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CEL351: Design of Hydraulic Structures
CEL351: Design of Hydraulic Structures
GRAVITY DAMS
GRAVITY DAMS
ƒA gravity dam is a solid structure, made of concrete or
masonry, constructed across a river to create a reservoir on its
upstream
ƒThe section of the gravity dam is approximately triangular in
shape, with its apex at its top and maximum width at bottom.
ƒ The section is so proportioned that it resists the various forces
acting on it by its own weight.
ƒ are usually consist of two sections; namely, the non-overflow
section and the overflow section or spillway section.
ƒ are particularly suited across gorges with very steep side slopes
where earth dams might slip and are usually cheaper than earth
dams if suitable soils are not available for their construction.
ƒWhere good foundations are available, gravity dams can be
built upto any height. It is the most permanent one, and requires
little maintenance. The most ancient gravity, dam on record was
built in Egypt more than 400 years B.C. of uncemented masonry.
GRAVITY DAMS
GRAVITY DAMS
1. Axis of the dam: is the line of the upstream edge of the top (or
crown) of the dam. The axis of the dam in plan is also called the
base line of the dam. The axis of the dam in plan is usually
straight.
2. Length of the dam: is the distance from one abutment to the
other, measured along the axis of the dam at the level of the top
of the dam.
3. Structural height of the dam: is the difference in elevations of
the top of the dam and the lowest point in the excavated
foundation. It, however, does not include the depth of special
geological features of foundations such as narrow fault zones
below the foundation. In general, the height of the dam means its
structural height.
Basic Definitions
GRAVITY DAMS
GRAVITY DAMS
4. Toe and Heel: The toe of the dam is the downstream edge of
the base, and the heel is the upstream edge of the base.
5. Maximum base width of the dam: is the maximum horizontal
distance between the heel and the toe of the maximum section of
the dam in the middle of the valley.
6. Hydraulic height of the dam: is equal to the difference in
elevations of the highest controlled water surface on the
upstream of the dam (i. e. FRL) and the lowest point in the river
bed
Basic Definitions
GRAVITY DAMS
GRAVITY DAMS
GRAVITY DAMS
GRAVITY DAMS
1. Weight of the dam
2. Water pressure
3. Uplift pressure
4. Wave pressure
5. Earth and Silt pressure
6. Earthquake forces
7. Ice pressure
8. Wind pressure
9. Thermal loads.
Forces Acting on a Gravity Dam
GRAVITY DAMS
GRAVITY DAMS
These forces fall into two categories as:
a)Forces, such as weight of the dam and water pressure, which
are directly calculable from the unit weights of the materials and
properties of fluid pressures; and
b)Forces, such as uplift, earthquake loads, silt pressure and ice
pressure, which can only be assumed on the basis of assumption
of varying degree of reliability.
It is in the estimating of the second category of the forces that
special care has to be taken and reliance placed on available
data, experience, and judgment.
It is convenient to compute all the forces per unit length of the
dam
Forces Acting on a Gravity Dam
GRAVITY DAMS
GRAVITY DAMS
9 Main stabilizing force in a gravity dam
9 Dead load = weight of concrete or masonry or both + weight of
such appurtenances as piers, gates and bridges.
9 Weight of the dam per unit length is equal to the product of the
area of cross-section of the dam and the specific weight (or unit
weight) of the material.
9 Unit weight of concrete (24 kN/m3) and masonry (23 kN/m3)
varies considerably depending upon the various materials that
go to make them.
9 For convenience, the cross-section of the dam is divided into
simple geometrical shapes, such as rectangles and triangles, for
the computation of weights. The areas and controids of these
shapes can be easily determined. Thus the weight components
W1, W2, W3 etc. can be found along with their lines of action.
The total weight W of the dam acts at the C.G. of its section
Weight of Dam
GRAVITY DAMS
GRAVITY DAMS
Weight of Dam
W3
W2
W1
GRAVITY DAMS
GRAVITY DAMS
Water pressure on the upstream face is the main destabilizing
(or overturning) force acting on a gravity dam.
Tail water pressure helps in the stability.
Although the weight of water varies slightly with temp., the
variation is usually ignored. Unit Mass of water is taken as 1000
kg/m3 and specific weight = 10 kN/m3 instead of 9.81 kN/m3.
The water pressure always acts normal to the face of dam.
It is convenient to determine the components of the forces in the
horizontal and vertical directions instead of the total force on
the inclined surface directly.
Water Pressure (Reservoir and Tail Water Loads
GRAVITY DAMS
GRAVITY DAMS
Water Pressure (Reservoir and Tail Water Loads
The water pressure
intensity p (kN/m2)
varies linearly with the
depth of the water
measured below the
free surface y (m) and is
expressed as
y
p w
γ
=
GRAVITY DAMS
GRAVITY DAMS
Water Pressure (Reservoir and Tail Water Loads
U/s face vertical: When the upstream face of the dam is
vertical, the water pressure diagram is triangular in shape
with a pressure intensity of γwh at the base, where h is the
depth of water. The total water pressure per unit length is
horizontal and is given by
It acts horizontally at a height of h/3 above the base of the
dam.
2
2
1
h
P w
H γ
=
GRAVITY DAMS
GRAVITY DAMS
Water Pressure (Reservoir and Tail Water Loads
U/s face inclined: When the upstream face ABC is either
inclined or partly vertical and partly inclined, the force due to
water pressure can be calculated in terms of the horizontal
component PH and the vertical component PV. The horizontal
component is given as earlier and acts horizontal at a height of
(h/3) above the base. The vertical component PV of water
pressure per unit length is equal to the weight of the water in
the prism ABCD per unit length. For convenience, the weight
of water is found in two parts PV1 and PV2 by dividing the
trapezium ABCD into a rectangle BCDE and a triangle ABE.
Thus the vertical component PV = PV1 + PV2 = weight of water
in BCDE + weight of water in ABE. The lines of action of PV1
and PV2 will pass through the respective centroids of the
rectangle and triangle.
GRAVITY DAMS
GRAVITY DAMS
Uplift Pressure
ƒWater has a tendency to seep through the pores and fissures of
the material in the body of the dam and foundation material,
and through the joints between the body of the dam and its
foundation at the base. The seeping water exerts pressure.
ƒThe uplift pressure is defined as the upward pressure of water
as it flows or seeps through the body of dam or its foundation.
ƒA portion of the weight of the dam will be supported on the
upward pressure of water; hence net foundation reaction due to
vertical force will reduce.
ƒThe area over which the uplift pressure acts has been a
question of investigation from the early part of this century.
ƒ One school of thought recommends that a value one-third to
two-thirds of the area should be considered as effective over
which the uplift acts.
GRAVITY DAMS
GRAVITY DAMS
Uplift Pressure
The second school of thought, recommend that the effective
area may be taken approximately equal to the total area.
Code of Indian Standards (IS : 6512-1984):
¾There are two constituent elements in uplift pressure: the area
factor or the percentage of area on which uplift acts and the
intensity factor or the ratio which the actual intensity of uplift
pressure bears to the intensity gradient extending from head
water to tail water at various points.
¾The total area should be considered as effective to account for
uplift.
¾The pressure gradient shall then be extending linearly to
heads corresponding to reservoir level and tailwater level.
GRAVITY DAMS
GRAVITY DAMS
Uplift Pressure
Code of Indian Standards (IS : 6512-1984):
¾In case of drain holes: the uplift pressure at the line of drains
exceeds the tailwater pressure by one-third the differential
between the reservoir and tailwater heads. The pressure
gradient shall then be extended linearly to heads corresponding
to reservoir level and tailwater level.
¾In case of a crack: The uplift is assumed to be the reservoir
pressure from the u/s face to the end of the crack and from
there to vary linearly to the tailwater or drain pressure.
¾In absence of line of drains and for the extreme loading
conditions F and G, the uplift shall be taken as varying linearly
from the appropriate reservoir water pressure at the u/s face to
the appropriate tailwater pressure at the d/s face.
¾ Uplift pressures are not affected by earthquakes.
GRAVITY DAMS
GRAVITY DAMS
Uplift Pressure
GRAVITY DAMS
GRAVITY DAMS
Earth and Silt Pressure
ƒGravity dams are subjected to earth pressures on the
downstream and upstream faces where the foundation trench is
to be backfilled. Except in the abutment sections in specific
cases, earth pressures have usually a minor effect on the
stability of the structure and may be ignored.
ƒ Silt is treated as a saturated cohesionless soil having full uplift
and whose value of internal friction is not materially changed
on account of submergence.
ƒ IS code recommends that a) Horizontal silt and water
pressure is assumed to be equivalent to that of a fluid with a
mass of 1360 kg/m3, and b) Vertical silt and water pressure is
determined as if silt and water together have a density of 1925
kg/m3.
GRAVITY DAMS
GRAVITY DAMS
Earth and Silt Pressure
GRAVITY DAMS
GRAVITY DAMS
Ice Pressure
9Ice expands and contracts with changes in temperature.
9In a reservoir completely frozen over, a drop in the air
temperature or in the level of the reservoir water may cause the
opening up of cracks which subsequently fill with water and
freezed solid. When the next rise in temperature occurs, the ice
expands and, if restrained, it exerts pressure on the dam.
9Good analytical procedures exist for computing ice pressures,
but the accuracy of results is dependent upon certain physical
data which have not been adequately determined.
9Ice pressure may be provided for at the rate of 250 kPa
applied to the face of dam over the anticipated area of contact
of ice with the face of dam.
9The problem of ice pressure in the design of dam is not
encountered in India except, perhaps, in a few localities.
GRAVITY DAMS
GRAVITY DAMS
Wind Pressure
9Wind pressure does exist but is seldom a significant factor in
the design of a dam.
9Wind loads may, therefore, be ignored.
Thermal Load
9The cyclic variation of air temperature and the solar radiation
on the downstream side and the reservoir temperature on the
upstream side affect the stresses in the dam.
9Even the deflection of the dam is maximum in the morning
and it goes on reducing to a minimum value in the evening.
9Measures for temperature control of concrete in solid gravity
dams are adopted during construction.
9 Thermal are not significant in gravity dams and may be
ignored.
GRAVITY DAMS
GRAVITY DAMS
Wave Pressure
9The upper portions of dams are subject to the impact of
waves.
9Wave pressure against massive dams of appreciable height is
usually of little consequence.
9The force and dimensions of waves depend mainly on the
extent and configuration of the water surface, the velocity of
wind and the depth of reservoir water.
9The height of wave is generally more important in the
determination of the free board requirements of dams to
prevent overtopping by wave splash.
9 An empirical method has been recommended by T. Saville
for computation of wave height hw (m), which takes into account
the effect of the shape of reservoir and wind velocity over water
surface rather than on land by applying necessary correction.
GRAVITY DAMS
GRAVITY DAMS
Wave Pressure
9 Wind velocity of 120 km/h over water in case of normal pool
condition and of 80 km/h over water in case of maximum
reservoir condition should generally be assumed for calculation
of wave height if meteorological data is not available.
9Sometimes the following Molitor’s empirical formulae are
used to estimate wave height
for F < 32 km
for F > 32 km
where Vw = wind velocity in km/hr and F = fetch length of
reservoir in km.
4
/
1
)
(
271
.
0
763
.
0
032
.
0 F
F
V
h w
w −
+
=
F
V
h w
w 032
.
0
=
GRAVITY DAMS
GRAVITY DAMS
Wave Pressure
9Wave pressure diagrams can be approx by triangle l-2-3
w
w h
p 24
=
9Max pressure pw in
kPa occurs at 0.125
hw, above the still
water level and is
given by
9The total wave force
Pw, (in kN) is given by
the area of triangle
2
20 w
w h
P =
GRAVITY DAMS
GRAVITY DAMS
Earthquake Forces
9An earthquake sets random vibrations (waves) in the earth's
crust, which can be resolved in any three mutually
perpendicular directions. This motion causes the structure to
vibrate.
9The waves impart accelerations to the foundations under the
dam and causes its movement.
9Acceleration introduces an inertia force in the body of dam
and sets up stresses initially in lower layers and gradually in the
whole body of the dam.
9The vibration intensity of ground expected at any location
depends upon the magnitude of earthquake, the depth of focus,
distance from the epicentre and the strata on which the
structure stands.
GRAVITY DAMS
GRAVITY DAMS
Earthquake Forces
9 The response of the structure to the ground vibration is a
function of the nature of foundation soil; materials, form, size
and mode of construction of the structure; and the duration and
the intensity of ground motion.
9 Earthquake causes impulsive ground motion which is
complex and irregular in character, changing in period and
amplitude each lasting for small duration.
9 Earthquake is not likely to occur simultaneously with wind or
maximum flood or maximum sea waves.
9 The value of elastic modulus of materials, wherever required,
may be taken as for static analysis unless a more definite value
is available for use in such condition.
9Whenever earthquake forces are considered along with other
normal design forces, the permissible stresses in materials, in
the elastic method of design, may be increased by one-third.
GRAVITY DAMS
GRAVITY DAMS
Earthquake Forces
For the purpose of
determining the
seismic forces, the
country is classified
into five zones
GRAVITY DAMS
GRAVITY DAMS
Earthquake Forces
9The earthquake force experienced by a structure depends on
its own dynamic characteristics in addition to those of the
ground motion.
9 Response spectrum method takes into account these
characteristics and is recommended for use in case where it is
desired to take such effects into account.
9 IS:1893 - 1984 code specifies design criteria under
earthquake condition.
9As per IS Code, for dams up to 100 m height, the seismic
coefficient method shall be used for the design of the dams;
while for dams over 100 m height the response spectrum
method shall be used.
GRAVITY DAMS
GRAVITY DAMS
Earthquake Forces
9Basic seismic coefficients (α0) and seismic zone factors (F0) in
different zones shall be taken as given in Table. The design
seismic forces shall be computed on the basis of importance of
the structure I (Table) and its soil-foundation system β (Table).
9In Seismic Coefficient Method the design value of horizontal
seismic coefficient (αh) shall be computed as
In response Spectrum Method the response acceleration
coefficient is first obtained for the natural period and damping
of the structure and the design value of horizontal seismic
coefficient (αh) shall be computed using
0
α
β
α I
h =
g
S
IF a
h 0
β
α =
GRAVITY DAMS
GRAVITY DAMS
Earthquake Forces
GRAVITY DAMS
GRAVITY DAMS
Earthquake Forces
GRAVITY DAMS
GRAVITY DAMS
Earthquake Forces
GRAVITY DAMS
GRAVITY DAMS
Earthquake Forces
9Basic seismic coefficients (α0) and seismic zone factors (F0) in
different zones shall be taken as given in Table. The design
seismic forces shall be computed on the basis of importance of
the structure I (Table) and its soil-foundation system β (Table).
9In Seismic Coefficient Method the design value of horizontal
seismic coefficient (αh) shall be computed as
In response Spectrum Method the response acceleration
coefficient is first obtained for the natural period and damping
of the structure and the design value of horizontal seismic
coefficient (αh) shall be computed using
0
α
β
α I
h =
g
S
IF a
h 0
β
α =
GRAVITY DAMS
GRAVITY DAMS
Earthquake Forces
where Sa/g = average acceleration coefficient as read from Fig
for a damping of 5 percent and fundamental period of
vibration of the dam corresponding to
where H = height of the dam in m, B = base width of the dam in
m, γm = unit weight of the material of dam in N/m3, g =
acceleration due to gravity in m/s2, and Em, = modulus of
elasticity of the material in N/m2. Where a number of modes are
to be considered for seismic analysis αh shall be worked out
corresponding to the various mode periods and dampings and
then design forces shall be computed. If actual response spectra
is available then the same may be used directly instead of the
above equation.
m
m
gE
B
H
T
γ
2
55
.
5
=
GRAVITY DAMS
GRAVITY DAMS
Earthquake Forces
GRAVITY DAMS
GRAVITY DAMS
Earthquake Forces
Inertia forces: The inertia force acts in a direction opposite to
the acceleration imparted by, earthquake forces and is equal to
the product of the mass of the dam and the acceleration. For
dams up to 100 m height the horizontal seismic coefficient shall
be taken as 1.5 times seismic coefficient αh at the top of the dam
reducing linearly to zero at the base. This inertia force shall be
assumed to act from upstream to downstream or downstream to
upstream to get the worst combination for design. It causes an
overturning moment about the horizontal section adding to that
caused by hydrodynamic force.
Effect of Horizontal Acceleration: causes
two forces: (1) Inertia force in the body of
the dam, and (2) Hydrodynamic pressure of
water.
GRAVITY DAMS
GRAVITY DAMS
Earthquake Forces
where W = total weight of the masonry or concrete in the dam
in N, and = height of the centre of gravity of the dam above the
base in m. For any horizontal section at a depth y below top of
the dam shear force, Vy, and bending moment My, may be
obtained as follows
For dams over 100 m height the response spectrum method
shall be used. The base shear, VB and base moment MB may
be obtained by the following formulae:
h
B
h
B h
W
M
W
V α
α 9
.
0
6
.
0 =
=
B
m
y
B
v
y M
C
M
V
C
V '
'
=
=
GRAVITY DAMS
GRAVITY DAMS
Earthquake Forces
GRAVITY DAMS
GRAVITY DAMS
Earthquake Forces
where pey = hydrodynamic pressure intensity (Pa) at depth y, h
= depth of reservoir (m) and Cs = coefficient which varies with
shapes of u/s face and depth of water.
Hydrodynamic forces: Due to horizontal acceleration of the
foundation and dam there is an instantaneous hydrodynamic
pressure (or suction) exerted against the dam in addition to
hydrostatic forces. The direction of hydrodynamic force is
opposite to the direction of earthquake acceleration. Zanger
presented formulae based on electrical analogy and with
assumption that water is incompressible. The pressure variation
is elliptical-cum-parabolic. The hydrodynamic pressure at
depth y below the reservoir surface shall be determined as
follows h
C
p w
h
s
ey γ
α
=
GRAVITY DAMS
GRAVITY DAMS
Earthquake Forces
GRAVITY DAMS
GRAVITY DAMS
Earthquake Forces
where Cm = maximum value of Cs, which can be read from Fig.
or obtained from
Approximate values of Cs, for dams with vertical or constant
upstream slopes may be obtained as follows
⎪
⎭
⎪
⎬
⎫
⎪
⎩
⎪
⎨
⎧
⎟
⎠
⎞
⎜
⎝
⎛
−
+
⎟
⎠
⎞
⎜
⎝
⎛
−
=
h
y
h
y
h
y
h
y
C
C m
s 2
2
2
⎟
⎠
⎞
⎜
⎝
⎛
−
=
90
1
735
.
0
θ
m
C
where θ = angle, in degrees the u/s face of the dam makes with
vertical. If the height of the vertical portion of u/s face is equal to
or greater than one-half the total height of the dam, analyze it as
if vertical throughout. Otherwise use a sloping line connecting
the point of intersection of u/s face and the reservoir surface with
the heel.
GRAVITY DAMS
GRAVITY DAMS
Earthquake Forces
GRAVITY DAMS
GRAVITY DAMS
Earthquake Forces
Similarly, the moment of pressure about the joint upto which
the pressure is taken is given by half the sum of the moments of
the quarter ellipse and semi-parabola. Hence
The total pressure at depth y may be found by integrating the
pressure curve above that plane. Taking the pressure variation
to be elliptical-cum-parabolic, the total pressure at depth y will
be equal to the average of the areas of the quarter ellipse and
semi parabola. Hence
where Pey = hydrodynamic shear in N/m at any depth y, and Mey
= moment in N.m/m due to hydrodynamic force at any depth y.
y
p
y
p
y
p
P ey
ey
ey
ey 727
.
0
3
2
4
2
1
=
⎟
⎠
⎞
⎜
⎝
⎛
+
=
π
2
2
299
.
0
15
4
3
1
2
1
5
2
3
2
3
4
4
2
1
y
p
y
p
y
y
p
y
y
p
M ey
ey
ey
ey
ey =
⎟
⎠
⎞
⎜
⎝
⎛
+
=
⎟
⎠
⎞
⎜
⎝
⎛
×
+
×
=
π
π
GRAVITY DAMS
GRAVITY DAMS
Earthquake Forces
where PeV = increase (or decrease) in vertical component of load
due to hydrodynamic force, Pey2 = total horizontal component of
hydrodynamic force at elevation of the section being considered,
Pey1 = total horizontal component of hydrodynamic force at the
elevation at which the slope of dam face commences, and θ =
angle between the face of dam and the vertical. Moment due to
vertical component of reservoir and tail water load may be
obtained by determining lever arm from centroid of pressure dia.
Effect of Horizontal Acceleration on the Vertical Component of
Reservoir and Tail Water Load: Since the hydrodynamic
pressure (or suction) acts normal to the face of the dam, there
shall be a vertical component of this force if the face of the dam
against which it is acting is sloping, the magnitude at any
horizontal section being
( ) θ
tan
1
2 ey
ey
eV P
P
P −
=
GRAVITY DAMS
GRAVITY DAMS
Earthquake Forces
Effect of Vertical Acceleration: The effect of vertical
earthquake acceleration is to change the unit weight of water
and concrete or masonry. Acceleration upwards increases the
weight and acceleration downwards decreases the weight. Due
to vertical acceleration a vertical inertia force F = αVW is
exerted on the dam, in the direction opposite to that of the
acceleration. When the acceleration is vertically upwards, the
inertia force F = αVW acts vertically downwards, thus
increasing momentarily the downward weights. When the
acceleration is vertically downwards the inertia force F = αVW
acts upwards and decreases momentarily the downward weight.
For methods of design (seismic coefficient up to 100 m and
response spectrum over 100 m) Vertical seismic coefficient (αV)
shall be taken as 0.75 times the value of αh (of the respective
method) at the top of the dam reducing linearly to zero at the
base
Fdocuments.in gravity dams-ppt

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Fdocuments.in gravity dams-ppt

  • 1. CEL351: Design of Hydraulic Structures CEL351: Design of Hydraulic Structures
  • 2. GRAVITY DAMS GRAVITY DAMS ƒA gravity dam is a solid structure, made of concrete or masonry, constructed across a river to create a reservoir on its upstream ƒThe section of the gravity dam is approximately triangular in shape, with its apex at its top and maximum width at bottom. ƒ The section is so proportioned that it resists the various forces acting on it by its own weight. ƒ are usually consist of two sections; namely, the non-overflow section and the overflow section or spillway section. ƒ are particularly suited across gorges with very steep side slopes where earth dams might slip and are usually cheaper than earth dams if suitable soils are not available for their construction. ƒWhere good foundations are available, gravity dams can be built upto any height. It is the most permanent one, and requires little maintenance. The most ancient gravity, dam on record was built in Egypt more than 400 years B.C. of uncemented masonry.
  • 3. GRAVITY DAMS GRAVITY DAMS 1. Axis of the dam: is the line of the upstream edge of the top (or crown) of the dam. The axis of the dam in plan is also called the base line of the dam. The axis of the dam in plan is usually straight. 2. Length of the dam: is the distance from one abutment to the other, measured along the axis of the dam at the level of the top of the dam. 3. Structural height of the dam: is the difference in elevations of the top of the dam and the lowest point in the excavated foundation. It, however, does not include the depth of special geological features of foundations such as narrow fault zones below the foundation. In general, the height of the dam means its structural height. Basic Definitions
  • 4. GRAVITY DAMS GRAVITY DAMS 4. Toe and Heel: The toe of the dam is the downstream edge of the base, and the heel is the upstream edge of the base. 5. Maximum base width of the dam: is the maximum horizontal distance between the heel and the toe of the maximum section of the dam in the middle of the valley. 6. Hydraulic height of the dam: is equal to the difference in elevations of the highest controlled water surface on the upstream of the dam (i. e. FRL) and the lowest point in the river bed Basic Definitions
  • 6. GRAVITY DAMS GRAVITY DAMS 1. Weight of the dam 2. Water pressure 3. Uplift pressure 4. Wave pressure 5. Earth and Silt pressure 6. Earthquake forces 7. Ice pressure 8. Wind pressure 9. Thermal loads. Forces Acting on a Gravity Dam
  • 7. GRAVITY DAMS GRAVITY DAMS These forces fall into two categories as: a)Forces, such as weight of the dam and water pressure, which are directly calculable from the unit weights of the materials and properties of fluid pressures; and b)Forces, such as uplift, earthquake loads, silt pressure and ice pressure, which can only be assumed on the basis of assumption of varying degree of reliability. It is in the estimating of the second category of the forces that special care has to be taken and reliance placed on available data, experience, and judgment. It is convenient to compute all the forces per unit length of the dam Forces Acting on a Gravity Dam
  • 8. GRAVITY DAMS GRAVITY DAMS 9 Main stabilizing force in a gravity dam 9 Dead load = weight of concrete or masonry or both + weight of such appurtenances as piers, gates and bridges. 9 Weight of the dam per unit length is equal to the product of the area of cross-section of the dam and the specific weight (or unit weight) of the material. 9 Unit weight of concrete (24 kN/m3) and masonry (23 kN/m3) varies considerably depending upon the various materials that go to make them. 9 For convenience, the cross-section of the dam is divided into simple geometrical shapes, such as rectangles and triangles, for the computation of weights. The areas and controids of these shapes can be easily determined. Thus the weight components W1, W2, W3 etc. can be found along with their lines of action. The total weight W of the dam acts at the C.G. of its section Weight of Dam
  • 10. GRAVITY DAMS GRAVITY DAMS Water pressure on the upstream face is the main destabilizing (or overturning) force acting on a gravity dam. Tail water pressure helps in the stability. Although the weight of water varies slightly with temp., the variation is usually ignored. Unit Mass of water is taken as 1000 kg/m3 and specific weight = 10 kN/m3 instead of 9.81 kN/m3. The water pressure always acts normal to the face of dam. It is convenient to determine the components of the forces in the horizontal and vertical directions instead of the total force on the inclined surface directly. Water Pressure (Reservoir and Tail Water Loads
  • 11. GRAVITY DAMS GRAVITY DAMS Water Pressure (Reservoir and Tail Water Loads The water pressure intensity p (kN/m2) varies linearly with the depth of the water measured below the free surface y (m) and is expressed as y p w γ =
  • 12. GRAVITY DAMS GRAVITY DAMS Water Pressure (Reservoir and Tail Water Loads U/s face vertical: When the upstream face of the dam is vertical, the water pressure diagram is triangular in shape with a pressure intensity of γwh at the base, where h is the depth of water. The total water pressure per unit length is horizontal and is given by It acts horizontally at a height of h/3 above the base of the dam. 2 2 1 h P w H γ =
  • 13. GRAVITY DAMS GRAVITY DAMS Water Pressure (Reservoir and Tail Water Loads U/s face inclined: When the upstream face ABC is either inclined or partly vertical and partly inclined, the force due to water pressure can be calculated in terms of the horizontal component PH and the vertical component PV. The horizontal component is given as earlier and acts horizontal at a height of (h/3) above the base. The vertical component PV of water pressure per unit length is equal to the weight of the water in the prism ABCD per unit length. For convenience, the weight of water is found in two parts PV1 and PV2 by dividing the trapezium ABCD into a rectangle BCDE and a triangle ABE. Thus the vertical component PV = PV1 + PV2 = weight of water in BCDE + weight of water in ABE. The lines of action of PV1 and PV2 will pass through the respective centroids of the rectangle and triangle.
  • 14. GRAVITY DAMS GRAVITY DAMS Uplift Pressure ƒWater has a tendency to seep through the pores and fissures of the material in the body of the dam and foundation material, and through the joints between the body of the dam and its foundation at the base. The seeping water exerts pressure. ƒThe uplift pressure is defined as the upward pressure of water as it flows or seeps through the body of dam or its foundation. ƒA portion of the weight of the dam will be supported on the upward pressure of water; hence net foundation reaction due to vertical force will reduce. ƒThe area over which the uplift pressure acts has been a question of investigation from the early part of this century. ƒ One school of thought recommends that a value one-third to two-thirds of the area should be considered as effective over which the uplift acts.
  • 15. GRAVITY DAMS GRAVITY DAMS Uplift Pressure The second school of thought, recommend that the effective area may be taken approximately equal to the total area. Code of Indian Standards (IS : 6512-1984): ¾There are two constituent elements in uplift pressure: the area factor or the percentage of area on which uplift acts and the intensity factor or the ratio which the actual intensity of uplift pressure bears to the intensity gradient extending from head water to tail water at various points. ¾The total area should be considered as effective to account for uplift. ¾The pressure gradient shall then be extending linearly to heads corresponding to reservoir level and tailwater level.
  • 16. GRAVITY DAMS GRAVITY DAMS Uplift Pressure Code of Indian Standards (IS : 6512-1984): ¾In case of drain holes: the uplift pressure at the line of drains exceeds the tailwater pressure by one-third the differential between the reservoir and tailwater heads. The pressure gradient shall then be extended linearly to heads corresponding to reservoir level and tailwater level. ¾In case of a crack: The uplift is assumed to be the reservoir pressure from the u/s face to the end of the crack and from there to vary linearly to the tailwater or drain pressure. ¾In absence of line of drains and for the extreme loading conditions F and G, the uplift shall be taken as varying linearly from the appropriate reservoir water pressure at the u/s face to the appropriate tailwater pressure at the d/s face. ¾ Uplift pressures are not affected by earthquakes.
  • 18. GRAVITY DAMS GRAVITY DAMS Earth and Silt Pressure ƒGravity dams are subjected to earth pressures on the downstream and upstream faces where the foundation trench is to be backfilled. Except in the abutment sections in specific cases, earth pressures have usually a minor effect on the stability of the structure and may be ignored. ƒ Silt is treated as a saturated cohesionless soil having full uplift and whose value of internal friction is not materially changed on account of submergence. ƒ IS code recommends that a) Horizontal silt and water pressure is assumed to be equivalent to that of a fluid with a mass of 1360 kg/m3, and b) Vertical silt and water pressure is determined as if silt and water together have a density of 1925 kg/m3.
  • 19. GRAVITY DAMS GRAVITY DAMS Earth and Silt Pressure
  • 20. GRAVITY DAMS GRAVITY DAMS Ice Pressure 9Ice expands and contracts with changes in temperature. 9In a reservoir completely frozen over, a drop in the air temperature or in the level of the reservoir water may cause the opening up of cracks which subsequently fill with water and freezed solid. When the next rise in temperature occurs, the ice expands and, if restrained, it exerts pressure on the dam. 9Good analytical procedures exist for computing ice pressures, but the accuracy of results is dependent upon certain physical data which have not been adequately determined. 9Ice pressure may be provided for at the rate of 250 kPa applied to the face of dam over the anticipated area of contact of ice with the face of dam. 9The problem of ice pressure in the design of dam is not encountered in India except, perhaps, in a few localities.
  • 21. GRAVITY DAMS GRAVITY DAMS Wind Pressure 9Wind pressure does exist but is seldom a significant factor in the design of a dam. 9Wind loads may, therefore, be ignored. Thermal Load 9The cyclic variation of air temperature and the solar radiation on the downstream side and the reservoir temperature on the upstream side affect the stresses in the dam. 9Even the deflection of the dam is maximum in the morning and it goes on reducing to a minimum value in the evening. 9Measures for temperature control of concrete in solid gravity dams are adopted during construction. 9 Thermal are not significant in gravity dams and may be ignored.
  • 22. GRAVITY DAMS GRAVITY DAMS Wave Pressure 9The upper portions of dams are subject to the impact of waves. 9Wave pressure against massive dams of appreciable height is usually of little consequence. 9The force and dimensions of waves depend mainly on the extent and configuration of the water surface, the velocity of wind and the depth of reservoir water. 9The height of wave is generally more important in the determination of the free board requirements of dams to prevent overtopping by wave splash. 9 An empirical method has been recommended by T. Saville for computation of wave height hw (m), which takes into account the effect of the shape of reservoir and wind velocity over water surface rather than on land by applying necessary correction.
  • 23. GRAVITY DAMS GRAVITY DAMS Wave Pressure 9 Wind velocity of 120 km/h over water in case of normal pool condition and of 80 km/h over water in case of maximum reservoir condition should generally be assumed for calculation of wave height if meteorological data is not available. 9Sometimes the following Molitor’s empirical formulae are used to estimate wave height for F < 32 km for F > 32 km where Vw = wind velocity in km/hr and F = fetch length of reservoir in km. 4 / 1 ) ( 271 . 0 763 . 0 032 . 0 F F V h w w − + = F V h w w 032 . 0 =
  • 24. GRAVITY DAMS GRAVITY DAMS Wave Pressure 9Wave pressure diagrams can be approx by triangle l-2-3 w w h p 24 = 9Max pressure pw in kPa occurs at 0.125 hw, above the still water level and is given by 9The total wave force Pw, (in kN) is given by the area of triangle 2 20 w w h P =
  • 25. GRAVITY DAMS GRAVITY DAMS Earthquake Forces 9An earthquake sets random vibrations (waves) in the earth's crust, which can be resolved in any three mutually perpendicular directions. This motion causes the structure to vibrate. 9The waves impart accelerations to the foundations under the dam and causes its movement. 9Acceleration introduces an inertia force in the body of dam and sets up stresses initially in lower layers and gradually in the whole body of the dam. 9The vibration intensity of ground expected at any location depends upon the magnitude of earthquake, the depth of focus, distance from the epicentre and the strata on which the structure stands.
  • 26. GRAVITY DAMS GRAVITY DAMS Earthquake Forces 9 The response of the structure to the ground vibration is a function of the nature of foundation soil; materials, form, size and mode of construction of the structure; and the duration and the intensity of ground motion. 9 Earthquake causes impulsive ground motion which is complex and irregular in character, changing in period and amplitude each lasting for small duration. 9 Earthquake is not likely to occur simultaneously with wind or maximum flood or maximum sea waves. 9 The value of elastic modulus of materials, wherever required, may be taken as for static analysis unless a more definite value is available for use in such condition. 9Whenever earthquake forces are considered along with other normal design forces, the permissible stresses in materials, in the elastic method of design, may be increased by one-third.
  • 27. GRAVITY DAMS GRAVITY DAMS Earthquake Forces For the purpose of determining the seismic forces, the country is classified into five zones
  • 28. GRAVITY DAMS GRAVITY DAMS Earthquake Forces 9The earthquake force experienced by a structure depends on its own dynamic characteristics in addition to those of the ground motion. 9 Response spectrum method takes into account these characteristics and is recommended for use in case where it is desired to take such effects into account. 9 IS:1893 - 1984 code specifies design criteria under earthquake condition. 9As per IS Code, for dams up to 100 m height, the seismic coefficient method shall be used for the design of the dams; while for dams over 100 m height the response spectrum method shall be used.
  • 29. GRAVITY DAMS GRAVITY DAMS Earthquake Forces 9Basic seismic coefficients (α0) and seismic zone factors (F0) in different zones shall be taken as given in Table. The design seismic forces shall be computed on the basis of importance of the structure I (Table) and its soil-foundation system β (Table). 9In Seismic Coefficient Method the design value of horizontal seismic coefficient (αh) shall be computed as In response Spectrum Method the response acceleration coefficient is first obtained for the natural period and damping of the structure and the design value of horizontal seismic coefficient (αh) shall be computed using 0 α β α I h = g S IF a h 0 β α =
  • 33. GRAVITY DAMS GRAVITY DAMS Earthquake Forces 9Basic seismic coefficients (α0) and seismic zone factors (F0) in different zones shall be taken as given in Table. The design seismic forces shall be computed on the basis of importance of the structure I (Table) and its soil-foundation system β (Table). 9In Seismic Coefficient Method the design value of horizontal seismic coefficient (αh) shall be computed as In response Spectrum Method the response acceleration coefficient is first obtained for the natural period and damping of the structure and the design value of horizontal seismic coefficient (αh) shall be computed using 0 α β α I h = g S IF a h 0 β α =
  • 34. GRAVITY DAMS GRAVITY DAMS Earthquake Forces where Sa/g = average acceleration coefficient as read from Fig for a damping of 5 percent and fundamental period of vibration of the dam corresponding to where H = height of the dam in m, B = base width of the dam in m, γm = unit weight of the material of dam in N/m3, g = acceleration due to gravity in m/s2, and Em, = modulus of elasticity of the material in N/m2. Where a number of modes are to be considered for seismic analysis αh shall be worked out corresponding to the various mode periods and dampings and then design forces shall be computed. If actual response spectra is available then the same may be used directly instead of the above equation. m m gE B H T γ 2 55 . 5 =
  • 36. GRAVITY DAMS GRAVITY DAMS Earthquake Forces Inertia forces: The inertia force acts in a direction opposite to the acceleration imparted by, earthquake forces and is equal to the product of the mass of the dam and the acceleration. For dams up to 100 m height the horizontal seismic coefficient shall be taken as 1.5 times seismic coefficient αh at the top of the dam reducing linearly to zero at the base. This inertia force shall be assumed to act from upstream to downstream or downstream to upstream to get the worst combination for design. It causes an overturning moment about the horizontal section adding to that caused by hydrodynamic force. Effect of Horizontal Acceleration: causes two forces: (1) Inertia force in the body of the dam, and (2) Hydrodynamic pressure of water.
  • 37. GRAVITY DAMS GRAVITY DAMS Earthquake Forces where W = total weight of the masonry or concrete in the dam in N, and = height of the centre of gravity of the dam above the base in m. For any horizontal section at a depth y below top of the dam shear force, Vy, and bending moment My, may be obtained as follows For dams over 100 m height the response spectrum method shall be used. The base shear, VB and base moment MB may be obtained by the following formulae: h B h B h W M W V α α 9 . 0 6 . 0 = = B m y B v y M C M V C V ' ' = =
  • 39. GRAVITY DAMS GRAVITY DAMS Earthquake Forces where pey = hydrodynamic pressure intensity (Pa) at depth y, h = depth of reservoir (m) and Cs = coefficient which varies with shapes of u/s face and depth of water. Hydrodynamic forces: Due to horizontal acceleration of the foundation and dam there is an instantaneous hydrodynamic pressure (or suction) exerted against the dam in addition to hydrostatic forces. The direction of hydrodynamic force is opposite to the direction of earthquake acceleration. Zanger presented formulae based on electrical analogy and with assumption that water is incompressible. The pressure variation is elliptical-cum-parabolic. The hydrodynamic pressure at depth y below the reservoir surface shall be determined as follows h C p w h s ey γ α =
  • 41. GRAVITY DAMS GRAVITY DAMS Earthquake Forces where Cm = maximum value of Cs, which can be read from Fig. or obtained from Approximate values of Cs, for dams with vertical or constant upstream slopes may be obtained as follows ⎪ ⎭ ⎪ ⎬ ⎫ ⎪ ⎩ ⎪ ⎨ ⎧ ⎟ ⎠ ⎞ ⎜ ⎝ ⎛ − + ⎟ ⎠ ⎞ ⎜ ⎝ ⎛ − = h y h y h y h y C C m s 2 2 2 ⎟ ⎠ ⎞ ⎜ ⎝ ⎛ − = 90 1 735 . 0 θ m C where θ = angle, in degrees the u/s face of the dam makes with vertical. If the height of the vertical portion of u/s face is equal to or greater than one-half the total height of the dam, analyze it as if vertical throughout. Otherwise use a sloping line connecting the point of intersection of u/s face and the reservoir surface with the heel.
  • 43. GRAVITY DAMS GRAVITY DAMS Earthquake Forces Similarly, the moment of pressure about the joint upto which the pressure is taken is given by half the sum of the moments of the quarter ellipse and semi-parabola. Hence The total pressure at depth y may be found by integrating the pressure curve above that plane. Taking the pressure variation to be elliptical-cum-parabolic, the total pressure at depth y will be equal to the average of the areas of the quarter ellipse and semi parabola. Hence where Pey = hydrodynamic shear in N/m at any depth y, and Mey = moment in N.m/m due to hydrodynamic force at any depth y. y p y p y p P ey ey ey ey 727 . 0 3 2 4 2 1 = ⎟ ⎠ ⎞ ⎜ ⎝ ⎛ + = π 2 2 299 . 0 15 4 3 1 2 1 5 2 3 2 3 4 4 2 1 y p y p y y p y y p M ey ey ey ey ey = ⎟ ⎠ ⎞ ⎜ ⎝ ⎛ + = ⎟ ⎠ ⎞ ⎜ ⎝ ⎛ × + × = π π
  • 44. GRAVITY DAMS GRAVITY DAMS Earthquake Forces where PeV = increase (or decrease) in vertical component of load due to hydrodynamic force, Pey2 = total horizontal component of hydrodynamic force at elevation of the section being considered, Pey1 = total horizontal component of hydrodynamic force at the elevation at which the slope of dam face commences, and θ = angle between the face of dam and the vertical. Moment due to vertical component of reservoir and tail water load may be obtained by determining lever arm from centroid of pressure dia. Effect of Horizontal Acceleration on the Vertical Component of Reservoir and Tail Water Load: Since the hydrodynamic pressure (or suction) acts normal to the face of the dam, there shall be a vertical component of this force if the face of the dam against which it is acting is sloping, the magnitude at any horizontal section being ( ) θ tan 1 2 ey ey eV P P P − =
  • 45. GRAVITY DAMS GRAVITY DAMS Earthquake Forces Effect of Vertical Acceleration: The effect of vertical earthquake acceleration is to change the unit weight of water and concrete or masonry. Acceleration upwards increases the weight and acceleration downwards decreases the weight. Due to vertical acceleration a vertical inertia force F = αVW is exerted on the dam, in the direction opposite to that of the acceleration. When the acceleration is vertically upwards, the inertia force F = αVW acts vertically downwards, thus increasing momentarily the downward weights. When the acceleration is vertically downwards the inertia force F = αVW acts upwards and decreases momentarily the downward weight. For methods of design (seismic coefficient up to 100 m and response spectrum over 100 m) Vertical seismic coefficient (αV) shall be taken as 0.75 times the value of αh (of the respective method) at the top of the dam reducing linearly to zero at the base