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Yield Lines and Tensile Membrane Action - a New Look
Ian Burgess
University of Sheffield
Why did TMA become an issue?
Cardington
Max beam temperature ~1150C
cf. Code critical temperature ~ 680C
Max beam temperature ~1150C
cf. Code critical temperature ~ 680C
Fracture
Fracture
Compression failure
BRE Membrane Test
UK post-Cardington design guidance
Fire Safe Design (SCI P288) A new approach to multi-storey steel framed buildings
• Based on observations of Cardington tests.
• Checked using simplified (BRE-Bailey) design method.
Fire Safe Design (SCI P288) A new approach to multi-storey steel framed buildings
• Based on observations of Cardington tests.
• Checked using simplified (BRE-Bailey) design method.
TSLAB v3.0
TSLAB v3.0 (SCI) Excel-based free software updating BRE method:
• Thermal analysis to give weighted average reinforcement mesh temperature at any time.
• Optimises mesh size for FLS loading at required fire resistance time – or for burn-out.
TSLAB v3.0 (SCI) Excel-based free software updating BRE method:
• Thermal analysis to give weighted average reinforcement mesh temperature at any time.
• Optimises mesh size for FLS loading at required fire resistance time – or for burn-out.
BRE (770°C) TSLAB BRE (770°C) TSLAB
FRACOF
FRACOF
• Based on a European project
• Outcome almost identical to UK simplified (BRE-Bailey) design method. A few changes to safety factors, extra deflection check.
FRACOF
• Based on a European project
• Outcome almost identical to UK simplified (BRE-Bailey) design method. A few changes to safety factors, extra deflection check.
The basis: Hayes (1968)
Where are we now?
Small-deflection yield-line mechanism
rl
nl
l
g
Hogging rotations about edges of panel
Sagging rotations about internal yield lines
Tensile crack across short mid-span
Large-deflection failure crack observed experimentally and used in Bailey/BRE, FRACOF and NZ SPM
Yield-line pattern is optimized for minimum failure load. Yield-line pattern is optimized for minimum failure load.
Current simplified methods of representing TMA
C S
T2
T1
1. Large deflection progressively enhances yield-line load capacity
2. Limiting value of deflection due to integrity failure given by through-depth tensile cracking.
1. Large deflection progressively enhances yield-line load capacity
2. Limiting value of deflection due to integrity failure given by through-depth tensile cracking.
1.1KT0L/2
(Ultimate strength of reinforcement across Fracture)
C S
T2
T1
Basic mechanics of enhancement:
• Kinematics doesn’t work.
• Why elastic tension distributions?
• Illogical aggregation of enhancements .
Basic mechanics of enhancement:
• Kinematics doesn’t work.
• Why elastic tension distributions?
• Illogical aggregation of enhancements .
Problems with current simplified methods
𝑒1 = 𝑒1𝑚 + 𝑒1𝑏
𝑒2 = 𝑒2𝑚 + 𝑒2𝑏
𝑒 = 𝑒1 −𝑒1 − 𝑒21 + 2𝜇𝑎2
𝑒1 = 𝑒1𝑚 + 𝑒1𝑏
𝑒2 = 𝑒2𝑚 + 𝑒2𝑏
𝑒 = 𝑒1 −𝑒1 − 𝑒21 + 2𝜇𝑎2
For the heated case:.
Mechanically illogical superposition of incompatible cases for limiting deflection.
For the heated case:.
Mechanically illogical superposition of incompatible cases for limiting deflection.
Problems with current simplified methods
𝑤𝜀 =0.5𝑓𝑠𝑦
𝐸𝑠
3𝐿2
8 𝑤𝜀 =
0.5𝑓𝑠𝑦
𝐸𝑠
3𝐿2
8 𝑤𝜃 =
𝛼 𝑇2 − 𝑇1 𝑙2
16ℎ 𝑤𝜃 =
𝛼 𝑇2 − 𝑇1 𝑙2
16ℎ
First thoughts on enhancement
Kinematically consistent large-deflection behaviour
Principles:
• Based on small-deflection yield-line mechanism (flat facets) plus any necessary pure membrane tension cracks.
• Internal work is done in plastic stretching of rebar mesh.
• Rebar ductility to fracture can be defined. Provisionally, rebar gauge length for x or y bars is spacing of transverse bars (weld points as anchors).
• Pattern of yield lines and tension cracks must be kinematically consistent as a mechanism.
Principles:
• Based on small-deflection yield-line mechanism (flat facets) plus any necessary pure membrane tension cracks.
• Internal work is done in plastic stretching of rebar mesh.
• Rebar ductility to fracture can be defined. Provisionally, rebar gauge length for x or y bars is spacing of transverse bars (weld points as anchors).
• Pattern of yield lines and tension cracks must be kinematically consistent as a mechanism.
N.B. Considering only the mechanics of TMA modelling – without temperature distribution.
g
Hogging rotations about edges of panel
Sagging rotations about internal yield lines
A
Yield lines at small deflection (usual mechanism)
rl
nl
l
Angle g, or intersection length nl, optimised for minimum failure load.
Crack b1 Crack b1
Crack b1 Crack b1
Cra
ck b2
Cra
ck b2
Crack b3 Crack b3
Crack a Crack a
Crack a Crack a
b
2b
2b
a
A
Slab facets at high deflection (usual mechanism)
nl
q
dA
DA
A A’
l/2 f
dA
D’A
A
A’
Plastic theory
External work= S(force resultant x vertical movement)
External work= Internal plastic work from stretching rebars
Rebar extensions
Crack opening at rebar level.
h
x
mt t
s
mt t z
Assumed reduced effective depth.
Assumed debonded rebar length
h
“Anchor” points Assumed gauge length
Internal plastic work in rebars
Crack Rebar
direction
Maximum rebar
length/l
Intact rebar length/l if bars fractured
Internal plastic energy Factor for
whole slab
a x 4
y 4
y 4c*
x 2
y 2
Short
edge x 0 2c*
* c=0 for isolated slab, c=1 for continuous slab.
Enhancement of yield-line capacity 9m x 6m slab, rebar fracture ductility 5%
0.0
0.5
1.0
1.5
2.0
2.5
0.0 1.0 2.0 3.0 4.0 5.0 6.0 7.0 8.0 9.0 10.0
Cap
acit
y en
han
cem
ent
fact
or
dA/d1
Initial yield line capacity
Slab capacity
b3 fracture start
b3 fracture
complete
b2 fracture start
ay fracture start
ax fracture start
ay fracture complete
ax fracture
complete
Sequence of rebar fractures
0.0
0.5
1.0
1.5
2.0
2.5
0.0 2.0 4.0 6.0 8.0 10.0
Enh
ance
men
t fa
cto
r
dA/d1
b3 fracture
start
9m x 6m slab: C30, S500, 5% rebar fracture ductility.
Sequence of rebar fractures
0.0
0.5
1.0
1.5
2.0
2.5
0.0 2.0 4.0 6.0 8.0 10.0
Enh
ance
men
t fa
cto
r
dA/d1
b
b2 fracture
start
9m x 6m slab: C30, S500, 5% rebar fracture ductility.
Sequence of rebar fractures
0.0
0.5
1.0
1.5
2.0
2.5
0.0 2.0 4.0 6.0 8.0 10.0
Enh
ance
men
t fa
cto
r
dA/d1
b
b3 fracture
complete
9m x 6m slab: C30, S500, 5% rebar fracture ductility.
Sequence of rebar fractures
0.0
0.5
1.0
1.5
2.0
2.5
0.0 2.0 4.0 6.0 8.0 10.0
Enh
ance
men
t fa
cto
r
dA/d1
b ay fracture
start
9m x 6m slab: C30, S500, 5% rebar fracture ductility.
Sequence of rebar fractures
0.0
0.5
1.0
1.5
2.0
2.5
0.0 2.0 4.0 6.0 8.0 10.0
Enh
ance
men
t fa
cto
r
dA/d1
b ax fracture
start
9m x 6m slab: C30, S500, 5% rebar fracture ductility.
Sequence of rebar fractures
0.0
0.5
1.0
1.5
2.0
2.5
0.0 2.0 4.0 6.0 8.0 10.0
Enh
ance
men
t fa
cto
r
dA/d1
b ay fracture
complete
ax fracture
complete
9m x 6m slab: C30, S500, 5% rebar fracture ductility.
0.0
0.5
1.0
1.5
2.0
2.5
0.0 1.0 2.0 3.0 4.0 5.0 6.0 7.0 8.0 9.0 10.0
Cap
acit
y en
han
cem
ent
fact
or
dA/d1
Enhancement of yield-line capacity 9m x 6m slab, effect of ductility
Ductility 5%
Ductility 7.5%
Ductility 10%
Different plate aspect ratios (10% ductility)
0.0
0.5
1.0
1.5
2.0
2.5
0.0 1.0 2.0 3.0 4.0 5.0 6.0 7.0 8.0 9.0 10.0
Cap
acit
y en
han
cem
ent
fact
or
dA/d1
r=2.0 r=1.5 r=1.0
r=1.0
r=2.0
r=1.5
r=10.0
r=10.0
Q & A
Q: Isn’t this counter-intuitive?
Surely a long plate effectively just folds about its central hinge ……
Q: Isn’t this counter-intuitive?
Surely a long plate effectively just folds about its central hinge ……
A2: Also …
Plastic mechanism theory is inherently upper-bound - we have to find the right mechanism.
A2: Also …
Plastic mechanism theory is inherently upper-bound - we have to find the right mechanism.
A1: No …
There’s still considerable change of geometry to stretch the rebar, apart from folding, away from the central zone.
A1: No …
There’s still considerable change of geometry to stretch the rebar, apart from folding, away from the central zone.
Alternative kinematically admissible mechanisms
TMA Enhancements from other mechanisms
Comparison of Mechanisms A and B 9m x 6m slab, rebar fracture ductility 5%
0.0
0.5
1.0
1.5
2.0
2.5
0.0 1.0 2.0 3.0 4.0 5.0 6.0 7.0 8.0 9.0 10.0
Cap
acit
y en
han
cem
ent
fact
or
dA/d1
Comparison of Mechanisms A and C 9m x 6m slab, rebar fracture ductility 5%
0.0
0.5
1.0
1.5
2.0
2.5
0.0 1.0 2.0 3.0 4.0 5.0 6.0 7.0 8.0 9.0 10.0
Cap
acit
y en
han
cem
ent
fact
or
dA/d1
Comparison of Mechanisms A and C 9m x 6m slab, rebar fracture ductility 5%
0.0
0.5
1.0
1.5
2.0
2.5
0.0 1.0 2.0 3.0 4.0 5.0 6.0 7.0 8.0 9.0 10.0
Cap
acit
y en
han
cem
ent
fact
or
dA/d1
0.0
0.5
1.0
1.5
2.0
2.5
0.0 1.0 2.0 3.0 4.0 5.0 6.0 7.0 8.0 9.0 10.0
Cap
acit
y en
han
cem
ent
fact
or
dA/d1
Comparison of all mechanisms 600m (!!) x 6m slab, rebar fracture ductility 5%
What else can this approach do?
Other capabilities:
• Continuity across slab edges (if bisymmetric),
Asymmetric boundary conditions makes optimizing yield-line pattern complex.
• Orthotropic mesh
Can even rotate the yield-line pattern.
• Non-rectangular slabs
Isosceles triangles are easy, trapezia are harder to optimize.
Other capabilities:
• Continuity across slab edges (if bisymmetric),
Asymmetric boundary conditions makes optimizing yield-line pattern complex.
• Orthotropic mesh
Can even rotate the yield-line pattern.
• Non-rectangular slabs
Isosceles triangles are easy, trapezia are harder to optimize.
How does the mid-span crack happen?
Increasing deflection of yield-line mechanism
Yield-line mechanism is a plastic bending mechanism at small deflections.
Yield-line mechanism is a plastic bending mechanism at small deflections.
As deflections start to increase the yield-line pattern increases the rotations of its flat facets, with the rebar yielding until it fractures.
As deflections start to increase the yield-line pattern increases the rotations of its flat facets, with the rebar yielding until it fractures.
So the initial large-deflection mechanism is Mechanism B. So the initial large-deflection mechanism is Mechanism B.
Force equilibrium of Mechanism B
S
C1
T1 T2 C2
M1 M2
M3
Shape of concrete compression blocks is dictated by compatibility and equilibrium:
• Initially tension and compression at every point of yield-lines.
• As deflection increases concrete compression blocks concentrate towards slab corners, rebar fractures when it exceeds ductility.
• No tension within compression blocks
Shape of concrete compression blocks is dictated by compatibility and equilibrium:
• Initially tension and compression at every point of yield-lines.
• As deflection increases concrete compression blocks concentrate towards slab corners, rebar fractures when it exceeds ductility.
• No tension within compression blocks
Shape of concrete compression blocks is dictated by compatibility and equilibrium:
• Initially tension and compression at every point of yield-lines.
• As deflection increases concrete compression blocks concentrate towards slab corners, rebar fractures when it exceeds ductility.
• No tension within compression blocks
Shape of concrete compression blocks is dictated by compatibility and equilibrium:
• Initially tension and compression at every point of yield-lines.
• As deflection increases concrete compression blocks concentrate towards slab corners, rebar fractures when it exceeds ductility.
• No tension within compression blocks
Change of stress blocks – ductile y-reinforcement
Compression
Tension
z
y
x
y
Shape of concrete compression blocks is dictated by compatibility and equilibrium:
• Initially tension and compression at every point of yield-lines.
• As deflection increases concrete compression blocks concentrate towards slab corners, rebar fractures when it exceeds ductility.
• No tension within compression blocks
Shape of concrete compression blocks is dictated by compatibility and equilibrium:
• Initially tension and compression at every point of yield-lines.
• As deflection increases concrete compression blocks concentrate towards slab corners, rebar fractures when it exceeds ductility.
• No tension within compression blocks
Change of stress blocks – ductile y-reinforcement
Compression
Tension
z
y
x
y
Shape of concrete compression blocks is dictated by compatibility and equilibrium:
• Initially tension and compression at every point of yield-lines.
• As deflection increases concrete compression blocks concentrate towards slab corners, rebar fractures when it exceeds ductility.
• No tension within compression blocks
Shape of concrete compression blocks is dictated by compatibility and equilibrium:
• Initially tension and compression at every point of yield-lines.
• As deflection increases concrete compression blocks concentrate towards slab corners, rebar fractures when it exceeds ductility.
• No tension within compression blocks
Change of stress blocks – ductile y-reinforcement
Compression
Tension
z
y
x
y
Shape of concrete compression blocks is dictated by compatibility and equilibrium:
• Initially tension and compression at every point of yield-lines.
• As deflection increases concrete compression blocks concentrate towards slab corners, rebar fractures when it exceeds ductility.
• No tension within compression blocks
Shape of concrete compression blocks is dictated by compatibility and equilibrium:
• Initially tension and compression at every point of yield-lines.
• As deflection increases concrete compression blocks concentrate towards slab corners, rebar fractures when it exceeds ductility.
• No tension within compression blocks
Change of stress blocks – ductile y-reinforcement
Compression
Tension
z
y
x
y
Shape of concrete compression blocks is dictated by compatibility and equilibrium:
• Initially tension and compression at every point of yield-lines.
• As deflection increases concrete compression blocks concentrate towards slab corners, rebar fractures when it exceeds ductility.
• No tension within compression blocks
Shape of concrete compression blocks is dictated by compatibility and equilibrium:
• Initially tension and compression at every point of yield-lines.
• As deflection increases concrete compression blocks concentrate towards slab corners, rebar fractures when it exceeds ductility.
• No tension within compression blocks
Change of stress blocks – ductile y-reinforcement
Compression
Tension
z
y
x
y
Shape of concrete compression blocks is dictated by compatibility and equilibrium:
• Initially tension and compression at every point of yield-lines.
• As deflection increases concrete compression blocks concentrate towards slab corners, rebar fractures when it exceeds ductility.
• No tension within compression blocks
Shape of concrete compression blocks is dictated by compatibility and equilibrium:
• Initially tension and compression at every point of yield-lines.
• As deflection increases concrete compression blocks concentrate towards slab corners, rebar fractures when it exceeds ductility.
• No tension within compression blocks
Change of stress blocks – ductile y-reinforcement
Compression
Tension
z
y
x
y
Shape of concrete compression blocks is dictated by compatibility and equilibrium:
• Initially tension and compression at every point of yield-lines.
• As deflection increases concrete compression blocks concentrate towards slab corners, rebar fractures when it exceeds ductility.
• No tension within compression blocks
Shape of concrete compression blocks is dictated by compatibility and equilibrium:
• Initially tension and compression at every point of yield-lines.
• As deflection increases concrete compression blocks concentrate towards slab corners, rebar fractures when it exceeds ductility.
• No tension within compression blocks
Change of stress blocks – ductile y-reinforcement
Compression
Tension
z
y
x
y
With different rebar ductility, mesh can either fracture abruptly or progressively at any stage.
With different rebar ductility, mesh can either fracture abruptly or progressively at any stage.
Change of stress blocks – possibilities with less ductility
Tension
z
y
x
y
With different rebar ductility, mesh can either fracture abruptly or progressively at any stage.
With different rebar ductility, mesh can either fracture abruptly or progressively at any stage.
Change of stress blocks – possibilities with less ductility
Tension
x
y
z
y
With different rebar ductility, mesh can either fracture abruptly or progressively at any stage.
With different rebar ductility, mesh can either fracture abruptly or progressively at any stage.
Change of stress blocks – possibilities with less ductility
Tension
x
y
z
y
Maximum concrete tensile stress - Mechanism B
S
C1
T1 T2 C2
M1 M2
M3
C1
T1
S
M1
M2
M3
0 6 3 1 2 4 5 0
6
3
1
2
4
5
Stre
ss (
N/m
m2
)
Deflection/slab thickness
• Slab 9m x 6m • Concrete Grade 30 • Mesh A142, S500 • Thickness 120mm • Mesh depth 60mm • Ductile rebar – no
fractures
• Slab 9m x 6m • Concrete Grade 30 • Mesh A142, S500 • Thickness 120mm • Mesh depth 60mm • Ductile rebar – no
fractures
EC3 tensile strength for C30
[0.3fc0.67]
EC3 tensile strength for C30
[0.3fc0.67]
Maximum concrete tensile stress - Mechanism B
S
C1
T1
M
C1
T1
S
M1
M2
M3
• Slab 6m x 6m • Concrete Grade 30 • Mesh A142, S500 • Thickness 120mm • Mesh depth 60mm • Ductile rebar – no
fractures
• Slab 6m x 6m • Concrete Grade 30 • Mesh A142, S500 • Thickness 120mm • Mesh depth 60mm • Ductile rebar – no
fractures
M
0 6 3 1 2 4 5
Stre
ss (
N/m
m2
)
Deflection/slab thickness
0
3.0
1.5
0.5
1.0
2.0
3.5
2.5
EC3 tensile strength for C30
[0.3fc0.67]
EC3 tensile strength for C30
[0.3fc0.67]
What’s still to do?
• Complete cracking + enhancement for all ductility cases,
• Composite action with beams – complete and partial,
• A better rebar debonding approach,
………………………..
• The effect of thermal displacements,
• Temperature distribution through the slab,
………………………..
• Asymmetric continuity – edge panels,
• Different panel shapes,
• Integration with transverse edge beam bending.
• Complete cracking + enhancement for all ductility cases,
• Composite action with beams – complete and partial,
• A better rebar debonding approach,
………………………..
• The effect of thermal displacements,
• Temperature distribution through the slab,
………………………..
• Asymmetric continuity – edge panels,
• Different panel shapes,
• Integration with transverse edge beam bending.
Thank you