Fluid Kinematics Flashcards

1
Q

Define fluid particles

A

Points within the continuum that are moved by particle motion

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2
Q

Define the continuum model of fluids

A

A model where the fluid is defined as some continuous medium made up of fluid parcels.

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3
Q

Define fluid parcels

A

An infinitesimal portion of the continuum which contains an average of the properties of the fluid inside it.

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4
Q

Define the Eularian picture

A

Where fluid particles are labelled by their current position x.

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5
Q

Define the Lagrangian picture

A

Where fluid particles are labelled by their initial position a.

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6
Q

Define particle path (or trajectory). Which picture does this represent?

A

The path of a particle x(a,t) parametetrised by its initial position a and time t. Eulerian picture.

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7
Q

Define the time derivatives for the Eularian and Lagrangian pictures

A

(partial/partial t) holding x and a constant respectively. Denoted by (partial/partial t) and D/Dt respectively.

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8
Q

Define the material (or convective) derivative

A

The Lagrangian derivative of an Eulerian function, where we consider the rate of change of the function moving with the fluid.

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9
Q

Give (and explain) the two criteria for a particle path

A

Continuous and invertible, such that we can determine the initial position of a passing through x at time t.

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9
Q

Define particle velocity

A

The Lagrangian derivative of particle position x.

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10
Q

Define material curve

A

A line which threads through a subset of fluid elements x at time t and moves with them.

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11
Q

Define a streamline

A

The integral curve of Eulerian velocity u(x,t) at a fixed time. Streamlines satisfy the differential equation:
dx/ds = u(x(s),t)

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12
Q

Given a velocity field, compare the methods for finding streamlines and particle paths.

A

Streamlines - integrate with respect to some dummy variable s, defining initial particle positions as x_0, y_0, z_0.

Particle paths - integrate with respect to time and , defining initial particle positions as a,b,c.

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13
Q

State the case where streamlines and particle paths coincide

A

Where the flow is steady (not dependent on time).

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14
Q

Define a stream function (and the two conditions under which it can be defined)

A

A scalar function ψ(x,y,t) whose grad describes u when it is two-dimensional and divergence free.

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15
Q

Give the volume flow rate (per unit height) between to fluid particles.

A

The difference in the stream function evaluated at the location of the fluid particles i.e. psi(x_2)-psi(x_1).

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16
Q

Is the volume flow rate independent of the curve connecting the fluid particles? Why?

A

Yes: the flow is conservative and so independent of the curve.

17
Q

Define a streakline

A

A line formed from all the fluid elements passing through a point (a,b) between some t=0 and t>0.

18
Q

How do we determine streaklines

A

Find the particles paths, introducing parameter epsilon (between 0,t) such that a fluid particle passes through (a,b) at t=epsilon. Substitute the integration parameters this gives, into the particle paths.

19
Q

Describe how the Jacobian relates Lagrangian and Eulerian pictures

A

The Jacobian defines how a line segment connecting two adjacent fluid particles at t=0 evolve with time. In three dimensions, it describes how the volume of a fluid parcel evolves with time.

20
Q

Give (and explain) a constraint on the Jacobian

A

J cannot =0, since we require the map to be invertible.

21
Q

Define an incompressible flow

A

A flow which preserves the volume of every material subregion in the fluid domain D_t.

22
Q

Define a material scalar (or Lagrange invariant)

A

A function which has a zero material (or convective) derivative Df/Dt = 0

23
Q

Given a function f(x(a,t), t), give the material derivative and describe.

A

Df/Dt = ∂f/∂t + u · ∇f

LHS: Lagrangian
RHS: Eulerian
Found by chain rule

24
Q

Give the expression for the Jacobian relating E and L pictures

A

dx dy dz = J da db dc

25
Q

What are the Jacobian and divergence of an incompressible flow?

A

J = 1 and ∇ · u = 0.

26
Q

What is the relative change in jacobian J moving with the fluid?

A

1/J DJ/Dt = ∇ · u

27
Q

Define local analysis

A

Considering two neighboring points of the flow x + δx

28
Q

Define velocity gradient tensor

A

The tensor ∇u(x)_ij = = ∂u_i/∂x_j which defines the local structure of the velocity field

29
Q

What three flow components do we find in local analysis?

A

Body translation across Dt given by u(x,t)

Stretching/compression of Dt from symm part ∇u(x).

Rotation of Dt from anti-symm part of ∇u(x).

30
Q

Define vorticity

A

The pseudo-vector ω = ∇ × u

31
Q

Define circulation

A

The integral of u · dl around a closed curve γ

32
Q

State Stoke’s theorem

A

The integral of a function around closed loop γ is equivalent to the curl of the function through the surface enclosed by the loop

33
Q

Define a vortex tube

A

A bundle of vortex lines: the streamline analogue for vorticity; an integral curve of ω(x, t) at fixed time.

34
Q

Give Helmholtz’ rule for vortex tubes

A

If γ1 and γ2 are two closed curves encircling a vortex tube, their circulation is equal.

35
Q

Briefly describe ‘flow reconstruction’

A

Recovering an incomp velocity from a vorticity, knowing the velocity is not unique.

I.e. u and u’ := u + ∇φ have the same vorticity field.

36
Q

What are the boundary conditions for flow reconstruction?

A

∆φ = 0
n · (∇φ + u_v) = 0

37
Q

Define the method of images for flow reconstruction

A

Adding addition vortices which ensures the boundary condition, since BS is linear in w.

38
Q

What is the trick for differentiating over a changing volume?

A

Express integral in Lagrangian coords (over fixed volume D0 at t=0), diff and then re-express in Eulerian.

39
Q

What does circulation define for a vortex tube?

A

The ‘strength’ of the vortex tube; invariant along its length.

40
Q

State the divergence theorem

A

The volume integral of the divergence of a function is equivalent to the function flowing through a surface.