Areas and Centroids. Nothing. Straight Horizontal line. Straight Sloping Line. Parabola. Cubic

Similar documents
Derivatives Math 120 Calculus I D Joyce, Fall 2013

Math 113 HW #5 Solutions

f(a + h) f(a) f (a) = lim

Tangent Lines and Rates of Change

Pressure. Pressure. Atmospheric pressure. Conceptual example 1: Blood pressure. Pressure is force per unit area:

1.6. Analyse Optimum Volume and Surface Area. Maximum Volume for a Given Surface Area. Example 1. Solution

Determine the perimeter of a triangle using algebra Find the area of a triangle using the formula

Sections 3.1/3.2: Introducing the Derivative/Rules of Differentiation

ACT Math Facts & Formulas

13 PERIMETER AND AREA OF 2D SHAPES

SAT Subject Math Level 1 Facts & Formulas

New Vocabulary volume

Instantaneous Rate of Change:

EC201 Intermediate Macroeconomics. EC201 Intermediate Macroeconomics Problem set 8 Solution

2 Limits and Derivatives

Perimeter, Area and Volume of Regular Shapes

Research on the Anti-perspective Correction Algorithm of QR Barcode

Math Test Sections. The College Board: Expanding College Opportunity

Section 2.3 Solving Right Triangle Trigonometry

Answers to Exercises. Answers to Exercises 24.

f(x) f(a) x a Our intuition tells us that the slope of the tangent line to the curve at the point P is m P Q =

CHAPTER TWO. f(x) Slope = f (3) = Rate of change of f at 3. x 3. f(1.001) f(1) Average velocity = s(0.8) s(0) 0.8 0

Average and Instantaneous Rates of Change: The Derivative

Lecture 10: What is a Function, definition, piecewise defined functions, difference quotient, domain of a function

M(0) = 1 M(1) = 2 M(h) = M(h 1) + M(h 2) + 1 (h > 1)

MATHEMATICS FOR ENGINEERING DIFFERENTIATION TUTORIAL 1 - BASIC DIFFERENTIATION

Notes: Most of the material in this chapter is taken from Young and Freedman, Chap. 12.

2.1: The Derivative and the Tangent Line Problem

Verifying Numerical Convergence Rates

SAT Math Facts & Formulas

The Derivative as a Function

Geometric Stratification of Accounting Data

Chapter 7 Numerical Differentiation and Integration

Section 3.3. Differentiation of Polynomials and Rational Functions. Difference Equations to Differential Equations

In other words the graph of the polynomial should pass through the points

Lecture 8 Bending & Shear Stresses on Beams

Warm medium, T H T T H T L. s Cold medium, T L

Structural Axial, Shear and Bending Moments

FINITE DIFFERENCE METHODS

Mechanics of Materials. Chapter 4 Shear and Moment In Beams

f(x + h) f(x) h as representing the slope of a secant line. As h goes to 0, the slope of the secant line approaches the slope of the tangent line.

Once you have reviewed the bulletin, please

SAT Math Must-Know Facts & Formulas

Recitation #5. Understanding Shear Force and Bending Moment Diagrams

The EOQ Inventory Formula

ENGINEERING SCIENCE H1 OUTCOME 1 - TUTORIAL 3 BENDING MOMENTS EDEXCEL HNC/D ENGINEERING SCIENCE LEVEL 4 H1 FORMERLY UNIT 21718P

The use of visualization for learning and teaching mathematics

Projective Geometry. Projective Geometry

Heat Exchangers. Heat Exchanger Types. Heat Exchanger Types. Applied Heat Transfer Part Two. Topics of This chapter

MECHANICS OF SOLIDS - BEAMS TUTORIAL 2 SHEAR FORCE AND BENDING MOMENTS IN BEAMS

Shear Force and Moment Diagrams

Shear and Moment Diagrams. Shear and Moment Diagrams. Shear and Moment Diagrams. Shear and Moment Diagrams. Shear and Moment Diagrams

Volumes of Pyramids and Cones. Use the Pythagorean Theorem to find the value of the variable. h 2 m. 1.5 m 12 in. 8 in. 2.5 m

EDEXCEL NATIONAL CERTIFICATE/DIPLOMA MECHANICAL PRINCIPLES AND APPLICATIONS NQF LEVEL 3 OUTCOME 1 - LOADING SYSTEMS

UNIFORM FLOW. Key words Uniform flow; most economical cross-section; discharge; velocity; erosion; sedimentation

Grade 12 Assessment Exemplars

A strong credit score can help you score a lower rate on a mortgage

An inquiry into the multiplier process in IS-LM model

Water Pressure and Pressure Forces

The modelling of business rules for dashboard reporting using mutual information

Elements of a graph. Click on the links below to jump directly to the relevant section

Recall from last time: Events are recorded by local observers with synchronized clocks. Event 1 (firecracker explodes) occurs at x=x =0 and t=t =0

2.12 Student Transportation. Introduction

Math 229 Lecture Notes: Product and Quotient Rules Professor Richard Blecksmith

CHAPTER 8: DIFFERENTIAL CALCULUS

Chapter 10: Refrigeration Cycles

6. Differentiating the exponential and logarithm functions

Chapter 6 Tail Design

Catalogue no XIE. Survey Methodology. December 2004

Shell and Tube Heat Exchanger

Solutions by: KARATUĞ OZAN BiRCAN. PROBLEM 1 (20 points): Let D be a region, i.e., an open connected set in

Note nine: Linear programming CSE Linear constraints and objective functions. 1.1 Introductory example. Copyright c Sanjoy Dasgupta 1

Chapter 11. Limits and an Introduction to Calculus. Selected Applications

Chapter 4. Moment - the tendency of a force to rotate an object

THE GEOMETRY OF PYRAMIDS

Writing Mathematics Papers

- 1 - Handout #22 May 23, 2012 Huffman Encoding and Data Compression. CS106B Spring Handout by Julie Zelenski with minor edits by Keith Schwarz

Introduction to Beam. Area Moments of Inertia, Deflection, and Volumes of Beams

4.4 VOLUME AND SURFACE AREA

3 Ans. 1 of my $30. 3 on. 1 on ice cream and the rest on 2011 MATHCOUNTS STATE COMPETITION SPRINT ROUND

2-1 Position, Displacement, and Distance

In order to describe motion you need to describe the following properties.

KM client format supported by KB valid from 13 May 2015

Deflections. Question: What are Structural Deflections?

Plot the following two points on a graph and draw the line that passes through those two points. Find the rise, run and slope of that line.

6. LECTURE 6. Objectives

Graphing Linear Equations

Binary Search Trees. Adnan Aziz. Heaps can perform extract-max, insert efficiently O(log n) worst case

Theoretical calculation of the heat capacity

Torque and Rotational Equilibrium

Unemployment insurance/severance payments and informality in developing countries

Compute the derivative by definition: The four step procedure

Problem 1: Computation of Reactions. Problem 2: Computation of Reactions. Problem 3: Computation of Reactions

Optimized Data Indexing Algorithms for OLAP Systems

Worksheet 1. What You Need to Know About Motion Along the x-axis (Part 1)

Bending Stress in Beams

Copyright 2011 Casa Software Ltd. Centre of Mass

Factoring Synchronous Grammars By Sorting

What Does Your Quadratic Look Like? EXAMPLES

Statics of Structural Supports

Transcription:

Constructing Sear and Moment Diagrams Areas and Centroids Curve Equation Sape Centroid (From Fat End of Figure) Area Noting Noting a x 0 Straigt Horizontal line /2 Straigt Sloping Line /3 /2 Paraola /4 /3 is te lengt of te memer To Solve For Te Reactions: Cuic /5 /4 1) Draw a free ody of te eam sowing any actual distriuted loads. 2) Draw a second free ody, replacing any distriuted loads wit teir equivalent concentrated loads. Te magnitude of te loads can e computed from teir areas and placed at teir centroids, as listed in te tale aove. Note tat te areas sown are for te equations listed only. Tus te area for 3x 2 + 2x is not listed! Also, te zero ends of te paraolas, cuics, etc. are vertices (i.e. te sape starts wit zero slope.) Te areas are not listed for any oter conditions. 3) Sum moments aout te left reaction to determine te rigt reaction. Ten sum moments aout te rigt reaction to determine te left reaction. Ten sum forces vertically to ceck te results. 4) Erase te second load diagram wit te distriuted loads replaced y concentrated loads. Tis diagram is used ONLY to solve for te reactions. To Construct A Sear Diagram 1) Under te first load diagram, drop vertical lines at every concentrated load, at every concentrated moment, and at ot ends of every distriuted load.

2) Starting at te left end of te figure, do watever te loads tell you to do. If you cross a zero widt load (a concentrated load) going DOWN, te area under tat load (it s magnitude) will drive te sear diagram DOWN y te magnitude of tat load, over te zero widt distance. (Replace DOWN wit UP wen appropriate.) Tus after passing a concentrated load, te value of te sear diagram sould instantaneously cange y te magnitude of te load, and in te direction tat te load is pointing. 3) If you cross a distriuted load going DOWN, te magnitude under tat distriuted load (it s area) will drive te sear diagram DOWN y tat amount, over te ase dimension of te distriuted load. (Replace DOWN wit UP wen appropriate.) Tus after you finis passing over te widt of a distriuted load, te value of te sear diagram will ave canged y te magnitude of te distriuted load, and in te direction tat load is pointing. Distriuted loads tat point down drive te sear diagram down, and vise versa. 4) Te sape of te load diagram will determine te sape of te sear diagram directly elow. Te sape of te load diagram always turns into te next sape sown in te Areas and Centroids tale aove. Tus if te load is a straigt orizontal line, te sape of te sear diagram will e a straigt sloping line. If te load diagram is a paraola, te sear diagram will e a cuic. 5) You can tell if a triangular load diagram sould turn into a skinny paraola or a fat paraola y using te calculus: Te value at any point on any diagram turns into (integrates into) te slope of te next diagram. Tus if you see a zero magnitude load anywere on a eam, you sould see a zero magnitude slope on te sear diagram at tis same point. If you see small loads, tey sould turn into sear diagrams wit small slopes. If you see ig loads, tey sould turn into ig slopes on te sear diagram. 6) Since a concentrated moment as no up and down force, it does not cause any cange in te magnitude of te sear diagram at its point of application. Tat does not mean tat tey do not influence te sear diagram, ecause tey do. Tey influence it y canging te reactions, wic in turn influences te sear diagram. Tus you will see no cange in te sear diagram at te point of application of a concentrated moment. 7) To determine were te sear diagram crosses te x-axis: Xar = Starting Sear / Load Rate To Construct A Moment Diagram 1) Under te sear diagram, drop vertical lines at every point of interest including every time te sear diagram crosses te axis, and at concentrated moments. 2) Starting at te left end of te figure, do watever te sears tell you to do. If you cross a distriuted sear going DOWN, te magnitude under tat distriuted sear (it s area) will drive te moment diagram DOWN y tat amount, over te ase dimension of te distriuted sear. (Replace DOWN wit UP wen appropriate.) Tus after you finis passing over te widt of a distriuted sear, te value of te moment diagram will ave canged y te magnitude of te distriuted sear, and in te direction tat te sear tells you. Since te sear areas will not ave little arrows pointing up or down, as did te load diagrams, use sear areas aove te axis as positive (puses te moment diagram up) and sear areas elow te axis as negative (puses te moment diagram down.) 3) Te sape of te sear diagram will predict te sape of te moment diagram directly elow. Te sape of te sear diagram always turns into te next sape sown in te Areas and Centroids tale aove. Tus if te sear is a straigt sloping line, te sape of te sear

diagram will e a paraola. If te sear diagram is a paraola, te moment diagram will e a cuic. 4) You can tell if a triangular sear diagram sould turn into a skinny paraola or a fat paraola y using te calculus: Te value at any point on any diagram turns into (integrates into) te slope of te next diagram. Tus if you see a zero magnitude sear anywere on a eam, you sould see a zero magnitude slope on te moment diagram at tis same point. If you see small sears, tey sould turn into moment diagrams wit small slopes. If you see ig sears, tey sould turn into ig slopes on te moment diagram. 5) Concentrated moments cause te magnitude of te moment diagram to jump at teir points of application. Clockwise external moments applied to a eam cause te internal moment in te eam, to te rigt of te application point, to go positive (or more positive tan if te moment were not applied.) Tus, clockwise external moments applied to a eam cause te moment diagram to instantly jump up from its current value. Te amount tat te moment diagram jumps up is te magnitude of te applied moment. Counterclockwise moments cause te moment diagram to jump down. Tus you get te interesting effect tat positive externally applied moments (using your statics sign convention) cause negative jumps in te moment diagram (using your eam design sign convention.) Again, you must e drawing your diagrams from left to rigt for tese rules to apply.

Example: Load Sear Va Vd M Mc Mca Md Xar Mmax Ve Moment For La = 4 ft, L = 6 ft, Lc = 8 ft, Ld = 10 ft, P = 40 kips, M = 100 kip ft, and w = 20 kips/ft, Ra = 66.42 kips, Re = 173.57 kips Va = 66.43 kips, V = Vc = Vd = 26.43 kips, Ve = -173.57 kips M = 265.71 kip ft, Mca = 424.29 kip ft, Mc = 524.29 kip ft, Md = 735.71 kip ft Xar = 11.321 ft., Mmax = 753.18 kip ft

Procedure: 1) Te starting value on te present curve =. 2) As you go from to, 3) you cross an area under te present curve =. 4) Te area crossed is POSITIVE/NEGATIVE, 5) tus driving te next diagram UP/DOWN y tat amount at te end of te move, 6) tus giving a eigt of te next diagram = at te end of te move. 7) Te value on te left end of te present curve =, 8) tus te slope on te left end on te next curve =. 9) Te value on te rigt end of te present curve =, 10) tus te slope on te rigt end on te next curve =. 11) Te order of te present curve is, 12) tus te order of te next curve is. 13) Drawing te next curve tus gives wat sape of curve? 14) Concave up or down? (note value on tis curve = slope on te next curve) 15) Since te starting value of te next curve =, 16) and te constant rate at wic it is eing pused down from te curve aove =, 17) te next curve will cross te x-axis at 18) Te starting value on te present curve =. 19) As you go from to, 20) you cross an area under te present curve =. 21) Te area crossed is POSITIVE/NEGATIVE, 22) tus driving te next diagram UP/DOWN y tat amount at te end of te move, 23) tus giving a eigt of te next diagram = at te end of te move. 24) Te value on te left end of te present curve =, 25) tus te slope on te left end on te next curve =. 26) Te value on te rigt end of te present curve =, 27) tus te slope on te rigt end on te next curve =. 28) Te order of te present curve is, 29) tus te order of te next curve is. 30) Drawing te next curve tus gives wat sape of curve? 31) Concave up or down? (note value on tis curve = slope on te next curve) 32) Since te starting value of te next curve =, 33) and te constant rate at wic it is eing pused down from te curve aove =, 34) te next curve will cross te x-axis at.