Compressible Inviscid Flow 7 - Wave Propagation and Speed of Sound Flashcards

1
Q

What is a sound wave?

A

A weak perturbation propagating in space (isentropic)

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2
Q

Relationship between speed of sound and average molecular velocity

A

Proportional
Speed of sound is around 75% of the average molecular velocity
This is because the sound wave is propagated by molecular collisions
Compressibility becomes important when the flow velocity is comparable with the molecular velocity or speed of sound

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3
Q

How is the speed of sound variable?

A

Changes with temperature
Therefore changes with altitude

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4
Q

Define Mach number

A

Ratio of gas velocity to speed of sound
Most important non-dimensional parameter in compressible flows, making it possible to define subsonic, transonic, supersonic and hypersonic flows

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5
Q

Incompressible flow - Mach number and examples

A

M<0.3
Automotive
Liquid flow
Racing car

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6
Q

Subsonic flow - Mach number and examples

A

0.3<M<0.7
Light aircraft
Regional aircraft

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7
Q

Transonic flow - Mach number and examples

A

0.7<M<1.2
Flow field includes subsonic and supersonic regions even if flight speed is subsonic
Large transport aircraft (Airbus/Boeing)
Military aircraft

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8
Q

Supersonic flow - Mach number and examples

A

1.2<M<5
Concorde
Military aircraft
Missiles

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9
Q

Hypersonic flow - Mach number and examples

A

M>5
Spacecraft
Rockets
Space shuttle

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10
Q

Define total/stagnation conditions

A

If a fluid element is isentropically decelerated or stagnated to zero velocity, the resultant flow conditions at v=0 are the total conditions

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11
Q

Difference between static and total conditions

A

Static conditions are the actual fluid properties
The corresponding total state is achieved by an imaginary process where the fluid is reduced to rest isentropically
Total properties are another way of writing static properties to include flow velocity
In high pressure tank in a supersonic wind tunnel, total and static properties are the same as v=0

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12
Q

Total conditions for an adiabatic compressible process

A

Total enthalpy is constant
Therefore all other total constants are constant for a perfect gas

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13
Q

Total conditions for non-isentropic flows

A

Total conditions are viewed as local flow properties (e.g. total pressure can vary from point to point)

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14
Q

What is another way to view total pressure?

A

Capability of the flow to do useful work
Loss of total pressure is undesirable in engineering flow processes

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15
Q

What are critical conditions?

A

Sonic properties (i.e. putting M=1, sonic flow, into the relations)

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16
Q

Critical properties in isentropic flow

A

Constant

17
Q

Critical properties in adiabatic non-isentropic flow

A

Speed of sound and temperature are constant
Pressure and density may vary
This is because the first two relations only assume adiabatic condition

18
Q

Why is Bernoulli’s equation not applicable to compressible flows?

A

As Mach number increases, Bernoulli equation becomes less accurate as high order terms become larger
Bernoulli equation is the 1st order term of the Taylor expansion of the isentropic compressible flow relation at the low Mach number limit

19
Q

When is flow compressible?

A

Density ratio is 1 for incompressible flow
Density variation increases as Mach number increases
For M<0.3 the variation is <5%, close to incompressible flow

20
Q

Sound propagation in subsonic flow

A

Beeper (weak perturbation source) moves to left subsonically, M<1, v<a
Domain of disturbance moves with the wave front to infinite

21
Q

Wave propagation in supersonic flow

A

Beeper moves supersonically, M>1, v>a
Wave fronts form an envelope given by a straight line tangent to family of circles
This line/cone (3D) is the Mach wave front/Mach cone (3D), separating the domain of disturbance and domain and silence
This is why sonic boom sounds after supersonic aircraft passes overhead

22
Q

How are shock waves formed?

A

Strong perturbation waves are generated from all points on the aircraft surface
These waves pile up and coalesce, forming a standing wave (shock wave)

23
Q

Properties of shock waves

A

Extremely thin compression layer, typically of order 10^-4mm (0.1 micron)
Flow properties change drastically across the shock
Entropy increases across shock - physically irreversible process
Shock is adiabatic (no heat addition)
Total enthalpy and total temperature are unchanged across shocks

24
Q

When can a normal shock appear?

A

On aircraft wings at transonic speeds due to entropy increase

25
Q

Results of normal shocks

A

Reduced performance
Aerodynamic noise