Exit velocity of gas through two orifices

In summary, the study of exit velocity of gas through two orifices examines how gas flows through openings of varying sizes and shapes. It analyzes factors such as pressure, temperature, and orifice design that influence the velocity of gas as it exits. The findings provide insights into optimizing system performance in applications like fluid dynamics and engineering design, highlighting the importance of orifice configuration in controlling flow rates and efficiency.
  • #1
Albo
6
0
If a gas flowing through a tube would meet two orifices with different diameters in the same cross section, how much of the gas would flow through each orifice and what would the gas velocity be in dependence of orifice diameter?
 
Engineering news on Phys.org
  • #2
Welcome to PF.

Albo said:
If a gas flowing through a tube would meet two orifices with different diameters in the same cross section, how much of the gas would flow through each orifice and what would the gas velocity be in dependence of orifice diameter?
Do you mean 2 orifices in a flat cylindrical plate sealing the end of a tube? Can you show us a sketch? (use "Attach files" below the Edit window to upload a PDF or JPEG image)

Also, is this question for schoolwork? What do you think will happen to the flow through the 2 orifices?
 
  • #3
Hi! Thank you so much for the quick answer.

No the question isnt school related, i'm trying to develop a flow straightener element and trying to figure out the effect of combining different orifice sizes to the velocity profile and therefore the laminarity (if thats a word :D).

Yes you understood my question correctly! I'm thinking that the amount of gas flowing through each orifice is proportional to their cross sectional area. If i understand correctly tho the as the gas velocity through the orifice is antiproportional to the area the gas velocity through both orifices would be the same which suprised me. Just wanted to double check that i didnt mess something up
TwoOrificeProb.png
 
  • #4
Albo said:
Hi! Thank you so much for the quick answer.

No the question isnt school related, i'm trying to develop a flow straightener element and trying to figure out the effect of combining different orifice sizes to the velocity profile and therefore the laminarity (if thats a word :D).

Yes you understood my question correctly! I'm thinking that the amount of gas flowing through each orifice is proportional to their cross sectional area. If i understand correctly tho the as the gas velocity through the orifice is antiproportional to the area the gas velocity through both orifices would be the same which suprised me. Just wanted to double check that i didnt mess something upView attachment 333791
The head loss through each orifice would be the same as the other (as the orifices are in parallel). What system of equations did you solve to arrive at your conclusion?

EDIT: I assume you use:

$$ h_{l_1} = h_{l_2} $$

$$ h_l \approx \frac{ (V_o - V_u)^2}{2g} $$

Where ##V_o## is the orifice velocity, and ##V_u## is the velocity of the flow upstream.

$$ \frac{ (V_{o_1} - V_u)^2}{2g} =\frac{ (V_{o_2} - V_u)^2}{2g} $$

$$ \implies V_{o_1} = V_{o_2} $$

I wouldn't think it to be extremely precise, but perhaps its fine.
 
Last edited:
  • Like
Likes 256bits
  • #5
The distribution of the flow between the two orifices depends on the locations of the two orifices relative to one another and relative to the tube wall. This is a pretty complicated fluid mechanics problem, even for laminar flow.
 
  • Like
Likes Lord Jestocost, jack action and Lnewqban
  • #6
erobz said:
The head loss through each orifice would be the same as the other (as the orifices are in parallel).
How do you know that? Sorry if the answer to this question is straight forward but it isnt to me. Ofc the pressure at the outlet is the same for both orifices but wouldnt the pressure drop in the center of the orifice be different because its size dependent? Maybe im just confused.

Regarding your derivation: no i went much simpler and just assumed the orifices to be tubes (which they obviously are) with crossection A_1 and A_2. Then i assumed the volume flow through each tube is proportional to the area
-->
q1 = Q * A_1 / (A_1+A_2)
q2 = Q * A_2 / (A_1+A_2)

The velocity through a tube is then just the volume flow divided by the cross section
-->
v1 = q1/A_1
v2 = q2/A_2

This would always lead to
--> v1 = v2

Of course these assumptions are not true since im not accounting for pressure drop and since (like Chestermiller) said it depents strongly on orifice placement and relative position to the tube and so on... Im just looking for some qualitative feeling for it
 
  • #7
Chestermiller said:
The distribution of the flow between the two orifices depends on the locations of the two orifices relative to one another and relative to the tube wall. This is a pretty complicated fluid mechanics problem, even for laminar flow.
Yes that is true. For a real answer i would probably need some CFD simulations. But i dont want to go too much into detail with it and just find out experimentally if it works the way i want it too.

Basically my question originates from the problem: Which leads to a flow which is 'longer' 'stable' (laminar for a larger distance)?

(simplified ofc in top down view)

Version 1
1697729826159.png

or
Version 2
1697729778980.png
 
  • #8
Albo said:
How do you know that?
The approximate head loss for flow through an orifice? I looked it up in my textbook.

Or that the flows divide by head loss all other things equal?
Albo said:
Sorry if the answer to this question is straight forward but it isnt to me. Ofc the pressure at the outlet is the same for both orifices but wouldnt the pressure drop in the center of the orifice be different because its size dependent? Maybe im just confused.
I think it could ( and perhaps is by @Chestermiller ) be argued that it's an oversimplification and that ##V_{o_1} \neq V_{o_2}##.
 
  • #9
erobz said:
Or that the flows divide by head loss all other things equal?
Yeah this one. Which textbook are you referring to? id like to read it myself :)
 
  • #10
Albo said:
Yeah this one. Which textbook are you referring to? id like to read it myself :)
It's an "oldish" textbook now. Engineering Fluid Mechanics; Crowe, Elger, Williams, Roberson; 9th edition.
 
Last edited:
  • Like
Likes Albo
  • #11
Albo said:
Yeah this one.
Imagine you have a large pipe that splits into two of equal diameter. One of those pipes is 100 m long and the other is 1000 m long, they both eject to atmosphere without changing elevation. Your result says the flow divides equally (same areas), does that result seem reasonable to you?
 
Last edited:
  • #12
erobz said:
Imagine you have a large pipe that splits into two of equal diameter. One of those pipes is 100 m long and the other is 1000 m long, they both eject to atmosphere without changing elevation. Your result says the flow divides equally (same areas), does that result seem reasonable to you?
Interesting question and maybe this is where im confused. The pressure difference would be the same but the friction in the tube would slow down the gas in the longer tube more leading to a lower mass output, correct?
 
  • #13
Albo said:
Interesting question and maybe this is where im confused. The pressure difference would be the same but the friction in the tube would slow down the gas in the longer tube more leading to a lower mass output, correct?
Correct, there is more frictional work done on the flow in the longer tube. That equates to waste heat generation, which either warms the flow, or escapes via heat transfer to the environment. That extra heat is taken from the kinetic energy of the flows.

If you assume uniform flow properties over the cross section, you can write Work-Energy between the junction and each of the end points, the result is:

$$ \overbrace{\frac{V_1^2}{2g}}^{\text{kinetic head branch 1}} + \overbrace{\sum_{j \to 1} h_l}^{ \text{waste heat branch 1} }= \overbrace{\frac{V_2^2}{2g}}^{\text{kinetic head branch 2}} + \overbrace{\sum_{j \to 2} h_l}^{ \text{waste heat branch 2} } $$

The head loss in a branch can be found via Darcy-Weisbach:

$$ h_l = \frac{f L}{D} \frac{V^2}{2g} $$

Then you would use continuity ( incompressible flow ) to solve for the velocities (assuming the flow is slow enough to neglect effects compressibility - since you are considering "air" )

It should go without saying that there are obviously more refined flow models, but the idea should be fundamental.
 
Last edited:
  • Like
Likes Albo

FAQ: Exit velocity of gas through two orifices

What is the exit velocity of gas through an orifice?

The exit velocity of gas through an orifice is the speed at which the gas exits the orifice. It is influenced by factors such as the pressure difference across the orifice, the orifice size, and the properties of the gas.

How do you calculate the exit velocity of gas through an orifice?

The exit velocity of gas through an orifice can be calculated using the Bernoulli equation and the continuity equation. For an ideal gas, the simplified formula is \( v = \sqrt{\frac{2 \Delta P}{\rho}} \), where \( \Delta P \) is the pressure difference and \( \rho \) is the gas density.

What factors affect the exit velocity of gas through an orifice?

The exit velocity of gas through an orifice is affected by the pressure difference across the orifice, the size and shape of the orifice, the temperature and properties of the gas, and whether the flow is choked (sonic) or subsonic.

What is choked flow and how does it relate to exit velocity?

Choked flow occurs when the exit velocity of the gas reaches the speed of sound in the gas, limiting the maximum flow rate through the orifice. In this condition, further decreasing the downstream pressure does not increase the exit velocity.

How does the presence of two orifices affect the exit velocity of gas?

The presence of two orifices can affect the exit velocity depending on their arrangement (series or parallel) and the pressure conditions. In parallel, the flow rate divides between the orifices, potentially reducing the velocity through each. In series, the combined pressure drops and flow restrictions influence the exit velocity.

Back
Top