Beam Footing or Slab design by Limit State Method
Note:- Above design applicable to M35 grade only , for grades above M35, various coefficients changes as shown in following Design Procedure.
For Shear Design Flow Diagram as follows-
Procedure for DESIGN CHECKS
For a given cross-section, the ultimate axial load carrying capacity can be checked for uniform strain of ec2 if the applied force is pure compressive and for 0.9 εs if the applied axial force is pure tensile. The ultimate axial force carrying capacity of the section for given bending moment shall always be between these two limits. The position of neutral axis, x for which the ultimate force carrying capacity of the section matches with·the factored axial force acting on the section is obtained by solving the following equilibrium condition.
f(x) = Pus (x) + Puc (x) + N =
0
;Where N is the factored axial force applied
and Pus (x)
and Puc (x)
are the contributions from steel and concrete
respectively in the ultimate resistance of the section
and can be express as
Pus (x) = Σσs(x) As
Puc= ʃσd Ac
The
Direct Solution of Rectangular
Sections
In case of direct solution,
magnitude of compressive force (Cu) and its location is obtained from concrete
stress block in compression. The ultimate failure
of concrete is caused by crushing of concrete which requires the
limiting strain (Ecu) on extreme compressed fiber of
concrete. Following two cases are discussed
here:
1)
Neutral axis within the
section
2)
Neutral axis outside the
section
1)
Neutral axis within the section
a)
Parabolic - Rectangular stress block
When neutral axis is within the
section, strain in extreme compressed fiber is limited to £uc 2 and corresponding stress fcct· For rectangular section
of width b and neutral axis depth x the resultant force Cu is expressed by
Cu=β1fcdbx
And
its position, measured from extreme compressed edge is defined by βx2 . The expressions for β1 and β2, as function of strain
εc, are:
Table C 8.1 Values of β1 and β2
fck (N /mm)2 |
Upto 60 | 70 | 75 | 90 | 100 | 115 |
---|---|---|---|---|---|---|
β1 | 0.8095 | 0.74194 | 0.69496 | 0.63719 | 0.59936 | 0.58333 |
Î’2 | 0.416 | 0.39191 | 0.37723 | 0.36201 | 0.35294 | 0.35294 |
b)
Rectangular stress block
Instead of parabolic - rectangular stress block, more
simplified rectangular stress block
can be used for evaluating compressive force and its line of action. The expressions for β1 and β2 are simplified to,
β1 = λη β2 = λ/2
Table C8.2 Values of for Rectangular Stress Block
fck (N /mm) 2 |
Upto 60 | 70 | 75 | 90 | 100 | 115 |
---|---|---|---|---|---|---|
β1 | 0.8 | 0.76781 | 0.73625 | 0.675 | 0.61625 | 0.56 |
Î’2 | 0.4 | 0.39375 | 0.3875 | 0.375 | 0.3625 | 0.35 |
2)
Neutral axis outside the section
a)
Parabolic - Rectangular stress block
2 |
b) Rectangular stress blocK
Table C8.4 Values of λ, η and k
|
λ |
η |
k |
< 60 |
0.8 |
1 |
0.75 |
70 |
0.7875 |
0.975 |
0.73016 |
75 |
0.775 |
0.95 |
0.70968 |
90 |
0.75 |
0.9 |
0.66667 |
100 |
0.725 |
0.85 |
0.62069 |
115 |
0.7 |
0.8 |
0.57143 |
Table C 8.3. Values of b3 and b4
Parabolic Rectangle Constitutive Law | ||||||||||||
---|---|---|---|---|---|---|---|---|---|---|---|---|
x/h | fck = 60 N/mm2 | fck = 70 N/mm2 | fck = 75 N/mm2 | fck = 90 N/mm2 | fck = 100 N/mm2 | fck = 115 N/mm2 | ||||||
b3 |
b4 |
b3 |
b4 |
b3 |
b4 |
b3 |
b4 |
b3 |
b4 |
b3 |
b4 |
|
1 |
0.80952 |
0.41597 |
0.74194 |
0.39191 |
0.69496 |
0.37723 |
0.63719 |
0.36201 |
0.59936 |
0.35482 |
0.58333 |
0.35294 |
1.2 |
0.89549 |
0.45832 |
0.83288 |
0.43765 |
0.78714 |
0.42436 |
0.72968 |
0.41022 |
0.69249 |
0.40355 |
0.6772 |
0.40186 |
1.4 |
0.93409 |
0.4748 |
0.88197 |
0.45841 |
0.84129 |
0.44724 |
0.78831 |
0.43492 |
0.75381 |
0.42907 |
0.73986 |
0.42761 |
1.6 |
0.95468 |
0.48304 |
0.91168 |
0.4699 |
0.87615 |
0.46046 |
0.82826 |
0.44975 |
0.79679 |
0.44461 |
0.78422 |
0.44335 |
1.8 |
0.96693 |
0.48779 |
0.93113 |
0.47702 |
0.90007 |
0.46895 |
0.85695 |
0.45954 |
0.82834 |
0.45499 |
0.81702 |
0.45389 |
2 |
0.97481 |
0.49077 |
0.9446 |
0.48178 |
0.9173 |
0.47478 |
0.87838 |
0.46644 |
0.85234 |
0.46237 |
0.84211 |
0.4614 |
2.5 |
0.9855 |
0.49475 |
0.96464 |
0.48861 |
0.9442 |
0.48347 |
0.91348 |
0.47705 |
0.89255 |
0.47385 |
0.88448 |
0.47311 |
5 |
0.99702 |
0.49893 |
0.9906 |
0.49705 |
0.98285 |
0.49512 |
0.96937 |
0.49234 |
0.95972 |
0.49089 |
0.95622 |
0.49057 |
Table C 8.5
Values of b3 and b4 for
Rectangular Stress Block
Rectangle Constitutive Law |
||||||||||||
x/h |
fck = 60 N/mm2 |
fck = 70 N/mm2 |
fck = 75 N/mm2 |
fck = 90N/mm2 |
fck = 100N/mm2 |
fck = 115N/mm2 |
||||||
b3 |
b4 |
b3 |
b4 |
b3 |
b4 |
b3 |
b4 |
b3 |
b4 |
b3 |
b4 |
|
1 |
0.8 |
0.4 |
0.76781 |
0.39375 |
0.73625 |
0.3875 |
0.675 |
0.375 |
0.61625 |
0.3625 |
0.56 |
0.35 |
1.2 |
0.88889 |
0.4444 |
0.85601 |
0.43898 |
0.82344 |
0.43339 |
0.75938 |
0.42188 |
0.69695 |
0.40997 |
0.63636 |
0.39773 |
1.4 |
0.92308 |
0.4615 |
0.89154 |
0.4572 |
0.86011 |
0.45269 |
0.79773 |
0.44318 |
0.73623 |
0.43308 |
0.67586 |
0.42241 |
1.6 |
0.94118 |
0.47059 |
0.91073 |
0.46704 |
0.8803 |
0.4633 |
0.81964 |
0.45536 |
0.75946 |
0.44674 |
0.7 |
0.4375 |
1.8 |
0.9524 |
0.47619 |
0.9227 |
0.4732 |
0.89308 |
0.47004 |
0.8338 |
0.4632 |
0.7748 |
0.45577 |
0.71628 |
0.44767 |
2 |
0.96 |
0.48 |
0.931 |
0.4774 |
0.9019 |
0.4747 |
0.8438 |
0.4688 |
0.78572 |
0.46219 |
0.728 |
0.455 |
2.5 |
0.97143 |
0.4857 |
0.9434 |
0.4838 |
0.91534 |
0.48176 |
0.85909 |
0.4773 |
0.80282 |
0.47255 |
0.74667 |
0.46667 |
5 |
0.9882 |
0.4941 |
0.9619 |
0.4933 |
0.9355 |
0.4924 |
0.8827 |
0.4904 |
0.8298 |
0.48809 |
0.74677 |
0.48548 |
Above Tables are Taken from IRC.
Estimate the area
of steel =
Example : Ultimate moment = 150 kN/m, cover 50mm concrete M45 grade steel Fe
Step 1:
Depth required =
D = 142.2 + 10 +
50 = 203mm < 250m. Hence depth provided is adequate.
deff =250 – 50 –
10 = 190mm.
Step 2:
Hence steel yields
It can be noted
that an increase of 47mm in depth, the x/d
>
Step 3:
Suppose anybody assumes the balanced section lever arm itself and estimates the reinforcement then
Hence it is better
to estimate the neutral axis and arrive at the steel, in case of depth provided
is more than the requirement.
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