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Hydrology

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Energy of the streamline on the river bottom per unit of weight discharge ... Height of bottom z. Average velocity V in a cross-section ... – PowerPoint PPT presentation

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Title: Hydrology


1
Hydrology
  • Open channel
  • Flow
  • Acad. Year 2003-2004
  • FLTBW

2
Rivers in Dijle CA
Voer Bertem 41 km2
Discharge m³/s
Dijle St. Joris W 645 km2
10-19 April 2001
Days
3
Major event
Dijle Sint Joris Weert (640 km²)
20
(m³/s)
Flow in rivers
3
Voer Heverlee ( 51 km²)
(m³/s)
4
Rivier is not a simple channel
open water surface
Uniform flow rare, only in artificial
canals Backwater varying profile curves etc ...
real rivers
5
Bernouilli energy equation
y hab bot dsurf to stream
Energy -loss
Total potential
V12/2g
V2/2g
Open water surface
p1/g?d
H1
y
any streamline
H2
z1
Rivier bottom
z
Reference height
6
Bernouilli equation at any streamline
  • If no friction (ideal fluid with no viscosity)
  • However viscosity and no-slip boundary
  • Energy is lost ( hL ) along the longitudinal
    slope however H in any vertical is constant

Bernouilli equation see FTV physics course
7
Hydraulic radius in hydrology hydraulics
  • Definition in heat and mass transfer (FTV, Datta
    etc) hydraulic diameter dh
  • Definition in hydraulics hydraulic radius Rh R

hydraulic radius ? geometric radius
8
Uniform versus nonuniform flow
Sf
Uniform parallel watersurface bottom and energy
So
Non-uniform not parallel
9
Bernouilli energy equation
  • Energy of the streamline on the river bottom per
    unit of weight discharge
  • Pressure D expressed in waterdepth (D P/?g)
  • Height of bottom z
  • Average velocity V in a cross-section
  • Beware open canals (wet cross-section is not
    constant like in a filled pipe)
  • Head losses hL friction and local
  • In a vertical the potential remains constant (sum
    of pressure and elevation constant)

10
Uniform flow in channel
Slope of total energy-line (Sf) and longitudinal
slope of the bottom (S0) become equal (parallel)
Darcy-Weisbach (see FTV)
Requires constant cross-section and slope
energy losses by friction
11
Reynolds number laminar of turbulent
  • Water ?10-6 m²/s normally turbulent
  • 4 R is characteristic length (diameter pipe)
  • R A/P hydraulic radius (!!!!!!!)
  • Sheet flow over smooth surface could be laminar
    (rather exceptional)

12
Uniform open chanal-flow
  • Uniform (eenparig) constant cross-section
    watersurface, bottom- and energy line are
    parallel
  • gt friction loss in equilibrium with channel
    slope
  • Manning formula (turbulent)

Relation discharge-waterheight is uniform
Rather rare in natural rivers
13
Uniform flowin rectangular section
A
P wet perimeter
Ahw P2hw in hydraulics RA/P different as FTV
14
Mannings n
15
Artifical channels with uniform flow
Well defined cross-section and longitudinal slope
Concrete Channel
16
Velocity distribution in a channel
Air resistance (low)
Wet perimeter (higher friction)
17
Channel cross-sections
18
Specific energy
  • energy relative to channel bottom

2 !!!
19
Critical depth minimum specific energy for a
given Q
  • specific qs Q/B with B top width
  • E y Q2/2gA2 where Q/A qs/y
  • Take dE/dy (1 qs2/gy3) 0 (find minimum)
  • For a rectangular channel bottom width B,
  • 1. Emin 3/2Yc for critical depth y yc
  • yc/2 Vc2/2g
  • yc (Q2/gb2)1/3

20
Critical, sub- super-critical flow
In general for any channel, B top width (Q2/g)
(A3/B) at y yc Finally Fr V/(gy)1/2
Froude No. Fr 1 for critical flow Fr lt 1 for
subcritical flow Fr gt 1 for supercritical flow
21
Mild and steep slope
  • If uniform flow ( calculate by Mannings equation
    ) has Fr gt 1
  • gt steep slope with supercritical flow
  • If uniform flow has Fr lt 1
  • gt mild slope and subcritical flow
  • Transition goes via critical flow
  • Fr 1
  • Control sections often use critical flow
    conditions (see discharge measurement)

22
Change in slope and overfall
23
hydraulic jump UCL
critical flow
sub-critical flow
super-critical flow
24
Voer Heverlee
subcritical
ultrasonic level
critical
supercritical
25
Example of shallow river
26
Change in bed elevation (e.g. dip)
?
waterlevel
riverbed
27
Change in bed elevation (e.g. dip)
waterlevel
water
riverbed
reference level
Example with Q2 Frgt1 Frlt1
28
Important consequences
  • A pit in a river for
  • subcritical flow has lower velocities and will
    have more sediment trapping
  • supercritical flow has higher velocities and will
    erode

29
Rivier is not a simple channel
Uniform flow mostly in artificial canals (
irrigation) Backwater widening bends etc are
common in natural rivers
30
Examples non-uniform
31
Non uniform is part of the fun rafting
32
From super- to subcriticalHydraulic jump
  • Concept of specific force (not explained here)
  • the momentum (specific force) before and after
    the jump is the same
  • energy loss in the jump (local head losses) can
    be used for energy dissipation

33
hydraulic jump UCL
super-critical flow
sub-critical flow
Jump from super to sub-critical
34
Variations in velocity
  • Vertical profile
  • cross section

Bend
straight river
35
Meandering river
36
Spiral flow
37
Rehabilitation
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