Strut & Tie
Webinar 12.30 4 July 2016Charles Goodchild
BSc CEng MCIOB MIStructE The Concrete CentreWhat is Strut and Tie?
A structural element can be divided into:
•
B (or beam or Bernoulli) regions ‐ in which
oplane sections remain plane and odesign is based on ‘normal’ beam theory,and into
•
D (or disturbed) regions ‐ in which
oplane sections do not remain plane; o‘normal’ beam theory may be considered inappropriate oStrut & Tie may be used. ousually within hof a discontinuity: 2D (or disturbed) regions
3 D regions Pile caps Deep beams Discontinuities Holes Edge beams Pad footings Supports Loads Corbels Wall beamsWhy use Strut and Tie?
•
Simple Model for complex problems
•
Easy to understand
•
The engineer stays in control – it is not a
complicated computer analysis
•
Can provide more economical solutions
•
It is very powerful for the analysis of existing
structures
4What is strut and tie?
Strut‐and‐tie models (STM) are like trusses consisting of struts, ties and nodes. 5 a) Modelling Imagine or draw stress paths which show the elastic flow of forces through the structure b) STM Replace stress paths with polygons of forces to provide equilibrium. A deep beam Conventionally, struts are drawn as dashed lines, ties as full lines and nodes numbered. 5What is strut and tie?
Strut and tie models consist of: • Struts (concrete) • Ties (reinforcement) • Nodes (intersections of struts and ties). Eurocode 2 gives guidance for each of these. • In the UK this is the first time that S&T has been codified for general use. • It says that in principle, where non‐linear strain distribution exists, i.e. in D‐regions, strut and tie models may be used, e.g. for: • Pile caps • Deep beams • Supports • Concentrated loads • Openings, etc. 6Lower Bound method
Strut and tie models are based on the lower bound theorem
of plasticity which states that any distribution of stresses
resisting an applied load is safe providing:
Equilibriumis maintained and Stresses do not exceed “yield” 7Design Process
8Design Process
1. Define and isolate B and D regions
2. Develop an STM
3. Design the members of the STM – struts, ties and
nodes
4. Iterate to optimise the STM as necessary to
minimise strain energy
91. B & D regions
A structure can be divided into: •B (or beam or Bernoulli) regions and •D (or disturbed) regions 10 D regions 10As before:
11 a) Modelling Imagine or draw stress paths which show the elastic flow of forces through the structure b) STM
Replace stress paths with polygons of forces to provide equilibrium.
A deep beam
Conventionally, struts are drawn as dashed lines, ties as full lines and nodes numbered.
2. Develop an STM
11As before:
a) Consider a deep beam with an udl b) Consider elastic stresses (here using FEA) A A Consider elastic stresses in section A‐ADeveloping an STM
12Centroid of compressive force
Stress distribution within deep beam with udl
Section A‐A Centroid of tensile force
Developing an STM
13Developing an STM
a) Consider a deep beam with an udl b) Consider elastic stresses (here using FEA) c) Construct STM 14Construction of STMs
Elastic analyses of deeper beams with point load
Construction of STMs
Very deep beams
Construction of STMs
Good and bad model based on minimising length of ties
Minimise tie lengths (minimises energy used) 17 18
a)
Struts
b)
Ties
c)
Nodes
3. Design members
18P1 P2
Question: at failure which is bigger P
1or P
2?
•Concept by R Whittle/A Beeby, drawn by I Feltham. Used with permission3a) Struts
Possible answers: A) P1/P2 > 2.0 B) P1/P2 = 2.0 C) P1/P2 = 1.5 D) P1/P2 = 1.0 E) P1/P2 = 0.5 19 P1 P2
2P
13a) Struts
Answer: E) P
1/P
2= 0.5
20 Possible answers: A) P1/P2 > 2.0 B) P1/P2 = 2.0 C) P1/P2 = 1.5 D) P1/P2 = 1.0 E) P1/P2 = 0.5fcd fcd fctd, yy fctd,zz
Bi‐axial strength of Concrete
3a) Struts
0 0 22 Tension Reduction in compressive strength Where there is no transverse tension Rd,max= fcd = 0.85fck/1.5 = 0.57 fck Otherwise, where there is transverse tension Rd,max= 0.6 ’fcd Where: ’ = 1‐fck/250 Rd,max= 0.6 x (1‐fck/250) x 1.0 x fck/1.5 = 0.4 (1‐fck/250) fck3a) Struts
EC2 says:
23Discontinuities
Areas of non‐linear strain distribution are referred to as “discontinuities” Partial discontinuity Full discontinuity Curved compression trajectories lead to tensile forces3a) Struts
24Partial discontinuity
Tension, T, is taken by the reinforcement When b ≤ H/2 T = ¼ [(b – a )/b] F Reinforcement ties to resist the transverse force T may be “discrete” or can be “smeared” over the length of tension zone arising from the compression stress trajectories T T3a) Struts
25Full discontinuity
Tension, T, is taken by the reinforcement When b > H/2 T = ¼ (1 – 0.7a /h) F Reinforcement ties to resist the transverse force T may be “discrete” or can be “smeared” over the length of tension zone arising from the compression stress trajectories T3a) Struts
T 26Note the 2 componentsto the strut dimension
Dimensions of the strut are determined by dimensions of the nodes and assumptions made there.
3a) Struts
27Up to now we have been talking about prism struts.
3a) Fan Struts
In a uniformly loaded deep beam, the flow of internal forces may be visualized either by fan strut‐and‐tie
models or by using more elaborate discontinuous stress fields.
more realistic Usual to assume fan struts OK and check the common governing criterion. . . . . the CCT node Fan struts
Design strength, f
yd= f
yk/1.15
A
s= F
Ed/f
yd3b) Ties
NB. Reinforcement should be anchored into nodes. Anchorage may start in the extended nodal zone (= strut area) 29Nodes are typically classified as: CCC – Three compressive struts CCT – Two compressive struts and one tie CTT – One compressive strut and two ties
3c) Nodes
30CCC nodes
(e.g. column onto two pile cap) The maximum stress at the edge of the node: Rd,max = k1’fcd Where: k1 = 1.0 ’ = 1‐fck/250 Rd,max = (1‐fck/250) x 0.85 x fck/1.5 = 0.57 (1‐fck/250) fckThe stresses c0& Rd,2etc are all the same.
3c) Nodes
CCT nodes
(e.g. beam at end support)The maximum compressive stress is: Rd,max = k2’fcd Where: k2 = 0.85 ’ = 1-fck/250 Rd,max = 0.85 (1-fck/250) x 0.85 x fck/1.5 = 0.48 (1-fck/250) fck
(based on the more critical of the two struts)
3c) Nodes
32CTT nodes
(e.g. closing corner of a wall) The maximum compressive stress is: Rd,max = k2’fcd Where: k2 = 0.75 ’ = 1‐fck/250 σRd,max = 0.75 (1-fck/250) x 0.85 x fck/1.5 = 0.43 (1-fck/250) fck3c) Nodes
334) Iterate
2‐pile cap – probably not Cantilever wall beam (deep beam) with window – definitely 34Examples
35Pile‐cap worked example
Using a strut and tie model, what tension reinforcement is required for a pile cap supporting a 500 mm square column carrying 2500 kN (ULS), and itself supported by two‐piles of 600 mm diameter. fck= 30 MPa 2 500 kN (ULS) 2700 1400 150 Breadth = 900 mm 36 Angle of strut = tan‐1(900/1300) = 34.7° Width of strut* = 250/cos 34.7° = 304 mm Force per strut = 1250/cos 34.7° = 1520 kN Force in tie = 1250 tan 34.7° = 866 kN 2 500 kN (ULS) 1800 1400 1 250 kN (ULS) 100 Strut angle 500/2 = 250 1 250 kN (ULS) 34.7o34.7o 866 kNSTM
*Conventional but simplistic - see later
Pile‐cap worked example
Check stresses in strut Stress in strut (top) =1520 x 103/(304 x 500) =10.0 MPa Strength of strut (conservatively assuming some transverse tension): Rd,max = 0.4 (1‐fck/250) fck = 10.6 MPa Tie : Area of steel required: As ≥ 866 x 103/435 ≥ 1991 mm2 Use 5 H25s 866 kN Therefore OK Usually QED But for the sake of thoroughness . . . . .
Pile‐cap worked example
38 • Nodes: top Rd,2 = 10.0 MPa (as before) Rd,3 = 10.0 MPa (as before) Rd,1 = 2500 x 103/(5002) = 10.0 MPa Rd,max (for CCC node) = 0.57 (1‐fck/250) fck = 15.0 MPa 39 2500 kN 1520 kN 1520 kN 2500 kN 1520 kN 1520 kN (Upside down elevation!) (Elevation)
Pile‐cap worked example
(thorough)Nodes: bottom (as a check) Strut above Width of strut* = 600/cos 34.7° = 730 mm Stress in strut (bottom as an ellipse) Rd,2=1520 x 103/(600 x 730 x /4) = 4.4 MPa Rd,1= 1250 x 103/( x 3002) = 4.4 MPa Rd,max (for CCT node) = 0.48 (1‐fck/250) fck = 12.7 MPa OK = 1250 kN 1038 kN
*Conventional but simplistic - see later
Pile‐cap worked example
(thorough)40
Comparison:
Compare previously designed pile
cap using bending theory
MEd=2500 x 1.800/4 = 1125 kNm Assume:25 mm for tension reinforcement 12 mm link
d = h – cnom‐ link‐ 0.5
= 1400 – 75 ‐ 12 – 13 = 1300 mm
Pile‐cap worked example
(thorough)Comparison:
As= 1125 x 106/ (435 x 1270) = 2036 mm2 Use 5 H25 (2454 mm2) ' 025 . 0 30 1300 900 10 1125 2 6 ck 2 Ed K f bd M K 208 . 0 ' K
1 1 3.53 0.025
1270mm 2 1300 53 . 3 1 1 2 d K z K’ 1.00 0.208 0.95 0.195 0.90 0.182 0.85 0.168 0.80 0.153 0.75 0.137 0.70 0.120c.f. using S&T 1991mm2req’d and 5H25 provided
Pile‐cap worked example
(thorough)42
For the CCT node: wcos not used in previous calc.
So for the CCC node RE *previous statement that calculated strut dimensions were “Conventional but simplistic ‐ see later” In highly stressed situations in CCCs, fib bulletin 62 allows a local STM to take account of the reinforcement from columns.
Strut dimensions
Pile‐cap worked example
(thorough)43 Hence struts themselves are rarely critical.
2, 3 & 4 Pile‐caps
Forces in ties
Pile‐caps etc.
Detailing Detailing of reinforcement anchorage critical – 100% As needed up to extended node (large radius bends may be required) Using S&T, anchorage of 100% As required here cf 25% from here if using bending theoryPile‐caps etc.
45Detailing
Where flexural design has been used it is common UK practice to provide uniform distribution of reinforcement. However, EN 1992‐1‐1 Clause 9.8.1(3) suggests that “the tensile reinforcement . . . should be concentrated in the stress zones between the tops of the piles”. There is evidence to suggest that bunching orthogonal reinforcement leads to a standard 4‐pile cap being 15% stronger than using the same amount of uniformly distributed reinforcement. The requirement for concentrating reinforcement can be interpreted in different ways but the apparent shortcoming can be alleviated by providing transverse tension and tie‐back reinforcement to distribute forces from bars as indicated in Figure 5.5 (wait for it!). For pile caps supporting structures other than bridges, there would appear to be little reason to deviate from the advice given in BS8110 “ . . only the reinforcement within 1.5 times the pile diameter from the centre of a pile shall be considered to constitute a tension member of a truss”. So in this case, 5 no. H25s distributed across a 900 mm wide pile cap section is considered satisfactoryTensile force in tie
Tensile force in tie
Pile‐caps etc.
46Problem
Deep beam worked example
47STM
Deep beam worked example
48 Consider moment about B RA = 2529 x 3.05 / 4.30 = 1794 kN So RB = 2529 ‐ 1794 = 735 kN F12 = 1794 x 1.80 / 1.30 = 2484 kN strut F13 = 2484 x 1.25 / 1.80 = 1725 kN tie F34 = F56 = 735 kN ties Forces Check bearing stresses At node 2, under load F Ed = 2529 x 103 / (450 x 450) = 12.5 MPa CCC node ∴ Rd= 1.0 x (1 – 35/250) x 0.85 x 35 / 1.5 = 17.1 MPa ∴ OK At node 1 at support A (see Figure 5.8) Ed = 1794 x 103 / (475 x 450) = 8.39MPa CCT node ∴ Rd= 0.85 x (1 – 35/250) x 0.85 x 35 / 1.5 = 14.5 MPa ∴ OK At node 7 at support B OK by inspectionDeep beam worked example
49 Ties F13 = 1725 kN: As req’d = 1725 x 103 / (500/1.15) = 3968 mm2 Try 8H25 (3928 mm2 say OK) in two layers i.e. 2 x 4 H25 @ 50 mm cc by inspection provide bobs at end of bars F34 = F56 = 735 kN : As,req’d= 735 x 103 / (500/1.15) = 1690 mm2per tie i.e. per 3.05/3m say 1690 mm2/m. Try H16@225 both sides (1768 mm2/m) Bursting forces (bottle ties)Check strut 1‐2: F12 = 2484 KN strut has full discontinuity T = ¼ (1 – 0.7a/H) F
T = ¼ (1 – 0.7 x 0.18) x 2484 = 542.8 kN ∴ As reqd = 542.8 x 103 / (500 / 1.15)= 1248 mm2
To be placed between 0.2H and 0.5H from the loaded surface. i.e. 1248 mm2to be placed
over 0.3 x 1800 = 540 mm ≡ 2311 mm2/m over 540 mm at 1.25 in 1.30 slope.
Try H16@ 175 (1148 mm2/m) both ways both sides (2296 mm2/m both ways (say OK))
Deep beam worked example
50
Summary
Other examples
• T‐headed bars Vertical section: • Double headed T‐headed bars in shear assemblies Similar plan section: • Single headed T‐headed bars in short lap assemblies or anchorages. 52
Other examples
Other examples (advanced)
53Analysis of two-storey wall beam Analysis and design of a coupling beam (with hole) within a shear wall in a 54-storey block.
strut inclination method
cot sw s Rd, z fywd s A V 21.8 < < 45Eurocode 2 – Beam shear:
54
Other examples
Why use Strut and Tie?
•Simple Model for complex problems •Easy to understand •The engineer stays in control – it is not a complicated computer analysis •Can provide more economical solutions •It is very powerful for the analysis of existing structures 55Further reading
56
1) British Standards Institution (2004) EN‐1992‐1‐1:2004. Eurocode 2. Design of concrete structures. Part 1. General rules and rules for buildings, London, UK: BSI
2) Schlaich J. and Schäfer K. (1991) ‘Design and detailing of structural concrete using strut‐and‐tie models’, The Structural Engineer, 69 (6), pp. 113–125
3) International Federation for Structural Concrete (2011) fib Bulletin No. 61: Design examples for strut‐and‐tie models, Lausanne, Switzerland: fi b 4) Thurlimann B., Muttoni A. and Schwartz J. (1989) Design and detailing of reinforced concrete structures using stress fi elds, Zurich, Switzerland: Swiss Federal Institute of Technology
5) Goodchild C., Morrison J. and Vollum R. L. (2015) Strut‐and‐tie Models, London, UK: MPA The Concrete Centre 6) Schlaich J., Schäfer K. and Jennewein M. (1987) ‘Towards a consistent design of structural concrete’, PCI Journal, 32 (3), pp. 74–150 7) Sagaseta J. and Vollum R. L. (2010) ‘Shear design of short‐span beams’, Magazine of Concrete Research, 62 (4), pp. 267–282 8) CEB‐FIP (1990) Model Code for Concrete Structures, Lausanne, Switzerland: CEB‐FIP 9) British Standards Institution (2005) NA to BS EN 1992‐1‐1:2004 UK National Annex to Eurocode 2. Design of concrete structures. Part 1. General rules and rules for buildings, London, UK: BSI 10) British Standards Institution (2010) PD 6687‐1:2010 Background paper to the National Annexes to BS EN 1992‐1 and BS EN 1992‐3, London, UK: BSI 11) Hendy C. R. and Smith D. A. (2007) Designers’ Guide to EN 1992 Eurocode 2: Design of concrete structures. Part 2: concrete bridges, London, UK: Thomas Telford 12) Schlaich J. and Schäfer K. (2001) ‘Konstruieren im Stahlbetonbau’ (in German), BetonKalender (Vol 2), Berlin, Germany: Ernst & Sohn, pp. 311–492 13) Vollum R. L. and Fang L. (2014) ‘Shear enhancement in RC beams with multiple point loads’, Engineering Structures, 80, pp. 389–405 AMERICAN CONCRETE INSTITUTE, Building Code Requirements for Structural Concrete and Commentary ACI 318‐08, ACI, Farmington Hills MI 2008. “ACI 318”. 2 SCHLAICH, J., SCHAFER, K.: “Design and detailing of structural concrete using strut and tie models”, The Structural Engineer, Vol. 69, No. 6, March 1991, pp. 113‐125. 3 CEB‐FIP. Model Code for Concrete Structures, CEB‐FIP International Recommendations, 1990, “Model Code 90”. 4 CANADIAN STANDARDS ASSOCIATION (CSA A.23.3‐04). Design of Concrete Structures, 2004. 5 COLLINS M. P. and MITCHELL D. Prestressed Concrete Structures, 1st edn. Prentice Hall, Englewood Cliffs, New Jersey, 1991. 6 BRITISH STANDARDS INSTITUTION. BS EN 1992–1–1, Eurocode 2 – Part 1–1: Design of concrete structures – General rules and rules for buildings. BSI, 2004. 6a National Annex to Eurocode 2 – Part 1–1 incorporating Amendment 1. BSI, 2009. 7 HENDY, C R & SMITH D A. Designer’s Guide to EN 1992‐2, Eurocode 2: Design of concrete structures, Part 2: Concrete Bridges.Thomas Telford, London, 2007. 8 SAHOO K D, SINGH B & BHARGAVA P. Minimum Reinforcement for Preventing Splitting Failure in Bottle shaped Struts, ACI Structural Journal, March April 2011, pp. 206‐216. 9 SIGRIST V , ALVAREZ M & KAUFMANN W. Shear And Flexure In Structural Concrete Beams, ETH Honggerberg, Zurich, Switzerland, (Reprint from CEB Bulletin d’Information No. 223 “Ultimate Limit State Design Models” June 1995). 10 BRITISH STANDARDS INSTITUTION. BS 8004 Code of practice for Foundations, BSI, 1986. 11 BLEVOT, J. L., AND FREMY, R. “Semelles sur Pieux,” Institute Technique du Batiment et des Travaux Publics, V. 20, No. 230, 1967, pp. 223‐295. 12 BRITISH STANDARDS INSTITUTION. BS 8110‐1:1997 Structural use of concrete ‐ Part 1: Code of practice for design and construction, Amd 4, BSI,2007 13 THE INSTITUTION OF STRUCTURAL ENGINEERS. Standard Method of Detailing Structural Concrete. A Manual for best practice. (3rd edition) 2006, ISBN, 978 0 901297 41 9