Potential Flow Lecture 5 ME EN 412 Andrew Ning aning@byu.edu - - PDF document

potential flow
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Potential Flow Lecture 5 ME EN 412 Andrew Ning aning@byu.edu - - PDF document

Potential Flow Lecture 5 ME EN 412 Andrew Ning aning@byu.edu Outline Equation Hierarchy Potential Flow Panel Methods Other Considerations Equation Hierarchy Equation Hierarchy When is an inviscid flow assumption valid? Video: flow over


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SLIDE 1

Potential Flow

Lecture 5

ME EN 412 Andrew Ning aning@byu.edu

Outline

Equation Hierarchy Potential Flow Panel Methods Other Considerations

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SLIDE 2

Equation Hierarchy Equation Hierarchy

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SLIDE 3

When is an inviscid flow assumption valid? Video: flow over a car

Potential Flow

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SLIDE 4

Incompressible: ∇ · V = 0 Irrotational: ∇ × V = 0

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SLIDE 5

∇2φ = 0

Velocity Field

  • V = ∇φ

⇒ Vx = ∂φ ∂x, Vy = ∂φ ∂y , Vz = ∂φ ∂z

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SLIDE 6

Uniform Flow

φ = U cos αx + U sin αy ψ = −U sin αx+U cos αy Vx = U cos α Vy = U sin α

Source/Sink

φ = Λ 2π ln r ψ = Λ 2πθ Vr = Λ 2πr Vθ = 0

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SLIDE 7
  • 1. Is my use of social media impeding or inviting

the constant companionship of the Holy Ghost in my life?

  • 2. Does the time I spend on social media restrict
  • r enlarge my capacity to live, love, and serve in

meaningful ways? – Elder Bednar With that understanding, I no longer needed lists of dos and dont’s. When I had to make a decision whether or not an activity was appropriate for the Sabbath, I simply asked myself, What sign do I want to give to God? That question made my choices about the Sabbath day crystal clear. – Elder Nelson

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SLIDE 8

φ = Γ 2πθ ψ = − Γ 2π ln r Vr = 0 Vθ = Γ 2πr

Doublet

φ = κ cos θ 2πr ψ = −κ sin θ 2πr Vr = −κ cos θ 2πr2 Vθ = −κ sin θ 2πr2

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SLIDE 9

Combine uniform flow and a source. Combine uniform flow and a doublet.

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SLIDE 10

Panel Methods

  • Dr. John C. Vassberg
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SLIDE 11

Other Considerations Vortex Motion

https://youtu.be/dfY5ZQDzC5s

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SLIDE 12

Ground Effect

Boeing Phantom Works

Streamlines ∇2Ψ(x, y) = 0

(only in 2D)