Beam Design and Deflections

Similar documents
Wood Design. fv = shear stress fv-max = maximum shear stress Fallow = allowable stress Fb = tabular bending strength = allowable bending stress

Steel Design. Notation:

Steel Design. Notation:

Steel Design. Notation: a A A b A e

Stress Analysis Lecture 4 ME 276 Spring Dr./ Ahmed Mohamed Nagib Elmekawy

Karbala University College of Engineering Department of Civil Eng. Lecturer: Dr. Jawad T. Abodi

FLOW CHART FOR DESIGN OF BEAMS

Physics 8 Monday, November 20, 2017

Beam Bending Stresses and Shear Stress

DL CMU wall = 51.0 (lb/ft 2 ) 0.7 (ft) DL beam = 2.5 (lb/ft 2 ) 18.0 (ft) 5

[8] Bending and Shear Loading of Beams

Mechanics of Materials Primer

Chapter 8: Bending and Shear Stresses in Beams

Chapter Objectives. Design a beam to resist both bendingand shear loads

Design of Beams (Unit - 8)

Chapter 7: Bending and Shear in Simple Beams

Chapter 7: Internal Forces

Failure in Flexure. Introduction to Steel Design, Tensile Steel Members Modes of Failure & Effective Areas

DESIGN OF BEAMS AND SHAFTS

Solution: The moment of inertia for the cross-section is: ANS: ANS: Problem 15.6 The material of the beam in Problem

BEAM DEFLECTION THE ELASTIC CURVE

= 50 ksi. The maximum beam deflection Δ max is not = R B. = 30 kips. Notes for Strength of Materials, ET 200

BEAM A horizontal or inclined structural member that is designed to resist forces acting to its axis is called a beam


MECE 3321: Mechanics of Solids Chapter 6

CHAPTER 4. Stresses in Beams

5. What is the moment of inertia about the x - x axis of the rectangular beam shown?

CHAPTER 6: Shearing Stresses in Beams

Karbala University College of Engineering Department of Civil Eng. Lecturer: Dr. Jawad T. Abodi

Deflection of Flexural Members - Macaulay s Method 3rd Year Structural Engineering

PURE 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.

TORSION INCLUDING WARPING OF OPEN SECTIONS (I, C, Z, T AND L SHAPES)

Deflection of Flexural Members - Macaulay s Method 3rd Year Structural Engineering

3. BEAMS: STRAIN, STRESS, DEFLECTIONS

two structural analysis (statics & mechanics) APPLIED ACHITECTURAL STRUCTURES: DR. ANNE NICHOLS SPRING 2017 lecture STRUCTURAL ANALYSIS AND SYSTEMS

Finite Element Analysis Prof. Dr. B. N. Rao Department of Civil Engineering Indian Institute of Technology, Madras. Module - 01 Lecture - 13

Physics 8 Monday, November 23, 2015

Serviceability Deflection calculation

Internal Internal Forces Forces

SSC-JE MAINS ONLINE TEST SERIES / CIVIL ENGINEERING SOM + TOS

FIXED BEAMS IN BENDING

SUMMARY FOR COMPRESSION MEMBERS. Determine the factored design loads (AISC/LRFD Specification A4).

By Dr. Mohammed Ramidh

twenty one concrete construction: shear & deflection ARCHITECTURAL STRUCTURES: FORM, BEHAVIOR, AND DESIGN DR. ANNE NICHOLS SUMMER 2014 lecture

Types of Structures & Loads

7.4 The Elementary Beam Theory

structural analysis Excessive beam deflection can be seen as a mode of failure.

3 Hours/100 Marks Seat No.

A Simply supported beam with a concentrated load at mid-span: Loading Stages

This procedure covers the determination of the moment of inertia about the neutral axis.

Design of Reinforced Concrete Structures (II)

QUESTION BANK SEMESTER: III SUBJECT NAME: MECHANICS OF SOLIDS

QUESTION BANK DEPARTMENT: CIVIL SEMESTER: III SUBJECT CODE: CE2201 SUBJECT NAME: MECHANICS OF SOLIDS UNIT 1- STRESS AND STRAIN PART A

Case Study in Reinforced Concrete adapted from Simplified Design of Concrete Structures, James Ambrose, 7 th ed.

Chapter Objectives. Copyright 2011 Pearson Education South Asia Pte Ltd

SERVICEABILITY OF BEAMS AND ONE-WAY SLABS

2. Determine the deflection at C of the beam given in fig below. Use principal of virtual work. W L/2 B A L C

Purpose of this Guide: To thoroughly prepare students for the exact types of problems that will be on Exam 3.

7 TRANSVERSE SHEAR transverse shear stress longitudinal shear stresses

Physics 8 Wednesday, November 18, 2015

Chapter 6: Cross-Sectional Properties of Structural Members

National Exams May 2015

Bending Stress. Sign convention. Centroid of an area

Wood Design. = theoretical allowed buckling stress

REVIEW FOR EXAM II. Dr. Ibrahim A. Assakkaf SPRING 2002

Rigid and Braced Frames

PES Institute of Technology

EMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 5 Beams for Bending

Sabah Shawkat Cabinet of Structural Engineering Walls carrying vertical loads should be designed as columns. Basically walls are designed in

Advanced Structural Analysis EGF Section Properties and Bending

Dr. Hazim Dwairi. Example: Continuous beam deflection

Shear Force V: Positive shear tends to rotate the segment clockwise.

Strength of Materials Prof. Dr. Suraj Prakash Harsha Mechanical and Industrial Engineering Department Indian Institute of Technology, Roorkee

Physics 8 Wednesday, November 29, 2017

Singly Symmetric Combination Section Crane Girder Design Aids. Patrick C. Johnson

General Comparison between AISC LRFD and ASD

UNIVERSITY OF BOLTON SCHOOL OF ENGINEERING. BEng (HONS) CIVIL ENGINEERING SEMESTER 1 EXAMINATION 2016/2017 MATHEMATICS & STRUCTURAL ANALYSIS

SOLUTION (17.3) Known: A simply supported steel shaft is connected to an electric motor with a flexible coupling.

Chapter 8 Supplement: Deflection in Beams Double Integration Method

UNIT 1 STRESS STRAIN AND DEFORMATION OF SOLIDS, STATES OF STRESS 1. Define stress. When an external force acts on a body, it undergoes deformation.

6. Bending CHAPTER OBJECTIVES

Symmetric Bending of Beams

Properties of Sections

Strength of Materials Prof: S.K.Bhattacharya Dept of Civil Engineering, IIT, Kharagpur Lecture no 28 Stresses in Beams- III

2012 MECHANICS OF SOLIDS

8 Deflectionmax. = 5WL 3 384EI

External Work. When a force F undergoes a displacement dx in the same direction i as the force, the work done is

CH. 4 BEAMS & COLUMNS

Samantha Ramirez, MSE

D : SOLID MECHANICS. Q. 1 Q. 9 carry one mark each.

STRESS STRAIN AND DEFORMATION OF SOLIDS, STATES OF STRESS

Chapter 4.1: Shear and Moment Diagram

Mechanics of Solids notes

MODULE C: COMPRESSION MEMBERS

CIVIL DEPARTMENT MECHANICS OF STRUCTURES- ASSIGNMENT NO 1. Brach: CE YEAR:

Structural Steelwork Eurocodes Development of A Trans-national Approach

Problem 7.1 Determine the soil pressure distribution under the footing. Elevation. Plan. M 180 e 1.5 ft P 120. (a) B= L= 8 ft L e 1.5 ft 1.

Accordingly, the nominal section strength [resistance] for initiation of yielding is calculated by using Equation C-C3.1.

Design of a Multi-Storied RC Building

Consider an elastic spring as shown in the Fig.2.4. When the spring is slowly

Transcription:

Beam Design and Deflections tation: a = name for width dimension A = name for area Areq d-adj = area required at allowable stress when shear is adjusted to include self weight Aweb = area of the web of a wide flange section b = width of a rectangle = total width of material at a horizontal section = name for height dimension c = largest distance from the neutral axis to the top or bottom edge of a beam c1 = coefficient for shear stress for a rectangular bar in torsion d = calculus symbol for differentiation DL = shorthand for dead load E = modulus of elasticity fb = bending stress fp = bearing stress (see P) fv = shear stress fv-max = maximum shear stress Fb = allowable bending stress Fv = allowable shear stress Fp = allowable bearing stress Fy = yield strength Fyweb = yield strength of the web material h = height of a rectangle I = moment of inertia with respect to neutral axis bending Itrial = moment of inertia of trial section Ireq d = moment of inertia required at limiting deflection J = polar moment of inertia L = name for span length LL = shorthand for live load LRFD = load and resistance factor design M = internal bending moment Mmax = maximum internal bending moment Mmax-adj = maximum bending moment adjusted to include self weight Mn nominal flexure strength with the full section at the yield stress for LRFD Mu = maximum moment from factored loads for LRFD P = name for axial force vector Q = first moment area about a neutral axis R = radius of curvature of a deformed beam S = section modulus Sreq d = section modulus required at allowable stress T = torque (axial moment) V = internal shear force Vmax = maximum internal shear force Vmax-adj = maximum internal shear force adjusted to include self weight Vu = maximum shear from factored loads for LRFD w = name for distributed load wself wt = name for distributed load from self weight of member x = horizontal distance y = vertical distance actual = actual beam deflection allowable = allowable beam deflection limit = allowable beam deflection limit max = maximum beam deflection b = resistance factor for flexure in LRFD design v = resistance factor for shear for LRFD = density or unit weight = slope of the beam deflection curve = radial distance = symbol for integration = summation symbol 303

Criteria for Design Allowable bending stress or bending stress from LRFD should not be exceeded: Knowing M and Fb, the minimum section modulus fitting the limit is: F b S f b req' d Mc I M F b Besides strength, we also need to be concerned about serviceability. This involves things like limiting deflections & cracking, controlling noise and vibrations, preventing excessive settlements of foundations and durability. When we know about a beam section and its material, we can determine beam deformations. Determining Maximum Bending Moment Drawing V and M diagrams will show us the maximum values for design. Remember: V (w) M ( V) dv w dm V Determining Maximum Bending Stress For a prismatic member (constant cross section), the maximum normal stress will occur at the maximum moment. For a non-prismatic member, the stress varies with the cross section AND the moment. Deflections If the bending moment changes, M(x) across a beam of constant material and cross section then the curvature will change: The slope of the n.a. of a beam,, will be tangent to the radius of curvature, R: The equation for deflection, y, along a beam is: 1 slope M x EI ( ) Elastic curve equations can be found in handbooks, textbooks, design manuals, etc...computer programs can be used as well. Elastic curve equations can be superpositioned ONLY if the stresses are in the elastic range. 1 M ( x) R EI 1 1 y M ( x) EI EI 304

The deflected shape is roughly the shame shape as the bending moment diagram flipped but is constrained by supports and geometry. Boundary Conditions The boundary conditions are geometrical values that we know slope or deflection which may be restrained by supports or symmetry. At Pins, Rollers, Fixed Supports: y = 0 At Fixed Supports: = 0 At Inflection Points From Symmetry: = 0 The Slope Is Zero At The Maximum Deflection ymax:. dy slope 0 Allowable Deflection Limits All building codes and design codes limit deflection for beam types and damage that could happen based on service condition and severity. y x L max ( ) actual allowable value Use LL only DL+LL Roof beams: Industrial (no ceiling) L/180 L/120 Commercial plaster ceiling L/240 L/180 no plaster L/360 L/240 Floor beams: Ordinary Usage L/360 L/240 Roof or floor (damageable elements) L/480 305

Beam Loads & Load Tracing In order to determine the loads on a beam (or girder, joist, column, frame, foundation...) we can start at the top of a structure and determine the tributary area that a load acts over and the beam needs to support. Loads come from material weights, people, and the environment. This area is assumed to be from half the distance to the next beam over to halfway to the next beam. The reactions must be supported by the next lower structural element ad infinitum, to the ground. Design Procedure The intent is to find the most light weight member satisfying the section modulus size. 1. Know Fb (allowable stress) for the material or Fy & Fu for LRFD. 2. Draw V & M, finding Mmax. M max 3. Calculate Sreq d. This step is equivalent to determining fb Fb 2 S 4. For rectangular beams bh S 6 For steel or timber: use the section charts to find S that will work and remember that the beam self weight will increase Sreq d. And for steel, the design charts show the lightest section within a grouping of similar S s. w self wt A For any thing else, try a nice value for b, and calculate h or the other way around. ****Determine the updated Vmax and Mmax including the beam self weight, and verify that the updated Sreq d has been met.****** 5. Consider lateral stability 6. Evaluate horizontal shear stresses using Vmax to determine if f v Fv For rectangular beams, W s, and others: 7. Provide adequate bearing area at supports: T T 8. Evaluate shear due to torsion fv or F 2 v J c1ab (circular section or rectangular) 9. Evaluate the deflection to determine if max LL LLallowed and/or maxtotal T allowed **** note: when calculated > limit, Irequired can be found with: and Sreq d will be satisfied for similar self weight ***** FOR ANY EVALUATION: Redesign (with a new section) at any point that a stress or serviceability criteria is NOT satisfied and re-evaluate each condition until it is satisfactory. 306 3V V VQ fvmax or 2A A Ib f p P F A p web too big I req ' d I limit trial

Example 1 (superpositioning) 0.75 m Investigate using Beam Diagrams and Formulas. SOLUTION: C By examining the support conditions, we are looking for a cantilevered beam from Cases 18 through 23. There is a case for uniformly distributed load across the span (19) and for a load at any point (21). For both these cases, it shows that the maximum shear AND maximum moment are located at the fixed end. If we add the values, the shear and diagrams should look like this: V + M + We can find the maximum shear (at B) from V = P + wl = 10 kn + 2 kn/m 3 m = 16 kn The maximum moment (at B) will be M = Pb+wl 2 /2 = 10 kn 2.25 m + 2 kn/m (3 m ) 2 /2 = 31.5 kn-m The key values for the diagrams can be found with the general equations (Vx and Mx): VC = - wx = -2 kn/m 0.25 m = -0.5 kn ; VC = -P wx = -10 kn - 2 kn/m 0.25 m = -10.5 kn MC = -WX 2 /2 = 2 kn/m (0.25 m ) 2 /2 = 0.0625 kn-m We can find the maximum deflection by looking at the cases. Both say max. (at free end), so the values can be added directly. Superpositioning of values must be at the same x location. Assume E = 70x10 3 MPa and I = 45x10 6 mm 4 = 18.08 mm + 6.43 mm = 24.5 mm 307

Example 2 (pg 343) (superpositioning), using Beam Diagrams and Formulas. SOLUTION: By examining the support conditions, we are looking for beam with an overhang on one end from Cases 24 through 28. (Even though the overhang is on the right, and not on the left like our beam, we can still use the information by recognizing that we can mirror the figure about the left end.) There is a case for a load at the end (26) but none for a load in between the supports. This is because it behaves exactly like a simply supported beam in this instance (no shear or bending on the overhang). The case for this is #5 (reversed again). If we flip the diagrams (both vertically and horizontally) and add the values, the resulting shear and bending moment should look like this: V + M + We still have to find the peak values of shear and the location of the zero shear to find the critical moment values. (tice R1 is shown down.) k ft ft ft Pa wa 10 10 2 10 R1 2l a 2 20 10 10 D ft ft l 2l 20 220 ft k / ft ft k k R2(B) 10 2 10 10 20 (from the total downward load R1(D)) VA = -10 k VB = -10 k + 20 k = 10 k VD = 10 k 2 k/ft (10ft) = -10 k x (from B) = 10 k /2 k/ft = 5 ft MB = -10 k (10 ft ) = -100 k-ft (MC = -100 k-ft + 10 k (10 ft ) = 0) Mx = 0 +10 k/ft (5 ft )/2 = 25 k-ft VMAX = 10 k MMAX = -100 k-ft We can calculate the deflection between the supports. (And at the end for case 5 if we derive the slope!) Assume E = 29x10 3 ksi and I = 103 in 4 k ft ft k We ll investigate the maximum between the supports from case 26 (because it isn t obvious where the maximum will be.) ft 20 ft x l 11.55 (to left of D) and total max. case 26 xcase 5 with x (11.55 ft ) greater than a (10 ft ): 3 3 total 2 2 xl x a 2 wa l x 2 Pal.06415 4 2 te: Because there is only negative moment, the deflection is actually up! EI 24EIl 10 (10 )(20 ) (12.06415 k ft ft 2 in / ft 3 3 4 (29 10 ksi)(103 in ) k / ft ft 2 ft ft 2 (10 ) (20 10 ) 3 4 ft 24(29 10 ksi)(103 in )(20 ) [4(11.55 ft )(20 ft )-2(11.55 ft ) 2 -(10 ft ) 2 ](12 in/ft ) 3 = -1.484 in + 1.343 in = -0.141 in (up) ) 308

Beam Design Flow Chart Collect data: L,,, limits; find beam charts for load cases and actual equations ASD Allowable Stress or LRFD Design? LRFD Collect data: Fb & Fv Find Vmax & Mmax from constructing diagrams or using beam chart formulas Find Sreq d and pick a section from a table with Sx greater or equal to Sreq d Calculate self wt. using A found and. Find Mmax-adj & Vmax-adj. Collect data: load factors, Fy, Fu, and equations for shear capacity with V Find Vu & Mu from constructing diagrams or using beam chart formulas with the factored loads Pick a steel section from a chart having bmn Mu for the known unbraced length Calculate Sreq d-adj using Mmax-adj. Is Sx(picked) Sreq d-adj? (OR calculate fb. Is fb Fb?) Is Vu v(0.6fywebaweb) Yes pick a section with a larger web area Yes Calculate Areq d-adj using Vmax-adj. Is A(picked) Areq d-adj? (OR calculate fv. Is fv Fv?) pick a new section with a larger area Calculate max (no load factors!) using superpositioning and beam chart equations with the Ix for the section is max limits? This may be both the limit for live load deflection and total load deflection.) too big I req I ' d trial limit pick a section with a larger Ix Yes (DONE) 309