Study on Force Characteristics of Buried Pipeline Under Impact Load Caused by Bridge Pile Foundation Construction
|
|
- Wilfrid Bishop
- 5 years ago
- Views:
Transcription
1 American Journal of Mechanics and Alications 018; 6(): 6-67 htt:// doi: /j.ajma ISSN: (Print); ISSN: (Online) Study on Force Characteristics of Buried Pieline Under Imact Load Caused by Bridge Pile Foundation Construction She Yanhua School of Urban Construction, Yangtze University, Jingzhou, China address: To cite this article: She Yanhua. Study on Force Characteristics of Buried Pieline Under Imact Load Caused by Bridge Pile Foundation Construction. American Journal of Mechanics and Alications. Vol. 6, No., 018, doi: /j.ajma eceived: August 8, 018; Acceted: Setember 18, 018; Published: October 18, 018 Abstract: In the ile foundation construction of highway bridge, the imact hammer falls from a certain height, which roduces a great imact when it collides with soil. In order to gain a clear idea of force characteristics of buried ieline under imact load caused by bridge ile foundation construction, the effect of construction imacting load on buried ieline is analyzed theoretically. Firstly, taking advantage of Boussinesq solution and Mindlin solution, the distribution of additional load on the surface of ieline under imact load is analyzed, and the transmission and diffusion of imact force in soil are calculated by elastic half-sace theory. Secondly, the mechanical models of buried ieline under surface imacting and ile hole imacting are established resectively. Combined with Boussinesq equation, Mindlin calculation and infinite beam elastic foundation model, the calculation formula of buried ieline under imact load is obtained. Finally, according to the formula established above, an examle is given to calculate the additional bending moments and axial tension and comression stresses of buried ieline caused by bridge ile foundation construction, so as to estimate the effect of construction imacting load on buried ieline. The research results rovide some guidance for the stress analysis of buried ielines under such construction conditions. Keywords: Buried Pieline, Imacting Load, Pile Foundation Construction, Calculation Formula 1. Introduction In highway construction, scholars ut extra emhasis on the dynamic loads of buried ielines, such as the ramming loads [1], rolling stone imact loads [, 3], traffic loads [4, 5], blasting vibration loads [6, 7], which have been carried out on the effect of buried ielines and many achievements have been made. However, the effect of imact load caused by bridge unching ile construction on adjacent buried ielines is seldom studied, while it is very imortant to understand the influence of this kind of imact load ut on the buried ieline in ractical engineering. Therefore, the force characteristics of buried ieline under imact load caused by bridge ile foundation construction are studied. In the bridge ile foundation unching construction, the hammer will fall from a certain height. When colliding with soil mass, the larger imact is roduced. The influence of imact load on buried ieline is through the transfer of soil around the ie and the interaction between ie and soil, and finally acts on the ieline in the form of soil ressure. In the analysis of mechanical roerties of buried ieline, it is assumed that the ie is an infinitely long structure, only considering the joint action of the imact load and the soil ressure around the ie, and ignoring the influence of internal ressure, construction defects, chemical corrosion, temerature changes and other ancillary structures on the buried ieline.. Surface Additional Load Distribution of Buried Pieline The imact load has a strong instantaneous imacting force on the soil around the ieline, resulting in additional loads on the ieline. In the analysis of the additional load distribution on the ie surface, the elastic half sace theory is used to calculate the imacting force transmission and
2 American Journal of Mechanics and Alications 018; 6(): diffusion in the soil. Assuming that the soil is the uniform linear elastic infinite body, when a vertical concentrated force is acted on the surface of an elastic half sace, the elastic solution of the stress and dislacement caused by any oint in the elastic half sace is made by Boussinesq. As shown in Figure 1, the various stress comonents at any oint in the half sace are as follows[8, 9]: τ xy 3 3P z 3P 3 σz = cos θ 5 π = π (3) ( + ) ( + ) 3P xyz 1 ν xy z = τyx = 5 3 π 3 z (4) 3P yz 3Py τ yz = τzy = cos θ 5 3 π = π (5) 3P xz 3Px τzx = τxz = cos θ 5 3 π = π (6) In the above formula: Distance from ointm to oint O, = x + y + z = r + z = z cosθ, Figure 1. Force schematic diagram of arbitrary oint in the elastic semi-sace. 3P x z 1 ν z z x σx = + π 3 ( + z) + z ( + z) ( ) P y z 1 ν z z y σ y = + π 3 ( + z) + z ( + z) ( ) (1) () r The horizontal distance between the oint M and the oint of concentrated force acting, θ The angle between the line and the axis of the z coordinate, E Elastic modulus of foundation, v Poisson ratio of foundation. When the load of the surface action is distributed load, the Boussinesq solution can be used to calculate the stress and dislacement of the distribution load on the arbitrary oint in the elastic half sace by the integral of the load distribution surface. Assuming a rectangular uniform load on the foundation, the coordinates of the load center are ( x, y, z ) and the border length are resectivelyland b. Figure. Schematic diagram of ie force analysis.
3 64 She Yanhua: Study on Force Characteristics of Buried Pieline Under Imact Load Caused by Bridge Pile Foundation Construction As shown in Figure, the direction of the ie length is x axis, the direction of the width is y axis, and the vertical direction is z axis (vertical downward direction is ositive). The left end oint of the ie calculation section is the coordinate origin, and the coordinates of any oint on the ie are ( M,0,0 ). Then according to the above formula and coordinate transformation, the exression of vertical and horizontal additional loads on the surface ieline can be obtained as follows: q z 3z 3 y + 0.5b x + 0.5l π y 0.5b x 0.5l dxdy 5 = (7) q y y + 0.5b x + 0.5l y z z y + z ν 3 π z ( ) y 0.5b x 0.5l z ( ) = + (1 )[ ] dxdz In the formula (7) and (8), = ( x M) + y + z (8) The dislacements and stresses caused by horizontal concentrated forces acting on the interior of a semi-infinite body are roosed by Mindlin. The calculation model is shown in Figure 3. The horizontal stress exression at any oint in the half-sace caused by the force P along the x-axis (arallel to the half-sace surface) is as follows[10]: Px 1 µ (1 µ )(5 4 µ ) 3x 3(3 4 µ ) x 4(1 µ )(1 µ ) σx = ( + 8 π (1 µ ) ( + z + h) (3 + + ) 6 5 h µ z h ( + + ) x z h h x z (3 ) + (3 (3 )( + ) + )) z h (9) In the formula (9), µ Poisson's ratio for soil medium, the meaning of other symbols is shown in Figure 3. Figure 4. Mechanical analysis model of ieline under imact loads. The force of the imact on the ieline can be calculated by the Boussinesq equation as follows[11]: 3. Surface Imact Figure 3. Calculation Model of Mindlin. Under the imact of hammer droing, besides the imact on the surface, the stress on the ieline is also the self weight stress of the uer soil, as shown in Figure 4. P 3F = L πh [1 + ( ) ] H.5 In the formula (10): P The load imacted on the ie, (10) F Imact load on the surface, H Overlying layer thickness above ie, L Horizontal distance between imact load oint and the ieline. The force acted on the ie is: P = f P + P (11) s v In the formula (11): P the earth ressure above buried ieline, v
4 American Journal of Mechanics and Alications 018; 6(): f enetration coefficient associated with the ie buried deth[11], as shown in Table1. Table 1. Penetration coefficient ( f ) versus buried deth. buried deth (m) 0~ ~ ~0.9 >0.9 f Imacting in Pile Hole 4.1. Calculation of Soil Pressure Acting on Buried Pie Punching ile construction has great disturbance to strata. With the excavation of the ile hole, the hammer imacting on the soil causes the extrusion ressure around the ile hole wall. This horizontal extrusion ressure can be regarded as an internal force acting on a semi infinite body arallel to the x axis, and the two dimensional calculation model is shown in Figure 5. 6r E P = (14) 1 + u The P value is relaced into the formula (9), and the calculation arameters in formula (9) are as follows: =, = ( L D / ) + 4H, z = H, 1 L D 1 / 1 x = L D 1 /. Then the maximum horizontal earth ressure σmax acting on buried ielines can be obtained. 4.. Pieline Stress Calculation The soil ressure on the buried ieline caused by the unching construction makes the ie stress reach the maximum at the intersection oint of the x and y axis, and with this oint as the center, the ie stress gradually decreases until zero. The ie is extruded and bent under the action of active ressure and roduces tensile and comressive stresses along the axial direction. To determine the magnitude of this stress, it should first determine the buried ieline stress. Suose that under the action P( y ), the reaction force on the buried ieline is q( y ) and the friction between the uer and lower sides of the ieline is f, as shown in Figure 6. Figure 5. Model of unching construction effect on the ieline. It is assumed that the hammer imacting rocess is the rocess of ushing the soil of the same size into the soil layer without drainage. This causes large stress increment around the ile hole wall and it can be analyzed by the small hole exansion theory. The elastic theory and Mohr-Coulomb failure criterion are used to analyze the following results[1]: P = C (1) x In the formula (1), C u the soil undrained strength. The radius of lastic zone around the ile hole wall caused by hammer imacting is: = r In the formula (13): E soil elastic modulus, µ soil Poisson ratio, u E (1 + µ ) C u (13) r The exansion hole radius, taken by the hammer radius. In order to use the above Mindlin calculation model, P x is converted into an equivalent concentrated force (considering 3 times the radius of lastic range ), there is: Figure 6. Force analysis model of ieline. Because the size of buried ieline in the y axis is much larger than that in the x axis, it can be regarded as an infinite beam. If the deformation of the ieline along the y direction is w( x, y ), then there is: 4 d w( x, y) = D( P( y) f q( y)) (15) 4 dy In the formula (15): E Elasticity modulus of ie material, I The moment of inertia of the ie section, π 4 4 I = ( D d ), 64 D The outer diameter, d inner diameter of the ie. Since the distribution of P( y) is about X axisymmetric, it can be assumed to cosine function. If the force acting on the origin is P 0 andais the length unit, then there is:
5 66 She Yanhua: Study on Force Characteristics of Buried Pieline Under Imact Load Caused by Bridge Pile Foundation Construction 0 P 1 P( y) = sin( md / a)cos( my / a) dm (16) π m 0 The formula (16) is substituted (6) to get the bending moment of any section of the ieline, then ( P0 f ) π m 0 d w( x, y) sin( md / a)cos( my / a) M( y) = = ma dm dy + Ω (17) In the formula(17), Ω dimensionless quantity, determined by different foundation models. ka D For the Winkler foundation, Ω =, a D For the Pasternak foundation, Ω = ( m GP + ka ), For the homogeneous isotroic foundation, 3 Esma D Ω =. (1 ν) For simle calculation, the active ressure acting on the buried ieline is equivalent to the concentrated forceq at the origin of coordinates. Then the bending moment of the buried ieline can be obtained as follows[13]: For the Winkler Foundation: Q f β y M( y) = e (cos β y sin β y) (18) 4β In the above formula, β a comrehensive arameter related to the elastic roerties of ie and foundation, kd β = 4. 4 Then the maximum bending moment of the ie section is M max For the two arameter model, there is: M max * In the formula(0), 3 I(1 ν L = ), D 4 Q f = (19) 4β * ( Q f ) L = (0) 4α * 4 S + r Dk( L ) DGP( L ) α =, S =, r =. For homogeneous isotroic foundation model: M = 0.166( Q f ) D 16(1 ν) max 4 EsD * 0.77 (1) When Mmax is known, the tensile and comressive stresses on buried ieline caused by unching ile construction can be calculated as follows: 5. Examle Analysis Mmax 3DMmax σx = = 4 4 W π( D d ) () Taking the imact drilling construction of bridge ile foundation of ong-wu exressway crossing Shaanxi- Beijing gas ieline located Laiyuan as an examle, the ieline stress is analyzed. The diameter of unching hammer is 1.6m, the diameter of ile hole is m, and the horizontal distance between unching osition and ie center is 6m. The buried ieline is a X60 grade steel ie with the buried deth of 3m, outer diameter of 66cm, wall thickness of 8.7mm, and the modulus of 10GPa. The soil layer around the buried ieline is sandy cobble soil, with deformation modulus of 10MPa and Poisson's ratio of According to the above method, the influence of the construction of the unching ile on the buried ieline is estimated. The additional bending moment and the additional axial tension and ressure stress of the buried ieline caused by unching ile construction are calculated as follows: For the Winkler model: M max = 4.63kN m, σ = 1.6MPa. For the double arameter model: M max = 4.4kN m, σ = 1.55MPa. For the homogeneous and isotroic elastic model: M max = 4.1kN m, σ = 1.47MPa. From the above calculation results, it can be seen that the imact of unching ile construction on ieline is not obvious for the steel buried ieline with large tensile stress. 6. Conclusion In this aer, the effect of imacting load caused by bridge ile foundation construction on buried ieline is analyzed theoretically. The distribution of additional load on the surface of ieline under imact load is exounded. Based on the Boussinesq equation, the stress exression of buried ieline under the imact load of the ground surface is established. Based on the Mindlin calculation model and the model of the infinite beam elastic foundation, the calculation formula of the force of the buried ieline under the imact load of the ile hole is established. And the influence of unching ile construction on buried ieline is analyzed by taking a ractical roject as an examle. The research results can be helful for force theoretical analysis of buried ielines. Acknowledgements This work is financially suorted by National Natural Science Foundation of China ( NSFC, ) & Youth Talent Project of Yangtze University (015cqr06).
6 American Journal of Mechanics and Alications 018; 6(): eferences [1] Hang Chuanjun, Zhang Han, Zhang Jie et al., Journal of Safety Science and Technology, vol. 11, 015, [] Zhang Jie, Liang Zheng, Hang Chuanjun et al., Journal of Safety Science and Technology, vol. 7, 015, [3] Xiong Jian, Deng Qinglu, Zhang Hongliang et al., Safety and Environmental Engineering, vol. 0, 013, [4] Yang Guiling, Liu Kai, Wang Ming et al., Safety and Environmental Engineering, vol. 4, 017, [5] Li Xinliang, Li Suzhen, Shen Yong-gang, Journal of Zhejiang University (Engineering Science Edition), vol. 48, 014, [7] Liu Xue tong, Zheng Shuang ying, Guo Dong dong et al., Pieline Technique and Equiment, vol. 4, 015, [8] Yu Xiaojuan, He Shan. Soil Mechanics and Foundation Engineering[M]. Beijing: Higher Education Press, 018. [9] Kong Jun. Soil Mechanics and Foundation Engineering[M]. Beijing: China Electric Power Press, 005. [10]. D. Mindlin, Physics, vol. 7, 1936, [11] The American Society of Civil Engineers (ASCE). Guidelines for the design of buried steel ie[s]. USA, 005. [1] Hu Zhongxiong. Soil Mechanics and Environmental Soil Mechanics [M]. Shanghai: Tongji University Press, [13] Huang Yi, He Fangshe. A Beam, Plate, and Shell on an Elastic Foundation [M]. Beijing: Science Press, 005. [6] Zhong Dongwang, Huang Xiong, Si Jianfeng et al., Blasting, vol., 018,
Practical Algorithm for large diameter pile tip bearing capacity based on displacement control RUAN Xiang 1, a
Advances in ngineering Research (AR), volume 43 6th International Conference on nergy and nvironmental Protection (ICP 207) Practical Algorithm for large diameter pile tip bearing capacity based on displacement
More informationFlexible Pipes in Trenches with Stiff Clay Walls
Flexible Pies in Trenches with Stiff Clay Walls D. A. Cameron University of South Australia, South Australia, Australia J. P. Carter University of Sydney, New South Wales, Australia Keywords: flexible
More informationMechanical Engineering Ph.D. Preliminary Qualifying Examination Solid Mechanics February 25, 2002
student personal identification (ID) number on each sheet. Do not write your name on any sheet. #1. A homogeneous, isotropic, linear elastic bar has rectangular cross sectional area A, modulus of elasticity
More informationD : SOLID MECHANICS. Q. 1 Q. 9 carry one mark each. Q.1 Find the force (in kn) in the member BH of the truss shown.
D : SOLID MECHANICS Q. 1 Q. 9 carry one mark each. Q.1 Find the force (in kn) in the member BH of the truss shown. Q.2 Consider the forces of magnitude F acting on the sides of the regular hexagon having
More informationOptimal Design of Truss Structures Using a Neutrosophic Number Optimization Model under an Indeterminate Environment
Neutrosohic Sets and Systems Vol 14 016 93 University of New Mexico Otimal Design of Truss Structures Using a Neutrosohic Number Otimization Model under an Indeterminate Environment Wenzhong Jiang & Jun
More informationDeformation Effect Simulation and Optimization for Double Front Axle Steering Mechanism
0 4th International Conference on Comuter Modeling and Simulation (ICCMS 0) IPCSIT vol. (0) (0) IACSIT Press, Singaore Deformation Effect Simulation and Otimization for Double Front Axle Steering Mechanism
More informationLower bound solutions for bearing capacity of jointed rock
Comuters and Geotechnics 31 (2004) 23 36 www.elsevier.com/locate/comgeo Lower bound solutions for bearing caacity of jointed rock D.J. Sutcliffe a, H.S. Yu b, *, S.W. Sloan c a Deartment of Civil, Surveying
More informationA Numerical Method for Critical Buckling Load for a Beam Supported on Elastic Foundation
A Numerical Method for Critical Buckling Load for a Beam Suorted on Elastic Foundation Guo-ing Xia Institute of Bridge Engineering, Dalian University of Technology, Dalian, Liaoning Province, P. R. China
More informationAnalysis of cold rolling a more accurate method
Analysis of cold rolling a more accurate method 1.1 Rolling of stri more accurate slab analysis The revious lecture considered an aroximate analysis of the stri rolling. However, the deformation zone in
More informationUNIVERSITY OF SASKATCHEWAN ME MECHANICS OF MATERIALS I FINAL EXAM DECEMBER 13, 2008 Professor A. Dolovich
UNIVERSITY OF SASKATCHEWAN ME 313.3 MECHANICS OF MATERIALS I FINAL EXAM DECEMBER 13, 2008 Professor A. Dolovich A CLOSED BOOK EXAMINATION TIME: 3 HOURS For Marker s Use Only LAST NAME (printed): FIRST
More informationApplicability of the Hertz Contact Theory to Rolling Rubber Cylinders Model
International Journal of Mechanical Engineering and Applications 2016; 4(6): 242-248 http://www.sciencepublishinggroup.com/j/ijmea doi: 10.11648/j.ijmea.20160406.15 ISSN: 2330-023X (Print); ISSN: 2330-0248
More informationCHAPTER 4: BENDING OF BEAMS
(74) CHAPTER 4: BENDING OF BEAMS This chapter will be devoted to the analysis of prismatic members subjected to equal and opposite couples M and M' acting in the same longitudinal plane. Such members are
More informationAdam Paweł Zaborski. 8 Plasticity. reloading. 1. Bauschinger s effect. 2. unchanged yielding limit. 3. isotropic hardening
8 lasticity Introduction Definitions loading/unloading/reloading words commonly used in lasticity lastic strain a ermanent strain that doesn t vanish after unloading, lastically assive rocess a rocess
More informationRoots Blower with Gradually Expanding Outlet Gap: Mathematical Modelling and Performance Simulation Yingjie Cai 1, a, Ligang Yao 2, b
2nd International Conference on Advances in Mechanical Engineering and Industrial Informatics (AMEII 216) Roots Bloer ith Gradually Exanding Outlet Ga: Mathematical Modelling and Performance Simulation
More informationEstimating Laterally Loaded Pile Response
Estimating Laterally Loaded Pile Resonse C. Y. Lee, PhD Deartment of Civil Engineering College of Engineering Universiti Tenaga Nasional ABSTRACT A simlified and ractical aroach for estimating the laterally
More informationThe Ultimate Load-Carrying Capacity of a Thin-Walled Shuttle Cylinder Structure with Cracks under Eccentric Compressive Force
The Ultimate Load-Carrying Capacity of a Thin-Walled Shuttle Cylinder Structure with Cracks under Eccentric Compressive Force Cai-qin Cao *, Kan Liu, Jun-zhe Dong School of Science, Xi an University of
More informationDYNAMIC ANALYSIS OF PILES IN SAND BASED ON SOIL-PILE INTERACTION
October 1-17,, Beijing, China DYNAMIC ANALYSIS OF PILES IN SAND BASED ON SOIL-PILE INTERACTION Mohammad M. Ahmadi 1 and Mahdi Ehsani 1 Assistant Professor, Dept. of Civil Engineering, Geotechnical Group,
More informationA slope stability problem in Hong Kong
Introduction In the early 1970s a series of landslides occurred in Hong Kong as a result of excetionally heavy rains. These slides caused some loss of life and a significant amount of roerty damage. Consequently,
More informationMechanics of Solids. Mechanics Of Solids. Suraj kr. Ray Department of Civil Engineering
Mechanics Of Solids Suraj kr. Ray (surajjj2445@gmail.com) Department of Civil Engineering 1 Mechanics of Solids is a branch of applied mechanics that deals with the behaviour of solid bodies subjected
More informationPDDC 1 st Semester Civil Engineering Department Assignments of Mechanics of Solids [ ] Introduction, Fundamentals of Statics
Page1 PDDC 1 st Semester Civil Engineering Department Assignments of Mechanics of Solids [2910601] Introduction, Fundamentals of Statics 1. Differentiate between Scalar and Vector quantity. Write S.I.
More informationCalculation of Surrounding Rock Pressure Based on Pressure Arch Theory. Yuxiang SONG1,2, a
5th International Conference on Advanced Materials and Computer Science (ICAMCS 2016) Calculation of Surrounding Rock Pressure Based on Pressure Arch Theory Yuxiang SONG1,2, a 1 School of Civil Engineering,
More informationTrue Triaxial Tests and Strength Characteristics Study on Silty Sand Liang MA and Ping HU
217 2 nd International Conference on Test, Measurement and Computational Method (TMCM 217) ISBN: 978-1-6595-465- True Triaxial Tests and Strength Characteristics Study on Silty Sand Liang MA and Ping HU
More information8.7 Associated and Non-associated Flow Rules
8.7 Associated and Non-associated Flow Rules Recall the Levy-Mises flow rule, Eqn. 8.4., d ds (8.7.) The lastic multilier can be determined from the hardening rule. Given the hardening rule one can more
More informationCan ISO MRS and ASTM HDB Rated Materials Be Harmonized
an ISO MRS and ASTM HDB Rated Materials Be Harmonized Dr. Z. Jimmy Zhou The Dow hemical omany, USA Dr. Eugene F. Palermo Plastics Pie Institute, Washington D, USA ABSTRAT ISO MRS and ASTM HDB rating systems
More informationA Simple And Efficient FEM-Implementation Of The Modified Mohr-Coulomb Criterion Clausen, Johan Christian; Damkilde, Lars
Aalborg Universitet A Simle And Efficient FEM-Imlementation Of The Modified Mohr-Coulomb Criterion Clausen, Johan Christian; Damkilde, Lars Published in: Proceedings of the 9th Nordic Seminar on Comutational
More informationExperimental and numerical simulation studies of the squeezing dynamics of the UBVT system with a hole-plug device
Experimental numerical simulation studies of the squeezing dynamics of the UBVT system with a hole-plug device Wen-bin Gu 1 Yun-hao Hu 2 Zhen-xiong Wang 3 Jian-qing Liu 4 Xiao-hua Yu 5 Jiang-hai Chen 6
More informationAppraisal of Soil Nailing Design
Indian Geotechnical Journal, 39(1), 2009, 81-95 Appraisal of Soil Nailing Design G. L. Sivakumar Babu * and Vikas Pratap Singh ** Introduction Geotechnical engineers largely prefer soil nailing as an efficient
More informationDevelopment of self-adaptively loading for planetary roller traction-drive transmission
Available online www.jocr.com Journal of Chemical and Pharmaceutical Research, 013, 5(9):498-506 Research Article ISSN : 0975-7384 CODEN(USA) : JCPRC5 Develoment of self-adatively loading for lanetary
More informationEntrance exam Master Course
- 1 - Guidelines for completion of test: On each page, fill in your name and your application code Each question has four answers while only one answer is correct. o Marked correct answer means 4 points
More informationMechanics of Materials MENG 270 Fall 2003 Exam 3 Time allowed: 90min. Q.1(a) Q.1 (b) Q.2 Q.3 Q.4 Total
Mechanics of Materials MENG 70 Fall 00 Eam Time allowed: 90min Name. Computer No. Q.(a) Q. (b) Q. Q. Q.4 Total Problem No. (a) [5Points] An air vessel is 500 mm average diameter and 0 mm thickness, the
More informationJournal of Chemical and Pharmaceutical Research, 2013, 5(12): Research Article
Available online www.jocr.com Journal o Chemical and Pharmaceutical Research, 03, 5():043-047 Research Article ISS : 0975-734 CODE(USA) : JCPRC5 Otimization o the middle-die hole chamer o harmaceutical
More informationInternational Conference on Mechanics and Civil Engineering (ICMCE 2014)
International Conference on Mechanics and Civil Engineering (ICMCE 2014) Parametric Design and Experimental Study for Weak Area Structure of Circle Composite Fragile Cover Ran CAO 1,a, Guang-Ming ZHOU
More informationA slope stability problem in Hong Kong
7 A sloe stability roblem in Hong Kong 7.1 Introduction In the early 1970s a series of landslides occurred in Hong Kong as a result of excetionally heavy rains. These slides caused some loss of life and
More informationCalculating Method for the Axial Force of Washover String During Extracting Casing in Directional Well
Advances in Petroleum Exploration and Development Vol. 9, No., 05, pp. 86-9 DOI:0.3968/6634 ISSN 95-54X [Print] ISSN 95-5438 [Online] www.cscanada.net www.cscanada.org Calculating Method for the Axial
More informationSEMM Mechanics PhD Preliminary Exam Spring Consider a two-dimensional rigid motion, whose displacement field is given by
SEMM Mechanics PhD Preliminary Exam Spring 2014 1. Consider a two-dimensional rigid motion, whose displacement field is given by u(x) = [cos(β)x 1 + sin(β)x 2 X 1 ]e 1 + [ sin(β)x 1 + cos(β)x 2 X 2 ]e
More informationStress Analysis of Tensioning Bolt based on MATLAB
191 A publication of CHEMICAL ENGINEERING TRANSACTIONS VOL. 51, 016 Guest Editors: Tichun Wang, Hongyang Zhang, Lei Tian Copyright 016, AIDIC Servizi S.r.l., ISBN 978-88-95608-4-; ISSN 8-916 The Italian
More informationELASTICITY (MDM 10203)
ELASTICITY () Lecture Module 3: Fundamental Stress and Strain University Tun Hussein Onn Malaysia Normal Stress inconstant stress distribution σ= dp da P = da A dimensional Area of σ and A σ A 3 dimensional
More informationPressure-sensitivity Effects on Toughness Measurements of Compact Tension Specimens for Strain-hardening Solids
American Journal of Alied Sciences (9): 19-195, 5 ISSN 1546-939 5 Science Publications Pressure-sensitivity Effects on Toughness Measurements of Comact Tension Secimens for Strain-hardening Solids Abdulhamid
More informationME Final Exam. PROBLEM NO. 4 Part A (2 points max.) M (x) y. z (neutral axis) beam cross-sec+on. 20 kip ft. 0.2 ft. 10 ft. 0.1 ft.
ME 323 - Final Exam Name December 15, 2015 Instructor (circle) PROEM NO. 4 Part A (2 points max.) Krousgrill 11:30AM-12:20PM Ghosh 2:30-3:20PM Gonzalez 12:30-1:20PM Zhao 4:30-5:20PM M (x) y 20 kip ft 0.2
More informationEffect of Displacement Loading Rate on Mechanical Properties of Sandstone
Effect of Displacement Loading Rate on Mechanical Properties of Sandstone Jinghu Yang School of Resource and Safety Engineering, China University of Mining and Technology (Beijing) Ding No.11 Xueyuan Road,
More informationExperimental Approach to Determine the Stress at a Section of Semi Circular Curved Beam Subjected to Out-Of-Plane Load Using Strain Rosette
Experimental Approach to Determine the Stress at a Section of Semi Circular Curved Beam Subjected to Out-Of-Plane Load Using Strain Rosette Rakshith N 1, Dr. D S Ramakrishna 2, Srinivasa K 3, Md Nadeem
More informationGeo-E2010 Advanced Soil Mechanics L Wojciech Sołowski. 07 March 2017
Geo-E2010 Advanced Soil Mechanics L Wojciech Sołowski 07 March 2017 Soil modeling: critical state soil mechanics and Modified Cam Clay model Outline 1. Refresh of the theory of lasticity 2. Critical state
More informationFE FORMULATIONS FOR PLASTICITY
G These slides are designed based on the book: Finite Elements in Plasticity Theory and Practice, D.R.J. Owen and E. Hinton, 1970, Pineridge Press Ltd., Swansea, UK. 1 Course Content: A INTRODUCTION AND
More informationSTRESS. Bar. ! Stress. ! Average Normal Stress in an Axially Loaded. ! Average Shear Stress. ! Allowable Stress. ! Design of Simple Connections
STRESS! Stress Evisdom! verage Normal Stress in an xially Loaded ar! verage Shear Stress! llowable Stress! Design of Simple onnections 1 Equilibrium of a Deformable ody ody Force w F R x w(s). D s y Support
More informationEMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 2 Stress & Strain - Axial Loading
MA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 2 Stress & Strain - Axial Loading MA 3702 Mechanics & Materials Science Zhe Cheng (2018) 2 Stress & Strain - Axial Loading Statics
More informationStress Transformation Equations: u = +135 (Fig. a) s x = 80 MPa s y = 0 t xy = 45 MPa. we obtain, cos u + t xy sin 2u. s x = s x + s y.
014 Pearson Education, Inc., Upper Saddle River, NJ. All rights reserved. This material is protected under all copyright laws as they currently 9 7. Determine the normal stress and shear stress acting
More informationThe external thermal insulation composite system, a comprehensive stress-strain analysis
The external thermal insulation comosite system, a comrehensive stress-strain analysis Amilcare Collina MAPEI S..A. Italy a.collina@maei.it Gian Piero Lignola University of Nales Italy glignola@unina.it
More informationApplication of Automated Ball Indentation for Property Measurement of Degraded Zr2.5Nb
Journal of Minerals & Materials Characterization & Engineering, Vol. 10, No.7,.661-669, 011 jmmce.org Printed in the USA. All rights reserved Alication of Automated Ball Indentation for Proerty Measurement
More information2040. Damage modeling and simulation of vibrating pipe with part-through circumferential crack
24. Damage modeling and simulation of vibrating pipe with part-through circumferential crack Zhihong Yu 1, Laibin Zhang 2, Jinqiu Hu 3, Jiashun Hu 4 1, 2, 3 College of Mechanical and Transportation Engineering,
More informationREFINED STRAIN ENERGY OF THE SHELL
REFINED STRAIN ENERGY OF THE SHELL Ryszard A. Walentyński Deartment of Building Structures Theory, Silesian University of Technology, Gliwice, PL44-11, Poland ABSTRACT The aer rovides information on evaluation
More informationExperimental Research on Ground Deformation of Double Close-spaced Tunnel Construction
Research Journal of Applied Sciences, Engineering and Technology 4(22): 484-4844, 212 ISSN: 24-7467 Maxwell Scientific Organization, 212 Submitted: May 8, 212 Accepted: June 8, 212 Published: November
More informationUniversity of Pretoria Department of Mechanical & Aeronautical Engineering MOW 227, 2 nd Semester 2014
Universit of Pretoria Department of Mechanical & Aeronautical Engineering MOW 7, nd Semester 04 Semester Test Date: August, 04 Total: 00 Internal eaminer: Duration: hours Mr. Riaan Meeser Instructions:
More informationValidation of Stresses with Numerical Method and Analytical Method
ISSN 303-451 PERIODICALS OF ENGINEERING AND NATURAL SCIENCES Vol. 4 No. 1 (016) Available online at: http://pen.ius.edu.ba Validation of Stresses with Numerical Method and Analytical Method Enes Akca International
More informationSamantha Ramirez, MSE. Stress. The intensity of the internal force acting on a specific plane (area) passing through a point. F 2
Samantha Ramirez, MSE Stress The intensity of the internal force acting on a specific plane (area) passing through a point. Δ ΔA Δ z Δ 1 2 ΔA Δ x Δ y ΔA is an infinitesimal size area with a uniform force
More informationIDE 110 Mechanics of Materials Spring 2006 Final Examination FOR GRADING ONLY
Spring 2006 Final Examination STUDENT S NAME (please print) STUDENT S SIGNATURE STUDENT NUMBER IDE 110 CLASS SECTION INSTRUCTOR S NAME Do not turn this page until instructed to start. Write your name on
More informationAluminum shell. Brass core. 40 in
PROBLEM #1 (22 points) A solid brass core is connected to a hollow rod made of aluminum. Both are attached at each end to a rigid plate as shown in Fig. 1. The moduli of aluminum and brass are EA=11,000
More informationCHAPTER 6: Shearing Stresses in Beams
(130) CHAPTER 6: Shearing Stresses in Beams When a beam is in pure bending, the only stress resultants are the bending moments and the only stresses are the normal stresses acting on the cross sections.
More informationDetermination of Pile Bearing Capacity By In Situ Tests
Determination of Pile Bearing Caacity By In Situ Tests Qani V. Kadiri Faculty of Civil Engineering and Architecture, Prishtinë, Kosova Abstract - Jablanica is located in the western art of Kosovo along
More information1439. Numerical simulation of the magnetic field and electromagnetic vibration analysis of the AC permanent-magnet synchronous motor
1439. Numerical simulation of the magnetic field and electromagnetic vibration analysis of the AC permanent-magnet synchronous motor Bai-zhou Li 1, Yu Wang 2, Qi-chang Zhang 3 1, 2, 3 School of Mechanical
More informationNatural Boundary Element Method for Stress Field in Rock Surrounding a Roadway with Weak Local Support
Copyright 011 Tech Science Press CMES, vol.71, no., pp.93-109, 011 Natural Boundary Element Method for Stress Field in Rock Surrounding a Roadway with Weak Local Support Shuncai Li 1,,3, Zhengzhu Dong
More informationKeywords: pile, liquefaction, lateral spreading, analysis ABSTRACT
Key arameters in seudo-static analysis of iles in liquefying sand Misko Cubrinovski Deartment of Civil Engineering, University of Canterbury, Christchurch 814, New Zealand Keywords: ile, liquefaction,
More informationEstimation of the Residual Stiffness of Fire-Damaged Concrete Members
Copyright 2011 Tech Science Press CMC, vol.22, no.3, pp.261-273, 2011 Estimation of the Residual Stiffness of Fire-Damaged Concrete Members J.M. Zhu 1, X.C. Wang 1, D. Wei 2, Y.H. Liu 2 and B.Y. Xu 2 Abstract:
More informationEvaluation of straightening capacity of plate roll straightener
J. Cent. South Univ. (0) 9: 477 48 DOI: 0.007/s77 0 99 4 Evaluation of straightening caacity of late roll straightener WANG Yong qin( 王勇勤 ), LIU Zhi fang( 刘志芳 ), YAN Xing chun( 严兴春 ) State Key Laboratory
More informationThree-Dimensional simulation for the rock fragmentation induced by TBM with GFEM
Recent Advances in Rock Engineering (RARE 2016) Three-Dimensional simulation for the rock fragmentation induced by TBM with GFEM XY Xu, XH Tang and QS Liu School of Civil Engineering, Wuhan University,
More informationVERTICAL STRESS INCREASES IN SOIL TYPES OF LOADING. Point Loads (P) Line Loads (q/unit length) Examples: -Posts
VERTICAL STRESS INCREASES IN SOIL Point Loads (P) TYPES OF LOADING Line Loads (q/unit length) Revised 0/014 Figure 6.11. Das FGE (005). Examples: -Posts Figure 6.1. Das FGE (005). Examples: - Railroad
More informationMechanical Behaviors of Cylindrical Retaining Structures in Ultra-deep Excavation
Mechanical Behaviors of Cylindrical Retaining Structures in Ultra-deep Excavation Pengfei Xu Tongji University August 4, 2015 Outline Introduction Two circular excavations for anchorage foundations 3D
More informationINVESTIGATION OF LONGITUDINAL ELASTIC WAVE PROPAGATION THROUGH INTERSECTING WELDED BARS
8 Journal of Marine Science and Technology, Vol. 7, No. 1,. 8-16 (1999) INVESTIGATION OF LONGITUDINAL ELASTIC WAVE PROPAGATION THROUGH INTERSECTING WELDED BARS Ming-Te Liang* and Chiou-Jenn Chen** Keywords:
More informationStrength Study of Spiral Flexure Spring of Stirling Cryocooler
Sensors & Transducers 2013 by IFSA http://www.sensorsportal.com Strength Study of Spiral of Stirling Cryocooler WANG Wen-Rui, NIE Shuai, ZHANG Jia-Ming School of Mechanical Engineering, University of Science
More informationStability of Crane s Lifting Drum with Euler Distribution Forces
International Journal of Mechanical Engineering and Applications 2016; 4(5): 176-181 http://www.sciencepublishinggroup.com/j/ijmea doi: 10.11648/j.ijmea.20160405.12 ISSN: 2330-023X (Print); ISSN: 2330-0248
More information[5] Stress and Strain
[5] Stress and Strain Page 1 of 34 [5] Stress and Strain [5.1] Internal Stress of Solids [5.2] Design of Simple Connections (will not be covered in class) [5.3] Deformation and Strain [5.4] Hooke s Law
More informationImplementation and Validation of Finite Volume C++ Codes for Plane Stress Analysis
CST0 191 October, 011, Krabi Imlementation and Validation of Finite Volume C++ Codes for Plane Stress Analysis Chakrit Suvanjumrat and Ekachai Chaichanasiri* Deartment of Mechanical Engineering, Faculty
More informationChapter Objectives. Design a beam to resist both bendingand shear loads
Chapter Objectives Design a beam to resist both bendingand shear loads A Bridge Deck under Bending Action Castellated Beams Post-tensioned Concrete Beam Lateral Distortion of a Beam Due to Lateral Load
More informationIf the solution does not follow a logical thought process, it will be assumed in error.
Please indicate your group number (If applicable) Circle Your Instructor s Name and Section: MWF 8:30-9:20 AM Prof. Kai Ming Li MWF 2:30-3:20 PM Prof. Fabio Semperlotti MWF 9:30-10:20 AM Prof. Jim Jones
More informationNumerical simulation of bird strike in aircraft leading edge structure using a new dynamic failure model
Numerical simulation of bird strike in aircraft leading edge structure using a new dynamic failure model Q. Sun, Y.J. Liu, R.H, Jin School of Aeronautics, Northwestern Polytechnical University, Xi an 710072,
More informationThe University of Melbourne Engineering Mechanics
The University of Melbourne 436-291 Engineering Mechanics Tutorial Four Poisson s Ratio and Axial Loading Part A (Introductory) 1. (Problem 9-22 from Hibbeler - Statics and Mechanics of Materials) A short
More informationNumerical Simulation on Support of Roadway with Compound Roof and Large Cross Section
Numerical Simulation on Support of Roadway with Compound Roof and Large Cross Section YUE Zhong-wen, YANG Ren-shu, YAN Zhen-dong, WANG Guo-dong, WU Bao-yang School of Mechanics & Civil Engineering China
More informationThe Effects of Convolution Geometry and Boundary Condition on the Failure of Bellows
Indian Journal of Science and Technology, Vol 8(S1), 462 466, January 2015 ISSN (Online) : 0974-5645 ISSN (Print) : 0974-6846 DOI: 10.17485/ijst/2015/v8iS1/59417 The Effects of Convolution Geometry and
More informationJournal of Chemical and Pharmaceutical Research, 2014, 6(7): Research Article
Available online www.jocpr.com Journal of Chemical and Pharmaceutical Research, 4, 6(7): 44-4 Research Article ISSN : 975-784 CODEN(USA) : JCPRC5 Analysis on static characteristics of linear rolling guide
More informationTuesday, February 11, Chapter 3. Load and Stress Analysis. Dr. Mohammad Suliman Abuhaiba, PE
1 Chapter 3 Load and Stress Analysis 2 Chapter Outline Equilibrium & Free-Body Diagrams Shear Force and Bending Moments in Beams Singularity Functions Stress Cartesian Stress Components Mohr s Circle for
More informationFINITE GRID SOLUTION FOR NON-RECTANGULAR PLATES
th International Conference on Earthquake Geotechnical Engineering June 5-8, 7 Paper No. 11 FINITE GRID SOLUTION FOR NON-RECTANGULAR PLATES A.Halim KARAŞĐN 1, Polat GÜLKAN ABSTRACT Plates on elastic foundations
More informationNORMAL STRESS. The simplest form of stress is normal stress/direct stress, which is the stress perpendicular to the surface on which it acts.
NORMAL STRESS The simplest form of stress is normal stress/direct stress, which is the stress perpendicular to the surface on which it acts. σ = force/area = P/A where σ = the normal stress P = the centric
More informationMECHANICS OF MATERIALS
2009 The McGraw-Hill Companies, Inc. All rights reserved. Fifth SI Edition CHAPTER 3 MECHANICS OF MATERIALS Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Torsion Lecture Notes:
More informationQUESTION BANK DEPARTMENT: CIVIL SEMESTER: III SUBJECT CODE: CE2201 SUBJECT NAME: MECHANICS OF SOLIDS UNIT 1- STRESS AND STRAIN PART A
DEPARTMENT: CIVIL SUBJECT CODE: CE2201 QUESTION BANK SEMESTER: III SUBJECT NAME: MECHANICS OF SOLIDS UNIT 1- STRESS AND STRAIN PART A (2 Marks) 1. Define longitudinal strain and lateral strain. 2. State
More informationR13. II B. Tech I Semester Regular Examinations, Jan MECHANICS OF SOLIDS (Com. to ME, AME, AE, MTE) PART-A
SET - 1 II B. Tech I Semester Regular Examinations, Jan - 2015 MECHANICS OF SOLIDS (Com. to ME, AME, AE, MTE) Time: 3 hours Max. Marks: 70 Note: 1. Question Paper consists of two parts (Part-A and Part-B)
More informationMECHANICS OF MATERIALS
STATICS AND MECHANICS OF MATERIALS Ferdinand P. Beer E. Russell Johnston, Jr, John T. DeWolf David E Mazurek \Cawect Mc / iur/» Craw SugomcT Hilt Introduction 1 1.1 What is Mechanics? 2 1.2 Fundamental
More informationAssessing Slope Stability of Open Pit Mines using PCA and Fisher Discriminant Analysis
Assessing Sloe Stabilit of Oen Pit Mines using PCA and Fisher Discriminant Analsis Shiao Xiang College of Geoscience and Surveing Engineering, China Universit of Mining and echnolog (Beijing), Beijing
More information3D Elasticity Theory
3D lasticity Theory Many structural analysis problems are analysed using the theory of elasticity in which Hooke s law is used to enforce proportionality between stress and strain at any deformation level.
More informationInitial Stress Calculations
Initial Stress Calculations The following are the initial hand stress calculations conducted during the early stages of the design process. Therefore, some of the material properties as well as dimensions
More informationCHAPTER THREE SYMMETRIC BENDING OF CIRCLE PLATES
CHAPTER THREE SYMMETRIC BENDING OF CIRCLE PLATES * Governing equations in beam and plate bending ** Solution by superposition 1.1 From Beam Bending to Plate Bending 1.2 Governing Equations For Symmetric
More informationName (Print) ME Mechanics of Materials Exam # 1 Date: October 5, 2016 Time: 8:00 10:00 PM
Name (Print) (Last) (First) Instructions: ME 323 - Mechanics of Materials Exam # 1 Date: October 5, 2016 Time: 8:00 10:00 PM Circle your lecturer s name and your class meeting time. Gonzalez Krousgrill
More informationOptimisation of Pressure Loss and Flow Distribution at Pipe Bifurcation
ISSN 9 86 Volume, Issue 9 Setember 07 Otimisation of Pressure Loss and Flow Distribution at Pie Bifurcation Dr. Nagaraj Sitaram Professor, Deartment of Civil Engineering,School of Engineering Technology,
More informationFinite Element Analysis of V-Bending of Polypropylene Using Hydrostatic-Pressure-Dependent Plastic Constitutive Equation*
Materials Transactions, Vol. 48, No. 1 (7). 6 to 664 #7 The Jaan Society for Technology of Plasticity Finite Element Analysis of V-Bending of Polyroylene Using Hydrostatic-Pressure-Deendent Plastic onstitutive
More informationStudy on Settlement Prediction Model of High-Speed Railway Bridge Pile Foundation
Journal of Applied Science and Engineering, Vol. 18, No. 2, pp. 187 193 (2015) DOI: 10.6180/jase.2015.18.2.12 Study on Settlement Prediction Model of High-Speed Railway Bridge Pile Foundation Zhong-Bo
More informationExperimental investigation on monotonic performance of steel curved knee braces for weld-free beam-to-column connections
Experimental investigation on monotonic performance of steel curved knee braces for weld-free beam-to-column connections *Zeyu Zhou 1) Bo Ye 2) and Yiyi Chen 3) 1), 2), 3) State Key Laboratory of Disaster
More informationChapter 10: Flow Flow in in Conduits Conduits Dr Ali Jawarneh
Chater 10: Flow in Conduits By Dr Ali Jawarneh Hashemite University 1 Outline In this chater we will: Analyse the shear stress distribution across a ie section. Discuss and analyse the case of laminar
More informationModeling of Interfacial Debonding Induced by IC Crack for Concrete Beam-bonded with CFRP
Proceedings of the World Congress on Engineering 21 Vol II WCE 21, June 2 - July 1, 21, London, U.K. Modeling of Interfacial Debonding Induced by IC Crack for Concrete Beam-bonded with CFRP Lihua Huang,
More informationRobust Predictive Control of Input Constraints and Interference Suppression for Semi-Trailer System
Vol.7, No.7 (4),.37-38 htt://dx.doi.org/.457/ica.4.7.7.3 Robust Predictive Control of Inut Constraints and Interference Suression for Semi-Trailer System Zhao, Yang Electronic and Information Technology
More informationSTRENGTH OF MATERIALS-I. Unit-1. Simple stresses and strains
STRENGTH OF MATERIALS-I Unit-1 Simple stresses and strains 1. What is the Principle of surveying 2. Define Magnetic, True & Arbitrary Meridians. 3. Mention different types of chains 4. Differentiate between
More informationFinite Element Solutions for Geotechnical Engineering
Release Notes Release Date: June, 2017 Product Ver.: GTSNX 2017(v1.1) Integrated Solver Otimized for the next generation 64-bit latform Finite Element Solutions for Geotechnical Engineering 1. Analysis
More informationAn equivalent diameter in calculating borehole thermal resistance for spiral coil type GHE
The 01 World Congress on Advances in Civil, Environmental, and Materials esearch (ACEM 1) Seoul, Korea, August 6-30, 01 An equivalent diameter in calculating borehole thermal resistance for siral coil
More information