Fluids- Compressible Flow Flashcards

1
Q

At what sort of speeds does compressibility become significant?

A

Close to sound speed.

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2
Q

Rough sound speed in water?

A

1500m/s. Much faster than fastest submarines or underwater missiles

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3
Q

Formula for Mach number?

A

Ma=u/c
u is characteristic flow velocity
c is speed of sound in the fluid

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4
Q

Match different Mach numbers to types of flow

A

Under 0.3 is incompressible, density variation negligible.
Under 1 is subsonic flow, density effects are significant.
Around 1 is transonic flow, density effects and weak shock waves possible.
Over 1 is supersonic flow, density effects and shock waves possible.
Over 3 is hypersonic flow, strong shock waves possible.

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5
Q

Ideal gas law with density

A

P=ρRT

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6
Q

What is the ratio of specific heats (γ or k) for diatomic gases?

A

1.4 including for air

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7
Q

What is true about friction and heat exchange for isentropic processes?

A

No friction or heat exchange.

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8
Q

Express temperature, pressure and density before and after an isentropic process in terms of specific heat ratio

A

T2/T1=(ρ2/ρ1)^(γ-1)

P2/P1= (ρ2/ρ1)^γ = (T2/T1)^(γ/γ-1)

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9
Q

Formula for sound speed

A

c=rt(γRT)

Often around 340m/s in air

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10
Q

What is a stagnation point?

A

Where a streamline meets an object, around which the flow is passing, and all of the kinetic energy along the streamline is converted into pressure at this point.

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11
Q

How are stagnation conditions denoted?

A

With subscript o (zero)

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12
Q

Equation for stagnation temperature over static temperature

A

To/T=1+((γ-1)/2)Ma^2

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13
Q

Relation between stagnation and static pressure and density compared to that for temperature

A

Stag/stat=same for temp but
Pressure: to power of γ/γ-1
Density: to power of 1/γ-1

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14
Q

When are the critical conditions?

A

Properties when flow is sonic, Ma=1.

Denoted by subscript c or superscript *

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15
Q

Ratio of critical to stagnation temperature

A

T*/To=2/γ+1

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16
Q

Ratio of critical to stagnation pressure, density and sound speed in relation to that for temperature

A

Pressure: to power of γ/γ-1
Density: to power of 1/γ-1
Sound speed: to power of 1/2

17
Q

How to use stagnation to static relation without needing stagnation conditions

A

Use corresponding formula to find the ratio. Use the ratio for the initial property and the ration for the final property to eliminate stagnation and get relation between initial and final property.

18
Q

What is a nozzle?

A

A passage having variable section area designed to accelerate or decelerate a flow

19
Q

Where is back pressure?

A

The pressure outside of and after the nozzle exit

20
Q

How do flow properties in subsonic flow vary as area of nozzle increases?

A

P increases, T increases, ρ increases, velocity decreases, Ma decreases

21
Q

How do flow properties in supersonic flow vary as area of nozzle increases?

A

P decreases, temp decreases, density decreases, velocity increases, Ma increases.

22
Q

What is the maximum velocity in a converging nozzle?

A

Sonic velocity where Ma=1. This occurs at the exit plane (throat) of the nozzle.

23
Q

Describe converging-diverging nozzle and how it works

A

Attach a diverging flow section to the subsonic nozzle at the throat. If the flow at the throat is sonic, the diverging section can accelerate the flow so it is supersonic and result in Ma>1

24
Q

What can be said about the conditions of a fluid starting in a large tank or reservoir?

A

They are the stagnation conditions

25
Q

How to get ratio between critical and static conditions?

A

Product of critical over stagnation and stagnation over static.

26
Q

How to get formula for local nozzle area in relation to throat area

A

A/A*= product of critical over static ratios for density and velocity.
In compressible flow notes page14

27
Q

Formula for local flow velocity in isentropic flow

A

u=rt(2Cp(To-T))