Head loss due to sudden expansion

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Discussion Overview

The discussion centers on the head loss due to sudden expansion in fluid dynamics, exploring the derivation of related equations, assumptions regarding pressure, and the accuracy of these assumptions. Participants engage with theoretical aspects, practical applications, and experimental validations.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Experimental/applied

Main Points Raised

  • Some participants present the equation for head loss due to sudden expansion as Hl = (1/2g)*(v1-v2)^2, derived from Bernoulli, continuity, and momentum balance equations, questioning the assumption that pressure before and after the expansion is equal.
  • Others argue that the pressure just after the expansion is not equal to the pressure before, suggesting a different formulation involving pressure differences and correction factors.
  • One participant mentions an alternative expression for head loss, h_L=K_L*(V_1^2/2g), where K_L is defined in terms of the areas before and after the expansion, asserting that this matches experimental measurements.
  • Another participant shares their recent experimental findings that support the theoretical analysis of head loss, noting that the experimental value of K_L matched well with the analysis.
  • There is a discussion about the dimensional consistency of the equations presented, with participants clarifying the role of gravitational acceleration (g) in the equations.
  • Some participants express uncertainty regarding the accuracy of the pressure equality assumption used in deriving the head loss equations, suggesting that different pressure conditions could lead to different forms of the equations.
  • A participant inquires about practical values for K_L for use in calculations related to head loss in hydro plants, referencing guidelines from a penstock manual.
  • Another participant requests a derivation of the Darcy-Weisbach formula for head loss, indicating interest in further exploration of related concepts.
  • One participant challenges the interpretation of the pressure equality assumption, emphasizing its specific context in the momentum balance equation.

Areas of Agreement / Disagreement

Participants express differing views on the assumptions regarding pressure in the context of head loss due to sudden expansion, with no consensus reached on the accuracy of these assumptions or the preferred formulations of the equations.

Contextual Notes

The discussion highlights various interpretations of pressure conditions before and after an expansion, the dimensional analysis of equations, and the reliance on experimental data, indicating that assumptions may vary based on specific scenarios or applications.

Who May Find This Useful

This discussion may be useful for students, engineers, and researchers interested in fluid dynamics, particularly those focused on head loss calculations in practical applications such as hydro plants.

previah
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Hi all,

I'm sure a lot of you know about the head loss due to sudden expansion:

Hl = (1/2g)*(v1-v2)^2

This equation can be derived from Bernoulli, continuity and momentum balans equations. The underlying assumption in deriving this equation is that the pressure just after the expansion (say, p0) is equal to the pressure before the expansion (p1).

Now, I was wondering how accurate is this assumption? And what is the underlying physics behind this assumption?

best regards,
-Arman-
 
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previah said:
Hi all,

I'm sure a lot of you know about the head loss due to sudden expansion:

Hl = (1/2g)*(v1-v2)^2

This equation can be derived from Bernoulli, continuity and momentum balans equations. The underlying assumption in deriving this equation is that the pressure just after the expansion (say, p0) is equal to the pressure before the expansion (p1).
I don't see where you get the g from? Also, the pressure just after expansion isn't assumed to be the same as the pressure before. In fact, if a and b are just before and after the expansion,

\frac{p_a - p_b}{\rho} = \frac{a_b v_b^2 - a_a v_a^2}{2} + h_e

If you disregard the correction factors and use the momentum and continuity equation, you'll end up with

h_e = \frac{(v_a-v_b)^2}{2}
 
Well, the g should be there, otherwise the dimensions of your equation does not match:

m (n.e.) m^2/s^2

(how do you post an equation in a thread by the way?)

About the pressure: yes the (static) pressure is not the same between a and b. What I mean is the (static) pressure at border between small area and big area (so at position before b but just after a) is assumed to be equal to the (static) pressure at a. This is the underlying assumption in the momentum balans equation to get to the head loss equation I post earlier (it is far easier to explain if I can post a picture, but I do not know how).

best regards,
-Arman-
 
previah said:
Well, the g should be there, otherwise the dimensions of your equation does not match:

Well, they do match. Both the RHS and LHS of my equation has the dimension (m/s)^2

(how do you post an equation in a thread by the way?)
Click here for the tutorial thread. You can also click on the images to see the code.

About the pressure: yes the (static) pressure is not the same between a and b. What I mean is the (static) pressure at border between small area and big area (so at position before b but just after a) is assumed to be equal to the (static) pressure at a. This is the underlying assumption in the momentum balans equation to get to the head loss equation I post earlier (it is far easier to explain if I can post a picture, but I do not know how).
best regards,
-Arman-

I don't quite understand your question. To post a picture, look for the "manage attachments" button below the box where you type your text.
 
The expression for a sudden expansion that I am used to seeing is

h_L=K_L \left(\frac{V_1^2}{2g}\right)

where

K_L = \left(1-\frac{A_1}{A_2}\right)^2

According to my references, the sudden expansion is the only case in which the simple analysis actually matches actual measurements.
 
FredGarvin said:
The expression for a sudden expansion that I am used to seeing is

h_L=K_L \left(\frac{V_1^2}{2g}\right)

where

K_L = \left(1-\frac{A_1}{A_2}\right)^2

According to my references, the sudden expansion is the only case in which the simple analysis actually matches actual measurements.

Yeah, it's the same thing, with a factor of g throughout.

In fact, I did this very experiment in my momentum transfer lab this week, and the experimental value of k_l matched well with the analysis.
 
siddharth said:
In fact, I did this very experiment in my momentum transfer lab this week, and the experimental value of k_l matched well with the analysis.
Well, there we have it. I never did that particular experiment in my school days so it's nice to have real experimental back up to the books.
 
Bernoulli equation with pressure loss:

p_{1}+0.5\rho v_{1}^{2}=p_{2}+0.5\rho v_{2}^{2}+p_{L}

With p_{L} the pressure loss. The head loss, h_{L} can be computed by dividing the equation with \rho g, and after re-arranging:

h_{L} =\frac{p_{1}-p_{2}}{\rho g }+\frac{v_{1}^{2}-v_{2}^{2}}{2g }

Applying the momentum balans on the Control Volume between position 1 and 2 (see attachment):

p_{1}A_{1}+p_{0}\left(A_{2}-A_{1}\right)-p_{2}A_{2}=\rho \left(A_{2}v_{2}^{2}-A_{1}v_{1}^{2}\right)

And here when you make an assumption that the pressure p_{0} equals the pressure p_{1}. And after using continuity equation the equation becomes:

\frac{p_{2}-p_{1}}{\rho g }=\frac{v_{2}\left(v_{1}-v_{2}\right)}{g}

Fill this into the expression of the head loss (second equation), voila, you get the head loss due to sudden expansion:

h_{L} =\frac{\left(v_{1}-v_{2}\right)^{2}}{2g }

Now, this expression of the head loss is derived after we make an above mentioned assumption regarding the pressures. How accurate is this assumption then? I mean if the two pressures are not the same, the equation will have different form.

best regards,
-Arman-
 

Attachments

actually, the "head" has dimensions of length ...
 
  • #10
hi all..
i wanted to know the value of "k" for practical uses. i was calculating head loss in expansion after main inlet valve in hydro plant.
Going by penstock manual from Central water commission, New Delhi, the value of k =(1-a1/a2)sin(theta)
where ;
theta=one half of flare angle, a taper of 1:10 is recommended.
Some colleague say the value of k is to be taken from practical values or practical charts.
help
 
Last edited:
  • #11
can anyone derive for me the darcy weisbach formula for head loss
 
  • #12
Long time passed since your question, Dear previah
This is for the people who is concerned to head loss in sudden expansioning.

I am sure you're misunderstanding the underlying pressure equality assumption.

This assumption says "the pressure at the annular area, A2-A1,is equal to the pressure in A1" for the calculation of pressure difference perpendicular to control volume. This annular area contacts turbulent eddies.

So, as you say, " the pressure just after the expansion (say, p0) is equal to the pressure before the expansion (p1)" has completely different meaning.
 

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