Title: Fluid Dynamics
1Fluid Dynamics
2Fluid Dynamics Lecture Plan
- First consider fluids, stress relationships and
fluid types - Then consider factors affecting fluid flow, flow
velocity, and behavior in pipes vs open channels - Then understand what controls sediment movement
- Finally put flow and sediment together to
understand relationships to channel form and
erosion/deposition in stream systems
3Fluids
- Substances with no strength
- Deform when forces are applied
- Include water and gases
- Body Forces act on whole or bulk of fluid
- Resolve forces within plane of surface of body so
forces distributed in plane
4Understanding Flow and Sediment Transport
- Ability of river to erode and transport sediment
represents a balance between driving and
resisting forces - Flow and resistance equations are at the heart of
the discussion
5Understanding Flow and Sediment Transport
- Conservation Relations
- Water Mass (aka Continuity)
- Momentum (aka Newtons 2nd Law FMA)
- Energy
- Constitutive Relations
- Flow Resistance (Manning Equation)
- Sediment Transport (Shields, Hjulstrom, Bagnold)
6Pressure and Shear
- Shear (t) - exertedto surface
-
- Shear (t) F/A
- Pressure exerted - to surface F/A
7Stress and Strain
Shear (t) F/A
Shear Stress deforms block Deformation
Strain Strain proportional to ?
?
8Viscosity
- Measure of internal friction of fluid particles
- Molecular cohesiveness
- Resistance fluid has to shear (or flow)
- Dynamic viscosity µ shear stress/rate of
change of ? with time
t Shear Stress
9Kinematic Viscosity
µ viscosity ? density
- Viscosity constant at given T ? doesnt depend
on type of shearing stress or duration of stress
Newtonian Fluid - T? µ?
- Kinematic viscosity determines extent to which
fluid flow exhibits turbulence
10Types of Fluid Flow
- Laminar Flow flow persists as unidirectional
movement - Molecules flow parallel
- Movement up and down by diffusion
- Turbulent Flow highly distorted flow
- Large scale flow perpendicular to direction of
flow - Transfer of movement up and down by macroscale
processes - Turbulence irregular and random component of
fluid motion - Eddies highly turbulent water masses
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12Laminar vs Turbulent Flow
- Laminar flow velocity constant at a point over
time - Turbulence
- Most flows turbulent
- Slow settling velocity upward motion of water
particles - Increases effectiveness of fluid in eroding and
entraining particles from the bed but less
efficient transport agent - Velocity measured at a point over time tends
towards an average value but varies from instant
to instant - Resists distortion to much greater degree than
laminar flow - Apparent viscosity eddy viscosity
13Cross-sectional Measurements of Stream Channels
- You will see lots of different variables, terms,
and ways of expressing channel characteristics - Need to spend a little time understanding what
they are so that you can move between and among
equations and measurements.
14Max Depth(Stage)
Wetted Perimeter
Top Width
Hydraulic Radius A/P
Mean Depth Area/Top Width
15Shear Stress Laminar vs Turbulent Flow
Laminar Flow
Turbulent Flow
- Add apparent viscosity or eddy viscosity (?) to
turbulent flow shear stress equation - Turbulence exerts larger shear stress on adjacent
fluids than laminar
16Reynolds Number
Re UR?/µ UR/?
U mean flow velocity ? density R
hydraulic radius (A/P) µ viscosity ?
kinematic viscosity (µ/?)
- Balance between inertial forces (cause
turbulence) and viscous forces (suppress
turbulence) - Laminar Re lt 1000 viscous dominate shallow
depth or low velocity - Turbulent Re gt1000 inertial forces dominate
deep or fast flow
17Depth vs Hydraulic Radius
- Some equations use D (or L) developed in pipes
and adopted for open channels - In wide, shallow channels, RD so substitution is
ok and simplifies equations - In deep or incised channels this is not true
and errors are introduced
18Velocity Profiles and Bed Roughness
- In Turbulent Flow laminar/near laminar flow
occurs only very near bed - Smooth beds molecular viscous forces dominate
in thin layer close to bed boundary - Viscous sublayer / laminar sublayer
- Rough/Irregular beds
- Coarse sand or gravel
- Viscous sublayer destroyed by particles extending
through layer - Obstacles generate eddies at boundary of flow
- Presence/absence of sublayer important factor
in initiating grain movement
19Boundary Shear Stress
- As fluid flows across bed stress that opposes
motion of the fluid exists at the bed surface - Force/unit area parallel to bed
- Extremely important variable in determining
erosion and transport of sediment on the bed - F (fluid density, slope of bed, water depth, flow
velocity) - Boundary Shear Stress tends to increase as
velocity increases though in complex ways
20Boundary Shear Stress
cross-sectional area/wetted perimeter
21Boundary Shear Stress in Open Channel
Depth-Slope Product
- Newtons 2nd Law of Momentum
- Calculate boundary shear stress of flow moving
down channel - Adds g for gravitational acceleration to account
for weight of water moving along channel length
22Boundary Shear Stress
- BSS determined by force that flow exerts on bed
and related to flow velocity determines erosion
and transport of sediment on bed below a flow - BSS increases directly with
- ? fluid density
- ? diameter and depth of the stream channel
- ? slope of stream bed
- Greater ability to erode and transport sediment
- Water vs air
- Larger stream channels vs smaller
- Higher gradient streams vs lower
23Shear Velocity
U Shear Velocity
to Boundary Shear Stress
? Fluid Density
- Shear stress at bed function of shear velocity
(cm/s) - In rivers
- U vgDS D depth S slope
- Assumes steady, uniform flow
- Average shear velocity of section of channel
- Warning D can be a problem better to use R
- This is still based on flow in pipes
24Froude Number
g gravitational acceleration
L water depth
- Ratio between inertial and gravity forces
- Gravity influences way fluid transmits shallow
water waves - Dimensionless value (like Re)
25Froude Number
- Fr lt 1 Tranquil, Streaming, Subcritical
- Velocity of wave gt flow velocity
- Fr gt 1 Rapid, Shooting, Supercritical
- Waves cannot propagate upstream
- Fr has relationship to flow regimes
- Defines characteristic bedforms that develop
during flow over a bed
26Chezy Equation
- Velocity directly proportional to square root of
RS product where R A/P S Slope - Chezy coefficient (C) is a constant of
proportionality related to resisting factors in
system - Equation balances flow velocity with resisting
forces associated with bed roughness
27Manning Equation
- Similar to Chezy Equation
- Mannings n is presumed to be constant for a
given channel framework - Mannings n is also called Manning roughness
coefficient - Need estimate of n for each stream reach
- Can be controlled by sediment grain size or
bedforms controlled by Froude number
28Mannings n
- Can look up n in tables
- Can calculate n
- Can look up values in a photo guide from USGS
(Barnes, 1968)
29Mannings n Examples
30Mannings n Examples