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CE 416 Compression Members 1S AY2223

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CE 416
STRUCTURAL STEEL DESIGN
ENGR. AMIE LOU G. CISNEROS, ENP, MSCE
COLLEGE OF ENGINEERING AND TECHNOLOGY, COR JESU COLLEGE, DIGOS CITY
COMPRESSION MEMBERS
COMPRESSION MEMBERS
structural elements that are
subjected only to axial
compressive forces; that is
the loads are applied along a
longitudinal axis through the
centroid of the member
cross section
TYPES OF COMPRESSION MEMBERS
 Columns
 straight vertical members whose lengths are considerably
greater than their thickness
 Struts
 Short vertical members subjected to compressive loads
 Top chords of trusses
 Bracing members
 Compression flanges of rolled beams
3 GENERAL MODES BY WHICH AXIALLY LOADED
COLUMNS FAIL
1. FLEXURAL BUCKLING (EULER BUCKLING)
 The primary type of buckling
 Members are subject to flexure or bending, when they become unstable
2. LOCAL BUCKLING
 Occurs when some part or parts of the cross section of a column are so
thin that they buckle locally in compression before the other modes of
buckling can occur.
 The susceptibility of a column to local buckling is measured by the
width – thickness ratio of the parts of its cross – section.
3 GENERAL MODES BY WHICH AXIALLY LOADED
COLUMNS FAIL
3. FLEXURAL TORSIONAL BUCKLING
 May occur in columns that have certain cross – sectional
configurations
 These columns fail by twisting (torsion) or by a combination
of torsional and flexural buckling
EULER’S COLUMN BUCKLING THEORY
EULER’S COLUMN BUCKLING THEORY
 Column design and analysis was based on the Euler buckling
load theory.
 His analysis is based on the differential equations of the elastic
curve.
 Theory:
“When a column is loaded with the buckling load or Euler load, a
column will fail by sudden buckling or bending.”
EULER’S COLUMN BUCKLING THEORY
 If the column is hinged at both ends, the Euler critical load is
given as:
𝟐
𝒆
𝟐
 And the Euler critical stress is:
𝟐
𝟐
𝒆
𝒆
𝟐
𝟐
𝒆
EULER’S COLUMN BUCKLING THEORY
 And the Euler critical stress is:
 Thus,
= slenderness ratio
EFFECTIVE LENGTH
EFFECTIVE LENGTH
 The restraints placed on a column’s ends greatly affects its
stability. To counter these effects, an effective length factor,
K, is used to modify the unbraced length. This length
approximates the length over which the column actually
buckles and this may be shorter than the actual unbraced
length.
 Thus,
EFFECTIVE
LENGTH
SLENDERNESS RATIO
SLENDERNESS RATIO
 Steel columns are usually subdivided into two groups: long
and intermediate columns depending on their slenderness
ratio.
 The values of slenderness ratio are:
SLENDERNESS RATIO
 The critical slenderness ratio
corresponds to the
upper limit of elastic buckling failure, which is defined
by an average column stress equal to 0.50 , thus:
MINOR AND MAJOR AXIS BUCKLING
LIMITING SLENDERNESS RATIO
 Acc. Section 502.8 (NSCP), the limiting slenderness
ratio
for members whose design is based on
compressive force preferable shall not exceed 200. For
members whose design is based on tensile force, the
limiting slenderness ratio
preferable should not
exceed 300.
NSCP
ALLOWABLE COMPRESSIVE STRESS
 The
allowable column
slenderness ratio.
stress
 Inelastic buckling occurs when
buckling occurs when
 For intermediate columns,
.
varies
with
the
and elastic
NSCP
ALLOWABLE COMPRESSIVE STRESS
𝟑
𝒄
 For long columns, where
𝒌𝑳
𝒓
𝒄
𝟑
> 𝒄
𝟐
𝒂
𝟐
 Where
𝒌𝑳
𝒓
is the larger value of
𝑲𝒙 𝑳𝒙
𝒓𝒙
and
𝑲𝒚 𝑳𝒚
𝒓𝒚
LOCAL BUCKLING
LOCAL BUCKLING
 Local buckling of a plate element in a rolled shape or
built – up compression member may occur before
Euler buckling.
 The ability of plate sections to carry compressive loads
without buckling is determined by the width – thickness
ratio,
.
LOCAL BUCKLING
 Compression members are divided into stiffened and
unstiffened elements.
 STIFFENED ELEMENTS
 Are supported along two parallel edges
 UNSTIFFENED ELEMENTS
 Supported along one edge only
LOCAL BUCKLING
 To prevent local buckling, the following equation must be met if the plates
are to be fully effective.
𝒚
 For circular tubular sections whose ratios of outside diameter to wall
thickness to be fully effective, the following equation must be met.
𝒚
UNSTIFFENED ELEMENTS
ELEMENTS
H
•
Stems of tees
333
•
Double angles in contact
250
•
Compression Flanges of beams
250
•
Angles or plates projecting from girders, columns, or other
members and compression flange of plate girders
compression
250
𝐤𝐜
•
Stiffeners on plate girders
250
•
Flanges of tees and I – beams (use bf/2)
250
•
Single – angle struts or separated double – angle struts
200
LOCAL BUCKLING
LOCAL
BUCKLING
 If
,
 Otherwise,
STIFFENED ELEMENTS
ELEMENTS
H
•
Square and rectangular
box sections
625
•
cover plates with multiple
access holes
832
•
other uniformly
compressed members
664
UNSTIFFENED COMPRESSION
MEMBERS
UNSTIFFENED COMPRESSION ELEMENTS
 The allowable stress of unstiffened compression elements whose width –
thickness ratio exceeds the applicable non – compact limit given shall be
subject to a reduction factor 𝒔 .
 For single angles,
When
𝟐𝟎𝟎
𝑭𝒚
𝒃
𝒕
𝟒𝟎𝟕
𝑭𝒚
𝒔
𝒚
UNSTIFFENED COMPRESSION ELEMENTS
 When
𝒚
UNSTIFFENED COMPRESSION ELEMENTS
 For angles and plates projecting from columns or other
compression members, and for projecting elements of
compression flanges of beams and girders:
 When
𝑭𝒚
𝑭𝒚
𝒌𝒄
𝒔
𝒌𝒄
UNSTIFFENED COMPRESSION ELEMENTS
 When
𝑭𝒚
𝒌𝒄
ALLOWABLE STRESSES FOR
UNSTIFFENED COMPRESSION
MEMBERS
ALLOWABLE STRESSES FOR
UNSTIFFENED COMPRESSION MEMBERS
 The allowable stress for axially loaded compression members containing
unstiffened elements shall not exceed the following:
 When
𝒌𝑳
𝒓
𝒄
𝟐
𝒚
𝒂
𝟐
𝒄
ALLOWABLE STRESSES FOR
UNSTIFFENED COMPRESSION MEMBERS
𝟑
𝟑
𝒄
𝒄
𝟐
𝒄
𝒚
ALLOWABLE STRESSES FOR
UNSTIFFENED COMPRESSION MEMBERS
 Cross sections composed entirely of unstiffened elements,
𝒔
 Cross sections composed entirely of stiffened elements,
𝒂
 Cross sections composed of both stiffened and unstiffened
elements,
𝒔
𝒂
ALLOWABLE STRESSES FOR
UNSTIFFENED COMPRESSION MEMBERS
 When
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