Dynamics of Ideal Fluids Flashcards

1
Q

State the simple conservation of mass formula

A

d/dt INT_Dt ρ dV = 0

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2
Q

State the simple conservation of momentum formula

A

d/dt INT_Dt ρu dV

ρu = F with no d/dt

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3
Q

How can we derive the continuity equation?

A

Apply transport theorem to the conservation of mass

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4
Q

How do we describe the force on a fluid

A

The sum of some body force ρf and some surface force/unit area or stress σ · dS acting on the boundary

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5
Q

Define idea (inviscid) fluid

A

A fluid which neglects internal friction/viscosity between neighboring fluid elements.

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6
Q

Give the stress tensor for an ideal fluid

A

σij = −pδij

Any cross terms would correspond to tangential shears which are neglected in inviscid fluid model.

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7
Q

State the momentum equation

A

∂u/∂t + (u · ∇)u = f − 1/ρ ∇p

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8
Q

How are the incompressible Euler equations characterised?

A

By constant density ρ = ρ0

Incomp since continuity reduces to ∇ · u = 0

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9
Q

State the continuity equation

A

∂ρ/∂t + ∇ ·ρu = 0

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10
Q

What boundary conditions do we have for incomp Euler?

A

u·n = 0

No flow through boundaries

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11
Q

State the conservative KE proposition

A

In a fixed volume (V) with u · n = 0, the incompressible Euler equations with a conservative body force f = −∇U conserve kinetic energy.

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12
Q

Give the expressions for conservation of KE

A

dE/dt = 0

E = 1/2 INT_V ρ0|u|^2dV

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13
Q

Do we use transport theorem in conservation of KE?

A

No, we consider a fixed volume, rather than material curve.

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14
Q

State the Bernoulli function

A

B(x, t) = p/ρ0 + 1/2 |u|^2 +U

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15
Q

State Bernoulli’s theorem

A

In an incompressible steady flow of an ideal fluid, with conservative body force f = −∇U, the Bernoulli function is constant along streamlines

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16
Q

What are the conditions for time-dependent Bernoulli?

A

∇ × u = 0 and ∇ · u = 0

17
Q

State the vorticity equation (E)

A

∂ω/∂t + ∇ × (ω × u) = 0

18
Q

How do we find the vorticity equation?

A

Take the curl of the ideal momentum equation

19
Q

State the vorticity equation (L)

A

Dω/Dt = (ω · ∇)u

20
Q

Define helicity

A

The amount of ‘linkage’ between vortex lines in fluid flow

21
Q

What is the condition for conserved helicity and give equation

A

ω ·n = 0 on ∂V surface we have

dH/dt = 0

H = INT_V u·ω dV

22
Q

State Kelvin’s theorem

A

In an ideal, incompressible fluid with conservative body force, the circulation around a closed material curve γt is constant in time.

23
Q

How do we (generically) show time constance?

A

By getting the expression to look like a divergence theorem which vanishes due to ideal-ness of fluid.

24
Q

What do the indices σij of a stress tensor indicate?

A

i indicates the direction of the force and j indicates the surface

25
Q

How do we derive the momentum equation?

A

Use the div theorem on conservation of force and apply transport.

26
Q

Given a velocity, how can we find a pressure?

A

Take the divergence of the momentum equation

27
Q

How does time-dependent Bernoulli differ from std?

A

Replace u with ∇ϕ and add a ∂ϕ/∂t term

28
Q

How does vorticity behave in 2d?

A

It is a material scalar; it cannot increase and decrease but it can move around.