Lecture 2 Flashcards

(19 cards)

1
Q

What is the goal of dimensional analysis in fluid mechanics?

A

Dimensional analysis helps to simplify problems by identifying key variables and their relationships based on dimensions, reducing the complexity of equations and revealing fundamental scaling laws.

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2
Q

What are the dimensions of dynamic viscosity (ΞΌ)?

A

[ΞΌ]=M/LT

Where 𝑀 is mass, L is length, and 𝑇 is time.

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3
Q

How is shear stress related to viscosity?

A

Ο„=ΞΌ du/dy
​
which represents the force per unit area exerted due to viscosity.

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4
Q

What is the significance of the Buckingham Pi theorem?

A

It states that a problem with 𝑛 variables and π‘Ÿ fundamental dimensions has π‘›βˆ’π‘Ÿ independent dimensionless groups, which helps in reducing experimental and theoretical complexity.

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5
Q

How can dimensional analysis be used to estimate the time for an object to fall under gravity?

A

By balancing length 𝐿, gravity 𝑔, and time 𝑇, the characteristic time scale is:
π‘‡βˆΌ(𝐿/𝑔)^(1/2)
which gives an estimate of how long it takes an object to hit the ground.

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6
Q

What is the Reynolds number and why is it important?

A

Re=ρUL/μ
It determines the flow regime: low 𝑅𝑒 indicates laminar flow, while high 𝑅𝑒 suggests turbulent flow.

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7
Q

What is the relationship between flow rate and pressure drop in laminar pipe flow?

A

sing dimensional arguments:
π‘„βˆ(𝑅^4Δ𝑃)/πœ‡πΏβ€‹
which follows from the Hagen-Poiseuille equation.

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8
Q

What does the term β€œnatural time scale” refer to in fluid mechanics?

A

It is the characteristic time of a system, obtained via dimensional analysis, that determines the timescale of a flow process.

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9
Q

How can the time scale of oscillations in a spring-mass system be determined dimensionally?

A

By balancing force terms in:

π‘šπ‘₯Β¨+π‘˜π‘₯=0
the characteristic time is:
𝜏∼sqrt(π‘š/π‘˜)

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10
Q

What assumption allows for the thin-film approximation?

A

The assumption that the film height β„Ž is much smaller than the lateral dimensions, allowing simplifications in governing equations.

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11
Q

What is the governing equation for the height profile β„Ž(π‘Ÿ,𝑑) of a spreading axisymmetric drop?

A

βˆ‚h/βˆ‚t=Ξ»1/r * βˆ‚/βˆ‚r(h^nrβˆ‚h/βˆ‚r)

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12
Q

How does the spreading radius of a drop scale with time?

A

Using mass conservation and the governing PDE, the radius increases as:

𝑅(𝑑)βˆΌπ‘‘^1/8

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13
Q

How is the pressure field determined in the thin-film approximation?

A

By integrating the vertical momentum equation, the pressure field is:

𝑝(π‘Ÿ,𝑧,𝑑)=𝑝_0+πœŒπ‘”[β„Ž(π‘Ÿ,𝑑)βˆ’π‘§]

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14
Q

What is the velocity profile for a thin film spreading under gravity?

A

The velocity in the radial direction is:

𝑒_π‘Ÿ(π‘Ÿ,𝑧,𝑑)=(πœŒπ‘”/2πœ‡)(βˆ‚β„Ž/βˆ‚π‘Ÿ) 𝑧[π‘§βˆ’2β„Ž(π‘Ÿ,𝑑)]
which satisfies no-slip at the base and zero shear at the free surface.

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15
Q

What condition must the vertical velocity satisfy at the free surface?

A

Since fluid particles remain on the free surface, the kinematic boundary condition gives:

𝑒_𝑧 from (𝑧=β„Ž) =π‘’π‘Ÿ from (𝑧=β„Ž) (βˆ‚β„Ž/βˆ‚π‘Ÿ)+(βˆ‚β„Ž/βˆ‚π‘‘)

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16
Q

How does the falling speed of a cylindrical plug depend on the gap width πœ–?

A

By balancing forces (gravity, pressure gradient, and viscous resistance), the velocity scales as:

π‘ˆβˆπœ–^𝛽

where 𝛽≠2

17
Q

How can the viscosity πœ‡ΞΌ of a fluid be estimated using the falling plug method?

A

Using known geometry and weight of the plug, πœ‡ can be extracted from measurements of π‘ˆ with an error of 𝑂(πœ–)

18
Q

What equation describes vorticity diffusion?

A

By taking the curl of the momentum equation, vorticity πœ” satisfies: βˆ‚πœ”/βˆ‚π‘‘=πœˆβˆ‡2πœ”

19
Q

What is the physical significance of vorticity in fluid mechanics?

A

Vorticity represents the local rotation of fluid elements