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1
Geotechnical Engineering–II [CE-321]
BSc Civil Engineering – 5th Semester
by
Dr. Muhammad Irfan
Assistant Professor
Civil Engg. Dept. – UET Lahore
Email: mirfan1@msn.com
Lecture Handouts: https://groups.google.com/d/forum/geotech-ii_2015session
Lecture # 7A
28-Sep-2017
2
STRESS DISTRIBUTION IN SOIL
What causes stress in soil?
Two principle factors causing
stresses in soil.
1. Self weight of soil
2. External loads (Structural loads,
external load, etc.)
v
h

3
STRESS INCREASE (∆q) DUE TO
EXTERNAL LOAD
Determination of stress due to external load at any
point in soil
1. Approximate Method
2. Boussinesq’s Theory
3. Westergaard’s Theory
4
Q
  2522
3
5
3
2
3
2
3
zr
zQ
L
Qz
z




The above relationship for
z can be re-written as
   








 2522
1
1
2
3
zrz
Q
z


where
   252
1
1
2
3
zr
IB



QBI
z
Q
2

Independent of all material properties
Boussinesq’s Theory
for Point Load
5
Practice Problem #5
A concentrated load of 1000 kN is applied at the ground
surface. Compute the vertical stress
(i) at a depth of 4m below the load,
(ii) at a distance of 3m at the same depth.
(A) Use Boussinesq’s equation
(B) Use Westergaard’s equation P
   








 2522
1
1
2
3
zrz
Q
z


6
Vertical Stress caused by Line Load
x
z
z
z
Q/unit length
x
A
y
By integrating the point load equation along a line, stress due
to a line load (force per unit length) may be found.
Lz I
z
q

 
2
2
/1
12








zx
IL

Where,
q is line load in “per unit length”
7
Practical Problem #6
Following figure shows two line loads and a point load acting
at the ground surface. Determine the increase in vertical stress
at point A, which is located at a depth of 1.5 m.
Q = 10000 kN
z
2 m
A
1.5 m
2 m
3 m
q2 = 250 kN/m q1 = 150 kN/m
   








 2522
1
1
2
3
zrz
Q
z


   








 22
/1
12
zxz
q
z


Point Load
Line Load
8
STRESS INCREASE (∆q) DUE TO
EXTERNAL LOAD
 Point load
 Line Load
• But engineering loads typically act on areas and
not points or lines.
• Bousinesq solution for line load was thus
integrated for a finite area
Bz I
z
Q
2

Lz I
z
q

Uniformly Loaded
Circular Area
Uniformly Loaded
Rectangular Area
Trapezoidal,
Triangular, etc.
9
z
RO
STRESS UNDER UNIFORMLY LOADED
CIRCULAR AREA
Case-A: Vertical stress under the center of
circular footing
   






 232
1
1
1
zR
q
o
z
Boussinesq equation can be extended to a uniformly loaded
circular area to determine vertical stress at any depth.
where,
q = UDL (load/area)
RO = Radius of footing
10
STRESS UNDER UNIFORMLY LOADED
CIRCULAR AREA
Case-B: Vertical stress at any point in soil
z
a
RO
r
z
),( nmIq Zz 
where,
IZ = Shape function/ Influence factor
m = z/RO; n=r/RO
RO = Radius of footing
r = distance of Δσz from center of footing
z = depth of Δσz
11
STRESS UNDER UNIFORMLY LOADED CIRCULAR AREA
(Foster & Alvin, 1954; U.S. Navy, 1986) Assumptions: Semi-infinite elastic
medium with Poisson’s ratio 0.5.
(stress in percent of surface contact pressure)
12
A water tank is required to be constructed with a circular
foundation having a diameter of 16 m founded at a depth of 2 m
below the ground surface. The estimated distributed load on the
foundation is 325 kPa.
Assuming that the subsoil extends to a great depth and is
isotropic and homogeneous. Determine the stress z at points
(i) 10 m below NSL; at center of footing
(ii) 10 m below NSL; at distance of 8 m from central axis of footing
(iii) 18 m below NSL; at center of footing
(iv) 18 m below NSL; at distance of 8 m from central axis of footing
Neglect the effect of the depth of the foundation on the
stresses.
Practice Problem #7
13
STRESS UNDER UNIFORMLY LOADED
RECTANGULAR AREA
Bousinesq equation can be extended for uniformly loaded
rectangular area as;
),( nmIq recz 
where,
IZ = Shape function/ Influence factor
m = b/z; n=l/z
x
z
q
A
y
z
dx
dy
14
STRESS UNDER
UNIFORMLY
LOADED
RECTANGULAR
AREA
•14
z
L
n
z
B
m  ,
Log scale
15
STRESS UNDER UNIFORMLY LOADED
RECTANGULAR AREA
This methods gives stress at the corner of rectangular area
),( nmIq recz 
A B
D C
Case I
E
F
G
A B
D C
Case II
σz due to ABCD =
4 x σz due to EBFG
16
A 20 x 30 ft rectangular footing carrying a uniform load of 6000
lb/ft2 is applied to the ground surface.
Required
The vertical stress increment due to this uniform load at a depth
of 20 ft below the (i) corner, and (ii) center of loaded area.
G
A BE
D C
20 ft
30 ft
F
Practice Problem #8
17
E
FH
G
E
FH
I
STRESS UNDER UNIFORMLY LOADED
RECTANGULAR AREA
G
A B
D C
A B
D C
I
A B
D C
Case I Case II
σz due to ABCD =
4 x σz due to EBFG
Case III
σz due to ABCD = σz due to
(EBFI + IFCG + IGDH + AEIH)
18
E
I
STRESS UNDER UNIFORMLY LOADED
RECTANGULAR AREA
A B
D C
EF
GH
F
A B
D
C
Case IV
σz due to ABCD = 2 x σz due to ABEF
Case V
σz due to ABCD = 2 x σz due to EBCF
Case VI
σz due to ABCD = σz due to
(AEGI – BEGH – DFGI + CFGH)
A BE
D CF
19
CONCLUDED
REFERENCE MATERIAL
An Introduction to Geotechnical Engineering (2nd Ed.)
Robert D. Holtz & William D. Kovacs
Chapter #10

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Geotechnical Engineering-II [Lec #7A: Boussinesq Method]

  • 1. 1 Geotechnical Engineering–II [CE-321] BSc Civil Engineering – 5th Semester by Dr. Muhammad Irfan Assistant Professor Civil Engg. Dept. – UET Lahore Email: mirfan1@msn.com Lecture Handouts: https://groups.google.com/d/forum/geotech-ii_2015session Lecture # 7A 28-Sep-2017
  • 2. 2 STRESS DISTRIBUTION IN SOIL What causes stress in soil? Two principle factors causing stresses in soil. 1. Self weight of soil 2. External loads (Structural loads, external load, etc.) v h 
  • 3. 3 STRESS INCREASE (∆q) DUE TO EXTERNAL LOAD Determination of stress due to external load at any point in soil 1. Approximate Method 2. Boussinesq’s Theory 3. Westergaard’s Theory
  • 4. 4 Q   2522 3 5 3 2 3 2 3 zr zQ L Qz z     The above relationship for z can be re-written as              2522 1 1 2 3 zrz Q z   where    252 1 1 2 3 zr IB    QBI z Q 2  Independent of all material properties Boussinesq’s Theory for Point Load
  • 5. 5 Practice Problem #5 A concentrated load of 1000 kN is applied at the ground surface. Compute the vertical stress (i) at a depth of 4m below the load, (ii) at a distance of 3m at the same depth. (A) Use Boussinesq’s equation (B) Use Westergaard’s equation P              2522 1 1 2 3 zrz Q z  
  • 6. 6 Vertical Stress caused by Line Load x z z z Q/unit length x A y By integrating the point load equation along a line, stress due to a line load (force per unit length) may be found. Lz I z q    2 2 /1 12         zx IL  Where, q is line load in “per unit length”
  • 7. 7 Practical Problem #6 Following figure shows two line loads and a point load acting at the ground surface. Determine the increase in vertical stress at point A, which is located at a depth of 1.5 m. Q = 10000 kN z 2 m A 1.5 m 2 m 3 m q2 = 250 kN/m q1 = 150 kN/m              2522 1 1 2 3 zrz Q z                22 /1 12 zxz q z   Point Load Line Load
  • 8. 8 STRESS INCREASE (∆q) DUE TO EXTERNAL LOAD  Point load  Line Load • But engineering loads typically act on areas and not points or lines. • Bousinesq solution for line load was thus integrated for a finite area Bz I z Q 2  Lz I z q  Uniformly Loaded Circular Area Uniformly Loaded Rectangular Area Trapezoidal, Triangular, etc.
  • 9. 9 z RO STRESS UNDER UNIFORMLY LOADED CIRCULAR AREA Case-A: Vertical stress under the center of circular footing            232 1 1 1 zR q o z Boussinesq equation can be extended to a uniformly loaded circular area to determine vertical stress at any depth. where, q = UDL (load/area) RO = Radius of footing
  • 10. 10 STRESS UNDER UNIFORMLY LOADED CIRCULAR AREA Case-B: Vertical stress at any point in soil z a RO r z ),( nmIq Zz  where, IZ = Shape function/ Influence factor m = z/RO; n=r/RO RO = Radius of footing r = distance of Δσz from center of footing z = depth of Δσz
  • 11. 11 STRESS UNDER UNIFORMLY LOADED CIRCULAR AREA (Foster & Alvin, 1954; U.S. Navy, 1986) Assumptions: Semi-infinite elastic medium with Poisson’s ratio 0.5. (stress in percent of surface contact pressure)
  • 12. 12 A water tank is required to be constructed with a circular foundation having a diameter of 16 m founded at a depth of 2 m below the ground surface. The estimated distributed load on the foundation is 325 kPa. Assuming that the subsoil extends to a great depth and is isotropic and homogeneous. Determine the stress z at points (i) 10 m below NSL; at center of footing (ii) 10 m below NSL; at distance of 8 m from central axis of footing (iii) 18 m below NSL; at center of footing (iv) 18 m below NSL; at distance of 8 m from central axis of footing Neglect the effect of the depth of the foundation on the stresses. Practice Problem #7
  • 13. 13 STRESS UNDER UNIFORMLY LOADED RECTANGULAR AREA Bousinesq equation can be extended for uniformly loaded rectangular area as; ),( nmIq recz  where, IZ = Shape function/ Influence factor m = b/z; n=l/z x z q A y z dx dy
  • 15. 15 STRESS UNDER UNIFORMLY LOADED RECTANGULAR AREA This methods gives stress at the corner of rectangular area ),( nmIq recz  A B D C Case I E F G A B D C Case II σz due to ABCD = 4 x σz due to EBFG
  • 16. 16 A 20 x 30 ft rectangular footing carrying a uniform load of 6000 lb/ft2 is applied to the ground surface. Required The vertical stress increment due to this uniform load at a depth of 20 ft below the (i) corner, and (ii) center of loaded area. G A BE D C 20 ft 30 ft F Practice Problem #8
  • 17. 17 E FH G E FH I STRESS UNDER UNIFORMLY LOADED RECTANGULAR AREA G A B D C A B D C I A B D C Case I Case II σz due to ABCD = 4 x σz due to EBFG Case III σz due to ABCD = σz due to (EBFI + IFCG + IGDH + AEIH)
  • 18. 18 E I STRESS UNDER UNIFORMLY LOADED RECTANGULAR AREA A B D C EF GH F A B D C Case IV σz due to ABCD = 2 x σz due to ABEF Case V σz due to ABCD = 2 x σz due to EBCF Case VI σz due to ABCD = σz due to (AEGI – BEGH – DFGI + CFGH) A BE D CF
  • 19. 19 CONCLUDED REFERENCE MATERIAL An Introduction to Geotechnical Engineering (2nd Ed.) Robert D. Holtz & William D. Kovacs Chapter #10