Title: Hydrology
1Hydrology
- Open channel
- Flow
- Acad. Year 2003-2004
- FLTBW
2Rivers 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)
4Rivier is not a simple channel
open water surface
Uniform flow rare, only in artificial
canals Backwater varying profile curves etc ...
real rivers
5Bernouilli 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
6Bernouilli 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
7Hydraulic 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
8Uniform versus nonuniform flow
Sf
Uniform parallel watersurface bottom and energy
So
Non-uniform not parallel
9Bernouilli 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)
10Uniform 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
11Reynolds 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)
12Uniform 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
13Uniform flowin rectangular section
A
P wet perimeter
Ahw P2hw in hydraulics RA/P different as FTV
14Mannings n
15Artifical channels with uniform flow
Well defined cross-section and longitudinal slope
Concrete Channel
16Velocity distribution in a channel
Air resistance (low)
Wet perimeter (higher friction)
17Channel cross-sections
18Specific energy
- energy relative to channel bottom
2 !!!
19Critical 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
20Critical, 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
21Mild 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)
22Change in slope and overfall
23hydraulic jump UCL
critical flow
sub-critical flow
super-critical flow
24Voer Heverlee
subcritical
ultrasonic level
critical
supercritical
25Example of shallow river
26Change in bed elevation (e.g. dip)
?
waterlevel
riverbed
27Change in bed elevation (e.g. dip)
waterlevel
water
riverbed
reference level
Example with Q2 Frgt1 Frlt1
28Important 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
29Rivier is not a simple channel
Uniform flow mostly in artificial canals (
irrigation) Backwater widening bends etc are
common in natural rivers
30Examples non-uniform
31Non uniform is part of the fun rafting
32From 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
33hydraulic jump UCL
super-critical flow
sub-critical flow
Jump from super to sub-critical
34Variations in velocity
- Vertical profile
- cross section
Bend
straight river
35Meandering river
36Spiral flow
37Rehabilitation