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Study of flow over permeable bed
Presented by:
Narendra Kumar Patel
Advisors:
Junke Guo and David Admiraal
Department of Civil Engineering
Introduction
• Usually permeable bed is treated as solid surface and classical
logarithmic profile is generated with no-slip condition. However, at
porous bed surface, velocity is non-zero.
Porous Medium
Open Channel
Flow
Y
X
h
𝛅
uB
Introduction
• Research Objectives
• Determination of velocity profile
• Determination of transitional layer thickness
• To study the effect on flow capacity of channel with porous bed for different
types of flow
Approaches
• Theoretical
• Numerical
• Experimental
Theoretical Approach
• Steady, uniform flow above the bed can be solved using Navier-Stokes
equation and Darcy’s equation can be used for flow through the bed.
µ
𝑑2 𝑈
𝑑𝑦2 =
𝑑𝑝
𝑑𝑥
…. N-S equation
−
µ
𝑘
𝑈 =
𝑑 𝑝
𝑑𝑥
…. Darcy’s laws
• N-S is second order ODE and Darcy’s eq. is first order which makes
impossible to formulate rational boundary conditions.
Theoretical Approach
• Navier-Stocks Forchheimer Equation
• Laminar flow: In Bed =>
cn is Jacobi elliptic cosine function, F is elliptic integral of first kind
Above the bed=>
• Turbulent Flow: In Bed ->
Above the bed=>
Numerical Approach
• All governing equations are solved numerically in Ansys Fluent
software
• Equations are solved by computational fluid dynamics (CFD)
techniques
Numerical Approach
• Volume of fluid (VOF) result
Numerical Approach
• Velocity profile above bed at different porosity
Slope=3°, grain size=2mm, Bed thickness= 10cm
0.1
0.12
0.14
0.16
0.18
0.2
0.22
0.24
0.26
0.28
0 0.2 0.4 0.6 0.8 1 1.2
Depth,m
Velocity, m/s
Velocity Profile
P=0.2
P=0.4
P =0.6
Bed Level
Experimental Approach
• Flume is 48 ft long, 40cm wide and 50cm deep.
• Slope, flow rate, depth can be varied and velocity, discharge can be
measured
Experimental Approach
• Flow velocity above the bed is measured using Acoustic Doppler
Velocimetry (ADV).
Experimental Approach
• A fiber optics based sensor is developed to measure flow velocity in
sand bed
• Tracer is injected and Refractive index is measured to determine the
at two locations to determine velocity
Conclusions
• Theoretically, velocity profile over porous bed can be represented by
Jacobi elliptic function
• Slip velocity increases as porosity increases and maximum velocity
decreases.
• Flow capacity of channel decreases as bed porosity increases
Thank You
Questions ?
waterforfood.nebraska.edu

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18) Narendra Patel

  • 1. Study of flow over permeable bed Presented by: Narendra Kumar Patel Advisors: Junke Guo and David Admiraal Department of Civil Engineering
  • 2. Introduction • Usually permeable bed is treated as solid surface and classical logarithmic profile is generated with no-slip condition. However, at porous bed surface, velocity is non-zero. Porous Medium Open Channel Flow Y X h 𝛅 uB
  • 3. Introduction • Research Objectives • Determination of velocity profile • Determination of transitional layer thickness • To study the effect on flow capacity of channel with porous bed for different types of flow
  • 5. Theoretical Approach • Steady, uniform flow above the bed can be solved using Navier-Stokes equation and Darcy’s equation can be used for flow through the bed. µ 𝑑2 𝑈 𝑑𝑦2 = 𝑑𝑝 𝑑𝑥 …. N-S equation − µ 𝑘 𝑈 = 𝑑 𝑝 𝑑𝑥 …. Darcy’s laws • N-S is second order ODE and Darcy’s eq. is first order which makes impossible to formulate rational boundary conditions.
  • 6. Theoretical Approach • Navier-Stocks Forchheimer Equation • Laminar flow: In Bed => cn is Jacobi elliptic cosine function, F is elliptic integral of first kind Above the bed=> • Turbulent Flow: In Bed -> Above the bed=>
  • 7. Numerical Approach • All governing equations are solved numerically in Ansys Fluent software • Equations are solved by computational fluid dynamics (CFD) techniques
  • 8. Numerical Approach • Volume of fluid (VOF) result
  • 9. Numerical Approach • Velocity profile above bed at different porosity Slope=3°, grain size=2mm, Bed thickness= 10cm 0.1 0.12 0.14 0.16 0.18 0.2 0.22 0.24 0.26 0.28 0 0.2 0.4 0.6 0.8 1 1.2 Depth,m Velocity, m/s Velocity Profile P=0.2 P=0.4 P =0.6 Bed Level
  • 10. Experimental Approach • Flume is 48 ft long, 40cm wide and 50cm deep. • Slope, flow rate, depth can be varied and velocity, discharge can be measured
  • 11. Experimental Approach • Flow velocity above the bed is measured using Acoustic Doppler Velocimetry (ADV).
  • 12. Experimental Approach • A fiber optics based sensor is developed to measure flow velocity in sand bed • Tracer is injected and Refractive index is measured to determine the at two locations to determine velocity
  • 13. Conclusions • Theoretically, velocity profile over porous bed can be represented by Jacobi elliptic function • Slip velocity increases as porosity increases and maximum velocity decreases. • Flow capacity of channel decreases as bed porosity increases