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STABILITY OF COLD-FORMED ELEMENTS Czech Technical University in Prague 2E12 Design of steel structures for renewable energy systems 1 21/11/2010

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STABILITY OF COLD-FORMED ELEMENTSCzech Technical University in Prague

2E12 Design of steel structures for renewable energy systems 1

21/11/2010

Contents

21/11/20102E12 Design of steel structures for renewable energy systems

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Behavior features: local buckling of compression elements plane elements elements with stiffeners

shear lag web crippling

Cross-section check Beams restrained by sheeting Connections

Cross-section idealiseation

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C9 Design of steel structures for renewable energy systems

Cross-section

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Idealised section with radiuses r=0 when r<5t

Buckling in compression

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C9 Design of steel structures for renewable energy systems

Buckling strength

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Local buckling Distortional buckling

Section distortion

Global buckling Shear buckling

Sectional modes

Buckling strength

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Buckling strength

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Local buckling

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Theory + calculation procedures (see local buckling of plates)

Elements: doubly supported outstands

stiffened plain

1,052com comp

cr

bt k Eσ

σ σλ

σ= = com yfσ ≤

Stiffeners

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Edge stiffeners

Intermediate stiffeners

Stress distribution on stiffened plate

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Calculation model stiffener supports plane element stiffener itself can buckle (as compression member on

elastic foundation)

Buckling of edge stiffener

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Vran

y

Spring stiffness of stiffener

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Stress distribution - idealisation

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- distortional buckling

Calculation procedure

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1. Stiffener provides rigid support to the plate ⇒effective widths

2. K, As, Is3. Critical stress σcr4. for σcom = fy ⇒ χd (distortional buckling)5. σcom = χd fy6. Effective widths of parts adjacent to the stiffener7. As, Is8. iteration 3. – 7.9. tred = χd t

Final effective cross-section

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, 2 , 1e i e ib b≥

(Vrany)

Interaction of local and distortional buckling

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C9 Design of steel structures for renewable energy systems

http://www.ce.jhu.edu/bschafer/cufsm

Buckling modes

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C9 Design of steel structures for renewable energy systems

Check – cross-sections, members

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EN 1993-1-3

Limits: members0,45 ≤ t ≤ 15 mm sheeting 0,45 ≤ t ≤ 4 mm

Compression

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interaction of local and global buckling

=> χ

. 1b Rd eff y MN A fχ γ=

1

eff y effR

cr g cr g

A f ANN A A

λλσ λ

= = =

Buckling modes

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(Dub

ina)

Flexural-torsional buckling

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uniaxial symmetrical profiles

torsional buckling: flexural-torsional buckling: …combination

buckling curve b

2w

cr,T t2 2g o T

1 EIGIA i

πσ

= +

cr,TFσ cr,T cr,, yσ σ

( )22cr,y y yE iσ π=

Members subjected to bending

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C9 Design of steel structures for renewable energy systems

Bending

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Lateral-torsional buckling

Specific design of cold-formed members in bending subjected to lateral-torsional buckling

( ).eff Rd LT eff ydM W fχ=

Behaviour - Z section in bending

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Slender section → local buckling Edge stiffener – distortional buckling

Non-symmetry → distortion of cross-section Out-of-plane buckling of free flange in hogging moment areas

Cross-section distortion

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C D

+

--

++

-

++

--

Reality Idealized model

Cross-section distortion

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Simplified model

K

C D

+=

y

z

y

Calculation procedure EN1993-1-3

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Sagging moments:

Hogging moments:

,1

,

y EdEd yd y M

eff y

Mf f

Wσ γ= ≤ =

,1

,

y Ed fzEd yd y M

eff y fz

M M f fW W

σ γχ

= + ≤ =

Web crippling

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C9 Design of steel structures for renewable energy systems

(Vrany)

Web crippling

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C9 Design of steel structures for renewable energy systems

(Vrany)

Web crippling

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C9 Design of steel structures for renewable energy systems

Web crippling

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Eccentric compression to web Rw,Rd …equations derived experimentally

Web crippling

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Cases: Single web

Two or more webs

Web crippling

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Loading – cases: a) close to free end b) far from free end

a) from one side b) from both opposite sides

Rw,Rd = f(t2, r/t, f, ss …) product of individual factors

Interaction

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C9 Design of steel structures for renewable energy systems

Combination M+R

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Governing condition e.g. for corrugated sheeting, continuous beams

c,Rd w,Rd

1,25Ed EdM FM R

+ ≤

Combination compression + bending

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,E d E d ,z N yM N e∆ =

Shear lag

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C9 Design of steel structures for renewable energy systems

Shear lag

21/11/2010Thin walled and composite structures / Michal Jandera /

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by elastic analysis (I. order) ⇒ both tension and compression

factor of ratio Le/b0 … to solve when Le/b0 < 50

Shear lag

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for thin-walled sections, b0:

Effective width:

( )0

max

b

eff

y dyb

σ

σ=∫

Shear lag

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Effective width: Effective width factor

0effb bβ= ⋅

Connections

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C9 Design of steel structures for renewable energy systems

Connections

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Welds fillet t ≥ 3 mm (automatic … t ≥ 2 mm)MAG is best lap connections

spot

Connections

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Mechanical fasteners blind rivets screws 3 ≤ d ≤ 8 mm self-drilling (self-tapping) thread-cutting

cartridge fired pins bolts

Blind rivets

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Screws

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Different failure modes compared with classic bolts

New types of connections

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“Rossete” system

Adhesive bonding (problem of lifespan reliability)

Design aids

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C9 Design of steel structures for renewable energy systems

Design aids

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Tables

PROFIL

váha profilu řádek rozpětí pole L [m] rozpětí pole L [m]číslo 5,0 6,0 7,0 8,0 9,0 10,0 5,0 6,0 7,0 8,0 9,0 10,0

1 3,41 2,34 1,70 1,29 1,00 4,91 3,03 2,09 1,54 1,192 3,41 2,34 1,70 1,15 4,91 3,03 2,09 1,54 1,19

Z 250/2,0 3 3,28 1,86 1,15 4,91 3,03 2,09 1,48 1,027,80 kg/m 4 2,49 1,63 1,12 3,95 2,48 1,70 1,25

5 -2,44 -1,65 -1,19 -0,89 -0,69 -3,95 -2,64 -1,90 -1,43 -1,116 -1,92 -1,29 -0,91 -0,68 -0,52 -3,16 -2,08 -1,48 -1,10 -0,851 4,61 3,17 2,31 1,74 1,36 1,08 6,59 4,10 2,84 2,11 1,64 1,302 4,61 3,17 2,28 1,50 1,02 6,59 4,10 2,84 2,11 1,64 1,30

Z 250/2,5 3 4,25 2,42 1,49 0,97 6,59 4,10 2,84 1,92 1,329,70 kg/m 4 3,66 2,43 1,68 1,20 5,75 3,57 2,47 1,83 1,41 1,03

5 -3,31 -2,26 -1,63 -1,22 -0,95 -0,75 -5,29 -3,58 -2,59 -1,95 -1,52 -1,216 -2,81 -1,91 -1,37 -1,02 -0,78 -0,62 -4,53 -3,04 -2,19 -1,64 -1,27 -1,01

PROSTÝ NOSNÍK SPOJITÝ NOSNÍK S PŘESAHY

Design aids

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Software