This document outlines the theory and design of structures, specifically analyzing dams and retaining walls. It provides equations for calculating water pressure, forces on dams, and stress distribution at the base. It also derives the middle third rule for dam bases to prevent tensile stresses. An example problem is worked through calculating forces, locating the center of gravity, checking for failure modes, and stability against sliding. A second example is presented to calculate the minimum dam width required to prevent tension in the concrete.
Gantry girder
Gantry girder or crane girder hand operated or electrically operated overhead cranes in industrial building such as factories, workshops, steel works, etc. to lift heavy materials, equipment etc. and carry them from one location to other , within the building
The GANTRY GIRDER spans between brackets attached to columns, which may either be of steel or reinforced concrete. Thus the span of gantry girder is equal to centre to centre spacing of columns. The rails are mounted on gantry girders.
Loads acting on gantry girder
Gantry girder, having no lateral support in its length (laterally unsupported) has to withstand the following loads:
1. Vertical loads from crane :
Self weight of crane girder
Hook load
Weight of crab (trolley)
2. Impact load from crane :
As the load is lifted using the crane hook and moved from one place to another, and released at the required place, an impact is felt on the gantry girder.
3. Longitudinal horizontal force (Drag force) :
This is caused due to the starting and stopping of the crane girder moving over the crane rails, as the crane girder moves longitudinally, i.e. in the direction of gantry girder.
This force is also known as braking force, or drag force.
This force is taken equal to 5% of the static wheel loads for EOT or hand operated cranes.
4. Lateral load (Surge load) :
Lateral forces are caused due to sudden starting or stopping of the crab when moving over the crane girder.
Lateral forces are also caused when the crane is dragging weights across the' floor of the shop.
Types of gantry girders
Depending upon the span and crane capacity, there can be many forms of gantry girders. Some commonly used forms are shows in fig .
Rolled steel beams with or without plates, channels or angles are normally used for spans up to 8m and for cranes up to 50kN capacity.
Plate girder are suitable up to span 6 to 10 m.
Plate girder with channels, angles, etc. can be used for spans more than 10m
Box girder are used foe spans more than 12m.
Gantry girder
Gantry girder or crane girder hand operated or electrically operated overhead cranes in industrial building such as factories, workshops, steel works, etc. to lift heavy materials, equipment etc. and carry them from one location to other , within the building
The GANTRY GIRDER spans between brackets attached to columns, which may either be of steel or reinforced concrete. Thus the span of gantry girder is equal to centre to centre spacing of columns. The rails are mounted on gantry girders.
Loads acting on gantry girder
Gantry girder, having no lateral support in its length (laterally unsupported) has to withstand the following loads:
1. Vertical loads from crane :
Self weight of crane girder
Hook load
Weight of crab (trolley)
2. Impact load from crane :
As the load is lifted using the crane hook and moved from one place to another, and released at the required place, an impact is felt on the gantry girder.
3. Longitudinal horizontal force (Drag force) :
This is caused due to the starting and stopping of the crane girder moving over the crane rails, as the crane girder moves longitudinally, i.e. in the direction of gantry girder.
This force is also known as braking force, or drag force.
This force is taken equal to 5% of the static wheel loads for EOT or hand operated cranes.
4. Lateral load (Surge load) :
Lateral forces are caused due to sudden starting or stopping of the crab when moving over the crane girder.
Lateral forces are also caused when the crane is dragging weights across the' floor of the shop.
Types of gantry girders
Depending upon the span and crane capacity, there can be many forms of gantry girders. Some commonly used forms are shows in fig .
Rolled steel beams with or without plates, channels or angles are normally used for spans up to 8m and for cranes up to 50kN capacity.
Plate girder are suitable up to span 6 to 10 m.
Plate girder with channels, angles, etc. can be used for spans more than 10m
Box girder are used foe spans more than 12m.
Soil nailing, Cohesion less soil, experimental studies, horizontal vs inclined nails, illustrated example, equations - soil nailing, model test study, scale model experiments- soil nailing
Roof Truss Design (By Hamza Waheed UET Lahore )Hamza Waheed
This presentation defines, describes and presents the most effective and easy way to design a roof truss with all the necessary steps and calculations based on Allowable Stress Design. Soft-wares like MD Solids, Truss Analysis have been used. It is most convenient way to design a roof truss which is being the most important structural components of All types of steel bridges.
Content;
1. Top spherical dome.
2. Top ring beam.
3. Cylindrical wall.
4. Bottom ring beam.
5. Conical dome.
6. Circular ring beam.
The basics of enticing water tank design and the related components are broadly calculated in this document. The next few documents will demonstrate the design of Intze tank members like column, bracing and foundation. Keep following the updates.....
Explains in detail about the planning and designing of a G + 2 school building both manually and using software (STAAD Pro).
With the reference with this we could design a building of a school with 2 blocks and G + 2 building.
How to Make a Field invisible in Odoo 17Celine George
It is possible to hide or invisible some fields in odoo. Commonly using “invisible” attribute in the field definition to invisible the fields. This slide will show how to make a field invisible in odoo 17.
Soil nailing, Cohesion less soil, experimental studies, horizontal vs inclined nails, illustrated example, equations - soil nailing, model test study, scale model experiments- soil nailing
Roof Truss Design (By Hamza Waheed UET Lahore )Hamza Waheed
This presentation defines, describes and presents the most effective and easy way to design a roof truss with all the necessary steps and calculations based on Allowable Stress Design. Soft-wares like MD Solids, Truss Analysis have been used. It is most convenient way to design a roof truss which is being the most important structural components of All types of steel bridges.
Content;
1. Top spherical dome.
2. Top ring beam.
3. Cylindrical wall.
4. Bottom ring beam.
5. Conical dome.
6. Circular ring beam.
The basics of enticing water tank design and the related components are broadly calculated in this document. The next few documents will demonstrate the design of Intze tank members like column, bracing and foundation. Keep following the updates.....
Explains in detail about the planning and designing of a G + 2 school building both manually and using software (STAAD Pro).
With the reference with this we could design a building of a school with 2 blocks and G + 2 building.
How to Make a Field invisible in Odoo 17Celine George
It is possible to hide or invisible some fields in odoo. Commonly using “invisible” attribute in the field definition to invisible the fields. This slide will show how to make a field invisible in odoo 17.
The French Revolution, which began in 1789, was a period of radical social and political upheaval in France. It marked the decline of absolute monarchies, the rise of secular and democratic republics, and the eventual rise of Napoleon Bonaparte. This revolutionary period is crucial in understanding the transition from feudalism to modernity in Europe.
For more information, visit-www.vavaclasses.com
Read| The latest issue of The Challenger is here! We are thrilled to announce that our school paper has qualified for the NATIONAL SCHOOLS PRESS CONFERENCE (NSPC) 2024. Thank you for your unwavering support and trust. Dive into the stories that made us stand out!
Acetabularia Information For Class 9 .docxvaibhavrinwa19
Acetabularia acetabulum is a single-celled green alga that in its vegetative state is morphologically differentiated into a basal rhizoid and an axially elongated stalk, which bears whorls of branching hairs. The single diploid nucleus resides in the rhizoid.
Honest Reviews of Tim Han LMA Course Program.pptxtimhan337
Personal development courses are widely available today, with each one promising life-changing outcomes. Tim Han’s Life Mastery Achievers (LMA) Course has drawn a lot of interest. In addition to offering my frank assessment of Success Insider’s LMA Course, this piece examines the course’s effects via a variety of Tim Han LMA course reviews and Success Insider comments.
1. THEORY & DESIGN OF
STRUCTURES
C3 -05 (5S3 NVQ 2045)
Eng. Y.A.P.M Yahampath
B Sc. Eng (Hons), Dip Highway & Traffic Eng, AMIESL, AMECSL
2. Lecture Hours Allocated
Lecture / Tutorial Practical Demonstrations/
Industrial visits
Self Study Total
72 Hrs 00 Hrs 38 Hrs 110 Hrs
Unit Title Time (Hrs)
Combined Direct & Bending stresses 10
Principle stresses & strain 06
Structural design principles 06
Designing of Reinforced concrete
elements
26
Design of structural steel elements 18
Structural detailing 06
Total 72
3. AIM OF THE MODULE
To develop fundamental understanding of the behavior of structures with
particular reference to statically determinate civil engineering structures.
✓ To develop & understanding of the factors and constraints in determining
suitable structural components.
✓ To develop awareness of the economical, Engineering & esthetic aspect
in designing in selecting a particular structural component for given
condition.
✓ To introduce students to use codes of practice and design charts/ Tables
etc. for designing of structural elements.
4. Retaining Structures – Dams / Retaining walls
• Analysis of dams applying theory of combined stress
• Forces Applying on Dam
• Resultant force acting on base of a dam
• Stress variation diagram at the base of the dam
5.
6.
7.
8. When we consider water at given depth
the pressure acting on a water particle
in any direction is equal.
10. a = Top width of the dam
d = Bottom width of the dam
H = Height of the dam
h = Height of the water retain by the dam
ϒ w = Specific weight/ unit weight of the water (kN/ m3 ) (ϒ w = ρ wg)
Γ = Unit weight of the dam masonry (kN/ m3 )
Consider a unit length (b=1 m) of the dam,
Volume (m3) of unit length of the dam,
V = [(a+d)/2] x H X 1
Weight (KN) of unit length of the dam,
W = [(a+d)/2] x H X 1 X Γ
P = F/A (kN/ m2 )
ϒ = ρ g (g = 9.81 m/s-2)
ρ = M/V
ϒ = M/V X g
F = Ma = Mg
ϒ = F/V = kN/ m3
b
12. Water Pressure Equation
P = hρwg
• Hence the equation P = hρg represents the
pressure due to the weight of any fluid having an
average density ρ at any depth h below its
surface. Pressure varies with depth.
P = F/A
F = PA
dF = P.dA dA = 1.dy
dF = y.ρwg .1.dy
F = y.ρwg .1.dy = 1/2 ρwg y2 =1/2 ρwgh2
y
h
b=1 m
F
h
0
13. h
F
?
Water head
F = 1/2. (ρwg).h2 But, ϒw = ρwg
F = 1/2. ϒ w .h2 ϒ w = 1000 kg/m3 x 9.81 m/s-2 /1000 kN / m3
9.81 10 kN / m3
ϒ w = 1000 kg/m3 x 9.81 m/s-2 =10 kN/m3
14. The deeper the water, the more horizontal pressure it exerts on the dam. So at the surface of the
reservoir, the water is exerting no pressure and at the bottom of the reservoir, the water is
exerting maximum pressure. The force acts at the center of gravity of the triangle -- one-third of
the way up from the bottom.
h
F
h/3
Water head
h/3
15. F
W
G
h/3
R
J K
N
L
M
x
J K
N
L
M
h/3
x
F
W
X/F = h/3/W
X = F.h/3W
R
R2 = √ W2+F2
Φ
✓ W
✓ F
✓ R
✓ h/3
✓ Φ = W/F
X = ?
Using force diagram,
X = The
horizontal
distance
between
the center
of gravity of
the dam &
point where
the
resultant
force ( R )
pass
through the
dam base
16. F
Water head
h/3
h
b =1m
H
a
A B
w1
W
w2
R
Toe
XX-Axis
x
ZZ- Axis of
symmetry
G
G2
G1
a/2
d/2
(d-a)/3
e
X
K
L
YY-
Axis
(d-a)
17. Trapezoidal
Dam with
Water Face
Vertical
h
H
F
a
d/2
h/3
A B
Water head
w1
W w2
R
Heel Toe
L
x x
d/2
e
e = [L – d/2]
σmin = W/d { 1 – 6e/d } σmax = W/d { 1 + 6e/d }
Stress Distribution at base of the dam,
Axis of
symmetry
L = Liver arm
L = X+X
G
G2
G1
C+ C+
C+
T-
Heel Toe
18. Derivation of Middle third Rule for Dam Base
• The minimum stress (σMin) must be greater or equal to zero for no tensile stress
at any point along the width of the column.
Z = I/eMax
I = bd
3
/12
b = 1 m & d = d m,
I = 1.d3/12
eMax = d/2
Z = d
2
/6
A = b.d
But, b = 1 m
A = 1.d
σmin = W/A - M/Z
σmin > 0
W/A - M/Z > 0
M = We
W/d – We/ (d
2
/6) > 0
W/d - 6We/d
2
> 0
W/d { 1 – 6e/d } > 0
W/d = 0,
So,
{ 1 – 6e/d } > 0
d/6 > e
σ = W/A ± M/Z
Assume Bending around x-x,
19. Derivation of
Middle third
Rule for Dam
Base
d
1m
d/3 d/3 d/3
d/6 d/6
d/2
A B
A B
K
e
L
e = [L – d/2]
x
x
W
W
Y Y
z
z
Plan view of Base
L = Liver arm
L = X+X
Axis of symmetry Z-Z,
20. F
f
Friction Effect on Dam
Frictional force (f),
f = µR
considering equilibrium of vertical forces,
W = R
f = µ.W
If,
f > F
Hence no sliding effect.
If,
f < F
Failure due to sliding effect.
Safety factor against water pressure = f/F
f/F >1 - no sliding effect
W
G
R
A
21. Methods of failure
Tension in the base
If, d/3 < L < 2d/3 – No
failure( Resultant force
pass through the middle
third section of the base)
If, d/3 > L > 2d/3 –
Failure
Over turning
If, 0< L < d – No
failure( Resultant
force pass within the
section of the base)
If, 0 > L > d – Failure
( Resultant force pass
outside the section
of the base)
Sliding
If, f > F - No failure
If, f < F - Failure
22. • Check for Failure Due to Tension
in the base
• Check for Failure Due to
overturning
F
W
G
F
W
G
R R
d/3 d
23.
24. h =7m
F = ?
a =1.2m
h/3 =7/3m
Water head
W=?
H =8m
w1
w2
G2
G1
d =4.8 m
10kN/m3
24kN/m3
x
A B
Up stream
25. Considering a 1 m length of dam,
• F = 1/2. ϒ w .h2
• F = ½ X 10 kN/m3 X 72 m2
• F = 245 kN/m
• W = (1.2+4.8)/2 X 8 X 24 X 1
• W = 576kN/m
Using force diagram,
• X = F.h/3W
• X = (245 x 7)/(3 x 576)
• X = 0.99 m
26. To find location of the center of gravity of the dam section (X) ,
Consider the dam section only & split in to two shapes
(rectangle + triangle) with known center of gravity
Considering moments around A,
W.X = w1.x1 + w2.x2
576 x X = (8x1.2)x 24 x (1.2/2) + ½ x 8 x 3.6 x 24 x(1.2+3.6/3 )
X = 1.68 m
L = X+X
L = 1.68 + 0.99 = 2.67 m
w1
w2
G
G2
G1
W
X = ?
a/2 =0.6m
a =1.2m
d =4.8m
1.2+(3.6/3)= 2.4m
A
27. To find the eccentricity,
• e = [L – d/2]
• e = [2.67 – 4.8/2] = 0.27 m
X =1.68m
d =4.8m
1.2+(3.6/3)= 2.4m
a =1.2m
e = 0.27m
N/A
Stress Distribution at base of the dam,
σmin = W/d { 1 – 6e/d }
σmin = 576/4.8 x { 1 – 6 x 0.27/4.8 }
σmin = 79.5 kN/m2
σmax = W/d { 1 + 6e/d }
σmax = 576/4.8 x { 1 + 6 x 0.27/4.8 }
σmax = 160.5 kN/m2
28. σmin = 79.5 kN/m2
σmax = 160.5 kN/m2
Stress ( kN/m2 )
Distance ( m )
4.8 m
Toe
Heel
STRESS DISTRIBUTION DIAGRAM
0
29. • Check the middle third rule,
d =4.8 m
d/3=1.6m
d/6 =0.8m
d/2 =2.4m
A B
A B
K
e=0.27m
L=2.67m
R
d/3=1.6m d/3=1.6m
N/A
d/6 =0.8m
d/6 =0.8m > e=0.27m
Middle third rule satisfied.
1.6 < L=2.67m < 3.2
30. • Check the stability of the dam for Failure Due to Tension & overturning
• Check for Failure Due to Tension in
the base
Check if,
d/3 < L < 2d/3 – No failure
L = 2.67 m
d/3 = 4.8/3 = 1.6m
2d/3 = 2 x 4.8/3 = 3.2m
So,
1.6m < 2.67 m < 3.2m
Resultant force pass through the
middle third section of the base.
So, No failure due to tension
• Check for Failure Due to overturning
Check if,
0< L < d – No failure
L = 2.67 m
d = 4.8 m
So,
0 < 2.67m < 4.8
Resultant force pass within the section of
the base.
So, No failure due to over turning.
31. • If the coefficient of friction between soil and dam base is 0.6, Check the stability of the
dam
considering equilibrium of vertical forces,
R = W
R = 576 KN
Frictional force (f),
f = µR = µw = 0.6 x 576
f = 345.6 kN
But, F = 245 kN/m
So, 345.6 kN > 245 kN/m
If,
f > F
Hence no sliding effect.
Safety factor against water pressure = f/F = 345.6/245 = 1.4
F
f
W
G
R
32. Q2.
A concrete dam has its upstream face vertical & a top width of 3m. Its downstream face
has a uniform batter. It stores water to a depth of 15m with a freeboard of 2 m.
Calculate the minimum dam width(d) at the bottom for no tension in concrete.
ϒw = Specific weight/ unit weight of the water (10kN/ m3 ) (ϒw = ρ wg)
Γ = Unit weight of the dam masonry (25kN/ m3 )
Neglect uplift force.
33. h =15m
F = ?
a =3m
h/3 =5m
Water head
W=?
H =17m
w1
w2
G2
G1
d =? m
10kN/m3
25kN/m3
x
A B
Up stream
2m
x
L
34. Considering a 1 m length of dam,
• F = 1/2. ϒ w .h2
• F = ½ X 10 kN/m3 X 152 m2
• F = 1125 kN/m
• W = [(3+d)/2 X 17 X1]X 25
• W = 212.5(3+d)kN/m
Using force diagram,
• X = F.h/3W
• X = (1125 x 15)/[3 x 212.5(3+d)]
• X = 26.47/(3+d) m
36. To find location of the center of gravity of the dam section (X) , Consider the dam section only &
split in to two shapes (rectangle + triangle) with known center of gravity
Considering moments around A,
W.X = w1.x1 + w2.x2
212.5(3+d)X = (17x3)x 25 x (3/2) + ½ x 17 x (d-3) x 25 x [2+d/3]
1912.5X + 637.5dX = 5737.5 + 212.5d2 + 1275d - 637.5d - 3825
X = [d2 +3d + 9 ]/3(3+d)
L = X+X
L = 26.47/(3+d) + [d2 +3d + 9 ]/3(3+d)
L = [88.41 +d2 + 3d]/ 3(3+d)
37. To find the eccentricity,
• e = [L – d/2]
• e = [88.41 +d2 + 3d]/ 3(3+d) – d/2
• e = [176.82 - d2 – 3d] / (18 + 6d)
• Stress Distribution at base of the dam,
• σmin = W/d { 1 – 6e/d }
• The minimum stress (σMin) must be greater or equal to zero for no tensile stress
at any point along the width of the column.
• σmin >= 0
• W/d { 1 – 6e/d } >= 0
• d/6 >= e
• Minimum d value at,
• d/6 = e
• d = 6e
38. • d/6 = e = [176.82 - d2 – 3d] / (18 + 6d)
• d.(18 + 6d) = [176.82 - d2 – 3d] x 6
• d2 + 3d - 88.41 = 0
• d = 8.21m or d = -11. 021m
• d can’t be a negative value. So,
• d = 8.21m
39. Q3.
A trapezoidal shape concrete dam has a top width of 1m and base width of 7m. It
stores water to a depth of 10m without a freeboard.
i. List out assumptions clearly
ii. Find the total force due to upstream water and point of action
iii. Find the weight of the dam and point of action
iv. Calculate the ecstaticity of the resultant force at the base
v. Check the stability of the dam for Failure Due to Tension & overturning
vi. Find the factor of safety against sliding at the base
vii. Find the maximum and minimum stress at the base
viii. Draw the stress distribution diagram
µ = Friction coefficient between dam base and soil is 0.5
ϒ w = Specific weight/ unit weight of the water (10kN/ m3 ) (ϒ w = ρ wg)
Γ = Unit weight of the dam masonry (20kN/ m3 )
Neglect uplift force.
40. a =1m
h/3 =10/3m
Water head
W=?
h=H =10m
w1
w2
G2
G1
d =7 m
10kN/m3 20kN/m3
A B
Up stream
w3
G3
w4
G4
F = ?
x
R
L x e f
E D C
x1
x2
x3
x4
1m 5m
41. Considering a 1 m length of dam,
• F = 1/2. ϒ w .h2
• F = ½ X 10 kN/m3 X 102 m2
• F = 500 kN/m
• W = Weight of dam + weight of the AED water mass
• W = [(1+7)/2x 10 x 1x 20] + [½ x 10 x 1x1 x 10]
• W = 850kN/m
Using force diagram,
• X = F.h/3W
• X = (500 x 10)/[3 x 850]
• X = 1.96 m
Assumptions
Consider 1 m length of dam.
Neglect up thrust.
Water pressure force at h
depth is equal to any direction.
So consider water force acts
perpendicular to AE line.
Weight of AED section due to
water mass also added to total
weight of the dam.
42. To find location of the center of gravity of the dam section (X) , Consider the dam section only &
split in to four shapes (water trinangle+trinangle+rectangle + triangle) with known center of
gravity.
Considering moments around A,
W.X = w1.x1 + w2.x2 + w3.x3 + w4.x4
850X = (½ x1x10x1)x 10 x (1/3) + (½ x 1x10x1) x20x(2/3) + (1x10x1)x20x(1+0.5) + (½ x1x10x1) x20x(2+5/3)
850X = 16.667 +66.667 + 300 +1833.333
850X = 2216.667
X = 2.607 m
L = X+X
L = 1.96 + 2.607
L = 4.567 m
43. To find the eccentricity,
• e = [L – d/2]
• e = [ 4.567 – 7/2 ]
• e = 1.067m
• To satisfy middle third rule to avoid tension at the dam base,
• d/6 >= e
• But, d/6 = 7/6 = 1.1667m
• 1.1667m > 1.067m
• Dam base satisfy middle third rule, so no tension at the dam base.
44. • Check for Over turning
• If, 0< L < d – No failure( Resultant force pass within the section of the base)
• 0 < 4.567 m < 7m
• So resultant force pass within the section of base, no failure due to overturning
45. Check for Sliding,
considering equilibrium of vertical forces,
R = W
R = 850 KN
Frictional force (f),
f = µR = µw = 0.6 x 850
f = 510 kN
But, F = 500 kN/m
So, 510 kN > 500 kN/m
If,
f > F
Hence no sliding effect.
Safety factor against water pressure = f/F = 510/500 = 1.4
46. Stress Distribution at base of the dam,
σmin = W/d { 1 – 6e/d }
σmin = 850/7 x { 1 – 6 x 1.067/7 }
σmin = 10.37 kN/m2
σmax = W/d { 1 + 6e/d }
σmax = 850/7 x { 1 + 6 x 1.067/7 }
σmax = 232.48 kN/m2
47. σmin = 10.37 kN/m2
σmax = 232.48 kN/m2
Stress ( kN/m2 )
Distance ( m )
7 m
Toe
Heel
STRESS DISTRIBUTION DIAGRAM
0
48. Q4. Calculate the stresses of dam base for water level at D-C
a =0.8m
Water head
W=?
0.5m
w1
w2
G2
G1
d =1.4 m
10kN/m3
20kN/m3
Up stream
F = ?
R
L
f
x1
x2
B
D C
A
0.6m
0.5m
H=h=1m
x
w3
G3
w4
G4
x3
x4
0.2m
0.2m
x
e
E
I J
K
M
49. Considering a 1 m length of dam,
• F = 1/2. ϒ w .h2
• F = ½ X 10 kN/m3 X 12 m2
• F = 5kN/m
• W = Weight of dam + weight of the AEDIJM water mass
• W = [0.8x 1 x 1x 20]+[0.6x0.5x1x20] + [ 0.2x
1x1 x 10] + [0.6x0.5x1x10]
• W = (16+6+2+3) = 27kN/m
Using force diagram,
• X = F.h/3W
• X = (5x 1)/[3 x 27]
• X = 0.0617 m
Assumptions
Consider 1 m length of dam.
Neglect up thrust.
Water pressure force at h
depth is equal to any direction.
So consider water force acts
perpendicular to dam.
Weight of AEDIJM section due
to water mass also added to
total weight of the dam.
50. To find location of the center of gravity of the dam section (X) , Consider the dam section only &
split in to four shapes (water trinangle+trinangle+rectangle + triangle) with known center of
gravity.
Considering moments around A,
W.X = w1.x1 + w2.x2 + w3.x3 + w4.x4
27X = (0.2x1x1)x 10 x (0.2/2) + (0.6x0.5x1) x10x[0.2+(0.6/2)] + (0.6x0.5x1)x20x[0.2+(0.6/2)] + (1x0.8x1)
x20x[0.2+0.6+(0.8/2)]
27X = 0.2 + 4.5 + 3 + 19.2
27X = 26.9
X = 26.9/27
X = 0.996 m
L = X+X
L = 0.0617 + 0.996
L = 1.057 m
51. To find the eccentricity,
• e = [L – d/2]
• e = [ 1.057 – 1.4/2 ]
• e = 0.3579m
• To satisfy middle third rule to avoid tension at the dam base,
• d/6 >= e
• But, d/6 = 7/6 = 0.233m
• 0.233m < 0.3579m
• Dam base satisfy doesn't middle third rule, so tension will built up at the dam
base.
52. • Check for Over turning
• If, 0< L < d – No failure( Resultant force pass within the section of the base)
• 0 < 1.057 m < 1.4m
• So resultant force pass within the section of base, no failure due to overturning
53. Check for Sliding,
considering equilibrium of vertical forces,
R = W
R = 27KN
Frictional force (f),
f = µR = µw = 0.6 x 27
f = 16.2 kN
But, F = 5 kN/m
So, 16.2 kN > 5 kN/m
If,
f > F
Hence no sliding effect.
Safety factor against water pressure = f/F =16.2/5 = 3.24
54. Stress Distribution at base of the dam,
σmin = W/d { 1 – 6e/d }
σmin = 27/71.4 x { 1 – 6 x 0.3579/1.4 }
σmin = -10.29 kN/m2
σmax = W/d { 1 + 6e/d }
σmax = 27/1.4 x { 1 + 6 x0.3579 /1.4 }
σmax = 48.86 kN/m2
55. σmin = -10.29 kN/m2
σmax = 48.86 kN/m2
Stress ( kN/m2 )
Distance ( m )
1.4 m
Toe
Heel
STRESS DISTRIBUTION DIAGRAM
0