 1 ; and C.J. Burgoyne 2 Abtract Flexural retrofitting of reinforced concrete (RC) beam uing fibre reinforced polymer
More informationCAPACITY OF STIFFENED STEEL SHEAR PANELS AS A STRUCTURAL CONTROL DAMPER
CAPACITY OF STIFFENED STEEL SHEAR PANELS AS A STRUCTURAL CONTROL DAMPER H.B. Ge 1, K. Kaneko and T. Uami 3 1,3 Profeor, Department of Civil Engineering, Meijo Univerity, Nagoya 458-85, Japan Graduate Student,
More informationA FORMULATION AND PRELIMINARY RESULTS FOR SIMULATION OF SHIP MOTIONS COUPLED HEAVE, PITCH AND ROLL
8 th Intenational Confeence on the Stability of Ship and Ocean Vehicle Ecuela Técnica Supeio de Ingenieo Navale A FORMUATION AND PREIMINARY RESUTS FOR SIMUATION OF SHIP MOTIONS COUPED HEAVE, PITCH AND
More informationDetermination of storage lengths of right-turn lanes at signalized. intersections
Detemination of toage length of ight-tun lane at ignalized inteection By Jinghui Wang Lei Yu Hui Xu ABSTRACT Thi pape develop an analytical method of detemining toage length of ight-tun lane at ignalized
More informationA Generalized Two Axes Model of a Squirrel-Cage Induction Motor for Rotor Fault Diagnosis
SEBIAN JOUNAL OF ELECTICAL ENGINEEING Vol. 5, No. 1, ay 2008, 155-170 A Genealized Two Axe odel of a Squiel-Cage Induction oto fo oto Fault Diagnoi Sami Hamdani 1, Oma Touhami 2, achid Ibtiouen 2 Abtact:
More information1. Show that the volume of the solid shown can be represented by the polynomial 6x x.
7.3 Dividing Polynomials by Monomials Focus on Afte this lesson, you will be able to divide a polynomial by a monomial Mateials algeba tiles When you ae buying a fish tank, the size of the tank depends
More informationSTUDY ON 2-D SHOCK WAVE PRESSURE MODEL IN MICRO SCALE LASER SHOCK PEENING
Study Rev. Adv. on -D Mate. shock Sci. wave 33 (13) pessue 111-118 model in mico scale lase shock peening 111 STUDY ON -D SHOCK WAVE PRESSURE MODEL IN MICRO SCALE LASER SHOCK PEENING Y.J. Fan 1, J.Z. Zhou,
More informationBasic propositional and. The fundamentals of deduction
Baic ooitional and edicate logic The fundamental of deduction 1 Logic and it alication Logic i the tudy of the atten of deduction Logic lay two main ole in comutation: Modeling : logical entence ae the
More informationFall 2016 Semester METR 3113 Atmospheric Dynamics I: Introduction to Atmospheric Kinematics and Dynamics
Fall 06 Semeste METR 33 Atmospheic Dynamics I: Intoduction to Atmospheic Kinematics Dynamics Lectue 7 Octobe 3 06 Topics: Scale analysis of the equations of hoizontal motion Geostophic appoximation eostophic
More informationCHAPTER 3 CLASSICAL CONTROL TECHNIQUES FOR AC DRIVES
44 CHAPTER 3 CLASSICAL CONTROL TECHNIQUES FOR AC DRIVES 3.1 INTRODUCTION The contolle equied fo AC dive can be divided into two majo type: cala contol and vecto contol (Boe 1976). In cala contol, which
More informationTHE PREDICTION OF ELASTIC-PLASTIC STATE OF THE SOIL MASS NEAR THE TUNNEL WITH TAKING INTO ACCOUNT ITS STRENGTH ANISOTROPY
Intenational Jounal of Civil Engineeing and Technology (IJCIET) Volume 8, Iue 11, Novembe 017, pp. 68-694, Aticle ID: IJCIET_08_11_071 Available online at http://www.iaeme.com/ijciet/iue.ap?jtypeijciet&vtype8&itype11
More informationG 3. AN ELECTRONIC JOURNAL OF THE EARTH SCIENCES Published by AGU and the Geochemical Society
Geoytem G 3 AN ELECTRONIC JOURNAL OF THE EARTH SCIENCES Publihed by AGU and the Geochemical Society Aticle Volume 7, Numbe 8 22 Augut 26 Q812, doi:1.129/25gc1187 ISSN: 1525-227 Real contact and evolution
More informationCHAPTER 25 ELECTRIC POTENTIAL
CHPTE 5 ELECTIC POTENTIL Potential Diffeence and Electic Potential Conside a chaged paticle of chage in a egion of an electic field E. This filed exets an electic foce on the paticle given by F=E. When
More informationGauss Law. Physics 231 Lecture 2-1
Gauss Law Physics 31 Lectue -1 lectic Field Lines The numbe of field lines, also known as lines of foce, ae elated to stength of the electic field Moe appopiately it is the numbe of field lines cossing
More information7.2. Coulomb s Law. The Electric Force
Coulomb s aw Recall that chaged objects attact some objects and epel othes at a distance, without making any contact with those objects Electic foce,, o the foce acting between two chaged objects, is somewhat
More information( ) rad ( 2.0 s) = 168 rad
.) α 0.450 ω o 0 and ω 8.00 ω αt + ω o o t ω ω o α HO 9 Solution 8.00 0 0.450 7.8 b.) ω ω o + αδθ o Δθ ω 8.00 0 ω o α 0.450 7. o Δθ 7. ev.3 ev π.) ω o.50, α 0.300, Δθ 3.50 ev π 7π ev ω ω o + αδθ o ω ω
More informationConservation of Angular Momentum
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 0 1 1 1 1 1 1 1 Consevation of Angula Momentum Pupose: To investigate consevation of angula momentum by diectly measuing the moment of inetia and angula velocities
More informationA Neural Network for the Travelling Salesman Problem with a Well Behaved Energy Function
A Neual Netwok fo the Tavelling Saleman Poblem with a Well Behaved Enegy Function Maco Budinich and Babaa Roaio Dipatimento di Fiica & INFN, Via Valeio, 347 Tiete, Italy E-mail: mbh@tiete.infn.it (Contibuted
More information(Sample 3) Exam 1 - Physics Patel SPRING 1998 FORM CODE - A (solution key at end of exam)
(Sample 3) Exam 1 - Physics 202 - Patel SPRING 1998 FORM CODE - A (solution key at end of exam) Be sue to fill in you student numbe and FORM lette (A, B, C) on you answe sheet. If you foget to include
More information17.1 Electric Potential Energy. Equipotential Lines. PE = energy associated with an arrangement of objects that exert forces on each other
Electic Potential Enegy, PE Units: Joules Electic Potential, Units: olts 17.1 Electic Potential Enegy Electic foce is a consevative foce and so we can assign an electic potential enegy (PE) to the system
More information