Nominal Linear Velocity Gas flow

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Discussion Overview

The discussion revolves around calculating the nominal linear velocity of a gas flow in a complex system involving a nebulising gas. Participants explore the relationship between flow rate, tube dimensions, and velocity, particularly focusing on achieving a target velocity of 350 m/s for nitrogen gas flowing through an annular tube configuration.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant describes a system with a nebulising gas aiming for a linear velocity of 350 m/s, expressing confusion over calculations involving flow rate and tube dimensions.
  • Another participant questions the feasibility of achieving 350 m/s, noting that this speed is around the speed of sound for many gases.
  • Participants discuss the importance of using the correct cross-sectional area for calculations, suggesting that the gas flows through the annulus rather than the internal tube.
  • Calculations are presented showing that the current flow velocity is approximately 76 m/s, with further calculations indicating a maximum achievable flow velocity of around 104.7 m/s under certain conditions.
  • There is mention of compressibility effects becoming significant at velocities exceeding 0.3 Mach, with participants calculating Mach numbers based on flow velocities.
  • Some participants propose that the author of a referenced paper may have made an error regarding the gas flow velocity, suggesting it could pertain to the liquid flow instead.
  • Discussion includes the implications of reaching choked flow conditions when the outlet velocity reaches Mach 1, affecting maximum mass flow rates.

Areas of Agreement / Disagreement

Participants express uncertainty regarding the accuracy of the target velocity of 350 m/s, with some suggesting it may not be achievable based on current calculations. There is no consensus on the correct interpretation of the referenced paper or the maximum achievable flow rates.

Contextual Notes

Participants highlight the complexity of the system and the calculations involved, noting that assumptions about compressibility and flow dynamics may affect the results. The discussion remains open regarding the specific conditions under which the calculations apply.

Who May Find This Useful

This discussion may be useful for individuals working on gas flow systems, particularly in applications involving nebulisation, fluid dynamics, and those interested in the effects of compressibility on gas flow velocities.

Jamesan89
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Hello, thanks in advance for your help,

I am not a physicist, however have a fairly good grasp on mathematics, also this isn't homework or an assignment but a real world problem.

Currently trying to create a system with a nebulising gas at a linear velocity of 350 m/s. The calculations confusing me as the system is complex. The gas flow is through a 100 mm, doughnut shaped tube with an 363 um diameter centre and a 508 um total diameter. The gas flow is currently at 450 ml/min (using a gas flow meter).

My solution would be to convert the flow rate to ml/s (7.5 ml/s) and take the volume of the tube in m^3 by Pi*R^2*h and divide these values, however the output value is clearly not correct. A point in the right direction would be greatly appreciated .
 

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Please explain configuration a bit more . Also confirm the 350 m/s speed .
 
The nominal linear velocity I aim to achieve is 350 m/s, I am trying to work out if I am close to achieving this speed for the gas flow.

As for the configuration the gas is a sheath gas flow down the outer tube with a liquid flowing down the inner tube, therefore I really need to know the gas flow required (currently 450 ml/min) to achieve the desired linear velocity.
 
350 metres/sec is around speed of sound for many common gasses so there could be problems in achieving this speed .
 
We can start in a different place and derive an achievable velocity . What is pressure at inlet and outlet of annular tube and what is actual gas in use ?
 
The gas is nitrogen and the pressure at the inlet is 7 bar, I am unsure however of the pressure at the outlet of the tube. The nitrogen gas is at the highest pressure achievable using the labs equipment.

After doing some maths and thinking, would I be correct in saying the velocity of the gas currently is 76 m/s. I am starting to wonder whether 350 m/s is an error if its around that speed!
 
I will attach a paper and put this more into context, the linear velocity value of 350 m/s is found at the bottom right hand corner of the page
 

Attachments

See message .
 
Jamesan89 said:
Hello, thanks in advance for your help,

I am not a physicist, however have a fairly good grasp on mathematics, also this isn't homework or an assignment but a real world problem.

Currently trying to create a system with a nebulising gas at a linear velocity of 350 m/s. The calculations confusing me as the system is complex. The gas flow is through a 100 mm, doughnut shaped tube with an 363 um diameter centre and a 508 um total diameter. The gas flow is currently at 450 ml/min (using a gas flow meter).

My solution would be to convert the flow rate to ml/s (7.5 ml/s) and take the volume of the tube in m^3 by Pi*R^2*h and divide these values, however the output value is clearly not correct. A point in the right direction would be greatly appreciated .
It's not clear what you are doing here.

The continuity equation for fluid flow is Q = A*V, where Q is the flow rate, A is the cross sectional area of the conduit, and V is the flow velocity.

For tube ID = 0.363×10-3 m, A = 1.03×10-7 m2
flow rate Q = 7.5×10-3 l/s = 7.5×10-6 m3/s

flow velocity V = Q / A = 72.5 m/s

Once the velocity of a gas exceeds about 0.3 Mach (0.3 times the speed of sound), compressibility effects become significant.

The speed of sound in nitrogen at standard conditions is about 349 m/s. Therefore, your flow velocity has a Mach No. = 72.5 / 349 = 0.21, so the flow can be treated as incompressible for all practical purposes.
 
  • #10
Just a quick observation, according to the drawing the gas is flowing through the annulus rather than the internal tube and it appears to me you have used the tube's ID in the above calc.
 
  • #11
JBA said:
Just a quick observation, according to the drawing the gas is flowing through the annulus rather than the internal tube and it appears to me you have used the tube's ID in the above calc.
Then use the area of the annulus to calculate the velocity instead of the area of the tube.

The point is, Q = A*V is the correct formula to use, rather than what was described in the OP.

For the annulus, the ID = 0.363×10-3 m, OD = .508×10-3 m,
Annular area, A = 9.92×10-8 m2
flow rate Q = 7.5×10-3 l/s = 7.5×10-6 m3/s

flow velocity V = Q / A = 75.6 m/s

Mach No. = 75.6 / 349 = 0.22 which is still less than M = 0.3, so the flow can be assumed to be incompressible.
 
  • #12
Thanks for your messages and help with simplifying the calculations, I think the author of the paper must have made a mistake or have been referring to the liquid flow through the internal tube. The Gas flow is indeed going through the annulus.

From your reply the maximum flow I could expect to be achievable for my system would be
M = 0.3(max) so V = 349 * 0.3 = 104.7 m/s
Q = V * A s so Q = 104.7 m/s * 9.92x10^-8 m^2 = 1.04x10^-5 m^3/s or 624ml/min.
 
  • #13
Jamesan89 said:
Thanks for your messages and help with simplifying the calculations, I think the author of the paper must have made a mistake or have been referring to the liquid flow through the internal tube. The Gas flow is indeed going through the annulus.

From your reply the maximum flow I could expect to be achievable for my system would be
M = 0.3(max) so V = 349 * 0.3 = 104.7 m/s
Q = V * A s so Q = 104.7 m/s * 9.92x10^-8 m^2 = 1.04x10^-5 m^3/s or 624ml/min.

You can put more gas thru the tube, it's just that the calculations get more complicated due to the effects of compressibility. When the outlet velocity reaches M = 1, then the flow becomes choked, and the maximum mass flow is obtained. The length of the tube and the ratio of the inlet and outlet pressures all factor into what this maximum mass flow number actually is.
 

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