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SHC 410 Lecture Notes: Theme 13,14,15,18

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These are some of the SHC 410 handwritten notes I made during my time at the University of Pretoria. These notes cover examples, explanations and additional research. They are written on either the given lecture slides or in a separate notebook. Have a look at the bundle deals if you are planning on buying more than one set of notes, and please do not hesitate to contact me over the app. Happy studying students!

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Información del documento

Subido en
30 de mayo de 2021
Número de páginas
60
Escrito en
2020/2021
Tipo
Notas de lectura
Profesor(es)
Dr loots
Contiene
13,14,15,18

Temas

Vista previa del contenido



JKEARNEY
NOTES




SHC 410

, 3/02/2020 SedimentTranspo
Movement & Effect of sedimentation :
deposition of
-




sediment Structures
scouring& of foundations


.
.




↳ Canals
scouring sedimentation

.




↳ Reservoirs loss of
capacity





sedimenttransportoo.cc
Bed load boulders
Deposition {
rolling
* :


.
*
Suspended load suspended particles
:

water Colloidal water (difficult remove)
quality
← *
stays in to
:




roughness T )
* As Froude number increases (
more sediment can into suspension
go .




AMmountofmaterialtransporte.cl# → under
given conditions


Dependent
( interaction
on →


Quality &
Quantity of sediment

of stream to
Influences the
between )
Capacity transport

quality
& { Groupie # Sediment brought down depend on

of & of watershed
quantity Geology Topography
of rainfall Intensity
Duration & Distribution
sediment
Magnitude
*
.


, ,




Soil Moisture
Vegetal
* * cover


Grazing Surface
* * erosion




nation
24/7 Duration




Topootaµ¥¥¥¥
rainfall rainfall
Magnitude



8
Geology New grazing
i. ooo : :! ! LT Erosion .




Soil moisture

, Groupie of transport sediment
capacity stream to
→ a




Hydraulic
{ Slope Discharge Viscosity
* * *



Velocity
of
properties *
RoughnessRadius
* *
Density
the stream .
*
Hydraulic * Turbulence




cEE÷¥÷iEmois
of sediment
size &
gradation




inn roughness Tractive
forces
Q

radius
Hydraulic


Definitions
dice thick) above the bed
Bed
layer Flow
layer (2
grain
-
. .




Bed load Sediment that rolls / slides bed
along
→ .




i. e .
Contact Load .




Bed material → Sediment mixture of stream bed .




Bed material Part of total sediment
discharge } Cfoonupnodsqd of
grain sizes
the bed
discharge on .




Discharged
weighed
concentration unit volume of
.

Dry weight of sediment per
discharge
sediment moved
Load
by stream
- .




Sediment →
Quantity of sediment that
pass a 0 per
Discharge unit time .




Sediment
yield





Suspended load → Sediment supported
turbulence .
by upward components of

, Frictionformulao.Uniformflow.ee *
a-ureunuitynfotr.EE?onbat9Ees
/ 0pgµ
.




t } Gravity force in
pgtthxsinco flow direction
)
I #
← .




To×P×L } Shear force
↳ Perimeter
To
%
xPL=pgAL×sinco )
since sinlojretancofs .
} Shallow slope

To=pgA#
P


To=pgRSo

boundry stress
mean .

, Forcesonpartickso


-

#

£§€Ecaag#
-
a-


-
to

00800000
* shear force on bed W' (Ps p)
xgxvs ( weight)
= -




force
* on a
grain .




Unit area :
Ap Areaotpartice
=

nr of particles a. Ape
Total area D 502


To A FD xttp D 50 size of
passing
ooo : 50%

D 502


* Point where a particle is about to move :
Cf angle of repose
-




To =
Tcr
* if To > Ter -

unstable
To shear force particles will move
by water &
-




.




Ten -


force required to move the particle .




xDf
'
Tcr A
Cps pg xtanc
-
x




Volume
Tcr_ A ( Q)
( ps ptg xD
- Itxgttpxtan

, Incipent hreshd lmotiono .co 400




To =p
xgxRx5←{ When Rett 7400 →
TCR =

0,056 x (Ps p
-




)gxD5O
↳ Flow is turbulent around the bed
material fully
.




Read value from
When Re* L 400 →
graph
↳ Tcr x (Ps
Pg xD 50
-




number ← Re* 1,14×10-6 Mls
U*yD5o_
2

Reynolds
=
V
=


,


t
kinematic
viscosity .




& U*
=p# Density of the fluid
f p
-
.




Shear
velocity


:{
HRS valid
Dso is
only when D= 1,65
=Ps
=




IEEE ↳
*
assumptions .


, falllsettlingjveloc.it# submerged
of sediment
gelatine density
diapmeter
Fallingeocity LIFE
f- ilgbd and D=
lPs#
Constant & function of CD


Assume - Sf for
t
=L and CD -2
large D

form factor and CD -

24
REI
Consider a
falling particle :
( Ps p
)xgxt=LzCDxPxAxVFs2
-




ps-plxgxtTDT3-ICDxpxltgdxUFSZVFSZ-kxbgxf.DE
(


)
thus
VFs=y/¥×tg×d

VF5-AxilgxdxD.AT/IzxITFallVelocity:-
given



Rough VFs=T/2zgD⑦
a) sediment - CD -2

b) Fine sediment →
6=24*2
yr-s-yftfxrffxg.AT
& Re*=VFSxD
T

:tFs=gy
o

, Scourestimationo

Complexities:
* Non
Homogeneous mixtures of water a sediment
-




* 3D flow patterns
*
Difficulty establishing actual geometries .




actual scour depths
*
Observing
*
Highly variable properties .




long term t short term @ Piers & abutments



enteral
^

p
Total scour =
EG t contraction + Local scour


Alluvial channel scour →




Cohesive bed channel scour →



Scouring : As
ooo
a

Velocity
river scours the
decreases
depth

increases
scour potential increases




Scourcountermeasureso
① Hydraulic countermeasures
River Berms

training
↳ Bed armour
structures →
Spurs ,
Dykes ,


ing →
Riprap Gabi ons
,




ing
↳ Local scour armour →




② Structural →
Foundations


During maintenance →




{ EROSION If Hydraulic
Fwriaggestation }
:
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I am a civil engineering graduate from the University of Pretoria with an honours degree in Engineering and Technology Management. As I prepared for exams, I created "super summaries" and some handwritten notes of each course. I make handwritten notes of every lecture I attend and hope that they can be used to improve your understanding of the course material. If there are any issues or questions regarding the notes please contact me over the app. Happy studying !

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