page 1
page 2
page 3
page 4
page 5
page 6
page 7
page 8
page 9
page 10
page 11
page 12
page 13
page 14
page 15
page 16
page 17
page 18
page 19
page 20
page 21
page 22
page 23
page 24
page 25
page 26
page 27
page 28
page 29
page 30
page 31
page 32
page 33
page 34
page 35
page 36
page 37
page 38
page 39
page 40
page 41
page 42
page 43
page 44
page 45
page 46
page 47
page 48
page 49
page 50
page 51
page 52
page 53
page 54
page 55
page 56
page 57
page 58
page 59
page 60
page 61
page 62
page 63
page 64
page 65
page 66
page 67
page 68
page 69
page 70
page 71
page 72
page 73
page 74
page 75
page 76
page 77
page 78
page 79
page 80
page 81
page 82
page 83
page 84
page 85
page 86
page 87
page 88
page 89
page 90
page 91
page 92
page 93 page 94
page 95
page 96
page 97
page 98
page 99
page 100
page 101
page 102
page 103
page 104
page 105
page 106
page 107
page 108
page 109
page 110
page 111
page 112
page 113
page 114
page 115
page 116
page 117
page 118
page 119
page 120
page 121
page 122
page 123
page 124
page 125
page 126
page 127
page 128
page 129
page 130
page 131
page 132
page 133
page 134
page 135
page 136
page 137
page 138
page 139
page 140
page 141
page 142
page 143
page 144
page 145
page 146
page 147
page 148
page 149
page 150
page 151
page 152
page 153
page 154
page 155
page 156
page 157
page 158
page 159
page 160
page 161
page 162
page 163
page 164
page 165
page 166
page 167
page 168
page 169
page 170
page 171
page 172
page 173
page 174
page 175
page 176
page 177
page 178
page 179
page 180
page 181
page 182
page 183
page 184
page 185
< prev - next > Energy Hydro power civil_works_guidelines_for_micro_hydro (Printable PDF)
CIVIL WORKS GUIDELINES FOR MICRO-HYDROPOWER IN NEPAL
91
limiting diameters beyond a certain range which could affect
the optimisation process. An example of Penstock
Optimisation is shown in Example 6.2
6.5 Surge calculation
6.5.1 GENERAL
The thickness of the penstock pipe is determined by the gross
and surge heads of the scheme. It is therefore important to
have some understanding of the concept of surge before
calculating the pipe wall thickness.
A sudden blockage of water or rapid change in velocity in the
penstock (or any pipe that has pressure flow) results in very
high instantaneous pressure. This high pressure is known as
‘surge’ pressure or often referred to as “waterhammer”. Surge
pressure travels as positive and negative waves throughout
the length of the penstock pipe.
Water hammer occurs as the surge wave travels from the source
or the origin of the disturbance, along the pipeline until it
strikes some boundary condition (such as a valve or other
obstruction) and is then reflected or refracted. If the pipe is
strong enough to withstand the initial surge effect, the
pressure will ultimately dissipate through friction losses in
the water and pipe wall as well as through the forebay. The
speed of the surge wave (wave velocity) is dependent on such
factors as the bulk modulus of water, flexibility of the pipe
and the ratio of pipe diameter to wall thickness.
In hydropower schemes, positive surge characteristics are
different for different types of turbines. Surge head calcula-
tions for the two most common turbines used in micro-hydro
schemes are discussed here. Note that these calculations are
based on the initial (i.e. undampened) positive surge head.
In practice there will be some damping of the surge pressure
as the wave travels along the pipe, and whilst the pressure
fluctuation is uniform in the lower portion it diminishes
gradually to zero at the forebay, as shown in Figure 6.3.
However, the pipe is normally designed for static head plus
constant positive surge over the full penstock length.
Note that the negative surge can produce dangerous negative
(sub-atmospheric) pressure in a penstock if the profile is as in
Figure 6.3. Once the negative pressure reaches 10 metres the
water column separates, and subsequent rejoining will cause
high positive surge pressure sufficient to burst the penstock.
Sub-atmospheric pressures less than 10 metres can cause
inward collapse of the pipe wall, so should also be avoided. If
there is any possibility of negative pressure the pipe wall
thickness must be checked for buckling (see Section 6.6.2).
To avoid negative pressure, move the forebay to Point A in
Figure 6.3. Alternatively take measures to reduce the surge
pressure.
Figure 6.3 Surge pressures
“Bursting disc” technology could provide a reliable means of
safely releasing excess head in case of surge pressure without
increasing the pipe thickness (which is the convention). This
is discussed in Chapter 10.
6.5.2 PELTON TURBINE
For a Pelton turbine use the following method to calculate the
surge head:
1. First calculate the pressure wave velocity ‘a’ using the
equation below.
a = 1440 / 1+(2150 x d/E x t) m/s
where:
E is Young’s modulus in N/mm2. The value of Young’s modulus
for mild steel, PVC and HDPE can be seen in Table 6.2.
d is the pipe diameter (mm) t is the nominal wall thickness
(mm), not teffective
2. Then calculate the surge head (hsurge), using the following
equation: hsurge = av/g x 1/n where: n is the total no. of
nozzles in the turbine(s).
Note that in a Pelton turbine it is highly unlikely for more
than one nozzle to be blocked instantaneously. Therefore, the
surge head is divided by the number of nozzles (n). For example
if a penstock empties into two Pelton turbines with two nozzles
on each turbine, n = 4
The
velocity
in
the
penstock
(V)
is:
V
=
4Q
πd2
3. Now calculate the total head: htotal = hgross + hsurge
4. As a precaution, calculate the critical time, Tc, from the
following equation: Tc = (2L)/a
where:
Tc is the critical time in seconds,
L is the length of penstock in m,
‘a’ is the wave velocity calculated earlier.