6. Bernoulli's Equation Flashcards
The Bernoulli Function
Η(|x,t) = p/ρ + 1/2||u||² - |g.|x
The Bernoulli Equation
(|u . ∇) Η = 0
Bernoulli Function for an Ideal Fluid in Steady Flow
-for an ideal steady flow, the Bernoulli function:
Η(|x,t) = p/ρ + 1/2||u||² - |g.|x
-is constant along a streamline
Streamfunction and Bernoulli Function
-if a streamfunction ψ(|x) can be defined, Η is a function of ψ:
Η(|x) ≡ Η(ψ)
Bernoulli’s Theorem for Irrotational Flows
-for irrotational flows,
∂φ/∂t + Η = ∂φ/∂t + p/ρ + 1/2||∇φ||² - |g.|x
-is a function of time f(t), independent of position |x
Bernoulli’s Theorem for Steady, Irrotational Flows
-if the flow is steady as well as irrotational,
Η = p/ρ + 1/2||∇φ||² - |g.|x
-is constant, i.e. Η has the same value on all streamlines
Write down the velocity potential of a uniform stream U ^ez past a stationary sphere of radius a
-in cylindrical polar coordinates:
φ(r,z) = Uz(1 + a³/[2(r²+z²)^(3/2)]
-in spherical polar coordinates:
φ(r,z) = Ucosθ(r + a³/2r²)
D’Alembert’s Paradox
- it can be demonstrated that the drag force on any 3D solid body moving at uniform speed in a potential flow is zero
- in reality this is not true in reality since flows past 3D solid bodies are not potential
What is the pressure distribution on the surface of a solid sphere placed in a uniform stream?
p(θ) = p∞ + 1/2 ρU²(1 - 9/4 sin²θ)
Separation and Pressure
- an adverse pressure gradient, (|u.∇)p > 0
(i. e. pressure increasing in the direction of the flow along the surface) is bad news, it causes the flow to separate leaving a turbulent wake
How to reduce drag?
- the way to reduce drag is to reduce separation
- this can be done in two ways:
1) streamlining
2) surface roughness
Streamlining
- separation occurs because of adverse pressure gradients on the surface of solid bodies
- these can be reduced by using more ‘streamlined’ shapes that avoid diverging streamlines
Surface Roughness
-paradoxically, a rough surface can reduce drag by reducing separation
Bubble Oscillations
- the sound of a ‘babbling brook’ is due to the oscillation of air bubbles entrained into the stream
- the pitch depends on the size of the bubbles
What is the velocity potential for a sphere of radius a moving with velocity U in still water?
φ = - Ua³/2r² * cosθ