Inherently Adaptive Structural Materials. Technova Corporation
|
|
- Sydney Strickland
- 6 years ago
- Views:
Transcription
1 Inherently Adaptive Structural Materials Technova Corporation
2 Outline of the Presentation Structural and Adaptive Qualities of Bone Biomimetic Principles of Adaptive Materials Design & Evaluation of Integrated Adaptive Systems Processing of Nanocomposites Modeling and Validation of Structural Principles
3 Development of Bone Structure Cancellous Bone Compact Bone
4 Mechanisms of Bone Adaptation Loads Build of Bone Remodeling Strains Comparison Signal Electrical Potential Gradient Under Bending Bone Remodeling Under Bending
5 Consequences of Bone Adaptation Arrangement of Struts Along Principal Strain Lines Optimization of Topology
6 Outline of the Presentation Structural and Adaptive Qualities of Bone Biomimetic Principles of Adaptive Materials Design & Evaluation of Integrated Adaptive Systems Processing of Nanocomposites Modeling and Validation of Structural Principles
7 Key Constituents and Processes Piezoelectricity V = g.s.t Q = d.s.a Electrolysis V = Vo + i.r + Ve Q = n.f Solid Electrolytes
8 Experimental Validation of Electrolysis Through Solid Electrolyte Electrolytic Cell Current, ma Voltage, mv Voltammogram Micrographs
9 Design & Validation of Piezo-Driven Electrolysis Stress, MPa 30 Applied Stress: 1 Time, sec Piezoelectric Stack St ainless St eel Mesh Copper-Ion Conducting Polymer Copper Layer
10 Outline of the Presentation Structural and Adaptive Qualities of Bone Biomimetic Principles of Adaptive Materials Design & Evaluation of Integrated Adaptive Systems Processing of Nanocomposites Modeling and Validation of Structural Principles
11 Designs and Validation of a Basic System Replicated Multilayers of: Insulative Layer (Ti) Conductive Layer (Tc) Piezoelectric Layer (Tp) Solid Electrolyte Layer (Ts) Metallic Layer (Tm) T V = g 33.s.T p Q = d 33.s.(n.L 1.W 1 ) L L1 W1 W Schematic Presentation Processing and Test Set-Ups System T i T c T p T s T m I (conventional) 50 µm 50 µm 50 µm 50 µm 50 µm II (nanocomposite) 5 nm 5 nm 50 nm 40 nm 40 nm Alternative Designs
12 An Elaborate Adaptive Element e e A A Section A-A Nanolayered Composite Comprising Replicated: Insulative Nanolayer (Ti) Conductive Nanolayer (Tc) Piezoelectric Nanolayer (Tp) Solid Electrolyte Nanoayer (Ts) Metallic Nanoayer (Tm) Mass Transfer Mass Transfer e e (a) (b) (c) (d) (e)
13 Detailed System Design and Analysis 1 m 1 mm Nanolayered Composite Comprising Replicated: Insulative Nanolayer (Ti = 5 nanometer) Conductive Nanolayer (Tc = 5 nanometer) Piezoelectric Nanolayer (Tp = 150 nanometer) Solid Electrolyte Nanoayer (Ts = 40 nanometer) Metallic Nanoayer (Tm = 150 nanometer) A A 10 mm e Section A-A System Design 8.33 MPa 43 MPa -26 MPa 8.33 MPa e (a) Concentric Loading (b) Eccentric Loading (c) Concentricity Restored by Self-Adaptation Structural & Adaptive Analysis
14 Preliminary Assessment of Structural Implications
15 Preliminary Assessment of Structural Implications
16 Outline of the Presentation Structural and Adaptive Qualities of Bone Biomimetic Principles of Adaptive Materials Design & Evaluation of Integrated Adaptive Systems Processing of Nanocomposites Modeling and Validation of Structural Principles
17 Ionic Self-Assembly: Basic Principles Mechanism of Self-Assembly Build-Up of Nanolayers
18 Adaptation of Ionic Self-Assembly Sub st r at e / PEI Sub str at e PEI/[PSS/PAH]3 PAH/PS119 PEI/[PSS/PAH]3 Au]1 PAh/PS119/ZrO2 PEI/[PSS/PAH]3 Au/PAH]2 PEI/[PSS/PAH]3 Au/PAH]3 Multiple ZrO2/Polymer Layers Manual and Automated Processing Self-Assembly of Colloidal Nanoparticles
19 Self-Assembly of Piezoelectric and Conducting Nanolayers V C 0 Ionically Self-Assembled, Mult ilayer PSS/PDDA System ITO-Coated Glass Substrate Elect rode F Elect r ode Output VOltage, mv Applied Force, g
20 Outline of the Presentation Structural and Adaptive Qualities of Bone Biomimetic Principles of Adaptive Materials Design & Evaluation of Integrated Adaptive Systems Processing of Nanocomposite Modeling and Validation of Structural Principles
21 Section-Level Structural Modeling f cdac + f ldal = N Ac Al f c ydac + f l ydal = A c A l M Modeling Principles Effect of Hybrid Nanolayer Build-Up on RVC Section Behavior
22 Preliminary System-Level Analysis (a) Bending (b) Buckling (c) Yielding (d) Fracture Failure Modes Effect of Multi-Layer Polymer/Ceramic/Metal Build-Up on Bulk Properties of RVC Open-Cell System Property Density Elastic Modulus Tensile Strength Composite/Base Ratio
23 Preliminary Structural Evaluation Stress, MPa After Deposition of Polymeric Nanolayers As-Received Open-Cell Structure and Tension Test Set-Up Strain, mm/mm Effect of Polymer Nanolayers on Tensile Behavior of Open-Cell Structure
24 Summary & Conclusions Selection of adaptive system constituents and viable architectures Modeling, design and experimental validation of adaptive structures Implementation of nanocomposite processing techniques Modeling and validation of structural principles
Frontiers of Fracture Mechanics. Adhesion and Interfacial Fracture Contact Damage
Frontiers of Fracture Mechanics Adhesion and Interfacial Fracture Contact Damage Biology, Medicine & Dentistry The Next Frontiers For Mechanics One of the current challenges in materials & mechanics is
More informationPURE BENDING. If a simply supported beam carries two point loads of 10 kn as shown in the following figure, pure bending occurs at segment BC.
BENDING STRESS The effect of a bending moment applied to a cross-section of a beam is to induce a state of stress across that section. These stresses are known as bending stresses and they act normally
More informationComputational Analysis for Composites
Computational Analysis for Composites Professor Johann Sienz and Dr. Tony Murmu Swansea University July, 011 The topics covered include: OUTLINE Overview of composites and their applications Micromechanics
More informationSupplementary Figures
Fracture Strength (GPa) Supplementary Figures a b 10 R=0.88 mm 1 0.1 Gordon et al Zhu et al Tang et al im et al 5 7 6 4 This work 5 50 500 Si Nanowire Diameter (nm) Supplementary Figure 1: (a) TEM image
More informationSTANDARD SAMPLE. Reduced section " Diameter. Diameter. 2" Gauge length. Radius
MATERIAL PROPERTIES TENSILE MEASUREMENT F l l 0 A 0 F STANDARD SAMPLE Reduced section 2 " 1 4 0.505" Diameter 3 4 " Diameter 2" Gauge length 3 8 " Radius TYPICAL APPARATUS Load cell Extensometer Specimen
More information6.4 A cylindrical specimen of a titanium alloy having an elastic modulus of 107 GPa ( psi) and
6.4 A cylindrical specimen of a titanium alloy having an elastic modulus of 107 GPa (15.5 10 6 psi) and an original diameter of 3.8 mm (0.15 in.) will experience only elastic deformation when a tensile
More informationOptimizing the Design of Polymer Based Unimorph Actuator using COMSOL Multiphysics Vineet Tiwari, Rashiya Sharma, R. K. Dwivedi and Geetika Srivastava
Optimizing the Design of Polymer Based Unimorph Actuator using COMSOL Multiphysics Vineet Tiwari, Rashiya Sharma, R. K. Dwivedi and Geetika Srivastava Department of Physics and Materials Science & Engineering
More informationQUESTION BANK Composite Materials
QUESTION BANK Composite Materials 1. Define composite material. 2. What is the need for composite material? 3. Mention important characterits of composite material 4. Give examples for fiber material 5.
More informationD Y N A M I C M E C H A N I C A L A N A L Y S I S A N D I T S A D V A N T A G E S O V E R D E F L E C T I O N T E M P E R A T U R E U N D E R L O A D
D Y N A M I C M E C H A N I C A L A N A L Y S I S A N D I T S A D V A N T A G E S O V E R D E F L E C T I O N T E M P E R A T U R E U N D E R L O A D Sujan E. Bin Wadud TA Instruments 9 Lukens Drive, New
More informationElements of Polymer Structure and Viscoelasticity. David M. Parks Mechanics and Materials II February 18, 2004
Elements of Polymer Structure and Viscoelasticity David M. Parks Mechanics and Materials II 2.002 February 18, 2004 Outline Elements of polymer structure Linear vs. branched; Vinyl polymers and substitutions
More information3.032 Problem Set 2 Solutions Fall 2007 Due: Start of Lecture,
3.032 Problem Set 2 Solutions Fall 2007 Due: Start of Lecture, 09.21.07 1. In the beam considered in PS1, steel beams carried the distributed weight of the rooms above. To reduce stress on the beam, it
More informationThe science of elasticity
The science of elasticity In 1676 Hooke realized that 1.Every kind of solid changes shape when a mechanical force acts on it. 2.It is this change of shape which enables the solid to supply the reaction
More informationSupporting Information. Three-Dimensional Super-Resolution Imaging of Single Nanoparticle Delivered by Pipettes
Supporting Information Three-Dimensional Super-Resolution Imaging of Single Nanoparticle Delivered by Pipettes Yun Yu,, Vignesh Sundaresan,, Sabyasachi Bandyopadhyay, Yulun Zhang, Martin A. Edwards, Kim
More informationISSN: ISO 9001:2008 Certified International Journal of Engineering Science and Innovative Technology (IJESIT) Volume 2, Issue 4, July 2013
Delamination Studies in Fibre-Reinforced Polymer Composites K.Kantha Rao, Dr P. Shailesh, K. Vijay Kumar 1 Associate Professor, Narasimha Reddy Engineering College Hyderabad. 2 Professor, St. Peter s Engineering
More informationFig. 1. Different locus of failure and crack trajectories observed in mode I testing of adhesively bonded double cantilever beam (DCB) specimens.
a). Cohesive Failure b). Interfacial Failure c). Oscillatory Failure d). Alternating Failure Fig. 1. Different locus of failure and crack trajectories observed in mode I testing of adhesively bonded double
More information4.MECHANICAL PROPERTIES OF MATERIALS
4.MECHANICAL PROPERTIES OF MATERIALS The diagram representing the relation between stress and strain in a given material is an important characteristic of the material. To obtain the stress-strain diagram
More informationPiezoactuators. Jiří Tůma
Piezoactuators Jiří Tůma 1 Domain Piezoelectric effect Direct piezoelectric effect discovered the brothers Pierre and Jacques Curie. They found that certain crystalline materials (ceramics) having the
More informationStrength of Material. Shear Strain. Dr. Attaullah Shah
Strength of Material Shear Strain Dr. Attaullah Shah Shear Strain TRIAXIAL DEFORMATION Poisson's Ratio Relationship Between E, G, and ν BIAXIAL DEFORMATION Bulk Modulus of Elasticity or Modulus of Volume
More informationPLATE GIRDERS II. Load. Web plate Welds A Longitudinal elevation. Fig. 1 A typical Plate Girder
16 PLATE GIRDERS II 1.0 INTRODUCTION This chapter describes the current practice for the design of plate girders adopting meaningful simplifications of the equations derived in the chapter on Plate Girders
More informationCONSTITUTIVE MODELING AND OPTIMAL DESIGN OF POLYMERIC FOAMS FOR CRASHWORTHINESS
CONSTITUTIVE MODELING AND OPTIMAL DESIGN OF POLYMERIC FOAMS FOR CRASHWORTHINESS Jun Zhang December 19, 1997 Computational Mechanics Laboratory Department of Mechanical Engineering and Applied Mechanics
More informationAgricultural Science 1B Principles & Processes in Agriculture. Mike Wheatland
Agricultural Science 1B Principles & Processes in Agriculture Mike Wheatland (m.wheatland@physics.usyd.edu.au) Outline - Lectures weeks 9-12 Chapter 6: Balance in nature - description of energy balance
More informationPiezo Theory: Chapter 1 - Physics & Design
Piezoelectric effect inverse piezoelectric effect The result of external forces to a piezoelectric material is positive and negative electrical charges at the surface of the material. If electrodes are
More informationPES Institute of Technology
PES Institute of Technology Bangalore south campus, Bangalore-5460100 Department of Mechanical Engineering Faculty name : Madhu M Date: 29/06/2012 SEM : 3 rd A SEC Subject : MECHANICS OF MATERIALS Subject
More informationEquilibrium. the linear momentum,, of the center of mass is constant
Equilibrium is the state of an object where: Equilibrium the linear momentum,, of the center of mass is constant Feb. 19, 2018 the angular momentum,, about the its center of mass, or any other point, is
More informationNon-conventional Glass fiber NCF composites with thermoset and thermoplastic matrices. F Talence, France Le Cheylard, France
20 th International Conference on Composite Materials Copenhagen, 19-24th July 2015 Non-conventional Glass fiber NCF composites with thermoset and thermoplastic matrices. Thierry Lorriot 1, Jalal El Yagoubi
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 informationMechanical Properties
Mechanical Properties Elastic deformation Plastic deformation Fracture I. Elastic Deformation S s u s y e u e T I II III e For a typical ductile metal: I. Elastic deformation II. Stable plastic deformation
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 informationStrain Gages. Approximate Elastic Constants (from University Physics, Sears Zemansky, and Young, Reading, MA, Shear Modulus, (S) N/m 2
When you bend a piece of metal, the Strain Gages Approximate Elastic Constants (from University Physics, Sears Zemansky, and Young, Reading, MA, 1979 Material Young's Modulus, (E) 10 11 N/m 2 Shear Modulus,
More informationMulti Disciplinary Delamination Studies In Frp Composites Using 3d Finite Element Analysis Mohan Rentala
Multi Disciplinary Delamination Studies In Frp Composites Using 3d Finite Element Analysis Mohan Rentala Abstract: FRP laminated composites have been extensively used in Aerospace and allied industries
More informationneeded to buckle an ideal column. Analyze the buckling with bending of a column. Discuss methods used to design concentric and eccentric columns.
CHAPTER OBJECTIVES Discuss the behavior of columns. Discuss the buckling of columns. Determine the axial load needed to buckle an ideal column. Analyze the buckling with bending of a column. Discuss methods
More informationAC-829A. Issued on Apr. 15 th 2013 (Version 1.0)
Hitachi Chemical Co., Ltd. Hitachi Anisotropic Conductive Film ANISOLM AC-829A Issued on Apr. 15 th 2013 (Version 1.0) 1. Standard specification, bonding condition, storage condition and characteristic.....1
More informationAdvances in performance evaluation of asphalt binders
Advances in performance evaluation of asphalt binders Hussain U Bahia Professor University of Wisconsin, USA March 25, Lisbon, Potugal s:, design performance a, LNEC, 25 March 2010 Road Outline >Performance
More informationKeywords: textile composites, braided fabric, dynamic property, fracture aspect, matrix hybrid
Mechanical Properties and Fracture Behavior of Hybrid Braided Composite Tube Yuki Sasaki, Yoshitaka Tanaka, Akio Ohtani, Asami Nakai, Hiroyuki Hamada Kyoto Institute of Technology Matsugasaki, Sakyo-ku,
More informationEngineering Science OUTCOME 1 - TUTORIAL 4 COLUMNS
Unit 2: Unit code: QCF Level: Credit value: 15 Engineering Science L/601/10 OUTCOME 1 - TUTORIAL COLUMNS 1. Be able to determine the behavioural characteristics of elements of static engineering systems
More informationWhat is a Strain Gauge? Strain Gauge. Schematic View Of Strain Gauge
( ) : 1391-92 92 What is Strain? Strain is the amount of deformation of a body due to an applied force. More specifically, strain (ε) is defined as the fractional change in length. Strain can be positive
More informationOn Springback Prediction In Stamping Of AHSS BIW Components Utilizing Advanced Material Models
On Springback Prediction In Stamping Of AHSS BIW Components Utilizing Advanced Material Models Ming F. Shi and Alex A. Konieczny United States Steel Corporation Introduction Origin of Springback AHSS Springback
More informationOutline. 4 Mechanical Sensors Introduction General Mechanical properties Piezoresistivity Piezoresistive Sensors Capacitive sensors Applications
Sensor devices Outline 4 Mechanical Sensors Introduction General Mechanical properties Piezoresistivity Piezoresistive Sensors Capacitive sensors Applications Introduction Two Major classes of mechanical
More informationN = Shear stress / Shear strain
UNIT - I 1. What is meant by factor of safety? [A/M-15] It is the ratio between ultimate stress to the working stress. Factor of safety = Ultimate stress Permissible stress 2. Define Resilience. [A/M-15]
More informationResearch and Development of Parylene Thin-Film Deposition and Application for Water-Proofing
Advanced Materials Research Online: 2012-06-14 ISSN: 1662-8985, Vols. 538-541, pp 23-28 doi:10.4028/www.scientific.net/amr.538-541.23 2012 Trans Tech Publications, Switzerland Research and Development
More informationExperimentally Calibrating Cohesive Zone Models for Structural Automotive Adhesives
Experimentally Calibrating Cohesive Zone Models for Structural Automotive Adhesives Mark Oliver October 19, 2016 Adhesives and Sealants Council Fall Convention contact@veryst.com www.veryst.com Outline
More informationEAP - ElectroActive Polymers
A Short Introduction to Robotics Applications AIRLab - Artificial Intelligence and Robotics Lab Politecnico di Milano http://www.airlab.elet.polimi.it/ February 2007 Introduction to EAP Focus: Emulate
More informationJetting of Isotropic Conductive Adhesives with Silver Coated Polymer Particles
Jetting of Isotropic Conductive Adhesives with Silver Coated Polymer Particles Gustaf Mårtensson 1,2 Kalland, Erik 3, Redford, Keith 3, Oppland, Ottar 5 1 Chalmers University of Technology, Göteborg, Sweden
More informationFRACTURE IN PBX 9501 AT LOW RATES
FRACTURE IN PBX 9501 AT LOW RATES Cheng Liu & Richard Browning Los Alamos National Laboratory Los Alamos, NM 87545 Tensile, or mode I, fractures in PBX 9501 have a very large process zone that runs well
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 informationName :. Roll No. :... Invigilator s Signature :.. CS/B.TECH (CE-NEW)/SEM-3/CE-301/ SOLID MECHANICS
Name :. Roll No. :..... Invigilator s Signature :.. 2011 SOLID MECHANICS Time Allotted : 3 Hours Full Marks : 70 The figures in the margin indicate full marks. Candidates are required to give their answers
More informationME 2570 MECHANICS OF MATERIALS
ME 2570 MECHANICS OF MATERIALS Chapter III. Mechanical Properties of Materials 1 Tension and Compression Test The strength of a material depends on its ability to sustain a load without undue deformation
More informationCHAPTER 3 THE EFFECTS OF FORCES ON MATERIALS
CHAPTER THE EFFECTS OF FORCES ON MATERIALS EXERCISE 1, Page 50 1. A rectangular bar having a cross-sectional area of 80 mm has a tensile force of 0 kn applied to it. Determine the stress in the bar. Stress
More informationIntensity (a.u.) Intensity (a.u.) Raman Shift (cm -1 ) Oxygen plasma. 6 cm. 9 cm. 1mm. Single-layer graphene sheet. 10mm. 14 cm
Intensity (a.u.) Intensity (a.u.) a Oxygen plasma b 6 cm 1mm 10mm Single-layer graphene sheet 14 cm 9 cm Flipped Si/SiO 2 Patterned chip Plasma-cleaned glass slides c d After 1 sec normal Oxygen plasma
More informationSupplementary Information
Electronic Supplementary Material (ESI) for Journal of Materials Chemistry A. This journal is The Royal Society of Chemistry 2015 Supplementary Information Nacre-inspired Integrated Nanocomposites with
More informationA Transparent Perovskite Light Emitting Touch-
Supporting Information for A Transparent Perovskite Light Emitting Touch- Responsive Device Shu-Yu Chou, Rujun Ma, Yunfei Li,, Fangchao Zhao, Kwing Tong, Zhibin Yu, and Qibing Pei*, Department of Materials
More informationME 176 Final Exam, Fall 1997
Tuesday, December 16, 5:00 8:00 PM, 1997. Answer all questions for a maximum of 100 points. Please write all answers in the space provided. If you need additional space, write on the back sides. Indicate
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 informationMICROMECHANICAL ANALYSIS OF FRP COMPOSITES SUBJECTED TO LONGITUDINAL LOADING
MICROMECHANICAL ANALYSIS OF FRP COMPOSITES SUBJECTED TO LONGITUDINAL LOADING N. Krishna Vihari 1, P. Phani Prasanthi 1, V. Bala Krishna Murthy 2* and A. Srihari Prasad 3 1 Mech. Engg. Dept., P. V. P. Siddhartha
More informationModelling and numerical simulation of the wrinkling evolution for thermo-mechanical loading cases
Modelling and numerical simulation of the wrinkling evolution for thermo-mechanical loading cases Georg Haasemann Conrad Kloß 1 AIMCAL Conference 2016 MOTIVATION Wrinkles in web handling system Loss of
More informationMaterials Selection and Design Materials Selection - Practice
Materials Selection and Design Materials Selection - Practice Each material is characterized by a set of attributes that include its mechanical, thermal, electrical, optical, and chemical properties; its
More informationChapter 7. Highlights:
Chapter 7 Highlights: 1. Understand the basic concepts of engineering stress and strain, yield strength, tensile strength, Young's(elastic) modulus, ductility, toughness, resilience, true stress and true
More informationSupplementary Information
Supplementary Information Fabrication and evaluation of bending properties The hydrogel strip was fabricated by in situ photopolymerization. The gel network of polymerized actuator material is anionic
More informationWheatstone Bridge Nonlinearity
Index: Nonlinearity Wheatstone Bridge Nonlinearity Introduction General Considerations The "Unbalanced" Circuit The Unbalanced Circuit Table of Contents Output & Nonlinearity with Various Bridge/Strain
More informationRE-Ba 2 Cu 3 O 7-d coated conductor helical cables for electric power transmission and SMES
RE-Ba 2 Cu 3 O 7-d coated conductor helical cables for electric power transmission and SMES D.C. van der Laan and X.F. Lu University of Colorado & National Institute of Standards and Technology, Boulder,
More informationDesign of Power Electronics Reliability: A New, Interdisciplinary Approach. M.C. Shaw. September 5, 2002
Design of Power Electronics Reliability: A New, Interdisciplinary Approach M.C. Shaw September 5, 2002 Physics Department California Lutheran University 60 W. Olsen Rd, #3750 Thousand Oaks, CA 91360 (805)
More informationBiomaterial Scaffolds
Biomaterial Scaffolds Biomaterial Properties Surface properties Bulk properties Biological properties Types of Biomaterials Biological materials Synthetic materials Surface Properties The body reads the
More informationElastic Properties of Solid Materials. Notes based on those by James Irvine at
Elastic Properties of Solid Materials Notes based on those by James Irvine at www.antonine-education.co.uk Key Words Density, Elastic, Plastic, Stress, Strain, Young modulus We study how materials behave
More informationMarch 24, Chapter 4. Deflection and Stiffness. Dr. Mohammad Suliman Abuhaiba, PE
Chapter 4 Deflection and Stiffness 1 2 Chapter Outline Spring Rates Tension, Compression, and Torsion Deflection Due to Bending Beam Deflection Methods Beam Deflections by Superposition Strain Energy Castigliano
More informationPIEZOELECTRIC TECHNOLOGY PRIMER
PIEZOELECTRIC TECHNOLOGY PRIMER James R. Phillips Sr. Member of Technical Staff CTS Wireless Components 4800 Alameda Blvd. N.E. Albuquerque, New Mexico 87113 Piezoelectricity The piezoelectric effect is
More informationINFLUENCE OF TEMPERATURE ON BEHAVIOR OF THE INTERFACIAL CRACK BETWEEN THE TWO LAYERS
Djoković, J. M., et.al.: Influence of Temperature on Behavior of the Interfacial THERMAL SCIENCE: Year 010, Vol. 14, Suppl., pp. S59-S68 S59 INFLUENCE OF TEMPERATURE ON BEHAVIOR OF THE INTERFACIAL CRACK
More informationOutline. Tensile-Test Specimen and Machine. Stress-Strain Curve. Review of Mechanical Properties. Mechanical Behaviour
Tensile-Test Specimen and Machine Review of Mechanical Properties Outline Tensile test True stress - true strain (flow curve) mechanical properties: - Resilience - Ductility - Toughness - Hardness A standard
More informationME 243. Mechanics of Solids
ME 243 Mechanics of Solids Lecture 2: Stress and Strain Ahmad Shahedi Shakil Lecturer, Dept. of Mechanical Engg, BUET E-mail: sshakil@me.buet.ac.bd, shakil6791@gmail.com Website: teacher.buet.ac.bd/sshakil
More informationME 354, MECHANICS OF MATERIALS LABORATORY COMPRESSION AND BUCKLING
ME 354, MECHANICS OF MATERIALS LABATY COMPRESSION AND BUCKLING PURPOSE 01 January 2000 / mgj The purpose of this exercise is to study the effects of end conditions, column length, and material properties
More information2G HTS Coil Winding Technology Development at SuperPower
superior performance. powerful technology. 2G HTS Coil Winding Technology Development at SuperPower D.W. Hazelton, P. Brownsey, H. Song, Y. Zhang Tuesday, June 18, 2013 2013 CEC-ICMC Anchorage Alaska Paper
More informationDIGIMAT for NANO-COMPOSITES
DIGIMAT for NANO-COMPOSITES Document Version 2.0.1, February 2010 info@e-xstream.com www.e-xstream.com Materials: Engineering Plastics, Reinforced Plastics, Mineral and Clay fillers. e-xstream Technology:
More informationDon Robbins, Andrew Morrison, Rick Dalgarno Autodesk, Inc., Laramie, Wyoming. Abstract
PROGRESSIVE FAILURE SIMULATION OF AS-MANUFACTURED SHORT FIBER FILLED INJECTION MOLDED PARTS: VALIDATION FOR COMPLEX GEOMETRIES AND COMBINED LOAD CONDITIONS Don Robbins, Andrew Morrison, Rick Dalgarno Autodesk,
More informationSupporting Information. 15 January, Ms. ID: ac b. Parallel Screening of Electrocatalyst Candidates using Bipolar
Supporting Information 15 January, 2013 Ms. ID: ac-2012-03581b Parallel Screening of Electrocatalyst Candidates using Bipolar Electrochemistry Stephen E. Fosdick, Sean P. Berglund, C. Buddie Mullins, and
More informationCOMPLEX STRESS TUTORIAL 4 THEORIES OF FAILURE. You should judge your progress by completing the self assessment exercises.
COMPLEX STRESS TUTORIAL 4 THEORIES OF FAILURE This short tutorial covers no known elements of the E.C. or Edexcel Exams but should be studied as part of complex stress, structures and materials. You should
More informationExercise 2: Bending Beam Load Cell
Transducer Fundamentals The Strain Gauge Exercise 2: Bending Beam Load Cell EXERCISE OBJECTIVE When you have completed this exercise, you will be able to explain and demonstrate the operation of a board,
More informationUltrasonic Anisotropic Conductive Films (ACFs) Bonding of Flexible Substrates on Organic Rigid Boards at Room Temperature
Ultrasonic Anisotropic Conductive Films (ACFs) Bonding of Flexible Substrates on Organic Rigid Boards at Room Temperature Kiwon Lee, Hyoung Joon Kim, Il Kim, and Kyung Wook Paik Nano Packaging and Interconnect
More informationSimulation of a New PZT Energy Harvester with a Lower Resonance Frequency Using COMSOL Multiphysics. Zewail City Staff Sep, 2014
Simulation of a New PZT Energy Harvester with a Lower Resonance Frequency Using COMSOL Multiphysics Zewail City Staff Sep, 2014 Outline Introduction. Theoretical Background of Piezoelectric Transducer.
More informationEE C245 ME C218 Introduction to MEMS Design
EE C245 ME C218 Introduction to MEMS Design Fall 2007 Prof. Clark T.-C. Nguyen Dept. of Electrical Engineering & Computer Sciences University of California at Berkeley Berkeley, CA 94720 ecture 15: Beam
More informationPrediction of Micromechanical Behaviour of Elliptical Frp Composites
Prediction of Micromechanical Behaviour of Elliptical Frp Composites Kiranmayee.Nerusu Dept. of Mechanical Engg. P. V. P. Siddhartha Institute of Technology, Vijayawada 520 007, A.P, India. P. Phani Prasanthi
More informationSupporting Information. Light-Induced Bonding and Debonding with Supramolecular Adhesives
Supporting Information Light-Induced Bonding and Debonding with Supramolecular Adhesives Christian Heinzmann, Souleymane Coulibaly, Anita Roulin, Gina L. Fiore,* and Christoph Weder* Adolphe Merkle Institute,
More informationGeology 229 Engineering Geology. Lecture 5. Engineering Properties of Rocks (West, Ch. 6)
Geology 229 Engineering Geology Lecture 5 Engineering Properties of Rocks (West, Ch. 6) Common mechanic properties: Density; Elastic properties: - elastic modulii Outline of this Lecture 1. Uniaxial rock
More informationMechanics of Materials Primer
Mechanics of Materials rimer Notation: A = area (net = with holes, bearing = in contact, etc...) b = total width of material at a horizontal section d = diameter of a hole D = symbol for diameter E = modulus
More informationEE C247B / ME C218 INTRODUCTION TO MEMS DESIGN SPRING 2014 C. Nguyen PROBLEM SET #4
Issued: Wednesday, Mar. 5, 2014 PROBLEM SET #4 Due (at 9 a.m.): Tuesday Mar. 18, 2014, in the EE C247B HW box near 125 Cory. 1. Suppose you would like to fabricate the suspended cross beam structure below
More informationEE C245 ME C218 Introduction to MEMS Design
EE C245 ME C218 Introduction to MEMS Design Fall 2007 Prof. Clark T.-C. Nguyen Dept. of Electrical Engineering & Computer Sciences University of California at Berkeley Berkeley, CA 94720 Lecture 16: Energy
More informationThe numerical simulation research of an Ultra-Light Photovoltaic Cell multilayer composite structure
5th International Conference on Civil, Architectural and Hydraulic Engineering (ICCAHE 2016) The numerical simulation research of an Ultra-Light Photovoltaic Cell multilayer composite structure Kangwen
More informationImaging Methods: Scanning Force Microscopy (SFM / AFM)
Imaging Methods: Scanning Force Microscopy (SFM / AFM) The atomic force microscope (AFM) probes the surface of a sample with a sharp tip, a couple of microns long and often less than 100 Å in diameter.
More informationBecause the third wire carries practically no current (due to the voltmeter's extremely high internal resistance), its resistance will not drop any
Strain gauges If a strip of conductive metal is stretched, it will become skinnier and longer, both changes resulting in an increase of electrical resistance end-to-end. Conversely, if a strip of conductive
More informationMars Ascent Vehicle Hybrid Motor Structural Analysis
Mars Ascent Vehicle Hybrid Motor Structural Analysis MSFC - James Luce ER41 (Summer intern program) NASA Sensitive But Unclassified 1 Background: the MAV MAV: Mars Ascent Vehicle (MAV) is a small rocket
More informationX has a higher value of the Young modulus. Y has a lower maximum tensile stress than X
Bulk Properties of Solids Old Exam Questions Q1. The diagram shows how the stress varies with strain for metal specimens X and Y which are different. Both specimens were stretched until they broke. Which
More informationIntroduction of Nano Science and Tech. Basics of Solid Mechanics in Nanostructures. Nick Fang
Introduction of Nano Science and Tech Basics of Solid Mechanics in Nanostructures Nick Fang Course Website: nanohub.org Compass.illinois.edu ME 498 2006-09 Nick Fang, University of Illinois. All rights
More informationRock Mechanics Laboratory Tests for Petroleum Applications. Rob Marsden Reservoir Geomechanics Advisor Gatwick
Rock Mechanics Laboratory Tests for Petroleum Applications Rob Marsden Reservoir Geomechanics Advisor Gatwick Summary A wide range of well established and proven laboratory tests are available for petroleum
More informationBacillus spores as building blocks for stimuliresponsive materials and nanogenerators
Bacillus spores as building blocks for stimuliresponsive materials and nanogenerators Xi Chen, L Mahadevan, Adam Driks & Ozgur Sahin 1- Estimation of energy densities from the AFM based measurements Supplementary
More informationFIDUCIAL MARKS AS MEASURES OF THIN FILM CRACK ARREST TOUGHNESS
ORAL REFERENCE: ICF100572OR FIDUCIAL MARKS AS MEASURES OF THIN FILM CRACK ARREST TOUGHNESS Alex A. Volinsky 1, Michael L. Kottke 1, Neville R. Moody 3, Indira S. Adhihetty 1 and William W. Gerberich 2
More informationMaterials and Structures. Indian Institute of Technology Kanpur
Introduction to Composite Materials and Structures Nachiketa Tiwari Indian Institute of Technology Kanpur Lecture 16 Behavior of Unidirectional Composites Lecture Overview Mt Material ilaxes in unidirectional
More informationComputationally efficient modelling of pattern dependencies in the micro-embossing of thermoplastic polymers
Computationally efficient modelling of pattern dependencies in the micro-embossing of thermoplastic polymers Hayden Taylor and Duane Boning Microsystems Technology Laboratories Massachusetts Institute
More informationSolid Mechanics Homework Answers
Name: Date: Solid Mechanics Homework nswers Please show all of your work, including which equations you are using, and circle your final answer. Be sure to include the units in your answers. 1. The yield
More informationA Sample Durability Study of a Circuit Board under Random Vibration and Design Optimization
A Sample Durability Study of a Circuit Board under Random Vibration and Design Optimization By: MS.ME Ahmad A. Abbas Ahmad.Abbas@AdvancedCAE.com www.advancedcae.com Sunday, March 07, 2010 Advanced CAE
More informationMECHANICAL PROPERTIES OF SOLIDS
Chapter Nine MECHANICAL PROPERTIES OF SOLIDS MCQ I 9.1 Modulus of rigidity of ideal liquids is (a) infinity. (b) zero. (c) unity. (d) some finite small non-zero constant value. 9. The maximum load a wire
More informationCOURSE OUTLINE. Introduction Signals and Noise Filtering Sensors: Piezoelectric Force Sensors. Sensors, Signals and Noise 1
Sensors, Signals and Noise 1 COURSE OUTLINE Introduction Signals and Noise Filtering Sensors: Piezoelectric Force Sensors Piezoelectric Force Sensors 2 Piezoelectric Effect and Materials Piezoelectric
More informationStrain Measurement MEASUREMENT EXPERIMENT
Strain Measurement MEASUREMENT EXPERIMENT 1. OBJECT The objective of this experiment is to become familiar with the electric resistance strain gage techniques and utilize such gages for the determination
More information