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Transcript of Rcs1-Chapter5-ULS
1
Reinforced Concrete
Structures 1 - Eurocodes
RCS 1
Professor Marwan SADEKhttps://www.researchgate.net/profile/Marwan_Sadek
https://fr.slideshare.net/marwansadek00
Email : [email protected]
If you detect any mistakes, please let me know at : [email protected]
2
PLAN – RCS1
M. SADEK
Ch 1 : Generalities – Reinforced concrete in practice
Ch 2 : Evolution of the standards – Limit states
Ch 3 : Mechanical Characteristics of materials – Constitutive relations
Ch 4 : Durability and Cover
Ch 5 : Beam under simple bending – Ultimate limit state ULS
Ch 6 : Beam under simple bending – serviceability limit state SLS
Ch 7 : Section subjected to pure tension
3
Selected ReferencesFrench BAEL Code (91, 99)
Règles BAEL 91 modifiées 99, Règles techniques de conception et de calcul des ouvrages et constructions en béton armé, Eyrolles, 2000. J. Perchat (2000), Maîtrise du BAEL 91 et des DTU associés, Eyrolles, 2000. J.P. Mougin (2000), BAEL 91 modifié 99 et DTU associés, Eyrolles, 2000.….
EUROCODES H. Thonier (2013), Le projet de béton armé, 7ème édition, SEBTP, 2013. Jean-Armand Calgaro, Paolo Formichi ( 2013) Calcul des actions sur lesbâtiments selon l'Eurocode 1 , Le moniteur, 2013. J. M. Paillé (2009), Calcul des structures en béton, Eyrolles- AFNOR, 2009. Jean Perchat (2013), Traité de béton armé Selon l'Eurocode 2, Le moniteur,2013 (2ème édition) Manual for the design of concrete building structures to Eurocode 2, TheInstitution of Structural Engineers, BCA, 2006. A. J. Bond (2006), How to Design Concrete Structures using Eurocode 2, Theconcrete centre, BCA, 2006.https://usingeurocodes.com/
M. SADEK
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In addition to Eurocodes, the references that are mainly used to prepare this course material are : Thonier 2013
Perchat 2013
Paillé 2009
Some figures and formulas are taken from
Cours de S. Multon - BETON ARME Eurocode 2 (available on internet)
Cours béton armé de Christian Albouy
M. SADEK
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Chapter VBeam under simple bending – Ultimate limit
state ULS
1. Introduction
2. Design Assumptions
3. Rectangular Section without compression Steel
4. Rectangular Section with compression Steel
5. T Section
6. Particular rules
6M. SADEK
Embedded beam
Drop Beam
Inverted beam
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
7M. SADEK
Beam subjected to simple bending : M(x), V(x)
Note : In Reinforced concrete, bending stress and shear stress are treated separately.
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
8M. SADEK
Simple / Pure bending
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
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Initiation of cracking
Increase in Cracks
Excessive strain in Steel / Crushing of Concrete
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
10M. SADEK
Beam subjected to simple bending (ULS)
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
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ASSUMPTIONS
H1) Principle of Navier-Bernoulli : After deformation, plane sections
remain plane and normal to the axis of the beam (linear strain diagram)
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
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ASSUMPTIONS
H2) The tensile strength of the concrete is neglected
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
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ASSUMPTIONSH3) bundled bars are treated as a single bar of a diameter derived
from the equivalent total area and placed at the COG of the group
H4) Total bond between concrete and steel (no relative slip)
at the contact : s=c
H5) The design stress-strain diagram for the concrete and the steel
are :
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
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Stress-Strain Diagram for concrete under compression
a) Parabola-rectangle
b) Bi-linear
fcd :Design value of concrete compressive strength (cylinder, t28 days)
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
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c) Rectangular stress distribution
Note : In the present course, we will use the diagram c (simplified).
The use of diagrams a and b are authorized by the EC2, See Annexes
for more details
cc= 1 (FNA)
C = 1.5 (Persistent situation ) ; 1.2 (Accidental situation)
Stress-Strain Diagram for concrete under compression
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
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Design :
Horizontal top branch without the need to check the strain limit.
Inclined top branch with a strain limit (s ud = 0.9ud )
s = 1.2 (persistent)
1.0 (accidental)
Stress-Strain Diagram for concrete under compression
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
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Example : Persistent situation : fyd = fyk / s= 435 MPa
se = fyd/Es = 2.17.10-3
< se => s = 200 000
> se => s = 435 MPa.
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
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s > se
s 435 + 727 (s -2.17.10-3) < 466 MPa for steel B
s 435 + 952 ( s -2.17.10-3) < 454 MPa for steel A
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
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Rule of 3 Pivots :The design of a RC section at ULS is carried out assuming that the stress-strain
diagram through one of the 3 Pivots A, B or C.
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
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Pivot A (Not very frequent)
Steel : c cu
s = ud that depends on the steel type (A, B or C)(no limitation when the horizontal top branch diagram is used)
Difference with BAEL : The EC2 fix the pivot A at ud higher than 10x10-3 (BAEL)
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
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Pivot B (Common Case)
Concrete : c = cu2 =3.5 ‰ , c2 =2 ‰ (for fck50 MPa)
s ud
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
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Pivot C
(h-y) / h = c2/cu2 => y = (1-c2/cu2).h
(Compression, bending with axial force)
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
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Simple Bending, ULS
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
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Fundamental Combination (detail in Ch. 2)
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
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c
s
sc
Strain Diagram
Internal Forces
Fc,sc
Fsc
Fc
Fs
z
A : Cross sectional area of reinforcement (tension zone) (A or As)
d : Effective depth of a cross-section : distance from the C.O.G of the tension steel to the extreme
compression fibre
A’ : Cross sectional area of compression steel
d’ : distance from the C.O.G of the compression steel A’ to the extreme compression fibre
z : Lever arm of internal forces
M > 0
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
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Fc : Resultant of compression force in the concrete
Fsc : Resultant of compression force in the compression steel
Fc,sc : Resultant of Fc and Fsc
Fs : Resultant of tensile force at the tensile steel
x : Position of the N.A
c
s
sc
Strain Diagram
Internal Forces
x Fc,sc
Fsc
Fc
Fs
z
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
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c
s
scx Fc,sc
Fsc
Fc
Fs
z
Equilibrium of forces Fs = Fc,sc
Equilibrium of moments MEd = Fc,sc .z = Fs.z
3 Unknowns (in general) : A, A’, x
Strain Diagram
Internal Forces
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
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Rectangular section, Without compression steel (A’=0)
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
29
Simplification of the constitutive law of the Steel
EC2 3.1.7(3)
Rectangular section, Without compression steel (A’=0)
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
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1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
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Fc
FS
Fc = Fs
MED = Fc.z
z
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
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Dimensionless Form :
By substituting :
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
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fck 50 MPa, = 1 ; =0.8
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
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Note that :
x = u.d =(c / c+s) d
u = (c / c+s)
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
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Boundaries of Pivots A, B
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
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Steel type A ud = 22,5 .10-3AB = (3.5 / 3.5+22.5) = 0.135 AB = 0.102
Steel type B AB =0.072 AB = 0.056
Steel type C AB =0.049 AB = 0.039
fck 50 MPa, = 1 ; =0.8
Boundaries of Pivots A, B
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
37
Pivot B AB u
It can be noted that in general, the Pivot B is reached
c = cu2 =3.5 ‰ ; s ud
s = (1/u -1) cu
(The concrete reaches its maximum strength)
Boundaries of Pivots A, B
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
38
Pivot B AB u lim
The tensile steel stress should not be in the elastic domain (non economical
solution) ! In this case, the tensile steel section should be reduced , or a
compression steel should be added.
s ud but s se
Line BE (Pivot B & steel at
elastic limit)
Boundaries of Pivots A, B
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
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(fck 50 Mpa)
Persistant Situation Accidentelal Situation
s = 1.15 s = 1
fyk(MPa) lim lim lim lim
400 0.668 0.392 0.636 0.380
500 0.617 0.372 0.583 0.358
lim = BE
Pivot B AB u lim
Boundaries of Pivots A, B
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
40
Pivot A
s =ud ; c =cu
u AB
Boundaries of Pivots A, B
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
41
Tensile steel section A (fck 50 MPa)
a) Stress-Strain diagram with Inclined Top branch
i. u AB Pivot A
s = 455 MPa (Steel A) , 466 MPa (Steel B)
ii. AB u lim Pivot B
s = (1/u -1) cu
s 435 + 727 (s -2.17.10-3) < 466 MPa Steel B
s 435 + 952 (s -2.17.10-3) < 454 MPa Steel A
(A’=0, u lim )
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
42
Tensile steel sectiopn A (fck 50 MPa)
b) Stress-Strain diagram with horizontal Top branch
(A’=0, u lim )
s = fyd
Note : No limitation for the steel strain
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
43
Note 1
Effective depth d – Initial value dini
The exact value of d could not be determined before the choice of the steel
reinforcement.
Take d 0.9 h for common beams (this formula is not safe for embedded beam
and for slab with low thickness 20 cm)
Take d = h – cnom – 1 cm (Slab with a thickness 20 cm )
After the determination of the reinforcement, it becomes possible to calculate the
exact value of d=dreal. If dreal < dini , the steel reinforcement section As should be
recalculated.
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
44
Note 2
Approximate value of A (Quick check)
z 0.9 ; d 0.9 h
This formula doesn't give any information about the compression stress
in the concrete. It becomes obsolete if a compression steel is required.
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
45
Minimum Reinforcement (to prevent brittle failure)
For rectangular section bh, the ultimate resistant bending moment of Non-
reinforced concrete :MRc = (I/v) fctm = (b.h²/6) fctm
The minimum As,min section should resist the following moment
MRs = As,min fyk z
By considering MRc = MRs , and substituting z 0.9 h ; h d / 0.9
As,min = b.d.[fctm/(0.9 0.81 6)fyk] 0.23 b d fctm / fyk
L’EC2 replace the value of 0.23 by 0.26 and fix a lower limit of the quantity 0.26 fctm/fyk
with the value 0.0013
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
46
Minimum Reinforcement
Maximum Reinforcement
As,max = 0,04 Ac
Ac : denotes for the cross sectional area of the concrete
As,max : Maximum steel reinforcement in both compression and tension zones
As,min : Minimum tensile section of longitudinal steel reinforcement;
bt : denotes the mean width of the tension zone;
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
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Rectangular section , With compression steel (A’0)
u lim
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
48
3 unknowns (A, A’, x) / 2 equations ???
Infinite number of solutions
Possibility n°1 : Minimum of “A+ A’ " (long run)
Possibility n°2 : Concept of limit Moment (adopted in general)
- Resolution by the decomposition method - 2 imaginary sections
u lim
Rectangular section , With compression steel (A’0)
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
49
2 imaginary sections
Maximum capacity of the concrete Mlim A1
The compression steel A’ will resist (Med Mlim) A2
u lim Med Mlim= lim .b.d².fcd
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
50
cu
s
scx=lim.d
d’
d
A1 = Mlim / (1 – 0.4.lim).d.fyd
A’ = (Med – Mlim) / [sc . (d-d’)]
sc = 3,5.10-3. (1-d’/xlim)
The value of sc is close to 3 °/°° (>se), in other terms sc=fyd when using the diagram
with horizontal top branch, and a value slightly great than fyd when using the diagram
with inclined top branch.
In general, we take a value sc=fyd .
A2 = A’. sc / s = A’. fyd / s
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
51
A1 = Mlim / [(1 – 0.4.lim).d.fyd]
A2 = A’. sc / s
A’ = (Med – Mlim) / [fyd . (d-d’)]
When using same types and grade for A and A’ sc = s = fyd
A2 = A’
A = A1 + A2
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
52
Note 1 : The EC2 don’t restrict the moment that could be supported by
the compression steel like the previous BAEL standard (40% Med).
However A’ is limited by the maximum requirement
A+A’ As,max = 0,04 Ac
Note 2 : Any compression longitudinal reinforcement (diameter )
which is included in the resistance calculation should be held by
transverse reinforcement with spacing not greater than 15 .
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect.Sec with A’ 6. Particular rules
53
T Section
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect. Sec with A’ 6. Particular rules
54
Effective width of flanges (all limit states)
l0 : distance between points of zero moment
(EC 2-1-1, 5.3.2)
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect. Sec with A’ 6. Particular rules
55
Effective width of flanges (All limit states)
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect. Sec with A’ 6. Particular rules
56
(EC 2-1-1, 5.3.2) Effective width of flanges (All limit states)
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect. Sec with A’ 6. Particular rules
57
Maximum resistant moment that could be supported by the
flange (flange in compression)
2f
uT eff f cd
hM b h f ( d )
1sA
ux fh
s 1sN
1cN
ff h,dz 501
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect. Sec with A’ 6. Particular rules
58
Case 1: Common case M Mu uT
bw
b = beff
d
hf
The Neutral Axis is located in the flange, the
flange is partially in compression
The T section is calculated as a rectangular
section (width beff and height h)
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect. Sec with A’ 6. Particular rules
59
Case 2: The Neutral Axis is located in the WebM Mu uT
Divide the section in 2 imaginary sections
The reinforcement section is expected to be very significant
bw
b=beff
d
hf
=
beff-bw
A1 A2
bw
+
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect. Sec with A’ 6. Particular rules
60
M Mu uT
1eff w
u uTeff
b bM M
b
Section A1 will resist:
bw
b=beff
d
hf
=
beff-bw
A1 A2
bw
+
A1= (beff-bw)×h0×fcd / s(s = fyd, diagram with horizontal top branch)
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect. Sec with A’ 6. Particular rules
61
M Mu uT
Section A2 will resist
Calculation identical to a rectangular section with a width
bw and a height h
bw
b=beff
d
hf
=
beff-bw
A1 A2
bw
+
M M Mu u u2 1
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect. Sec with A’ 6. Particular rules
62
M Mu uT
s = fyd , diagram with horizontal top branch or Pivot A (palier incliné)
s = to be determined function of s if Pivot B (diagram with inclined top branch). This stress could be used when calculating A1
cdw
uu fdb
M22
2 u u2 2125 1 1 2 , ( )
Note: Introduce A’ whenu2 > lim
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect. Sec with A’ 6. Particular rules
63
M Mu uT
bw
b=beff
d
hf
=
beff-bw
A1 A2
bw
+
A = A1 + A2
A1= (beff-bw)×h0×fcd / s
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect. Sec with A’ 6. Particular rules
64
Predimensioning of concrete section – Rectangular section
b
hIf b is not imposed , we can take
0.3 h b 0.5 h
We fix b, and we find the value of h
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect. Sec with A’ 6. Particular rules
65
b
hb/h 0.4 ; h 2.5 b
d 0.9 h = 2.25 d
Pivot B AB u lim
Steel B 0.056 u 0.372
0.056 Med / bd²fcd 0.372
Predimensioning – Rectangular section
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect. Sec with A’ 6. Particular rules
66
b
h
Other criterion
- Design at SLS + maximum deflection condition
Steel A
Predimensioning – Rectangular section
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect. Sec with A’ 6. Particular rules
67
Effective span of beams and slabs in buildings (EC2 - 5.3.2.2)
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect. Sec with A’ 6. Particular rules
68
Other detailing arrangements (EC2 - 9.2.1.2)
1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect. Sec with A’ 6. Particular rules
69
Extracted from Thonier (2013)1. Introduction 3. Rect.Sec. (A’=0) 5. T Section2.Assumptions 4. Rect. Sec with A’ 6. Particular rules
70
Exercices Rectangular section without compression steel:
Tensile steel reinforcement
o using the stress strain diagram with inclined top branch
o using the stress strain diagram with horizontal top branch
o Exact value of d
Rectangular section with compression steel:
Determination of the reinforcement steel sections (tension and
compression)
Predimensioning of a rectangular section of concrete and determination of
the steel reinforcement while taking in account the beam self weight
Design of T section