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Bearing Capacity of Shallow Foundations

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Bearing Capacity of Shallow

Foundations

(3)
(4)
(5)

Design Components

• Design is divided into two parts;

GEOTECHNICAL DESIGN:-

• The design that takes into account only the properties of soil is called as Geotechnical Design.

SCOPE OF DESIGN:-

• The scope of geotechnical design is;

• a) Df =?

• b) B =?

• c) L =?

GOAL:-

• The goal of geotechnical design is;

• Bearing capacity.

• Settlement should be within permissible limits.

(6)

SPECIFIC DESIGN OF FOUNDATION:-

• Design means the determination of;

• Df =?

• t =?

• B =?

• L =?

• As =?

P

G.S.L

Df

BXL

B

L

(7)
(8)
(9)
(10)
(11)
(12)
(13)
(14)

FOOTINGS WITH One Way

Eccentricity

(15)
(16)
(17)

eL eB

Q

B

L

(18)

Stability Problem

Bearing Capacity Failure

Bearing Capacity Analysis

•How do we estimate the maximum bearing pressure that the soil can withstand before failure occurs?

(19)

West side of foundation sank 24-ft

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(21)

Bearing Capacity Failures

Types/Modes of Failure general shear failure local shear failure

punching shear failure

(22)

B.C. Failures

Local shear

Intermediate case +/- gradual failure

Punching

Loose sands, weak clays (dr.) F. surf. not defined Gradual failure

General shear

Dense soils, Rock, NC clays Defined failure surf.

Fast failure

(23)

General Shear Failure

(24)

B.C. Failures

(Vesic, 1963 and 1973)

Deep

foundations

(25)

We design for the general shear case (for shallow foundations)

(26)

Bearing Capacity Theory LIMIT EQUILIBRIUM

1. Define the shape of a failure surface

2. Evaluate stresses vs. strengths along this surface

(27)

BC Factor

Bearing Capacity Theory LIMIT EQUILIBRIUM

Ultimate bearing capacity = qult = ?

(Bearing press. required to cause a BC failure)

Moments about point A

( ) ( )

= ( ) 2

) 2

( B

Bb B

Bb B s

Bb q

M A ult uπ σzD

zD u

c

ult

N s

q = + σ

zD u

ult s

q = 2π +σ

(28)
(29)
(30)

Terzaghi’s Bearing Capacity Theory

(31)

Terzaghi’s Bearing Capacity Theory

(32)

Terzaghi’s Bearing Capacity Theory

Terzaghi developed the theory for continuous foundations (simplest, 2D problem).

γ

γ

σ N BN

N c

q

ult

= '

c

+ '

zD q

+ 0 . 5 '

γ

γ

σ

N BN

N c

qult = 1.3 ' c + 'zD q + 0.4 '

γ

γ

σ N BN

N c

q

ult

= 1 . 3 '

c

+ '

zD q

+ 0 . 3 '

From model tests, he expanded the theory to:

(33)

N

c

= cohesion factor N

q

= surcharge factor

N

γ

= self wt factor

Terzaghi’s Bearing Capacity Theory

= f ( φ ’) for values

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(35)
(36)
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See Extra Handout

Further Developments

• Skempton (1951)

• Meyerhof (1953)

• Brinch Hanson (1961)

• De Beer and Ladanyi (1961)

• Meyerhof (1963)

• Brinch Hanson (1970)

• Vesic′ (1973, 1975)

(38)

Shape factors….…

Depth Factors …….

Load Inclination Factors ….

Base Inclinations factors ..

Ground Inclination Factors….

Bearing Capacity Factors ….

γ γ γ γ γ

γ γ

σ N s d i b g BN s d i b g

g b i d s N c

qult = c c c c c c + zD q q q q q q + 0.5

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(47)

CONTOH

B Df = 0,7 m

β= 200

φ= 300 c = 0

γ = 18 kN/m3 Q = 150 kN

Berapakah B dengan SF = 3

6 , 12 18

7 , 0 .

4 , 22

; 4 , 18

nilai diperoleh 1973

Vesic, tabel

Dari

2 1

=

×

=

=

=

=

+

=

γ

γ

γ

γ γ γ γ

f q

i d s qi

qd qs q u

D q

N N

F F F BN F

F F qN q

( )

1

20207 ,

1 0

7 , 30 0

sin 1

30 tan 2 1 1 /

2

= +

=

+

=

γd qd

F

B F B

B Df

11 , 20 0

1 1

605 , 90 0

1 20 1 90

0 2 0 2

2 0 2 0

0 0

 =



φ

 =



φ

β

=

 =



 =



β

=

γi qi

F F

m B

B B B

B qall Q

283 , 1 48

, 902 4

, 745 14

, 150 73

2

2

=

+

+

=

= 6

, 0 4 , 0 1 4

, 0 1

577 , 1 30 tan 1

tan 1

L 1 sangkar, B

bujur Fondasi

Dengan

=

=

=

= +

= φ +

=

=

γ L

F B

L B L

F B

s qs

[ ]

3 1

3

2 1

i d s qi

qd qs q all

u u

all

F F F BN F

F F qN q

q SF

q q

γ γ γ

γ γ

+

=

=

=

B B q

B B q

all all

48 , 902 4

, 745 14

, 73

441 , 705 13

, 235 44

, 3 221 1

+ +

=

+ +

=

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Groundwater Table Effect

(65)

Groundwater Table Effect;

Case I

1. Modify σ′zD

2. Calculate γ′ as follows:

w

b

γ γ

γ

γ ′ = = −

(66)

Groundwater Table Effect;

Case II

1. No change in σ′zD

2. Calculate γ′ as follows:





=

B D Dw

w 1

γ γ

γ

(67)

Groundwater Table Effect;

Case III

1. No change in σ′zD 2. No change in γ′

γ

γ ′ =

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