Design of a Cheap Thermal Switch. ENGR 0135 Due: 10/9/15 Professor Qing-Ming Wang Madison Milligan, Josh Haupt, Caroline Collopy
|
|
- Charlene Bryant
- 6 years ago
- Views:
Transcription
1 Design of a Cheap Thermal Switch ENGR 0135 Due: 10/9/15 Professor Qing-Ming Wang Madison Milligan, Josh Haupt, Caroline Collopy
2 ABSTRACT The purpose of this design project is to come up with a way to develop a cheaper version of a currently used thermal switch. This is to be done by reducing the temperature needed to cause enough stress in the central aluminum strip, which will make it snap and connect with either the steel plate to its left or the plate to its right. To be able to reduce the temperature however, the cross sectional area of each strip must be modified. So, we came up with a formula which incorporates the dimensions of the cross sectional area of the aluminum strip and the temperature change in order to develop a relationship between all variables in question, and to find a potential solution. We did this by using the connection between the deformation in each strip and between the forces acting in the strips; then by solving the system of equations, we found one formula. Included in this paper is an introduction to the problem, the steps taken to find the final formula, and an explanation as to how we used it to back up our final design solution. INTRODUCTION A thermal switch has been designed for incorporation into a low cost product. The switch consists of three metal strips clamped rigidly together in an assembly of insulating pieces. Currently, the aluminum strip snaps to the side at a temperature increase of about 180 F. We are asked to vary the dimensions of the central aluminum strip so the circuit will close at a temperature increase of only 105 F instead. We intend to solve this by deriving a formula that incorporates all variables in question. We hypothesize that if the temperature of closure is to be lowered, the cross sectional area will need to be lowered as well because the two are directly proportional.
3 ANALYSIS & DESIGN All calculations and logic used to develop a formula relating change in temperature to the crosssectional area of the aluminum strip are shown in Figure 1. Figure 1: Initial calculations for a formula
4 We verified this formula by plugging in the original dimensions and ensuring that the result was in fact 180 F. Using this formula, we re-arranged the variables to make it easier to find possible solutions for the width and thickness that would allow the temperature change to be 105 F. Those calculations are shown in figure 2. Figure 2: Manipulation of formula to find potential new Dimensions for aluminum strip ta also cannot be 0. Since the ultimate goal is to make a cheaper thermal switch, the cross sectional area also needs to be minimized. After trying out a few options, we realized that
5 regardless of the dimensions chosen, the cross sectional area will be reduced significantly from the original area of in² because of the drop in the desired change in temperature. A few suggestions are as followed: Option 1 ta = in wa = 1.51e-6 in Cross-sectional area = 8.17e-8 in 2 Option 2 ta = in wa = 1.21e-5 in Cross-sectional area = 8.83e-8 in 2 Option 3 ta = in wa = 3.30e-5 in Cross-sectional area = 9.90e-7 in 2 As ta decreases, the cross sectional area increases, so the ideal pair to pick would be the first. It allows for the temperature change as well as minimizes cross sectional area. (All original copies of the calculations are attached) DISCUSSION As the strips are attached at both ends, the total deformation of the aluminum strip (before failure) must be zero. When the temperature is raised on the switch, the stress induced on the aluminum will be compressive and the rigid supports will push the strip axially. With this in mind, we were able to use the following equations in the derivation of our formula: 1 δ!"!"# = δ! + δ! 2 αδtl + σl E = 0 We also used Euler s formula for the buckling of columns, along with the formula for the minimum second moment of inertia of the cross-section (3 and 4 respectively). 3 P!" = 4πEI L! 4 I = w!t!! 12 Using these fundamental formulas and our understanding of thermal expansion and statically indeterminate members, we derived our formula for determining the thickness and width of the aluminum strip.
6 CONCLUSION In conclusion, after relating the deformation of the switch s Aluminum and Steel components to give us ΔT as a function of the Aluminum strip s dimensions, we found that ta decreases, the cross sectional area increases. In order for the product to remain inexpensive, we decided on the experimental dimensions that allowed the smallest cross-sectional area while still resulted in only ΔT=105 F required for operation. Those dimensions were: t! = inches w! =1.51e-6 inches Our design was successful in the sense that it does decrease the change in temperature needed for the switch to activate to only 105 F while adhering to given restraints. However, in order to do this, we had to set width to a virtually non-existent size. This raises concerns in durability or manufacturing practicality for the product. To improve the design, we might suggest that the thickness and length may be allowed to vary. The lengths of all three strips must remain equal to each other, however lengthening them overall would also give more flexibility and options in way to decrease required changed in temperature while upholding cost efficiency.
Design Project 1 Design of a Cheap Thermal Switch
Design Project 1 Design of a Cheap Thermal Switch ENGR 0135 Statics and Mechanics of Materials 1 October 20 th, 2015 Professor: Dr. Guofeng Wang Group Members: Chad Foster Thomas Hinds Kyungchul Yoon John
More informationDesign Project 1 Design of a Cheap Thermal Switch ENGR 0135 October 13, 2016 Sangyeop Lee Jordan Gittleman Noah Sargent Seth Strayer Desmond Zheng
1 Design Project 1 Design of a Cheap Thermal Switch ENGR 0135 October 13, 2016 Sangyeop Lee Jordan Gittleman Noah Sargent Seth Strayer Desmond Zheng 2 Abstract This report will analyze our calculations,
More informationMAAE 2202 A. Come to the PASS workshop with your mock exam complete. During the workshop you can work with other students to review your work.
It is most beneficial to you to write this mock final exam UNDER EXAM CONDITIONS. This means: Complete the exam in 3 hours. Work on your own. Keep your textbook closed. Attempt every question. After the
More informationDesign of a Bi-Metallic Strip for a Thermal Switch. Team Design Project 2. Dr. William Slaughter. ENGR0145 Statics and Mechanics of Materials II
Design of a Bi-Metallic Strip for a Thermal Switch Team Design Project 2 Dr. William Slaughter ENGR0145 Statics and Mechanics of Materials II April 10, 2015 Jacob Feid Derek Nichols ABSTRACT The goal of
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 informationCritical Load columns buckling critical load
Buckling of Columns Buckling of Columns Critical Load Some member may be subjected to compressive loadings, and if these members are long enough to cause the member to deflect laterally or sideway. To
More informationCIV 207 Winter For practice
CIV 07 Winter 009 Assignment #10 Friday, March 0 th Complete the first three questions. Submit your work to Box #5 on the th floor of the MacDonald building by 1 noon on Tuesday March 31 st. No late submissions
More informationUnified Quiz M4 May 7, 2008 M - PORTION
9:00-10: 00 (last four digits) 32-141 Unified Quiz M4 May 7, 2008 M - PORTION Put the last four digits of your MIT ID # on each page of the exam. Read all questions carefully. Do all work on that question
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 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 informationSize Effects In the Crushing of Honeycomb Structures
45th AIAA/ASME/ASCE/AHS/ASC Structures, Structural Dynamics & Materials Conference 19-22 April 2004, Palm Springs, California AIAA 2004-1640 Size Effects In the Crushing of Honeycomb Structures Erik C.
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 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 informationGlossary Innovative Measurement Solutions
Glossary GLOSSARY OF TERMS FOR TRANSDUCERS, LOAD CELLS AND WEIGH MODULES This purpose of this document is to provide a comprehensive, alphabetical list of terms and definitions commonly employed in the
More informationUnit M1.5 Statically Indeterminate Systems
Unit M1.5 Statically Indeterminate Systems Readings: CDL 2.1, 2.3, 2.4, 2.7 16.001/002 -- Unified Engineering Department of Aeronautics and Astronautics Massachusetts Institute of Technology LEARNING OBJECTIVES
More informationSymmetric Bending of Beams
Symmetric Bending of Beams beam is any long structural member on which loads act perpendicular to the longitudinal axis. Learning objectives Understand the theory, its limitations and its applications
More informationStatics Principles. The laws of motion describe the interaction of forces acting on a body. Newton s First Law of Motion (law of inertia):
Unit 2 Review Statics Statics Principles The laws of motion describe the interaction of forces acting on a body Newton s First Law of Motion (law of inertia): An object in a state of rest or uniform motion
More informationSteel Cross Sections. Structural Steel Design
Steel Cross Sections Structural Steel Design PROPERTIES OF SECTIONS Perhaps the most important properties of a beam are the depth and shape of its cross section. There are many to choose from, and there
More informationLecture 11: The Stiffness Method. Introduction
Introduction Although the mathematical formulation of the flexibility and stiffness methods are similar, the physical concepts involved are different. We found that in the flexibility method, the unknowns
More informationRODS: STATICALLY INDETERMINATE MEMBERS
RODS: STTICLLY INDETERMINTE MEMERS Statically Indeterminate ackground In all of the problems discussed so far, it was possible to determine the forces and stresses in the members by utilizing the equations
More informationDirect and Shear Stress
Direct and Shear Stress 1 Direct & Shear Stress When a body is pulled by a tensile force or crushed by a compressive force, the loading is said to be direct. Direct stresses are also found to arise when
More informationENGN1300: Structural Analysis
ENGN1300: Structural Analysis Homework 4 Due Wednesday, March 3, 2010 Division of Engineering Brown University 1. For the statically indeterminate structure shown below, all members have identical values
More informationMechanical Design in Optical Engineering
OPTI Buckling Buckling and Stability: As we learned in the previous lectures, structures may fail in a variety of ways, depending on the materials, load and support conditions. We had two primary concerns:
More informationMechanics of Materials II. Chapter III. A review of the fundamental formulation of stress, strain, and deflection
Mechanics of Materials II Chapter III A review of the fundamental formulation of stress, strain, and deflection Outline Introduction Assumtions and limitations Axial loading Torsion of circular shafts
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 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 informationExternal Pressure... Thermal Expansion in un-restrained pipeline... The critical (buckling) pressure is calculated as follows:
External Pressure... The critical (buckling) pressure is calculated as follows: P C = E. t s ³ / 4 (1 - ν ha.ν ah ) R E ³ P C = Critical buckling pressure, kn/m² E = Hoop modulus in flexure, kn/m² t s
More informationFree Body Diagram: Solution: The maximum load which can be safely supported by EACH of the support members is: ANS: A =0.217 in 2
Problem 10.9 The angle β of the system in Problem 10.8 is 60. The bars are made of a material that will safely support a tensile normal stress of 8 ksi. Based on this criterion, if you want to design the
More informationDownloaded from Downloaded from / 1
PURWANCHAL UNIVERSITY III SEMESTER FINAL EXAMINATION-2002 LEVEL : B. E. (Civil) SUBJECT: BEG256CI, Strength of Material Full Marks: 80 TIME: 03:00 hrs Pass marks: 32 Candidates are required to give their
More informationAPPLICATION OF DIFFERENTIAL TRANSFORMATION METHOD FOR STABILITY ANALYSIS OF EULER BERNOULLI COLUMN
APPLICATION OF DIFFERENTIAL TRANSFORMATION METHOD FOR STABILITY ANALYSIS OF EULER BERNOULLI COLUMN Muralikrishnan.K 1, C.S.C. Devadass 2, M.G. Rajendran 3 1 P. G. Student, School of Civil Engineering Karunya
More informationLab Exercise #3: Torsion
Lab Exercise #3: Pre-lab assignment: Yes No Goals: 1. To evaluate the equations of angular displacement, shear stress, and shear strain for a shaft undergoing torsional stress. Principles: testing of round
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 informationCork Institute of Technology. Autumn 2007 Mechanics of Materials (Time: 3 Hours)
Cork Institute of Technology Bachelor of Engineering (Honours) in Mechanical Engineering- Stage 2 (NFQ Level 8) Autumn 2007 Mechanics of Materials (Time: 3 Hours) Instructions Answer Five Questions Question
More informationModal Analysis: What it is and is not Gerrit Visser
Modal Analysis: What it is and is not Gerrit Visser What is a Modal Analysis? What answers do we get out of it? How is it useful? What does it not tell us? In this article, we ll discuss where a modal
More informationINSPIRE GK12 Lesson Plan. Elastic Deformation of Materials: An Investigation of Hooke s Law Length of Lesson
Lesson Title Elastic Deformation of Materials: An Investigation of Hooke s Law Length of Lesson 1.5 hours Created By Justin Warren Subject Physics Grade Level 11-12 State Standards Physics: 1 c, d, f;
More informationUnit 18 Other Issues In Buckling/Structural Instability
Unit 18 Other Issues In Buckling/Structural Instability Readings: Rivello Timoshenko Jones 14.3, 14.5, 14.6, 14.7 (read these at least, others at your leisure ) Ch. 15, Ch. 16 Theory of Elastic Stability
More informationLAB 9: EQUILIBRIUM OF NON-PARALLEL FORCES
Name Date artners LAB 9: EQUILIBRIUM O NON-ARALLEL ORCES 145 OBJECTIVES OVERVIEW To study the components of forces To examine forces in static equilibrium To examine torques To study the conditions for
More informationTechnical Note PP TN Engineering Considerations for Temperature Change
Technical Note PP 814 - TN Engineering Considerations for Temperature Change www.performancepipe.com Like most materials, polyethylene is affected by temperature change. However, polyethylene s response
More informationCE 320 Structures Laboratory 1 Flexure Fall 2006
CE 320 Structures Laboratory 1 Flexure Fall 2006 General Note: All structures labs are to be conducted by teams of no more than four students. Teams are expected to meet to decide on an experimental design
More informationMECHANICS OF MATERIALS. Prepared by Engr. John Paul Timola
MECHANICS OF MATERIALS Prepared by Engr. John Paul Timola Mechanics of materials branch of mechanics that studies the internal effects of stress and strain in a solid body. stress is associated with the
More informationRODS: THERMAL STRESS AND STRESS CONCENTRATION
RODS: HERML SRESS ND SRESS CONCENRION Example 5 rod of length L, cross-sectional area, and modulus of elasticity E, has been placed inside a tube of the same length L, but of cross-sectional area and modulus
More informationAircraft Stress Analysis and Structural Design Summary
Aircraft Stress Analysis and Structural Design Summary 1. Trusses 1.1 Determinacy in Truss Structures 1.1.1 Introduction to determinacy A truss structure is a structure consisting of members, connected
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 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 informationBOOK OF COURSE WORKS ON STRENGTH OF MATERIALS FOR THE 2 ND YEAR STUDENTS OF THE UACEG
BOOK OF COURSE WORKS ON STRENGTH OF MATERIALS FOR THE ND YEAR STUDENTS OF THE UACEG Assoc.Prof. Dr. Svetlana Lilkova-Markova, Chief. Assist. Prof. Dimitar Lolov Sofia, 011 STRENGTH OF MATERIALS GENERAL
More information8/1/2009. CAE 7962 Presentation
CAE 7962 Presentation Gavin Patey Dameion Moores Aaron Henstridge Ashley Burke Brendan Harvey Fabio Faragalli Introduction Choosing mesh properties Explanation of the types of studies available and the
More informationMechanical Design in Optical Engineering. For a prismatic bar of length L in tension by axial forces P we have determined:
Deformation of Axial Members For a prismatic bar of length L in tension by axial forces P we have determined: σ = P A δ ε = L It is important to recall that the load P must act on the centroid of the cross
More informationLecture 8: Flexibility Method. Example
ecture 8: lexibility Method Example The plane frame shown at the left has fixed supports at A and C. The frame is acted upon by the vertical load P as shown. In the analysis account for both flexural and
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 informationChapter 12 Elastic Stability of Columns
Chapter 12 Elastic Stability of Columns Axial compressive loads can cause a sudden lateral deflection (Buckling) For columns made of elastic-perfectly plastic materials, P cr Depends primarily on E and
More information9 MECHANICAL PROPERTIES OF SOLIDS
9 MECHANICAL PROPERTIES OF SOLIDS Deforming force Deforming force is the force which changes the shape or size of a body. Restoring force Restoring force is the internal force developed inside the body
More informationMembers Subjected to Combined Loads
Members Subjected to Combined Loads Combined Bending & Twisting : In some applications the shaft are simultaneously subjected to bending moment M and Torque T.The Bending moment comes on the shaft due
More informationIntroduction to Continuous Systems. Continuous Systems. Strings, Torsional Rods and Beams.
Outline of Continuous Systems. Introduction to Continuous Systems. Continuous Systems. Strings, Torsional Rods and Beams. Vibrations of Flexible Strings. Torsional Vibration of Rods. Bernoulli-Euler Beams.
More informationSTRESS, STRAIN AND DEFORMATION OF SOLIDS
VELAMMAL COLLEGE OF ENGINEERING AND TECHNOLOGY, MADURAI 625009 DEPARTMENT OF CIVIL ENGINEERING CE8301 STRENGTH OF MATERIALS I -------------------------------------------------------------------------------------------------------------------------------
More informationto introduce the principles of stability and elastic buckling in relation to overall buckling, local buckling
to introduce the principles of stability and elastic buckling in relation to overall buckling, local buckling In the case of elements subjected to compressive forces, secondary bending effects caused by,
More informationUNIT I SIMPLE STRESSES AND STRAINS
Subject with Code : SM-1(15A01303) Year & Sem: II-B.Tech & I-Sem SIDDHARTH GROUP OF INSTITUTIONS :: PUTTUR Siddharth Nagar, Narayanavanam Road 517583 QUESTION BANK (DESCRIPTIVE) UNIT I SIMPLE STRESSES
More informationCOMPRESSION AND BENDING STIFFNESS OF FIBER-REINFORCED ELASTOMERIC BEARINGS. Abstract. Introduction
COMPRESSION AND BENDING STIFFNESS OF FIBER-REINFORCED ELASTOMERIC BEARINGS Hsiang-Chuan Tsai, National Taiwan University of Science and Technology, Taipei, Taiwan James M. Kelly, University of California,
More informationTheory of structure I 2006/2013. Chapter one DETERMINACY & INDETERMINACY OF STRUCTURES
Chapter one DETERMINACY & INDETERMINACY OF STRUCTURES Introduction A structure refers to a system of connected parts used to support a load. Important examples related to civil engineering include buildings,
More informationProject. First Saved Monday, June 27, 2011 Last Saved Wednesday, June 29, 2011 Product Version 13.0 Release
Project First Saved Monday, June 27, 2011 Last Saved Wednesday, June 29, 2011 Product Version 13.0 Release Contents Units Model (A4, B4) o Geometry! Solid Bodies! Parts! Parts! Body Groups! Parts! Parts
More informationMECHANICS OF MATERIALS
Third E CHAPTER 1 Introduction MECHANICS OF MATERIALS Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf Lecture Notes: J. Walt Oler Texas Tech University Concept of Stress Contents Concept of Stress
More informationSTRAIN GAUGES YEDITEPE UNIVERSITY DEPARTMENT OF MECHANICAL ENGINEERING
STRAIN GAUGES YEDITEPE UNIVERSITY DEPARTMENT OF MECHANICAL ENGINEERING 1 YEDITEPE UNIVERSITY ENGINEERING FACULTY MECHANICAL ENGINEERING LABORATORY 1. Objective: Strain Gauges Know how the change in resistance
More informationME 025 Mechanics of Materials
ME 025 Mechanics of Materials General Information: Term: 2019 Summer Session Instructor: Staff Language of Instruction: English Classroom: TBA Office Hours: TBA Class Sessions Per Week: 5 Total Weeks:
More informationIf the number of unknown reaction components are equal to the number of equations, the structure is known as statically determinate.
1 of 6 EQUILIBRIUM OF A RIGID BODY AND ANALYSIS OF ETRUCTURAS II 9.1 reactions in supports and joints of a two-dimensional structure and statically indeterminate reactions: Statically indeterminate structures
More informationConceptual question Conceptual question 12.2
Conceptual question 12.1 rigid cap of weight W t g r A thin-walled tank (having an inner radius of r and wall thickness t) constructed of a ductile material contains a gas with a pressure of p. A rigid
More informationMEMS Project 2 Assignment. Design of a Shaft to Transmit Torque Between Two Pulleys
MEMS 029 Project 2 Assignment Design of a Shaft to Transmit Torque Between Two Pulleys Date: February 5, 206 Instructor: Dr. Stephen Ludwick Product Definition Shafts are incredibly important in order
More informationCHAPTER 5 Statically Determinate Plane Trusses
CHAPTER 5 Statically Determinate Plane Trusses TYPES OF ROOF TRUSS TYPES OF ROOF TRUSS ROOF TRUSS SETUP ROOF TRUSS SETUP OBJECTIVES To determine the STABILITY and DETERMINACY of plane trusses To analyse
More informationWhat Every Engineer Should Know About Structures
What Every Engineer Should Know About Structures Part C - Axial Strength of Materials by Professor Patrick L. Glon, P.E. This is a continuation of a series of courses in the area of study of physics called
More informationChapter 5 CENTRIC TENSION OR COMPRESSION ( AXIAL LOADING )
Chapter 5 CENTRIC TENSION OR COMPRESSION ( AXIAL LOADING ) 5.1 DEFINITION A construction member is subjected to centric (axial) tension or compression if in any cross section the single distinct stress
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 informationCHAPTER 5 Statically Determinate Plane Trusses TYPES OF ROOF TRUSS
CHAPTER 5 Statically Determinate Plane Trusses TYPES OF ROOF TRUSS 1 TYPES OF ROOF TRUSS ROOF TRUSS SETUP 2 ROOF TRUSS SETUP OBJECTIVES To determine the STABILITY and DETERMINACY of plane trusses To analyse
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 informationQUESTION BANK SEMESTER: III SUBJECT NAME: MECHANICS OF SOLIDS
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 Hooke s law. 3. Define modular ratio,
More informationEffect of uniform and gradient thermal loadings on cylindrical steel reservoirs (analytical investigation)
Journal of Civil Engineering and Construction Technology Vol. (3), pp. 9-3, March 13 Available online at http://www.academicjournals.org/jcect DOI:.597/JCECT1.91 ISS 11-3 13 Academic Journals Full Length
More informationSN QUESTION YEAR MARK 1. State and prove the relationship between shearing stress and rate of change of bending moment at a section in a loaded beam.
ALPHA COLLEGE OF ENGINEERING AND TECHNOLOGY DEPARTMENT OF MECHANICAL ENGINEERING MECHANICS OF SOLIDS (21000) ASSIGNMENT 1 SIMPLE STRESSES AND STRAINS SN QUESTION YEAR MARK 1 State and prove the relationship
More informationInteractive Buckling of Cold-Formed Steel Sections Applied in Pallet Rack Upright Members
Interactive Buckling of Cold-Formed Steel Sections Applied in Pallet Rack Upright Members D. Dubina, V. Ungureanu, A. Crisan Politehnica University of Timişoara Peculiarities of cold-formed thin-walled
More information1 Force Sensing. Lecture Notes. 1.1 Load Cell. 1.2 Stress and Strain
Lecture Notes 1 Force Sensing 1.1 Load Cell A Load Cell is a structure which supports the load and deflects a known amount in response to applied forces and torques. The deflections are measured to characterize
More informationTHE INFLUENCE OF THERMAL ACTIONS AND COMPLEX SUPPORT CONDITIONS ON THE MECHANICAL STATE OF SANDWICH STRUCTURE
Journal of Applied Mathematics and Computational Mechanics 013, 1(4), 13-1 THE INFLUENCE OF THERMAL ACTIONS AND COMPLEX SUPPORT CONDITIONS ON THE MECHANICAL STATE OF SANDWICH STRUCTURE Jolanta Błaszczuk
More informationSNAP Centre Workshop. Solving Systems of Equations
SNAP Centre Workshop Solving Systems of Equations 35 Introduction When presented with an equation containing one variable, finding a solution is usually done using basic algebraic manipulation. Example
More informationHigh Tech High Top Hat Technicians. An Introduction to Solid Mechanics. Is that supposed to bend there?
High Tech High Top Hat Technicians An Introduction to Solid Mechanics Or Is that supposed to bend there? Why don't we fall through the floor? The power of any Spring is in the same proportion with the
More informationStructural Dynamics Lecture Eleven: Dynamic Response of MDOF Systems: (Chapter 11) By: H. Ahmadian
Structural Dynamics Lecture Eleven: Dynamic Response of MDOF Systems: (Chapter 11) By: H. Ahmadian ahmadian@iust.ac.ir Dynamic Response of MDOF Systems: Mode-Superposition Method Mode-Superposition Method:
More informationDissectable Leyden Jar P6-3380
WWW.ARBORSCI.COM Dissectable Leyden Jar P6-3380 BACKGROUND: This apparatus is designed to demonstrate the principles of static electricity, the use of a Leyden jar, and to allow the student to investigate
More informationMechanical Properties of Materials
Mechanical Properties of Materials Strains Material Model Stresses Learning objectives Understand the qualitative and quantitative description of mechanical properties of materials. Learn the logic of
More informationInvestigation of basic elements loading and tension of heavy hydraulic presses for metallurgical production
Investigation of basic elements loading and tension of heavy hydraulic presses for metallurgical production Ganush V. I. National metallurgical academe of Ukraine Ostroverhov N. P., Sultan A. V., Dzichkovky
More informationChapter 4 Deflection and Stiffness
Chapter 4 Deflection and Stiffness Asst. Prof. Dr. Supakit Rooppakhun Chapter Outline Deflection and Stiffness 4-1 Spring Rates 4-2 Tension, Compression, and Torsion 4-3 Deflection Due to Bending 4-4 Beam
More information1. Introduction. 1.1 Overview of Study:
1. Introduction 1.1 Overview of Study: Hot and cold fluid passing through long pipes causes thermal expansion and contraction in the piping system. The fluid passing through pipes also creates fluctuations
More informationM.S Comprehensive Examination Analysis
UNIVERSITY OF CALIFORNIA, BERKELEY Spring Semester 2014 Dept. of Civil and Environmental Engineering Structural Engineering, Mechanics and Materials Name:......................................... M.S Comprehensive
More information1.105 Solid Mechanics Laboratory
1.105 Solid Mechanics Laboratory General Information Fall 2003 Prof. Louis Bucciarelli Rm 5-213 x3-4061 llbjr@mit.edu TA: Attasit Korchaiyapruk, Pong Rm 5-330B x 3-5170 attasit@mit.edu Athena Locker: /mit/1.105/
More informationIf you take CT5143 instead of CT4143 then write this at the first of your answer sheets and skip problem 4 and 6.
Delft University of Technology Faculty of Civil Engineering and Geosciences Structural Mechanics Section Write your name and study number at the top right-hand of your work. Exam CT4143 Shell Analysis
More informationSOLUTION (17.3) Known: A simply supported steel shaft is connected to an electric motor with a flexible coupling.
SOLUTION (17.3) Known: A simply supported steel shaft is connected to an electric motor with a flexible coupling. Find: Determine the value of the critical speed of rotation for the shaft. Schematic and
More informationENG2000 Chapter 7 Beams. ENG2000: R.I. Hornsey Beam: 1
ENG2000 Chapter 7 Beams ENG2000: R.I. Hornsey Beam: 1 Overview In this chapter, we consider the stresses and moments present in loaded beams shear stress and bending moment diagrams We will also look at
More informationtwenty steel construction: columns & tension members ARCHITECTURAL STRUCTURES: FORM, BEHAVIOR, AND DESIGN DR. ANNE NICHOLS FALL 2013 lecture
ARCHITECTURAL STRUCTURES: FORM, BEHAVIOR, AND DESIGN DR. ANNE NICHOLS Cor-Ten Steel Sculpture By Richard Serra Museum of Modern Art Fort Worth, TX (AISC - Steel Structures of the Everyday) FALL 2013 lecture
More informationModule 2 Selection of Materials and Shapes. IIT, Bombay
Module Selection of Materials and Shapes Lecture 3 Selection of Materials - II Instructional objectives This is a continuation of the previous lecture. By the end of this lecture, the student will further
More informationMECE 3321: MECHANICS OF SOLIDS CHAPTER 5
MECE 3321: MECHANICS OF SOLIDS CHAPTER 5 SAMANTHA RAMIREZ TORSION Torque A moment that tends to twist a member about its longitudinal axis 1 TORSIONAL DEFORMATION OF A CIRCULAR SHAFT Assumption If the
More informationChapter 1 General Introduction Instructor: Dr. Mürüde Çelikağ Office : CE Building Room CE230 and GE241
CIVL222 STRENGTH OF MATERIALS Chapter 1 General Introduction Instructor: Dr. Mürüde Çelikağ Office : CE Building Room CE230 and GE241 E-mail : murude.celikag@emu.edu.tr 1. INTRODUCTION There are three
More informationFatigue Life Analysis Of Joint Bar Of Insulated Rail Joint
Fatigue Life Analysis Of Joint Bar Of Insulated Rail Joint Washimraja Sheikh, Piyush M. Sirsat, Nakul K. Mahalle RTM Nagpur University, Priyadarshini College of Engineering, Assistant Professor, Department
More informationMATERIALS. Why do things break? Why are some materials stronger than others? Why is steel tough? Why is glass brittle?
MATERIALS Why do things break? Why are some materials stronger than others? Why is steel tough? Why is glass brittle? What is toughness? strength? brittleness? Elemental material atoms: A. Composition
More informationTolerance Ring Improvement for Reducing Metal Scratch
International Journal of Scientific and Research Publications, Volume 2, Issue 11, November 2012 1 Tolerance Ring Improvement for Reducing Metal Scratch Pattaraweerin Woraratsoontorn*, Pitikhate Sooraksa**
More informationFLEXIBILITY METHOD FOR INDETERMINATE FRAMES
UNIT - I FLEXIBILITY METHOD FOR INDETERMINATE FRAMES 1. What is meant by indeterminate structures? Structures that do not satisfy the conditions of equilibrium are called indeterminate structure. These
More informationDesign Calculations & Real Behaviour (Hambly s Paradox)
Design Calculations & Real Behaviour (Hambly s Paradox) Carol Serban 1. Introduction The present work is meant to highlight the idea that engineering design calculations (lately most of the time using
More informationEsben Byskov. Elementary Continuum. Mechanics for Everyone. With Applications to Structural Mechanics. Springer
Esben Byskov Elementary Continuum Mechanics for Everyone With Applications to Structural Mechanics Springer Contents Preface v Contents ix Introduction What Is Continuum Mechanics? "I Need Continuum Mechanics
More information