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