Beam-Columns. Members Under Combined Forces Most beams and columns are subjected to some degree of both bending and axial load e.g. Statically Indeterminate.

Slides:



Advertisements
Similar presentations
ENCE 455 Design of Steel Structures
Advertisements

Design of Seismic-Resistant Steel Building Structures
Compression Members.
CHAPTER OBJECTIVES Discuss the behavior of columns.
Limit States Flexure Shear Deflection Fatigue Supports Elastic Plastic
Beams Stephen Krone, DSc, PE University of Toledo.
ENCE 710 Design of Steel Structures
DESIGN OF MEMBERS FOR COMBINED FORCES
DESIGN OF MEMBERS FOR COMBINED FORCES
REVIEW OF STEEL DESIGN KNOWLEDGE BASE REQUIRED: STRENGTH OF MATERIALS
Beam-Columns.
Beams and Frames.
LRFD-Steel Design Dr. Ali Tayeh Second Semester
Chapter 13 Buckling of Columns
ENCE 455 Design of Steel Structures
STEEL DESIGN (I) CE 408 ( 2 – 3 – 3 ) Semester 062
Chap. (6) Compression Members Columns: Beam-Columns: Columns Theory:
Compression Members.
Column Theory - Column Strength Curve
Biaxial Bending AISC Chapter H
Beams.
Compression Members.
BC-11 The horizontal beam column shown below is subjected to service live loads as shown. The member is laterally braced at its ends. Check its capacity.
Combined Bending & Axial Forces (BEAM – COLUMNS)
Compression Members.
Combined Load Member Design
Beams Beams: Comparison with trusses, plates t
Combined Bending & Axial Forces (BEAM – COLUMNS)
LRFD- Steel Design Dr. Ali I. Tayeh First Semester Dr. Ali I. Tayeh First Semester.
LRFD-Steel Design 1.
Beams. BEAMS A structural member loaded in the transverse direction to the longitudinal axis. Internal Forces: Bending Moments and Shear.
Dr. Ali I. Tayeh First Semester
LRFD- Steel Design Dr. Ali I. Tayeh First Semester Dr. Ali I. Tayeh First Semester.
Design of Combined Bending and Compression Members in Steel.
1Combined Forces Theory Developed by Scott Civjan University of Massachusetts, Amherst.
CTC 422 Design of Steel Structures
LRFD – Floor beam Unbraced top flange. Lateral Torsion Buckling  We have to check if there is plastic failure (yielding) or lateral-torsion buckling.
LRFD- Steel Design Dr. Ali I. Tayeh second Semester Dr. Ali I. Tayeh second Semester.
CTC / MTC 222 Strength of Materials
Second Order Analysis In the previous classes we looked at a method that determines the load corresponding to a state of bifurcation equilibrium of a perfect.
Design of Thin-Walled Members
1 BEAM-COLUMNS PROF. V. KALYANARAMAN Department of Civil Engineering Indian Institute of Technology Madras Chennai
Chapter 5 Introduction to Axially Loaded Compression Members.
STEEL DESIGN KNOWLEDGE BASE REQUIRED: STRENGTH OF MATERIALS STEEL DESIGN REVIEW OF TIMBER DESIGN BEARING PROBLEM TIMBER DESIGN SOIL MECHANICS REVIEW OF.
General Comparison between AISC LRFD and ASD
Columns Zach Gutzmer, EIT Civil and Environmental Engineering South Dakota State University.
Dr S R Satish Kumar, IIT Madras 1 Section 9 Members subjected to Combined Forces (Beam-Columns)
DESIGN OF MEMBERS FOR COMBINED FORCES
62323: Architectural Structures II
Design of Beams for Flexure
Flexural-Torsional Buckling
Design of Steel Beams Dr. Bashar Behnam.
contents Design of beams (week 11,12,13), (10,17,24 Nov.)
Dr. Ali I. Tayeh First Semester
Columns and Other Compression Members
Unit-5. Torsion in Shafts and Buckling of Axially Loaded Columns
CE579 - Structural Stability and Design
Revision for Mechanics of Materials
Design of Beams - Limit States
Compression Members.
Buckling & Stability Critical Load
Structure I Course Code: ARCH 208 Dr. Aeid A. Abdulrazeg
Chapter 13 – Buckling of Columns
Second Order Analysis In the previous classes we looked at a method that determines the load corresponding to a state of bifurcation equilibrium of a perfect.
Beam-Columns.
Second Order Analysis In the previous classes we looked at a method that determines the load corresponding to a state of bifurcation equilibrium of a perfect.
REVIEW OF STEEL DESIGN KNOWLEDGE BASE REQUIRED: STRENGTH OF MATERIALS
Design of Steel Beams Dr. Bashar Behnam.
Section 9 Members subjected to Combined Forces (Beam-Columns)
Section 9 Members subjected to Combined Forces (Beam-Columns)
Presentation transcript:

Beam-Columns

Members Under Combined Forces Most beams and columns are subjected to some degree of both bending and axial load e.g. Statically Indeterminate Structures P1P1 P2P2 C E A D F B

Interaction Formula REQUIRED CAPACITY P r P c M rx M cx Mry Mcy

Axial Capacity P c

Elastic Buckling Stress corresponding to the controlling mode of failure (flexural, torsional or flexural torsional) Fe:Fe: Theory of Elastic Stability (Timoshenko & Gere 1961) Flexural BucklingTorsional Buckling 2-axis of symmetry Flexural Torsional Buckling 1 axis of symmetry Flexural Torsional Buckling No axis of symmetry AISC Eqtn E4-4 AISC Eqtn E4-5 AISC Eqtn E4-6

Axial Capacity P c LRFD

Axial Capacity P c ASD

Moment Capacities

Moment Capacity M cx or M cy REMEMBER TO CHECK FOR NON- COMPACT SHAPES

Moment Capacity M cx or M cy REMEMBER TO ACCOUNT FOR LOCAL BUCKLING IF APPROPRIATE

Moment Capacity M cx or M cy LRFDASD

Axial Demand

Axial Demand P r LRFDASD factoredservice

Demand

Second Order Effects & Moment Amplification W P P M y y x=L/2 =  M x=L/2 =    P  wL 2 /8 + P  additional moment causes additional deflection

Second Order Effects & Moment Amplification Consider M max =    P  additional moment causes additional deflection

Design Codes AISC Permits Second Order Analysis or Moment Amplification Method Compute moments from 1 st order analysis Multiply by amplification factor

Braced vs. Unbraced Frames Eq. C2-1a

Braced vs. Unbraced Frames Eq. C2-1a M nt = Maximum 1 st order moment assuming no sidesway occurs M lt = Maximum 1 st order moment caused by sidesway B 1 = Amplification factor for moments in member with no sidesway B 2 = Amplification factor for moments in member resulting from sidesway

Braced Frames P r = required axial compressive strength = P u for LRFD = P a for ASD P r has a contribution from the P  effect and is given by

Braced Frames a = 1 for LRFD = 1.6 for ASD

Braced Frames C m coefficient accounts for the shape of the moment diagram

Braced Frames C m For Braced & NO TRANSVERSE LOADS M 1 : Absolute smallest End Moment M 2 : Absolute largest End Moment

Braced Frames C m For Braced & NO TRANSVERSE LOADS COSERVATIVELY C m = 1

Unbraced Frames Eq. C2-1a M nt = Maximum 1 st order moment assuming no sidesway occurs M lt = Maximum 1 st order moment caused by sidesway B 1 = Amplification factor for moments in member with no sidesway B 2 = Amplification factor for moments in member resulting from sidesway

Unbraced Frames

a= 1.00 for LRFD = 1.60 for ASD = sum of required load capacities for all columns in the story under consideration = sum of the Euler loads for all columns in the story under consideration

Unbraced Frames Used when shape is known e.g. check of adequacy Used when shape is NOT known e.g. design of members

Unbraced Frames I = Moment of inertia about axis of bending K 2 = Unbraced length factor corresponding to the unbraced condition L = Story Height R m = 0.85 for unbraced frames  H = drift of story under consideration  H = sum of all horizontal forces causing  H

Homework