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CIVE 572
Final Project
   Daniel Robb
Outline

• Describe the problem
• Present the theory
• Show the results
Problem Statement


Use the upwind scheme and a staggered
grid to calculate open channel flow into
a sloped channel with a side basin.
Geometry
             L


W




         b

             b
     L        b     W
    4m       1m     2m
Geometry


So
     1



            L


             So
           0.001
Given Parameters


• Initial water depth d = 0.05 m
• Friction coefficient cf = 0.008
• Slope So = 0.001
Governing Equations
                2D Shallow Water Equations

∂ζ        ∂qx        ∂qy
∂t    +   ∂x    +   h ∂x   =0

∂qx       ∂F uuh         ∂F uvh           ∂ζ              1        2     2    1
 ∂t   +     ∂x       +     ∂y     =   −gh ∂x   + ghSx −   2 cf u(u     +v )   2



∂qy       ∂F vuh         ∂F vvh           ∂ζ              1                   1
 ∂t   +    ∂x       +     ∂y      =   −gh ∂y   + ghSy −   2 cf v(u2      2
                                                                       +v )   2




      qi qj
Fij =
       h
Numerical Scheme
 Upwind - First Order Accurate

ui = ui + O(∆)
ˆ                   if   ui > 0
                         ˆ

ui = ui+1 + O(∆)
ˆ                   if   ui < 0
                         ˆ

  ui   ui
       ˆ    ui+1    if   ui > 0
                         ˆ

  ui   ui
       ˆ    ui+1    if   ui < 0
                         ˆ
Initial Conditions


  In the basin:

• Constant water depth: d = 0.05 m
• No initial velocity: u = 0, v = 0
Boundary Conditions

  At the inlet and outlet:

• Periodic boundary conditions
  Along the walls:

• Non-penetrating
Periodic BCs
    h(0,j) h(1,j)                             h(imax,j) h(imax+1,j)



                  h(0, j) = h(imax , j)

                  h(imax+1 , j) = h(1, j)

                  qx (0, j) = qx (imax , j)

                  qx (imax+1 , j) = qx (1, j)




qx(0,j) qx(1,j)                        qx(imax,j)     qx(imax+1,j)
Uniform Flow Depth



          yo
So
     1
Governing Equations
                2D Shallow Water Equations

∂ζ        ∂qx        ∂qy
∂t    +   ∂x    +   h ∂x   =0

∂qx       ∂F uuh         ∂F uvh           ∂ζ              1        2     2    1
 ∂t   +     ∂x       +     ∂y     =   −gh ∂x   + ghSx −   2 cf u(u     +v )   2



∂qy       ∂F vuh         ∂F vvh           ∂ζ              1                   1
 ∂t   +    ∂x       +     ∂y      =   −gh ∂y   + ghSy −   2 cf v(u2      2
                                                                       +v )   2




      qi qj
Fij =
       h
Governing Equations
                2D Shallow Water Equations

∂ζ        ∂qx        ∂qy
∂t    +   ∂x    +   h ∂x   =0

∂qx       ∂F uuh         ∂F uvh           ∂ζ              1        2     2    1
 ∂t   +     ∂x       +     ∂y     =   −gh ∂x   + ghSx −   2 cf u(u     +v )   2



∂qy       ∂F vuh         ∂F vvh           ∂ζ              1                   1
 ∂t   +    ∂x       +     ∂y      =   −gh ∂y   + ghSy −   2 cf v(u2      2
                                                                       +v )   2




      qi qj
Fij =
       h
Governing Equations
               Momentum in x-direction



∂qx       ∂F uuh       ∂F uvh           ∂ζ              1        2     2    1
 ∂t   +     ∂x     +     ∂y     =   −gh ∂x   + ghSx −   2 cf u(u     +v )   2
Governing Equations
               Momentum in x-direction


      0
∂qx       ∂F uuh       ∂F uvh           ∂ζ              1        2     2    1
 ∂t   +     ∂x     +     ∂y     =   −gh ∂x   + ghSx −   2 cf u(u     +v )   2
Governing Equations
               Momentum in x-direction


      0       0             0
∂qx       ∂F uuh       ∂F uvh           ∂ζ              1        2     2    1
 ∂t   +     ∂x     +     ∂y     =   −gh ∂x   + ghSx −   2 cf u(u     +v )   2
Governing Equations
               Momentum in x-direction


      0       0             0                0
∂qx       ∂F uuh       ∂F uvh           ∂ζ              1        2     2    1
 ∂t   +     ∂x     +     ∂y     =   −gh ∂x   + ghSx −   2 cf u(u     +v )   2
Governing Equations
               Momentum in x-direction


      0       0             0                0                          0
∂qx       ∂F uuh       ∂F uvh           ∂ζ              1        2     2    1
 ∂t   +     ∂x     +     ∂y     =   −gh ∂x   + ghSx −   2 cf u(u     +v )   2
Governing Equations
 Momentum in x-direction




                1      2
       ghS0 =   2 cf u
Governing Equations
 Momentum in x-direction

                  1      2
       ghS0 =     2 cf u
            
                2ghS0
       u=         cf

              
                  2S0
       Fr =        cf


       F r = 0.5
Free Surface
Free Surface (Side Basin)
Velocity Field
Velocity (Magnitude)
Vorticity Field

      ×
   ω=∇ u
   

   ∂v   ∂u
ω=    −
   ∂x ∂y
Vorticity Field
Basin Resonance
       A
        1




        3
   B         B’

        2

        A’
Basin Resonance


                   2Γ                                                      k=0
          Tn =        √
               (k + 1) gd

                                                                           k=1




                                                                           k=2
Ref: Sorensen, R. M. (2006). Basic coastal engineering, Springer Verlag.
Transverse Section (A-A’)
 Height (m)
Height vs. Time At (1)
Height vs. Time At (1)
Height vs. Time At (1)  (2)
Longitudinal Section (B-B’)
Height (m)
Height vs. Time At (3)
Height vs. Time At (3)
Height vs. Time At (3)
Observations
• Oscillating flow mechanisms are often
  described by a Strouhal Number (S)
                 fn L
           S=     U

                         −1
           fn = 0.125s
           L = 3m
           U = 0.35m/s
           S = 1.1
Observations
• Vortex shedding at the leading edge of
  the basin

• Some vortices recirculate in the basin
  while others are entrained by the
  main flow.
• Resonant transverse flow oscillations
• As the transverse sloshing increases,
  so does the vortex shedding.
Questions ???


Thank you for your attention

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CIVE 572 Final Project Numerical Modeling of Open Channel Flow with a Side Basin