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Hydraulics of Structures

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Frequently, when the drop inlet is the same size as the remainder of the pipe, orifice flow will control and the pipe will never flow full. – PowerPoint PPT presentation

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Title: Hydraulics of Structures


1
Hydraulics of Structures
2
What are structures?
  • Structures in this context are simply something
    placed in the channel to either measure or
    control flow.
  • Example A principle spillway is used as part of
    a dam design to control the rate at which water
    is discharged from a reservoir.
  • Include both inlet and outlet control devices.
  • Control devices can operate as
  • Open channel flow in which the flow has a free
    surface or
  • Pipe flow in which the flow is in a closed
    conduit under pressure.

3
Most basic principle of hydraulics of structures
  • As head on a structure increases, the flow that
    is discharged through the structure increases.
  • Figure 5.1 (Haan et al., 1994) shows the
    head-discharge relationships for several flow
    control structures.

4
Weirs
  • At its most basic, just an obstruction placed in
    a channel that constricts flow as it goes over a
    crest.
  • The crest is the edge of the weir over which the
    water flows.
  • As the water level (head) over the crest
    increases, the flow rate increases dramatically.
  • Two basic types of weirs
  • sharp crested
  • broad crested

5
Sharp Crested Weirs
  • A sharp crested weir is defined by a thin crest
    over which the water springs free as it leaves
    the upstream face of the weir.
  • Flow over a weir is also called the nappe.
  • Sharp crested weirs are generally constructed of
    sheet metal or similar thin material.

6
Sharp Crested Weir
7
Sharp Crested Weirs
  • Can have several shapes
  • Triangular (or v-notch)
  • Rectangular
  • Trapezoidal
  • Classified by the shape of its notch.
  • V-notch weirs have greater control under low flow
    conditions.
  • Rectangular weirs have larger capacity but are
    less sensitive for flow measurement.

8
Sharp Crested Weirs-General
h
H
dh
z
9
  • Making the assumption that the velocity head at
    the upstream point will be much smaller than the
    velocity head as the flow goes over the weir we
    assume v12/2g is negligible and

10
Integrating this from h 0 to h H gives
11
Rectangular Weirs
A rectangular weir that spans the full width of
the channel is known as a suppressed weir.
12
  • Hydraulic head (H) for weirs is simply the height
    of the water surface above the weir crest,
    measured at a point upstream so that the
    influence of the velocity head can be ignored.
  • L is the length of the weir.
  • The coefficient of discharge (C) is dependent
    upon units and of the weir shape.
  • For a suppressed weir with H/h lt 0.4 (where h is
    the height of the weir) C 3.33 can be used.
  • For 0.4 lt H/h lt 10, C 3.27 0.4 H/h

13
A rectangular weir that does not span the whole
channel is called a weir with end contractions .
The effective length of the weir will be less
than the actual weir length due to contraction of
the flow jet caused by the sidewalls.
Where N is the number of contractions and L is
the measured length of the crest.
14
Triangular (v-notch ) weirs
  • Used to measure flow in low flow conditions.

15
  • For Q 90, K 2.5 (typically), tan (Q/2) 1
    therefore,

16
  • Note Your handout with Figure 12.28 presents
    the equation for a v-notch weir as

with
17
Broad Crested Weirs
H
W
Where L is the width of the weir.
18
Broad Crested Weirs
  • Broad crested weirs support the flow in the
    longitudinal direction (direction of flow).
  • They are used where sharp-crested weirs may have
    maintenance problems.
  • The nappe of a broad crested weir does not spring
    free.

19
Roadway Overtopping
Where Qo overtopping flowrate Cd - overtopping
discharge coefficient L length of roadway
crest HWr upstream depth
Cd ktCr Cr discharge coefficient kt
submergence factor Figure 5.7
20
Orifices
  • An orifice is simply an opening through which
    flow occurs.
  • They can be used to
  • Control flow as in a drop inlet
  • Measure the flow through a pipe.

21
  • The discharge equation for orifice flow is

Where C is the orifice coefficient (0.6 for
sharp edges, 0.98 for rounded edges). A is the
cross-sectional area of the orifice in ft2 g is
the gravitational constant H is the head on the
orifice
22
  • At low heads, orifices can act as weirs.
  • Calculate the discharge using the suppressed weir
    equation where L is equal to the circumference of
    the pipe.
  • Calculate the discharge using the orifice
    equation.
  • The lower discharge will be the actual discharge.

23
Pipes as Flow Control Devices
H
H
Energy Grade Line
D
0.6D
L
Elbow and Transition
24
(No Transcript)
25
Head Loss Coefficients
  • Ke is the entrance head loss coefficient and is
    typically given a value of 1.0 for circular
    inlets.
  • Kb is the bend head loss coefficient and is
    typically given a value of 0.5 for circular
    risers connected to round conduits.
  • For risers with rectangular inlets, the bend head
    losses and entrance head losses are typically
    combined to a term Ke where values of Ke can be
    found in Table 5.3 and

26
Head Loss Coefficients
  • Kc is the head loss coefficient due to friction.
  • Values for Kc are given in Tables 5.1 and 5.2 for
    circular and square pipes.
  • Kc is multiplied by L, the entire length of the
    pipe, including the riser.

27
  • Frequently, when the drop inlet is the same size
    as the remainder of the pipe, orifice flow will
    control and the pipe will never flow full.
  • If it is desirable to have the pipe flowing full,
    it may be necessary to increase the size of the
    drop inlet.

28
Using Flow Control Structures as Spillways
  • A given drop inlet spillway can have a variety of
    discharge relationships, given the head.
  • At the lowest stages the riser acts as a weir.
  • As the level of the reservoir rises, water
    flowing in from all sides of the inlet interferes
    so that the inlet begins to act as an orifice.
  • As the level continues to rise, the outlet
    eventually begins to flow full and pipe flow
    prevails.
  • A stage-discharge curve is developed by plotting
    Q vs. H for each of the three relationships. The
    minimum flow for a given head is the actual
    discharge used.

29
Rockfill Outlets as Controls
ROCKFILL
HYDRAULIC PROFILE
dh
h1
have
h2
dl
30
Rockfill Outlets
  • Advantages
  • Abundant
  • Generally available
  • Usually inexpensive
  • Relative permanence

31
Rockfill Outlets
  • Major expenses
  • Grading
  • Transporting
  • Placing stone

32
Rockfill Outlets
  • Used for
  • Protective channel linings and breakwaters
  • Add stability to dams
  • Provide energy dissipation zones for reservoir
    outlets
  • Flow control structure

33
Modified Darcy-Weisbach Equation
34
Rockfill as Control Structure Model
Reynolds Number Equation
Friction factor
35
Friction Factor-Reynolds Number Relationship
36
h2 have Relationships
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