Lecture 5 Flashcards

(25 cards)

1
Q

What is the fundamental assumption in incompressible flow analysis?

A

The continuity equation ∇⋅𝑢=0, meaning the fluid density remains constant and there is no volumetric expansion or compression.

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2
Q

How does the Navier-Stokes equation simplify for unidirectional flows?

A

The nonlinear convective term 𝑢⋅∇𝑢 vanishes, making the equations linear.

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3
Q

What are some common types of unidirectional flows?

A

Pipe flow, Taylor-Couette flow, flow between plates, and rotating cylinder flow.

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4
Q

Why is the velocity component only in the primary flow direction for straight channels and pipes?

A

Because of translational symmetry along the primary flow axis, leading to no dependence on that coordinate.

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5
Q

What are the four types of pressure-driven pipe flows?

A

Steady pressure gradient with stationary boundaries, steady gradient with moving boundaries, time-dependent gradient with stationary boundaries, and time-dependent gradient with moving boundaries.

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6
Q

What is the vorticity equation, and why is it important?

A

t describes the evolution of vorticity due to viscous diffusion:
∂𝜔/∂𝑡=𝜈∇^2𝜔
It shows how vorticity diffuses over time due to viscosity.

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7
Q

What is the velocity profile for steady, pressure-driven pipe flow?

A

Parabolic, given by:
𝑢(𝑟)=𝑅^2/4𝜇𝐿 Δ𝑃(1−(𝑟/𝑅)2)

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8
Q

How does the volumetric flow rate Q depend on pipe radius?

A

Q∝R^4
according to the Hagen-Poiseuille equation:
𝑄=(𝜋𝑅^4/8𝜇𝐿)(Δ𝑃)

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9
Q

What is Darcy’s Law and when is it useful?

A

Q=(−k/μ)ΔP, useful for flow through porous media.

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10
Q

What is the Reynolds number and its significance in pipe flow?

A

Re= ρUR/μ
Re<2000 → laminar
Re>4000 → turbulent
2000<Re<4000 → transitional

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11
Q

What happens to the flow profile when the Reynolds number increases?

A

It transitions from parabolic (laminar) to a more uniform (turbulent) profile.

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12
Q

What is Stokes’ First Problem?

A

A suddenly moving plate in a viscous fluid generates a velocity field evolving due to vorticity diffusion

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13
Q

How does the velocity profile evolve over time?

A

The velocity follows:
𝑢(𝑦,𝑡)=𝑈erf(𝑦/sqrt(4𝜈𝑡))

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14
Q

What is the characteristic length scale for vorticity diffusion in this problem?

A

sqrt(νt), which grows over time.

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15
Q

How does shear stress at the plate scale with time?

A

τ∼μU/sqrt(νt)

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16
Q

How does vorticity behave away from the plate?

A

It exponentially decays, given by:
𝜔=(𝑈_0/sqrt(𝜋𝜈𝑡)) 𝑒^−(𝑦^2/4𝜈𝑡)

17
Q

What is Stokes’ Second Problem?

A

A plate oscillating sinusoidally in a viscous fluid.

18
Q

What is the characteristic penetration depth of the oscillatory motion?

A

δ=sqrt(v/ω)

19
Q

What is the velocity field in an oscillating flat plate problem?

A

u(y,t)=U_0e^(−y/δ) cos(ωt−y/δ).

20
Q

How does vorticity behave in this problem?

A

Confined to a boundary layer of thickness
𝑂(sqrt(𝜈/𝜔))

21
Q

What is pulsatile flow?

A

Flow driven by a periodic pressure gradient, important in applications like blood flow.

22
Q

What is the governing equation for pulsatile pipe flow?

A

The unsteady Navier-Stokes equation with a time-dependent pressure gradient.

23
Q

What is the Womersley number, and what does it represent?

A

Wo= R/(sqrt(ν/ω)), comparing inertial to viscous effects.

24
Q

What happens when 𝑊𝑜≪1?

A

Flow is quasi-steady, meaning it follows the pressure gradient closely.

25
What happens when 𝑊𝑜≫1?
Flow behaves like a solid-body oscillation, except for thin boundary layers near the walls.