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University of Hongkong reinforced concrete design
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Theory and Design of Structures IReinforced Concrete Design
Scope• Rectangular singly and doubly reinforced beams• Elastic design• Limit state design concepts; material strength
and loading• Flexural strength and shear strength of beams;
one-way slabs
References1. BS8110: 1985, Structural use of concrete – Part 3: Design charts for
singly reinforced beams, doubly reinforced beams and rectangularcolumns, BSI, London, 1985.
2. BS8110: 1997, Structural use of concrete – Part 1: Code of practice for design and construction, BSI, London, 1997.
3. Code of practice for structural use of concrete 2004, second edition, Buildings Department, Hong Kong, 2008.
4. Design of structural elements: concrete, steelwork, masonry and timber design to British standards and Eurocodes, 2nd ed., C. Arya, Spon Press, London, 2003.
5. Reinforced concrete design, 5th ed., W.H. Mosley, J.H. Bungey and R. Hulse, Macmillan Press, Basingstoke, 1999.
6. Reinforced concrete designer’s handbook, 10th ed., C.E. Reynolds and J.C. Steedman, E. & F.N. Spon, London, 1988.
7. Reinforced concrete design to BS8110: simply explained, A.H. Allen, E. & F.N. Spon, London, 1988.
8. Structural design in concrete to BS8110, L.H. Martin, P.C.L. Croxton and J.A. Purkiss, Edward Arnold, London, 1989.
Introduction• Steel reinforcement is introduced into a concrete
beam mainly to carry tension, thereby resulting in a reinforced concrete (RC) beam.
• Components: concrete and reinforcing bars (rebars)
Rectangular beam T-beam
Tensionreinft.
Singly reinforced beam
Tension reinft.
Doubly reinforced beam
Comp. reinft.
Stirrup carrier or link hanger
Stirrup or link
Introduction
Figure 1(a) Plain concrete beam under loading.
fc
fc′
b
d
Z = b d 2 / 6
*
*
Compressive strength
Compression
Tension
Modulus of rupture
Cracks & collapses!
Plain concrete beam (Unreinforced concrete beam)
Introduction
Figure 1(b) Reinforced concrete beam under loading.
T Section
(cracked)
C
a
M = C⋅a = T⋅a
Compression
Tension
Neutral axis
Load increases
N.A.
Concrete cracks
• Distinct yield point• Linear relationship within elastic range• Beyond the yield point, plastic deformation
followed by work hardening
Properties of steel
stre
ss
strain
Y.P.
Stress-strain curves for steel.
• No clearly defined yield point• Portion of the curve below 1/3 of the ultimate
strength is nearly linear• Beyond that, it becomes elasto-plastic
Properties of concrete
stre
ss
strainStress-strain curves for concrete
Methods of design1. Elastic theory (elastic method in CP114 and
previous HK codes)
2. Ultimate load / load factor method (load factor method in CP114 and previous HK codes)
3. Limit states design philosophy (BS8110, CP110 and present HK concrete code)
Elastic design of an RC section
Elastic method• At working load, the maximum stress in the
concrete is a certain fraction of the cube strength and the maximum stress in the steel is a certain fraction of the yield stress At working load
≤ fcu / (FOS)conc
≤ fy / (FOS)steel
Elastic methodAssumptions:• Plane sections remain plane after bending• The materials are linearly elastic • The tensile strength of concrete is ignored• For analysis, the “composite section”
(comprising concrete and steel) is considered as an equivalent section of concrete
Symbols:b = breadthh = total depthd = effective depthx = neutral axis depthAs = area of tension reinft.
pcb = permissible compressive stress in concrete due to bending
pst = permissible tensile stress in steelαe = Es / Ec = modular ratio
d
b
h
As
b
x
αe As
N.A.
Figure 3. Assumptions in elastic design.
Concrete in tension ignored
Equivalent area of steel reinft.
• The position of N.A. varies:
N.A.
Plain concrete section before cracking
Reinforced concrete section after cracking
N.A. N.A.
y
x y
x
Let the section be subjected to uniform stress σ = 1Total force
Taking moment about y-axis
Therefore
Similarly
∫∫=
dA
dAxx
AdAdAF === ∫∫σ
dAxdAxxF ∫∫ =⋅=⋅ σ
∫∫=
dA
dAyy
Determination of centroidRevision
d
b
h
As
b
x
αe As
N.A.
Figure 3. Assumptions in elastic design.
Taking moment about N.A. (uniform stress creates a resultant through N.A.)
021 2 =−+ dAxAbx sese αα
( ) ( )( )b
dAbAAx sesese ααα 2)4(2 ++−
=
bdA
bA
bA sesese ααα 22
+
+−=
( )xdAbx se −= α2
21
( )23
31 xdAbxI se −+= α
d
b
h
As
b
x
αe As
N.A.
Figure 3. Assumptions in elastic design.
At top fibre,At steel level,
xIZc =
cbc
cb pI
MxZMf ≤==
( ) es xd
IZα−
=
( )st
e
sst p
IxdM
ZMf ≤
−==
αI
My=σ
To convert stress from equivalent section
Design resistance moment is the smaller of
• Under-reinforced:
• Over-reinforced:
• Balanced:
xpIZpM cb
ccbc ==
( )xdpIZpM
e
stssts −
==α
pst pcb
Under-reinforced
Over-reinforced
Balanced
stst pf =
stst pf <
stst pf =
cbcb pf <
cbcb pf =
cbcb pf =
Simplified interpretation
ExampleElastic design of RC slab
ExampleA 225mm thick reinforced concrete slab spans an effective distance of 7.5m between two brick walls. The slab is designed to support an imposed load comprising a uniformly distributed load and a transverse line load at mid-span. The main reinforcement is T20/150 and the secondary reinforcement is T12/300. The cover provided to the main reinforcement is 15mm. The screeding and ceiling finish together weigh 0.5kN/m2 and the density of reinforced concrete is assumed to be 24kN/m3.
Unit width
Example(a) Using the elastic method, calculate the maximum safe
bending moment per unit width that can be carried by the slab ifpermissible tensile stress in steel = 250N/mm2;permissible bending stress in concrete = 13.3N/mm2; andmodular ratio = 15.
(b) If the uniformly distributed imposed load is 5kN/m2, determine the maximum safe transverse line load that can be carried at mid-span.
(c) Calculate the maximum stresses in concrete and steel if the slab is subjected to a uniformly distributed imposed load of 5kN/m2 and a transverse line load of 6kN/m at mid-span. Draw a sketch showing how the stresses are distributed along the depth of the mid-span section.
Solution(a) Maximum safe bending moment per unit widthConsider 1m width of slab. The dimensions arespan = 7.5m, b = 1000mm, h = 225mm, and cover = 15mm
The reinforcement isMain reinft.: T20/150Secondary reinft.: T12/300
Effective depth d = 225 – 15 – 20/2 = 200mm
d
Sectional area of reinft.
Allowable stresses
Modular ratio
( ) /mmm2094150100020
422 =
=
πsA
2N/mm250=stp 2N/mm3.13=cbp
15=eα
Solution
Average no. of bars in a 1m strip
Let the neutral axis depth be x.Taking moment about the neutral axis,
The second moment of area is
( )( ) ( )( )( )xx −= 2002094151000 221
0628200031410500 2 =−+ xx
mm0.85=x
( )( )( ) ( )( )( )2331 0.852002094150.851000 −+=I
46 mm101.620 ×=
Solution
The section moduli are
The maximum safe moment is the smaller of
Hence the maximum safe moment is 89.88kNm and the section is under-reinforced.
366
mm10295.70.85101.620
×=×
==xIZc
( ) ( )( )36
6
mm103595.0150.85200
101.620×=
−×
=−
=e
s xdIZ
α
( )( ) kNm02.97Nmm1002.973.1310295.7 66 =×=×=cM
( )( ) kNm88.89Nmm1088.89250103595.0 66 =×=×=sM
Solution(b) Maximum safe transverse line load at mid-spanSelf-weight Screeding and ceiling finishTotal DL of 1m stripUniformly distributed LLLet knife edged live load be
( )( )( ) kN/m4.5225.00.124 =kN/m5.0=kN/m9.55.04.5 =+=
Solution
2kN/m5UDLL =
kN/mKELL P=
7.5 m
P kN/m LL 5.9 kN/m2 DL 5 kN/m2 LL
Moment caused by DL and LL
Thereforegiving maximum
Solution
( )( )( ) ( ) ( )5.75.759.5 412
81 P++=
( )kNm/m875.164.76 P+=
88.89875.164.76 =+ PkN/m06.7=P
7.5 m
P kN/m LL 5.9 kN/m2 DL 5 kN/m2 LL
(c) If and Bending moment
The stresses are( )( ) kNm/m89.876875.164.76 =+=M
2kN/m5UDLL = kN/m6KELL == P
( )kNm/m875.164.76 PM +=
26
6
N/mm05.1210295.71089.87
=××
==c
cb ZMf
26
6
N/mm5.244103595.01089.87
=××
==s
st ZMf
Solution
85
200
12.05N/mm2
244.5N/mm2
Figure 4. Stress distribution (not to scale).
Elastic method• The ratio of the yield stress (or cube strength) to the
permissible stress in steel (or concrete respectively) is called the stress factor of safety.
• When a structure is designed on an elastic basis with a stress factor of 2, it does not mean that the structure will carry twice the working load before it fails. Supposing
How about this? Will it fail? Usually not! Why not?
P
2P
fy / 2
fcu / 2
Elastic methodDrawbacks of elastic method
P 2P
Not twice corresponding stresses at P
2P
< fcu
< fy
P
fy / 2
fcu / 2Note: Not to scale
Ultimate load design method• When the ultimate load design method is
adopted, the structure is designed so that the working load is some fraction of the ultimate load.
• The load that the structure can carry is calculated.
• The ratio of the ultimate load to the working load is called the load factor of safety, and hence ultimate load design method is often called load factor design method.
Ultimate load design method• The structure is designed so that the working
load is some fraction of the ultimate load. The load that the structure can carry is calculated.
Load factor of safety = Pult / P
P
Pult Failure!
Limit State Design of RC Structures
Ultimate limit state (ULS)• collapseServiceability limit states (SLS)• Excessive deflection• Cracking• Vibration• Etc.
Limit state design of RC structures
• γf = 1.0 is usually applied to all load combinations at the serviceability limit state (SLS)
• For ultimate limit state (ULS), γf are as shown (HK and UK codes)
Partial safety factors for load γf
Limit state design of RC structuresChoice of partial safety factors for load γf
1.0 Gk × ½ B > 1.4 Wk × ½ H
Limit state design of RC structures
1.0 Gk
1.4 Wk
To be checked at ULS
GkWk
Nominal Loads
H/2
B/2 B/2
H/2
• γm for ULS are as shown (HK and UK codes)Partial safety factors for strength of material γm
Limit state design of RC structures
• Because of the non-linear stress-strain relationship of concrete, the stress distribution in an RC section varies with the applied bending moment.
Stress development in RC section
d h
b At working load (stress condition for elastic design)
Beyond working load
At failure (stress condition for ultimate load design)
Stress development in a reinforced concrete section.
Limit state design of RC structures
Stress development in RC section
Limit state design of RC structures
σ
ε
ε σ
fcu
Small curvature and strains
45°
Stress development in RC section
Limit state design of RC structures
σ
ε
ε σ
fcu
Large curvature and strains
45°
Assumptions:1. The strain distribution across the section is linear.2. The tensile strength of concrete is ignored.3. The compressive strain of concrete is the criterion for
failure of the RC beam section. The ULS is reached when the concrete strain at the extreme compression fibre εcc reaches a specified ultimate value of εcu where
for
for
0035.0=cuε MPa60≤cuf6000006.00035.0 −×−= cucu fε
MPa60>cuf
Limit state design of RC structures
0
0.001
0.002
0.003
0.004
0 20 40 60 80 100Concrete grade
Ulti
mat
e co
ncre
te s
train
4. The maximum concrete compressive stress at failure is taken to be (0.67fcu)/γm, which is equal to 0.45fcunoting that γm = 1.5 for concrete in flexure.
Limit state design of RC structures
The factor of 0.67 is to allow for difference between bending strength and cube strength.
Ideal case Reality
Strength over-estimated
cmc u Ef γ34.1
Parabol ic curve
Strain εcu
Stre
ss
mcuf γ67.0
Figure 6. Short-term design stress-strain curve for normal-weight concrete (Fig. 3.8 of Code of Practice for Structural Use of Concrete 2004 Second Edition)
+= 3.2146.3
m
cuc
fE
γ kN/mm2
for 20MPa ≤≤ cuf 100MPa
0035.0=cuε
for 60≤cuf MPa
6000006.00035.0 −−= c ucu fε
for 60>c uf MPa
Εc
To be enlarged …
Limit state design of RC structures
cmc u Ef γ34.1
Parabolic curve
Strain εcu
Stre
ss
mcuf γ67.0
Figure 6. Short-term design stress-strain curve for normal-weight concrete (Fig. 3.8 of Code of Practice for Structural Use of Concrete 2004 Second Edition)
+= 3.2146.3
m
cuc
fE
γ kN/mm2
for 2 0MPa ≤≤ cuf 100MPa
0035.0=cuε
for 60≤cuf MPa
6000006.00035.0 −−= c ucu fε
for 60>c uf MPa
Εc
5. At failure of the RC beam section, the distribution of concrete compressive stress may be defined by the idealized stress-strain curve or the simplified rectangular stress block.
Limit state design of RC structures
s = 0.9x for ≤cuf 45 MPa s = 0.8x for 45 < ≤cuf 70 MPa s = 0.72x for 70 < ≤cuf 100 MPa
Strain Stress Neutral Axis
Figure 7. Simplified stress block for concrete at ULS
εcu0.67 fcu / γm
x
s 0035.0=cuε for 60≤cuf MPa
6000006.00035.0 −−= cucu fε for 60>cuf MPa
Simplified Idealized
To be enlarged …
Limit state design of RC structures
s = 0.9x for ≤cuf 45 MPa s = 0.8x for 45 < ≤cuf 70 MPas = 0.72x for 70 < ≤cuf 100 MPa
Strain Stress Neutral Axis
Figure 7. Simplified stress block for concrete at ULS
εcu 0.67 fcu / γm
x
s 0035.0=cuε for 60≤cuf MPa
6000006.00035.0 −−= cucu fε for 60>cuf MPa
Simplified Idealized
6. The maximum steel stress is taken to be fy/γm, which is equal to 0.87fy noting that γm = 1.15 for reinforcement. Assuming a Young’s modulus of Es = 200000 N/mm2, the yield strain of the design stress-strain curve is therefore
Limit state design of RC structures
20000087.0 yf fy / γm
fy / γm
Tension
Compression
Strain
Stre
ss
200 kN/mm2
Figure 8. Short-term design stress-strain curve for reinforcement (Fig. 3.9 of Hong Kong Concrete Code)
• BS8110: 1985 & HK Code: γm = 1.15; fy/γm = 0.87fy
• BS8110: 1997γm = 1.05; fy/γm = 0.95fy
7. Where a section is designed to resist flexure only, the lever arm should not be greater than 0.95d, where d = effective depth.
Limit state design of RC structures
Section with strain diagrams and stress blocks
Strains
ccε
scε
stε
d
d ' A'
s
As
Section
b
(b) Rectangular
parabolic
Stress Blocks
(a) Triangular
Neutral axis
x s
(c) Equivalent rectangular
Classification of RC sections
Classification of RC sectionsAn RC section may be• Under-reinforced• Critical / balanced• Over-reinforced
Ben
ding
mom
ent M
Curvature φ
Over-reinforced
Under-reinforced
Under-reinforced section• The tension reinforcement is smaller than a certain
amount known as the balanced steel content.• Upon loading, tension reinforcement will reach the
yield strength first.• It is assumed that at failure, the steel stress is the design
yield stress.• This tension failure is ductile.• Sequence:
(a) steel yielding and concrete cracking; and(b) then concrete crushing
εcc < εcu
εst > yield strain
Fst
Fcc
Under-reinforced section
Balanced section• A balanced or critical section has exactly the balanced
steel content.• At the failure of a balanced section, the concrete reaches
the maximum strain εcu at the same time when the steel reaches the yield strain.
εcc = εcu
εst = yield strain
Fst
Fcc
Balanced section.
εcc = εcu
εst < yield strain
Fst
Fcc
Over-reinforced section.
Over-reinforced section• The tension reinforcement is more than a certain
amount known as the balanced steel content.• Upon loading, concrete reaches its compression
capacity first.• Concrete reaches the maximum strain εcu while the steel
strain is still below the yield strain.
Over-reinforced section• Over-reinforced sections will fail suddenly in a brittle
manner, i.e. compression failure.• To prevent a brittle failure without warning, most
design codes impose certain restrictions.• For example, in the Hong Kong Concrete Code
for ;for ; orfor and no moment
redistribution
dx 5.0≤dx 4.0≤dx 33.0≤
2N/mm45≤cuf2N/mm7045 ≤< cuf
2N/mm10070 ≤< cuf
Ultimate moment of resistance of a singly reinforced rectangular section
Design of RC sections• Consider ULS first, followed by SLS.• Simplified rectangular stress block is used.• For simplicity in demonstration, it is assumed that the
concrete grade does not exceed 45, and therefore
Singly reinforced section with rectangular stress distribution (fcu ≤ 45)
Fcc
0.67fcu /γm ≅ 0.45 fcu
Stress distribution
Fst
s/2
z
s = 0
.9x
d
b
Section
As
x
εst
Strain distribution
Neutral axis
εcu
0035.0=cuε dx 5.0≤
To be enlarged …
Under-reinforced section
An under-reinforced section at failure (fcu ≤ 45).
Fcc
0.67fcu /γm ≅ 0.45 fcu
Stress distribution
Fst
s/2
z
s = 0
.9x
Strain distribution
xεcc = εcu
εst > 0.87 fy / Es
d
Under-reinforced section• The resultant compressive force in concrete Fcc is
given by
( ) ( ) xbfbxfxbfF cucu
m
cucc 402.09.0
5.167.09.067.0
===γ
An under-reinforced section at failure (fcu ≤ 45).
Fcc
0.67fcu /γm ≅ 0.45 fcu
Stress distribution
Fst
s/2
z
s = 0
.9x
Strain distribution
xεcc = εcu
εst > 0.87 fy / Es
d
Under-reinforced section• Assuming that the steel reinforcement has yielded,
the resultant tensile force Fst
• Equating the compression Fcc to tension Fst
sysy
sm
ysstst AfA
fA
fAfF 87.0
15.1=
=
==
γ
sycu Afbxf 87.0402.0 =
bfAf
xcu
sy164.2= (1)
• It should have yielded. Check ifor
• The maximum value of the neutral axis depth ratio x/d is dependent on fy, subject to additional requirement of the Hong Kong Concrete Code limiting the ratio x/d to a maximum of 0.33 to 0.5 depending upon the concrete cube strength fcu.
Under-reinforced section
x
εcc = εcu
εst > 0.87 fy / Es
d
Strain distribution of an under-reinforced section at failure
syst Ef87.0>εsycu
cu
Efdx
87.0+<
εε
• The lever arm z can be worked out as
• Applying Eq. (2) and assuming a concrete cube strength fcu not exceeding 40N/mm2 (x/d ≤ 0.5)
• When a section is designed to resist only flexure, the lever arm z should not be assumed to be greater than 0.95 times the effective depth d, thus
Under-reinforced section
xdxdz 45.02)9.0( −=−= (2)
dddxdz 775.02/45.045.0 =−≥−=
dz 775.0≥
Fcc
0.67fcu /γm ≅ 0.45 fcu
Stress distribution (fcu ≤ 45)
Fst
s/2
z
s = 0
.9x
95.0775.0 ≤≤ dz
• The ultimate moment M of the section can be worked out in terms of the concrete stress as
• The ultimate moment M of the section can also be worked out in terms of the steel stress as
Under-reinforced section
zFM cc= zxbfcu402.0=
zzdbfcu
−
=45.0
402.0
( )zzdbfM cu −= 9.0 (3)
zFM st= zAf sy87.0=
Fcc
0.67fcu /γm ≅ 0.45 fcu
Stress distribution (fcu ≤ 45)
Fst
s/2
z
s = 0
.9x
Fcc
0.67fcu /γm ≅ 0.45 fcu
Stress distribution (fcu ≤ 45)
Fst
s/2
z
s = 0
.9x
• On substituting the lever arm z from Eq. (2) and the neutral axis depth x from Eq. (1), the above equation appears as
( )xdAfM sy 45.087.0 −=
×−=
bfAf
dAfcu
sysy 164.245.087.0
−=
bfAf
dAfMcu
sysy 974.087.0 (4)
bfAf
xcu
sy164.2= (1)
xdxdz 45.02)9.0( −=−= (2)
• Dividing Eq. (4) throughout by bd2 gives
where the tension reinforcement ratio is ρ = As/bd
Under-reinforced section
−
=
dbA
ff
dbAf
dbM s
cu
ysy 974.0187.02
−=
cu
yy f
ff
dbM ρρ 974.0187.02 (5)
−=
bfAf
dAfMcu
sysy 974.087.0 (4)
• The limiting moment of resistance for a singly reinforced concrete section can be worked out by setting x/d = 0.5 or z/d = 0.775 and invoking Eq. (3)
Under-reinforced section
( )zzdbfM cu −= 9.0 (3)
2156.0 bdfM cu= (6)
• Considering both steel yielding and concrete crushing, the ultimate moment M based on steel yielding is
while the moment M based on concrete crushing is
• The actual ultimate moment is the smaller of the above two values. If the applied moment exceeds 0.156fcubd2, compression reinforcement is required.
−=
bfAf
dAfMcu
sysy 974.087.0
2156.0 bdfM cu=
Balanced section
A balanced section at failure (fcu ≤ 45).
Fcc
0.67fcu /γm ≅ 0.45 fcu
Stress distribution
Fst
s/2
z
s = 0
.9x
Strain distribution
x
εcc = εcu = 0.0035
εst = 0.87 fy / Es
d
• At the failure of a balanced section, the concrete reaches the maximum strain at the same time when the steel reaches the design yield strain of 0.87fy/Es, and thus
Balanced section
sy Efxdx
87.00035.0
=− 0035.087.0
0035.0+
=sy Efd
x
A balanced section at failure (fcu ≤ 45).
Fcc
0.67fcu /γm ≅ 0.45 fcu
Stress distribution
Fst
s/2
z
s = 0
.9x
Strain distribution
x
εcc = εcu = 0.0035
εst = 0.87 fy / Es
d • Equating the compression Fcc to tension Fst
• The tension reinforcement ratio for a balanced section
• The ultimate moment M of the section can be calculated from Eq. (5) by setting ρ to be ρb
Balanced section
sycu Afbxf 87.0402.0 =
+
=
===
0035.087.00035.0462.0
462.087.0
402.0
syy
cu
y
cu
y
cusb
Efff
dx
ff
dfxf
dbAρ
(7a)
Fcc
0.67fcu /γm ≅ 0.45 fcu
Stress distribution (fcu ≤ 45)
Fst
s/2
z
s = 0
.9x
−=
cu
yy f
ff
dbM ρρ 974.0187.02 (5)
• Alternatively, a simpler (but approximate) definition of a balanced section is one having a neutral axis depth ratio x/d of 0.5 while the steel reaches the design yield strain of 0.87fy/Es, and thus
Balanced section
x εcc
εst = design yield strain in steel = 0.87 fy / Es
d
Strain distribution of a balanced section at failure (fcu ≤ 45)
x/d = 0.5
=
===
y
cu
y
cu
y
cusb f
fdx
ff
dfxf
dbA 231.0462.0
87.0402.0ρ
(7b)
Over-reinforced section
An over-reinforced section at failure (fcu ≤ 45).
Fcc
0.67fcu /γm ≅ 0.45 fcu
Stress distribution
Fst
s/2
z
s = 0
.9x
Strain distribution
xεcc = εcu
εst < 0.87 fy / Es
d
• An over-reinforced section fails by crushing of concrete while the tension reinforcement remains elastic, i.e. fs < 0.87fy
• The steel stress can be determined as follows:
Over-reinforced section
x εcc = 0.0035
εst < 0.87 fy / Es
d
Strain distribution of an over-reinforced section at failure
sxdx
ε0035.0
=−
−
=x
xds 0035.0ε
−
==x
xdEEf sssst 0035.0ε
• Equating the compression Fcc to tension Fst,
• After solving for the neutral axis depth x from Eq. (8), the lever arm z can be worked out from Eq. (2). The ultimate moment M of the section can then be calculated from Eq. (3).
Over-reinforced section
−
=x
xdAEbxf sscu 0035.0402.0
0)(0035.0402.0 2 =−+ dxAEbxf sscu (8)
Fcc
0.67fcu /γm ≅ 0.45 fcu
Stress distribution (fcu ≤ 45)
Fst
s/2
z
s = 0
.9x xdxdz 45.02)9.0( −=−= (2)
( )zzdbfM cu −= 9.0 (3)
Ultimate moment of resistance of a doubly reinforced rectangular section
Doubly reinforced rectangular section• Compression reinforcement is required when
K = M / fcubd2 > 0.156• Other alternatives: increase in size, increase in concrete
grade, or their combinations• Assume first that all reinforcement has yielded. Later
modify in case some or all of the reinforcement does not reach the design yield stress.
• For simplicity, the area of concrete in compression has not been deducted to allow for the concrete displaced by the compression reinforcement.
• It is also assumed for demonstration purpose that the concrete grade does not exceed 45.
Doubly reinforced rectangular section
Doubly reinforced section with rectangular stress distribution (fcu ≤ 45)
d
b
Section
As
A's d'
Des
irabl
e x
= d/
2
εst
Strain distribution
Neutral axis
εcu = 0.0035
εsc Fcc
0.67fcu /γm=0.45 fcu
Stress distribution
Fst
s = 0
.9x
z
Fsc
• Assume first that all reinforcement has yielded
Doubly reinforced section with rectangular stress distribution (fcu ≤ 45)
d
b
Section
As
A'sd'
Des
irabl
e x
= d/
2
εst
Strain distribution
Neutral axis
εcu = 0.0035
εsc Fcc
0.67fcu /γm=0.45 fcu
Stress distribution
Fst
s = 0
.9x
z
Fsc
( ) ( ) xbfbxfxbfF cucu
m
cucc 402.09.0
5.167.09.067.0
===γ
sysy
sm
ysscsc AfA
fA
fAfF ′=′
=′
=′= 87.0
15.1γ
sysy
sm
ysstst AfA
fA
fAfF 87.0
15.1=
=
==
γ
• For equilibrium of the section
so that with the reinforcement at yieldscccst FFF +=
sycusy AfxbfAf ′+= 87.0402.087.0
( )bfAAf
xcu
ssy
402.087.0 ′−
= (9)
Fcc
0.67fcu /γm=0.45 fcu
Stress distribution (fcu ≤ 45)
Fst
s = 0
.9x
z
Fsc • The stresses fst and fsc of the tension and compression reinforcement respectively should be the design yield stress provided that the respective strains εst and εscsatisfy the following conditions:
Doubly reinforced section with rectangular stress distribution (fcu ≤ 45)
d
b
Section
As
A'sd'
x
εst
Strain distribution
Neutral axis
εcu = 0.0035
εsc Fcc
0.67fcu /γm=0.45 fcu
Stress distribution
Fst
s = 0
.9x
z
Fsc
yst ff 87.0=
ysc ff 87.0=
s
yst E
fx
xd 87.00035.0 ≥
−
=ε
s
ysc E
fx
dx 87.00035.0 ≥
′−
=ε
if
if
(10)
(11)
• If the previous conditions are satisfied, the assumption that all the reinforcement has reached the design yield stress is correct. Thus the ultimate moment M is
Doubly reinforced section with rectangular stress distribution (fcu ≤ 45)
d
b
Section
As
A's d'
x
εst
Strain distribution
Neutral axis
εcu = 0.0035
εsc Fcc
0.67fcu /γm=0.45 fcu
Stress distribution
Fst
s = 0
.9x
z
Fsc
)()45.0( ddFxdFM sccc ′−+−=
)(87.0)45.0(402.0 ddAfxdbxfM sycu ′−′+−= (12)
• When the previous checks reveal that not all the reinft. has yielded, the value of NA depth x calculated from Eq. (9) is incorrect and has to be recalculated
Doubly reinforced section with rectangular stress distribution (fcu ≤ 45)
d
b
Section
As
A'sd'
x
εst
Strain distribution
Neutral axis
εcu = 0.0035
εsc Fcc
0.67fcu /γm=0.45 fcu
Stress distribution
Fst
s = 0
.9x
z
Fsc
bfAfAfx
cu
sscsst
402.0′−
=
−
==x
xdEEf sstsst 0035.0ε
′−
==x
dxEEf sscssc 0035.0ε
(13) (14)
(15)Apply as appropriate
• The ultimate moment M of the section is
Doubly reinforced section with rectangular stress distribution (fcu ≤ 45)
d
b
Section
As
A's d'
x
εst
Strain distribution
Neutral axis
εcu = 0.0035
εsc Fcc
0.67fcu /γm=0.45 fcu
Stress distribution
Fst
s = 0
.9x
z
Fsc
)()45.0( ddFxdFM sccc ′−+−=
)()45.0(402.0 ddAfxdbxfM sscu ′−′′+−= (16)
Summary of procedures for flexural design of RC beams (fcu ≤ 45MPa)
Flexural design of RC beams1. Classification of section
Let the required ultimate moment be M.Work out K where K = M / fcubd2
• If K ≤ 0.156, no compression reinforcement is needed and the section may be designed as a singly-reinforced section.
• If K > 0.156, compression reinforcement is needed and the section must be designed as a doubly-reinforced section. Alternatively the section size may be increased, or the concrete grade may be increased.
Flexural design of RC beams2. Singly-reinforced section
zFM cc=
zxbfcu402.0=
zzdbfcu
−
=45.0
402.0
( )zzdbfcu −= 9.0
( )( )dzdzdbfM cu //19.02 −=
Fcc
0.67fcu /γm ≅ 0.45 fcu
Stress distribution (fcu ≤ 45)
Fst
s/2
z
s = 0
.9x
Flexural design of RC beams
Substituting K = M / fcubd2
Having solved for z, the steel area As is determined from
Fcc
0.67fcu /γm ≅ 0.45 fcu
Stress distribution (fcu ≤ 45)
Fst
s/2
z
s = 0
.9x
( )( )dzdzdbfM cu //19.02 −=
09.0/)/()/( 2 =+− Kdzdz
( )9.0/25.05.0/ Kdz −+=
( )[ ]9.0/25.05.0 Kdz −+=
zAfzFM syst 87.0==zf
MAy
s 87.0=
Flexural design of RC beams3. Doubly-reinforced section
Assume that x = d / 2
Assume that the compression steel has yielded
Therefore
)()45.0( ddFxdFM sccc ′−+−=
)()45.0(402.0 ddAfxdbxf ssccu ′−′+−=
2156.0)45.0(402.0 bdfxdbxf cucu =−
ysc ff 87.0=
Fcc
0.67fcu /γm=0.45 fcu
Stress distribution (fcu ≤ 45)
Fst
s = 0
.9x
z
Fsc
)(87.0156.0 2 ddAfbdfM sycu ′−′+=
)(87.0156.0 2
ddfbdfMA
y
cus ′−
−=′
Flexural design of RC beamsCheck whether the compression steel has yielded or not. If
then the compression steel has yielded, i.e.To compute the required tension steel, note the equilibrium condition
Fcc
0.67fcu /γm=0.45 fcu
Stress distribution (fcu ≤ 45)
Fst
s = 0
.9x
z
Fsc
s
ysc E
fd
ddx
dx 87.02/
2/0035.00035.0 ≥
′−
=
′−
=ε
ysc ff 87.0=
scccst FFF +=
sycusy AfxbfAf ′+= 87.0402.087.0
y
sycus f
AfdbfA
87.087.0201.0 ′+
=
Shear Strength
Shear Strength• The shear force is numerically equal to the rate of
change of bending moment, i.e. dM/dx = V.• Shear transfer in RC beams relies heavily on the
tensile and compressive strength of concrete.• A shear failure is in general non-ductile.• To suppress this type of failure, the shear strength of a
member must be somewhat in excess of that associated with the maximum flexural strength it can possibly develop.
Types of shear failure• Generally, there are five types
of failure related to shear and flexure for RC beams.
• The behaviour of shear failure depends on the shear-span / depth ratio (av/d) where av is the distance between the point load and the nearest support.
P P
av avL
Bending moment
P.av
Shear force
P
-P
Diagonal compression
Diagonal tension
v
vv
v
v
vv
v
An element at neutral axis
Types of shear failure in reinforced concrete beams
(b) Type II 6 > av/d > 2
V
d
Dowel force crack leading to bond failure
Compression zone fails
av
(a) Type I av/d > 6 V
d
Shear crack
Bending crack
Beam fails when compression zone crushes
av
(c) Type III av/d < 2
V
d
Shear crack suddenly appears followed by failure in compression zone
av
(d) Type IV av/d = 0 Punching shear
V
(e) Type V With shear reinforcement
V Vertical links
Bent-up bars
Shear cracks
Types of shear failure
Type I: av/d > 6• The bending moment is large compared to the shear
force.• The failure is similar to that expected in pure bending.• Normally the tension reinft. is close to yield or has
already yielded.• Only minimum shear reinforcement is required.
(a) Type I av/d > 6 V
d
Shear crack
Bending crack
Beam fails when compression zone crushes
av
• At failure, horizontal cracks will appear running along the tension reinforcement. These horizontal cracks reduce the shear resistance of the section by destroying the dowel force and also reduce the bond stress between the steel and concrete.
• Normally the tension reinforcement does not reach yield.
(b) Type II 6 > av/d > 2
V
d
Dowel force crack leading to bond failure
Compression zone fails
av
Type II: 2 < av/d < 6• The initial flexural cracks
become inclined early in the loading process.
Type III: av/d < 2• Typical form of shear failure• Flexural cracks do not develop but shear cracks at
roughly 45° suddenly appear leading to collapse.• Normally the tension reinforcement does not reach
yield.
(c) Type III av/d < 2
V
d
Shear crack suddenly appears followed by failure in compression zone
av
Type IV: av/d ≅ 0• A punching shear failure• The shear resistance of the section is at a maximum.• The addition of shear reinforcement in the form of
vertical links does not increase the shear resistance above the punching shear value.
(d) Type IV av/d = 0 Punching shear
V
Type V: Shear reinforcement provided• The shear reinforcement increases the shear resistance
against failure types I, II and III.• Diagonal cracks normally develop.• At failure, the shear reinforcement and the longitudinal
reinforcement yield, provided that the reinforcement is anchored well and the member is not over-reinforced.
(e) Type V With shear reinforcement
V Vertical links
Bent-up bars
Shear cracks
Components of shear resistance
• Concrete compression zoneshear carried by the uncracked concrete compression zone Vcz (20-40%)
• Aggregate interlockvertical component of aggregate interlock across the diagonal crack Va (35-50%)
( ) scsdacz VVVVVVV +=+++=
Shear transfer in beam with web reinforcement.
Vcz
Vd
Vs
Concrete compression
Steel tension
Va Aggregate interlock
(19)
Components of shear resistance
• Dowel actionshear force carried by the dowel action of longitudinal tension reinft. Vd (35-50%)
• Shear reinforcementshear force carried by shear reinft. or web reinft. (stirrups / links, or bent-up bars) Vs (max 50%)
( ) scsdacz VVVVVVV +=+++=
Shear transfer in beam with web reinforcement.
Vcz
Vd
Vs
Concrete compression
Steel tension
Va
Dowel bar
Shear reinforcement
Links or stirrups.
CL
Combined system with links and bent-up bars.
CL
Bent-up bar
• The provision of shear reinforcement increases the ductility of the beam and considerably reduces the likelihood of a sudden and catastrophic failure.
Shear reinforcementContribution of links to shear strength:• Improving the contribution of the dowel action
A link can effectively support a longitudinal bar that is being crossed by a flexural shear crack close to a link
• Suppressing flexural tensile stresses in the concrete by means of the diagonal compressive force resulting from truss action
A flexural shear crack
CL
Truss analogy
CL
Shear reinforcementContribution of links to shear strength:• Limiting the opening of diagonal cracks within the
elastic range, thus enhancing and preserving the shear transfer by aggregate interlock
• Providing confinement, when the links are sufficiently closely spaced, and thus increasing the strength of the concrete core
C L
Shear reinforcementContribution of links to shear strength:• Preventing the breakdown of bond when splitting
cracks develop in anchorage zones because of dowel and anchorage forces
Splitting
Derivation of shear stress in links
Truss analogy
CLA
A
β
sv
bv d'
d
total cross sectional area of links at the N.A. breadth of sectioncharacteristic strength of links (not to be taken as more than 460 N/mm2)spacing of links along the memberdesign (average) shear stress at a cross section design concrete shear stress
svA
vb
yvf
vsv
cv
Derivation of shear stress in links
Truss analogy
CLA
A
β
sv
bv d'
d
• The shear resistance Vs is contributed by the tension in the links that are crossed by the section line
⋅= svyvs AfV 87.0
( )
′−=
vsvyv s
ddAf βcot87.0 βcot87.0
′−=
vsvyv s
ddAf
( ) βcot87.0 vsvyvs sdAfV ≅
( no. of links crossed by section line)
⇒ 2AA
A
Derivation of shear stress in links CL
A
A
β
sv
( ) βcot87.0 vsvyvs sdAfV ≅
( )vsvyvs sdAfV 87.0=
cs VVV −=dvbV v=dbvV vcc =
( ) vsvyvvc sAfbvv 87.0=−
( )yv
cv
v
sv
fvvb
sA
87.0−
=
• Experiments have led to the recommendation that β could be taken as 45°, giving
• From (19), and introducing
(20)
sc VVV += (19)AppliedResisted by concrete
(21)
The design concrete shear stress vc can be obtained from Table 6.3 of Hong Kong Concrete Code
where
=
mv
sc ddb
Akkvγ140010079.0
4/13/1
21
an enhancement factor equal to 2d/av for shear-span / depth ratio (av/d) less than 2; otherwise k1 = 1
for concrete with cube strength fcu > 25MPa, but fcu should not be taken as greater than 80 N/mm2
=1k
( ) 3/12 25cufk =
Shear design
(22)
The design concrete shear stress vc can be obtained from Table 6.3 of Hong Kong Concrete Code
where
=
mv
sc ddb
Akkvγ140010079.0
4/13/1
21
tensile steel percentage which should not be taken as greater than 3a ratio that should not be taken as less than 1.partial safety factor for strength of materials taken as 1.25
Shear design
(22)
=dbA
v
s100
=d/400=mγ
• To avoid web crushing or compression zone failure, the average shear stress v should not exceed or 7.0 N/mm2, whichever is the smaller.
• The provision of shear reinft. should be in accordance with the following (Table 6.2 of HK Concrete Code)
• Note that the design shear resistance vr provided by minimum links is taken asvr = 0.4 N/mm2
for fcu ≤ 40 N/mm2
vr = 0.4 (fcu/40)2/3 N/mm2
for fcu > 40 N/mm2
cuf8.0
0.0
0.2
0.4
0.6
0.8
1.0
0 20 40 60 80 100Concrete grade
Des
ign
shea
r res
ista
nc
Shear design
There are three cases to be considered in shear design.(a) v < 0.5 vc throughout the beam
Provide minimum links in beams of structural importance. Minimum links may be omitted in members of minor structural importance.
(b) 0.5 vc < v < (vc + vr)Provide minimum links equivalent to additional shear strength of vr, i.e.Setting
Shear design
yv
vvrsv f
sbvA87.0
≥
( )vsvyvs sdAfV 87.0= (20)dbvV vrs =
There are three cases to be considered in shear design.(c) (vc + vr) < v < 0.8√fcu or 7.0 N/mm2
Provide links according to (21), namely
Shear design
( )yv
cvvsv f
vvsbA87.0
−≥
Min. links preferred
Min. links
Links depending on shear stress
Prohibited!
0 0.5 vc
vc vc + vr
0.8√fcu or 7.0 N/mm2
Procedure for design for shear1. Calculate the design shear stress at the section from
.2. Check whether the design shear stress v is within the
upper limit, i.e. or 7.0 N/mm2.3. Calculate the percentage of longitudinal tension
reinforcement and determine the design concrete shear stress vc from Table 6.3 of Hong Kong Concrete Code or the associated equation.
4. Determine the form and area of shear reinforcement, if any, from Table 6.2 of Hong Kong Concrete Code.
dbVv v=
cufv 8.0<
Procedure for design for shear5. Choose suitable link size and spacing sv, ensuring that
.6. At least 50% of the shear resistance provided by the
steel should be in the form of links.
dsv 75.0≤
Deflection control DL, LL, etc
M
Fst
Mild steel High yield steel
Low fs & high As
High fs & low As
High εs, high curvature & high deflection
Low εs, low curvature & low deflection
Parameters:• Breadth b• Effective depth d• Steel area As
• A set of basic span / effective depth ratios are used to control deflections. These ratios are normally more critical for slabs.
• The basic ratios are modified to account for the amounts of tension and compression reinforcement and the stresses there.
Basic span / effective depth ratios for rectangular sections with spans less than 10m
Cantilever 7Simply supported 20Continuous 26
Deflection control
• The modification factor for tension reinforcement can be calculated by
• The design service stress in the tension reinforcement in a member may be estimated from
• Similarly, the modification factor for compression reinforcement
Deflection control
( )( ) 0.2
9.012047755.0 2 ≤
+−
+bdM
fs
bprovs
reqsys A
Aff
β1
32
×=
tionredistribubeforesectionatmomenttionredistribuaftersectionatmoment
=bβ
5.1100
3100
1 ≤
′+
′+
bdA
bdA provsprovs
(23)
(24)
• Concrete slabs behave primarily as flexural members, and therefore the design is similar to that for beams.
• The shear stresses are usually low in a slab except when there are heavy concentrated loads.
• Compression reinforcement is seldom required except at supports.
• Common methods of analysis:- Elastic analysis- Yield line theory by Johansen- Strip method by Hillerborg
Design of slabs
Design of slabs
1000
Unit width
No. of bars required = Area of one bar
Max. spacing = No. of bars required
1000
= 1000 × area of one bar
Ast
Ast
Two-way slab
Main reinft. Secondary
reinft.
One-way slab
• The slab is often assumed to be built up of parallel strips (beams) of 1m width (i.e. b=1000mm).
• The area of tension reinforcement is • A suitable bar diameter and spacing can be worked out
by • Min. reinforcement (esp. secondary reinft.):
for high yield steel (fy = 460 MPa) for mild steel (fy = 250 MPa)
• Shear stress• Avoid using shear reinforcement in slabs
One-way slabs
zfMA ys 87.0=
sAbar) one of (area 1000 = spacing maximum ×
10013.0 bh10024.0 bh
cuv fdbVv 8.0≤=
Examples
Example 1: Design of a singly reinforced rectangular section
A rectangular beam of breadth 260 mm and effective depth to tension reinforcement 440 mm is required to resist an ultimate bending moment 185 kNm. Determine the area of tension reinforcement As required given the characteristic material strengths are fy = 460 MPa and fcu= 30 MPa. Hence determine the shear reinforcement using mild steel with characteristic strength fyv = 250 MPaif the ultimate shear force is 150 kN.
260mm
440m
m
156.0123.030440260
101852
6
2 <=××
×==
cufbdMK
( ) mm3689.025.05.0 =−+= Kdz
Example 1Design data:
M = 185 kNm V = 150 kN b = 260 mmd = 440 mm fcu = 30 MPa fy = 460 MPafyv = 250 MPa
Determine if compression reinforcement is requiredK factor
and therefore compression steel is not requiredLever arm zArea of tension reinft. required As
26
mm125636846087.0
1018587.0
=××
×==zf
MAy
s
Example 1Area of tension reinft. required As = 1256mm2
Select suitable arrangement of reinforcementProvide 4T20, giving As prov = 1257mm2 O.K.
MPa31.144026010150 3
=××
==db
Vvv
Example 1Shear design:Determine the average shear stress
Check the average shear stress to avoid web crushing or compression zone failure
O.K.7.00MPaMPa38.48.0MPa31.1 <=<= cufv
10.1440260
1257100100=
××
=dbA
v
s
1909.0440400400
<==d
(Take 1)
( )8020.12530
25≤== cu
cu ff
25.1=mγ
Determine the design concrete shear stress vc
=
m
cu
v
sc
fddb
Avγ1
2540010079.0
3/14/13/1
Example 1
(Use As provided)
( ) ( ) ( )
MPa31.1MPa69.025.1120.1110.179.0
125
40010079.0
3/14/13/1
3/14/13/1
=<=
=
=
v
fddb
Avm
cu
v
sc γ
Example 1
MPa09.14.069.0MPa31.1 =+=+>= rc vvvCheck if minimum links are sufficient
Links more than the minimum amount are necessary
Example 1
( ) 2mm14825087.0
)69.031.1(20026087.0
=×
−××=
−≥
yv
cvvsv f
vvsbA
Determine the amount of links requiredLet sv = 200mm
Provide R10 links at 200 mm spacing
(Asv prov = 157 mm2) O.K.
Check if the spacing is acceptable:
200mm ≤ 0.75×440mm = 330mm O.K.
Example 1Asv req’d = 148 mm2
Provide R10 links at 200 mm spacing
(Asv prov = 157 mm2) O.K.
A rectangular beam has a breadth 250 mm and an effective depth to tension reinforcement 460 mm. The concrete has a characteristic strength of 25 MPa. The steel reinforcement has a modulus of elasticity of 200,000 MPa and a yield strength of 320 MPa. Calculate the section moment capacity of the following tension steel areas: (a) balanced steel area; (b) 2500mm2; and (c) 5160mm2.
Example 2: A singly reinforced rectangular section with diff. amounts of tension reinft.
250mm
460m
m
Example 2
Design data:Breadth b = 250 mmEffective depth d = 460 mmConcrete cube strength fcu = 25 MPaSteel yield strength fy = 320 MPaYoung’s modulus of steel Es = 200,000 MPa
250mm
460m
m
(a) Balanced section1. Determine the neutral axis depth x and lever arm z
The neutral axis depth x can be worked out by considering the strain distribution:
The lever arm z is therefore:
( )sy Efxdx
87.00035.0
=−
mm3290035.087.0
0035.0=
+=
sy
s
EfdEx
mm31245.0 =−= xdz
Strain distribution
x
εcc = εcu = 0.0035
εst = 0.87 fy / Es
d
2. Determine the balanced steel areaFrom equilibrium considerations:
The balanced steel ratio ρbcan be determined as
3. Determine the moment capacity
sycu Afbxf 87.0402.0 =
( )( ) 0258.0462.0 == dxff ycubρ
2mm2969=sA
Fcc
0.67fcu /γm ≅ 0.45 fcu
Stress distribution (fcu ≤ 45)
Fst
s/2
z
s = 0
.9x
kNm9.25787.0 == zAfM sy
(a) Balanced section (b) Section with As = 2500 mm2
1. Determine the type of reinforced concrete sectionThe tension reinforcement ratio ρ is
Therefore this section is under-reinforced and tension failure occurs.
0258.00217.0 =<== bs bdA ρρ
Fcc
0.67fcu /γm ≅ 0.45 fcu
Stress distribution (fcu ≤ 45)
Fst
s/2
z
s = 0
.9x
(b) Section with As = 2500 mm2
2. Determine the neutral axis depth x and lever arm zThe neutral axis depth x can be worked out by considering equilibrium as
The lever arm z is therefore
3. Determine the moment capacityThe moment capacity M is
sycu Afbxf 87.0402.0 =
( )( ) mm277164.2 == bAffx scuy
mm33545.0 =−= xdz
kNm2.23387.0 == zAfM sy
(c) Section with As = 5160 mm2
1. Determine the type of reinforced concrete sectionThe tension reinforcement ratio ρ is
Therefore this section is over-reinforced and compression failure occurs.
0258.00449.0 =>== bs bdA ρρ
Strain distribution
x εcc = εcu
εst < 0.87 fy / Es
d
Fcc
0.67fcu /γm ≅ 0.45 fcu
Stress distribution (fcu ≤ 45)
Fst
s/2
z
s = 0
.9x
(c) Section with As = 5160 mm2
2. Determine the neutral axis depth x and lever arm zThe neutral axis depth x can be worked out by considering equilibrium as
The lever arm z is therefore
sscu AEx
xdbxf
−
= 0035.0402.0
( ) 00035.0402.0 2 =−+ dxAEbxf sscu
01066.136120005.2512 92 =×−+ xx
mm367=x
mm29545.0 =−= xdz
Fcc
0.67fcu /γm ≅ 0.45 fcu
Stress distribution (fcu ≤ 45)
Fst
s/2
z
s = 0
.9x
(c) Section with As = 5160 mm2
3. Determine the moment capacityThe moment capacity M is based on compression in concrete, namely
The steel strain is checked to make sure that it has indeed not yielded
kNm8.273)(9.0 2 =−= zdzbfM cu
sscu Afbxf =402.0
( ) 001392.087.0
000892.0402.0
=<
===
sy
ss
cu
s
ss
EfAE
bxfEfε
O.K.
Variation of moment capacity with amount of tension reinforcement
0
50
100
150
200
250
300
0.00 0.01 0.02 0.03 0.04 0.05Tension reinforcement ratio ρ
Mom
ent c
apac
ity (k
Nm
Example 3: A doubly reinforced rectangular section with different concrete grades
A rectangular beam has a breadth of 280 mm and an effective depth to tension reinft. of 510 mm. The depth to compression reinft. is 50mm. The areas of tension and compression reinft. are 2580 mm2 and 650 mm2
respectively. The steel reinft. has a modulus of elasticity of 200,000 MPa and a yield strength of 330 MPa. Calculate the moment capacity if the concrete has a characteristic strength of
(a) 35MPa (εcu = 0.0035, x ≤ 0.5d and s = 0.9x); and
(b) 70MPa (εcu = 0.0033, x ≤ 0.4d and s = 0.8x).
Example 3: Doubly reinforced sectionDesign data:
b = 280 mmd = 510 mm (depth to tension reinft.)d' = 50 mm (depth to compression reinft.)As = 2580 mm2
A's = 650 mm2
fy = 330 MPaEs = 200000 MPa
280mm
510m
m
50m
m
(a) Concrete strength fcu = 35 MPa1. Initial estimation of internal forces
Assuming that all reinforcement reaches design yield stresses, the forces acting on the section are
2. Consider the equilibrium of forces
N6.3939402.0 xbxfC cuc ==
N18661587.0 =′= sys AfC
N74071887.0 == sy AfT
TCC sc =+
7407181866156.3939 =+xmm141=x
Cc
0.67fcu /γm=0.45 fcu
Stress distribution (fcu ≤ 45)
T s =
0.9
x
z
Cs
3. Check validity of assumptionsCheck steel strains:
Therefore the comp. steel has yielded.
Therefore the tension steel has also yielded. The previous assumptions are valid.
(a) Concrete strength fcu = 35 MPa
( ) 001436.087.0
002259.00035.0
==>
=
′−
=′
syy
s
Efxdx
ε
ε
( ) 001436.087.0
009160.00035.0
==>
=
−
=
syy
s
Efx
xd
ε
ε
x
εst
Strain distribution
Neutral axis
εcu = 0.0035
εsc
Cc
0.67fcu /γm=0.45 fcu
Stress distribution (fcu ≤ 45)
T
s = 0
.9x
z
Cs
4. Moment capacityThe moment capacity M is
( ) ( )0.402 0.45 0.87
333.9 kNmcu y sM f bx d x f A d d′ ′= − + −
=
(a) Concrete strength fcu = 35 MPa
(b) Concrete strength fcu = 70 MPa1. Initial estimation of internal forces
Assuming that all reinforcement reaches design yield stresses, the forces acting on the section are
2. Consider the equilibrium of forces Cc
0.67fcu /γm=0.45 fcu
Stress distribution (45 < fcu ≤ 70)
T
s = 0
.8x
z
Cs
N18661587.0 =′= sys AfC
N74071887.0 == sy AfT
TCC sc =+
7407181866157.7003 =+xmm79=x
N7.70033573.0)8.0)(5.1/67.0( xbxfbxfC cucuc ===
3. Check validity of assumptionsCheck steel strains:
Therefore the comp. steel has NOT yielded.
Therefore the tension steel has yielded. The previous assumptions have to be amended.
(b) Concrete strength fcu = 70 MPa
x
εst
Strain distribution
Neutral axis
εcu = 0.0035
εsc
( ) 001436.087.0
001211.00033.0
==<
=
′−
=′
syy
s
Efxdx
ε
ε
( ) 001436.087.0
018004.00033.0
==>
=
−
=
syy
s
Efx
xd
ε
ε
4. Amendment of assumptionsThe steel compressive force Cs and neutral axis depth x are updated assuming that the compression steel remains elastic.
(b) Concrete strength fcu = 70 MPa
x
xdxEAEAC ssssss
710145.2429000
)0033.0(
×−=
′−′=′′= ε
N7.7003 xCc =
N740718=T
x
εst
Strain distribution
Neutral axis
εcu = 0.0035
εsc Fcc
0.67fcu /γm=0.45 fcu
Stress distribution(45 < fcu ≤ 70)
Fst
s = 0
.8x
z
Fsc
4. Amendment of assumptions
(b) Concrete strength fcu = 70 MPa
TCC sc =+
010145.23117187.7003 72 =×−− xx
mm82=x
xCs710145.2429000 ×−=
N7.7003 xCc =
N740718=T
Cc
0.67fcu /γm=0.45 fcu
Stress distribution(45 < fcu ≤ 70)
T
s = 0
.8x
z
Cs
5. Re-check validity of assumptions Check steel strains:
Therefore the compression steel has NOT yielded.
Therefore the tension steel has yielded. The revised assumptions are valid.
(b) Concrete strength fcu = 70 MPa
( ) 001436.087.0
001288.00033.0
==<
=
′−
=′
syy
s
Efxdx
ε
ε
( ) 001436.087.0
01722.00033.0
==>
=
−
=
syy
s
Efx
xd
ε
ε
x
εst
Strain distribution
Neutral axis
εcu = 0.0035
εsc
6. The moment capacity M is
(b) Concrete strength fcu = 70 MPa
( ) ( )kNm1.351
4.03573.0=
′−′′+−= ddAExdbxfM ssscu ε
Cc
0.67fcu /γm=0.45 fcu
Stress distribution(45 < fcu ≤ 70)
T
s = 0
.8x
z
Cs
Example 4: Design of a reinforced rectangular slab
Design an R.C. slab to span between two 230 mm brick walls 4.5 m apart c/c to carry a live load of 3.0 kN/m2. Assume the floor finishes and ceiling loads to weigh 1.0 kN/m2. The characteristic material strengths are fcu = 30 MPa, fy = 460 MPa (high-yield steel) and fy = 250 MPa(mild steel). Take the basic span-effective depth ratio as 20. Try the following two cases: (a) using high-yield steel; and (b) using mild steel.
4500 mm Main reinforcement
Secondary reinforcement
Cross section of a slab
Example 4: Design of slabDesign data:Span L = 4500 mmWall thickness t = 230 mmBreadth b = 1000 mmBasic span / eff. depth ratio = 20fcu = 30 MPafy = 460 MPa (high yield steel)fy = 250 MPa (mild steel)Cover = 25 mm (for mild exposure) Density of R.C. = 24 kN/m3
Floor finishes & ceiling loads = 1.0 kN/m2
Live load = 3.0 kN/m2
(a) Using high yield steel1. Estimate the effective depth of slab
Assume modification factor (m.f.) = 1.3Minimum effective depth d = span / (20 × m.f.)
= 173 mmTherefore, try effective depth d = 180 mm
2. Estimate the self-weight of slabAssume bar diameter = 10 mmOverall depth of slab h= effective depth + bar diameter / 2 + cover = 210 mmSelf-weight of slab = overall depth × density
= 5.04 kN/m2
d
3. Estimate the design loadsTotal dead load Gk = 1.0 + 5.04 = 6.04 kN/m2
Live load Qk = 3.0 kN/m2
Ultimate load w = 1.4 Gk + 1.6 Qk= 13.26 kN/m2
4. Estimate the design moment per unit width at mid-spanM = wL2 / 8
= 33.55 kNm
(a) Using high yield steelFloor finishes & ceiling loads
Self-weight of slab
5. Check the span / effective ratio
Assume design service stress fs = 460 × 2/3 = 307 MPaModification factor
Limiting span / effective depth ratio= 20 × 1.28= 25.6
Actual span / effective depth ratio = 4500 / 180 = 25.0 < 25.6 O.K.
Hence the span / effective depth ratio is satisfactory.
(a) Using high yield steel
MPa04.12 =bdM
( ) 0.228.19.0120
47755.0 2 <=+−
+=bdM
fs
6. Determination of the lever arm zThe K factor is
Therefore compression steel is not required.The lever arm z is then determined:
> 0.95Take giving
7. The area of tension reinforcement As is
Provide T10 at 150mm centresAs prov = 524 mm2/m O.K.
(a) Using high yield steel
156.0035.02 <== bdfMK cu
960.09.025.05.0 =−+= Kdz95.0=dz mm171=z
m/mm49087.0 2== zfMA ys
Provide T10 at 150mm centresAs prov = 524 mm2/m O.K.
(a) Using high yield steel
Results obtained by truncation
8. Check for shearAt the face of support, the shear force V and shear stress v are worked out as follows.
(a) Using high yield steel
( ) kN3.282 =−= tLwV
MPa38.48.0157.0 =<== cuv fdbVv
291.01801000524100100
=×
×=
dbA
v
s
122.2180400400
≥==d
( )8020.12530
25≤== cu
cu ff
8. Check for shear
Therefore no shear reinforcement is required.
(a) Using high yield steel
25.1=mγ
( ) ( ) ( )
MPa157.0MPa543.025.1120.122.2291.079.0
125
40010079.0
3/14/13/1
3/14/13/1
=>=
=
=
v
fddb
Avm
cu
v
sc γ
9. Distribution steelThe required amount of distribution steel is then determined.Area of transverse high yield steel reinforcement
= 0.13 bh / 100 = 273 mm2/mProvide T10 at 250 mm centres, As prov = 314 mm2/m
O.K.
(a) Using high yield steel
(b) Using mild steel1. Estimate the effective depth of slab
Assume modification factor (m.f.) = 1.7Minimum effective depth d = span / (20 × m.f.)
= 132 mmTry overall depth of slab h = 180 mmAssume bar diameter = 12 mmEffective depth d= overall depth of slab - cover - bar diameter / 2= 180 – 25 – 12 / 2 = 149 mm O.K.
2. Estimate the self-weight of slabSelf-weight of slab = overall depth × density
= 4.32 kN/m2
Different approach
3. Estimate the design loadsTotal dead load Gk = 1.0 + 4.32 = 5.32 kN/m2
Live load Qk = 3.0 kN/m2
Ultimate load w = 1.4 Gk + 1.6 Qk= 12.25 kN/m2
4. Estimate the design moment per unit width at mid-spanM = wL2 / 8
= 31.01 kNm
Floor finishes & ceiling loadsSelf-weight of slab
(b) Using mild steel
5. Check the span / effective ratio
Assume design service stress fs = 250 × 2/3 = 167 MPaModification factor
Limiting span / effective depth ratio= 20 × 1.67= 33.4
Actual span / effective depth ratio = 4500 / 149 = 30.2 < 33.4 O.K.
Hence the span / effective depth ratio is satisfactory.
(b) Using mild steel
MPa40.12 =bdM
( ) 0.267.19.0120
47755.0 2 <=+−
+=bdM
fs
6. Determination of the lever arm zThe K factor is
Therefore compression steel is not required.The lever arm z is then determined:
7. The area of tension reinforcement As is
Provide R12 at 100mm centresAs prov = 1131 mm2/m O.K.
(b) Using mild steel
156.0047.02 <== bdfMK cu
945.09.025.05.0 =−+= Kdzmm141=z
m/mm101187.0 2== zfMA ys
Substantially more reinforcement provided!
Provide R12 at 100mm centresAs prov = 1131 mm2/m O.K.
(b) Using mild steel
Results obtained by truncation
8. Re-check modification factorRe-check modification factor using the updated service stress in the tension reinforcement fs:
where
Revised limiting span / effective depth ratio= 20 × 1.74 = 34.8 > 30.2 O.K.
(b) Using mild steel
( )( )bprovsreqsys AAff β132
= 1=bβ
MPa0.149=sf
( ) 0.274.19.0120
47755.0.. 2 <=+−
+=bdM
ffm s
9. Check for shearAt the face of support, the shear force V and shear stress v are worked out as follows.
(b) Using mild steel
( ) kN2.262 =−= tLwV
MPa38.48.0176.0 =<== cuv fdbVv
759.01491000
1131100100=
××
=dbA
v
s
168.2149400400
≥==d
( )8020.12530
25≤== cu
cu ff
9. Check for shear
Therefore no shear reinforcement is required.
(b) Using mild steel
25.1=mγ
( ) ( ) ( )
MPa176.0MPa784.025.1120.168.2759.079.0
125
40010079.0
3/14/13/1
3/14/13/1
=>=
=
=
v
fddb
Avm
cu
v
sc γ
10.Distribution steelThe required amount of distribution steel is then determined.Area of transverse mild steel reinforcement
= 0.24 bh / 100 = 432 mm2/mProvide R10 at 150 mm centres, As prov = 524 mm2/m
O.K.
(b) Using mild steel
Results obtained by truncation
The End