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The Islamic university - Gaza Faculty of Engineering Civil Engineering Department CHAPTER (3) Instructor : Dr. Jehad Hamad BEARING CAPACITY OF SHALLOW STRIP FOUNDATIONS
Transcript
Page 1: CH3

The Islamic university - Gaza

Faculty of Engineering

Civil Engineering Department

CHAPTER (3)

Instructor : Dr. Jehad Hamad

BEARING CAPACITY OF SHALLOW STRIP FOUNDATIONS

Page 2: CH3

DEFINITION OF SOILDEFINITION OF SOIL

Soil is a mixture of irregularly shaped mineral particles of various

sizes containing voids between particles. The particles are a by-

product of mechanical and chemical weathering of rock and

described as gravels, sands, silts, and clays.

Any manmade structure should, one way or another, rest

and/or transmit its load to the underlying soil

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BEARING CAPACITY OF SOILSBEARING CAPACITY OF SOILS

oBearing capacity: is the ability of soil to safely carry the pressure

placed on the soil from any engineered structure without undergoing

a shear failure with accompanying large settlements.

oTherefore, settlement analysis should generally be performed

since most structures are sensitive to excessive settlement.

Page 4: CH3

Types of FoundationsTypes of Foundations

ShallowFoundations

DeepFoundations

Spread Mat or Raft

Friction PilesBelled Pier

Page 5: CH3

Bearing Capacity of Shallow Foundations

Bearing Capacity of Shallow Foundations

Soil Bearing Capacity is Controlled by:

ØBearing Capacity Analysis:

§ Terzaghi’s Theory (1943), based on Prandtl theory (1920).

§ General B.C. Equation.

ØSettlement Analysis:

§ Immediate Settlement.

§ Consolidation Settlement.

Page 6: CH3

Failure Modes for Shallow Foundations

Failure Modes for Shallow Foundations

oGeneral Shear Failure

oLocal Shear Failure

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oPunching Shear Failure

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This failure alerted engineers to the mechanism of how surface loads may exceeded the shear strength of the soils beneath the foundation.

Page 9: CH3

Terzaghi B/C AssumptionsTerzaghi B/C Assumptions

BD f ≤Ø The foundation is considered to be shallow if

However ,in recent studies ,the foundation is considered to

be shallow if . Other wise it is considered to be

deep foundation.

Ø Foundation is considered to be strip if

Ø The soil from the ground surface to the bottom of the

foundation is replaced by a surcharge .

4/ ≤BDf

00.0/ →LB

fDq γ=

Page 10: CH3

oModes of foundation

failure in sand

Page 11: CH3

General ConceptGeneral Concept

Z o n e I, A c tiv e

Z o n e s II, T ra n s it io n

Z o n e s III , P a s s iv e

Page 12: CH3

General ConceptGeneral Concept

o Active zone, just below thefoundation.

o Transition zone, between the activeand passive zones.

o Passive zone, near the groundsurface, just beside the foundation.

passive active

Transition

Three zones do exist:

Page 13: CH3

Terzaghi Bearing EquationTerzaghi Bearing Equation

qult = qult = c Nc

qult = c Nc + γ1 D Nq + 0.5B γ2 Nγ

qult = c Nc + γ1 D Nq

Cohesion Term

Above F.L.

Below F.L.

Page 14: CH3

Terzaghi Bearing EquationTerzaghi Bearing Equation

are Terzaghi B/C Coefficients ,f(φ)(See table 3.1- P139)

are the soil shear strength parameters

Nc, Nq, Nγ

Φ c

Page 15: CH3

oVariation of

&

for circular and rectangular

plates on the surface of a

sand.

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oRange of settlement

of circular & rectangular

plates at ultimate Load

in sand.

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Terzaghi’s Equation for Different Foundation Shapes

Terzaghi’s Equation for Different Foundation Shapes

qu = c Nc + γ1 D Nq + 0.5 B γ2 Nγ

qu net = c Nc + γ1 D (Nq - 1) + 0.5 B γ2 Nγ

qu = 1.3c Nc + γ1 D Nq + 0.4B γ2 Nγ

qu= c Nc + γ1 D Nq + 0.3 B γ2 Nγ

Continuous Footing:

Square Footing:

Circular Footing:

Page 19: CH3

• Strip Footing

• Square footing

• Circular footing

'''

21

32

γγBNqNcNq qcu ++=

''' 4.0867.0 γγBNqNcNq qcu ++=

''' 3.0867.0 γγBNqNcNq qcu ++=

Φ=Φ − tan

32tan 1'

''' ,, γNNN qcFactors for bearing capacity given fromtable 3.2 P.140

Page 20: CH3
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Bearing Capacity of Clay, φ = 0Bearing Capacity of Clay, φ = 0

qult = c Nc + γ1 D Nq + 0.50 B γ2 N γ

For Clay:

Nc = 5.70, Nq = 1.0, Nγ = 0.0

qult = 5.70 cu + γ1 D

qult net = 5.70 cu

cu = qu/2 qu Unconfined compressive strength

qall net = 1.90 cu

Page 22: CH3

Bearing Capacity of Sand, cu = 0Bearing Capacity of Sand, cu = 0

qult = c Nc + γ1 D Nq + 0.50 B γ2 N γ

For Sand:

Nc, Nq, Nγ are determined from curve, and cu = 0, then:

qult = γ1 D Nq + 0.50 B γ2 N γ

Page 23: CH3

Gross and Net Bearing Capacity“Factor of Safety”

Gross and Net Bearing Capacity“Factor of Safety”

qult (net)= qult - γ1 D

Gross allowable bearing capacity

Net ultimate B/C

Net allowable B/C

γ1 D is the overburden pressure

..

SFq

q ultall =

..

SFq

q netultnetall =

Page 24: CH3

Effect of Water Table on B/C

):1(Case

γ1 D = γ D1 + γsub D2,γ2 = γsub

qult = c Nc + γ1 D Nq + 0.5B γ2 Nγ

Page 25: CH3

Effect of Water Table on B/C

):2(Case

γ1 D = γDf , γ2 = γsub+d/B (γ−γsub)

qult = c Nc + γ1 D Nq + 0.5B γ2 Nγ

Page 26: CH3

Effect of Water Table on B/C

):3(Case

The water has no effect on bearing capacity

qult = c Nc + γ1 D Nq + 0.5B γ2 Nγ

γ = Bulk unit weightγsub = Submerged Unit weight

γsub = γsat - γwater

Page 27: CH3

Meyerhof’s equationMeyerhof’s equation

• Nc, Nq, Nγ are Meyerhof’s B/C Factors, f(φ)

(See table 3.3- P144)

• Shape Factors

• Depth Factors

• Inclination Factors(See table 3.4 in the text book)

idsqiqdqsqcicdcscu FFFBNFFFqNFFFcNq γγγγγ5.0++=

Page 28: CH3
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Page 31: CH3

٣١

Fci, Fqi, Fγ i

P

Footings with inclined loadsFootings with inclined loads

Inclined Load Factors

L

Page 32: CH3

Eccentrically Loaded FoundationEccentrically Loaded Foundation

B’=B-2e , L’=L , A’=B’*L’To find shape factors: use B’,L’To find depth factors: use B, LTo find the gross ultimate load

idsqiqdqsqcicdcscu FFFNBFFFqNFFFcNq γγγγγ '' 5.0++=

'' AqQ uu ×=

Page 33: CH3

±

×=

×±

×=

×±

×=

××±

×=

=

=

=×=

±=

Be

LBP

LBeP

LBP

LB

ePLB

P

LB

BePLB

Pq

Bc

LBI

PeMLBA

IMc

APq

616

61

121

2/2/

121.

223

3

oFor e<B/6:

×=

+

×=

Be

LBPq

Be

LBPq

61

61

min

max

Page 34: CH3

)2(34

max eBLPq−

=

oFor e = B/6:

oFor e > B/6:

0.0

61

min

max

=

+

×=

qBe

LBPq

Page 35: CH3

Failure of eccentrically loaded foundation

Page 36: CH3

Two way eccentricityTwo way eccentricity

How to find A' ?

By

Lx

ePMePM

×=×=

idsqiqdqsqcicdcscu FFFNBFFFqNFFFcNq γγγγγ '' 5.0++=

Page 37: CH3

61&

61

≥≥Be

Le BL

'

''

11'

1

1

11'

),max(

35.1

35.1

21

LAB

LBLLeLL

Be

BB

LBA

L

B

=

=

−=

−=

=

oCase (I)

Page 38: CH3

610&

21

<<<Be

Le BL

oCase (II)

( )

graph. eThrough th :

&LL

:axis- xLe

:axis-y

. figureat look L and L find To

),max(........21

21L

21

'

''

21'

21'

Be

LL

LAB

LLLBLLA

B

=

=+=

Page 39: CH3

210&

61

<<<Be

Le BL

( )

graph. eThrough th :

&BB:axis-x

Be :axis-y

beside figureat look B and B find To

21

21

B

21

''

21'

Le

BB

LAB

LBBA

L

=

+=

oCase (III)

Page 40: CH3

61&

61

<<Be

Le BL

( )( )

graph. eThrough th :

&LL:axis-x

Be :axis-y

beside figureat look B and L find To

21

22

B

22

''

222'

Le

BB

LAB

LLBBBLA

L

=

−++=

oCase (IV)

Page 41: CH3

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