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Distributed Flow Routing

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Fg = Gravity force due to weight of water in the C.V. ... Fw = wind shear force due to frictional resistance of wind at the water surface ... – PowerPoint PPT presentation

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Title: Distributed Flow Routing


1
Distributed Flow Routing
Venkatesh Merwade, Center for Research in Water
Resources
  • Surface Water Hydrology, Spring 2005
  • Reading 9.1, 9.2, 10.1, 10.2

2
Outline
  • Flow routing
  • Flow equations for Distributed Flow Routing (St.
    Venant equations)
  • Continuity
  • Momentum
  • Dynamic Wave Routing
  • Finite difference scheme

3
Flow Routing
  • Definition procedure to determine the flow
    hydrograph at a point on a watercourse from a
    known hydrograph(s) upstream
  • Why do we route flows?
  • Account for changes in flow hydrograph as a flood
    wave passes downstream
  • This helps in
  • Accounting for storages
  • Studying the attenuation of flood peaks

4
Flow Routing Types
  • Lumped (Hydrologic)
  • Flow is calculated as function of time, no
    spatial variability
  • Governed by continuity equation and flow/storage
    relationship
  • Distributed (Hydraulic)
  • Flow is calculated as a function of space and
    time
  • Governed by continuity and momentum equations

5
Flow routing in channels
  • Distributed Routing
  • St. Venant equations
  • Continuity equation
  • Momentum Equation

What are all these terms, and where are they
coming from?
6
Assumptions for St. Venant Equations
  • Flow is one-dimensional
  • Hydrostatic pressure prevails and vertical
    accelerations are negligible
  • Streamline curvature is small.
  • Bottom slope of the channel is small.
  • Mannings equation is used to describe resistance
    effects
  • The fluid is incompressible

7
Continuity Equation
Q inflow to the control volume q lateral
inflow
Rate of change of flow with distance
Outflow from the C.V.
Change in mass
Reynolds transport theorem
Elevation View
Plan View
8
Continuity Equation (2)
Conservation form
Non-conservation form (velocity is dependent
variable)
9
Momentum Equation
  • From Newtons 2nd Law
  • Net force time rate of change of momentum

Sum of forces on the C.V.
Momentum stored within the C.V
Momentum flow across the C. S.
10
Forces acting on the C.V.
  • Fg Gravity force due to weight of water in the
    C.V.
  • Ff friction force due to shear stress along the
    bottom and sides of the C.V.
  • Fe contraction/expansion force due to abrupt
    changes in the channel cross-section
  • Fw wind shear force due to frictional
    resistance of wind at the water surface
  • Fp unbalanced pressure forces due to
    hydrostatic forces on the left and right hand
    side of the C.V. and pressure force exerted by
    banks

Elevation View
Plan View
11
Momentum Equation
Sum of forces on the C.V.
Momentum stored within the C.V
Momentum flow across the C. S.
12
Momentum Equation(2)
Local acceleration term
Convective acceleration term
Pressure force term
Gravity force term
Friction force term
Kinematic Wave
Diffusion Wave
Dynamic Wave
13
Momentum Equation (3)
Steady, uniform flow
Steady, non-uniform flow
Unsteady, non-uniform flow
14
Applications of different forms of momentum
equation
  • Kinematic wave when gravity forces and friction
    forces balance each other (steep slope channels
    with no back water effects)
  • Diffusion wave when pressure forces are
    important in addition to gravity and frictional
    forces
  • Dynamic wave when both inertial and pressure
    forces are important and backwater effects are
    not negligible (mild slope channels with
    downstream control)

15
Dynamic Wave Routing
Flow in natural channels is unsteady, nonuniform
with junctions, tributaries, variable
cross-sections, variable resistances, variable
depths, etc etc.
16
Solving St. Venant equations
  • Analytical
  • Solved by integrating partial differential
    equations
  • Applicable to only a few special simple cases of
    kinematic waves
  • Numerical
  • Finite difference approximation
  • Calculations are performed on a grid placed over
    the (x,t) plane
  • Flow and water surface elevation are obtained for
    incremental time and distances along the channel

x-t plane for finite differences calculations
17
i-1, j1
i-1, j1
i1, j1
?t
i-1, j
i1, j
i, j
?x
?x
Cross-sectional view in x-t plane
x-t plane
h0, Q0, t1
h1, Q1, t1
h2, Q2, t2
?t
h0, Q0, t0
h1, Q1, t0
h2, Q2, t0
?x
?x
18
Finite Difference Approximations
  • Explicit
  • Implicit

Temporal derivative
Temporal derivative
Spatial derivative
Spatial derivative
Spatial and temporal derivatives use unknown time
lines for computation
Spatial derivative is written using terms on
known time line
19
Example
20
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