Asking for help with a physical problem that uses a piston to push water

In summary, the figure shows that F is the external force oriented to the left on the outside face of the piston.
  • #1
vxiaoyu18
93
13
Homework Statement
One of my own problems.
Relevant Equations
F=ρgHS
Consult a physical problem that USES piston to absorb water:
Pistons with surface areas S1, S2 and S are placed horizontally at the same height (H).
S1 = S2
S=S1+S2
When F starts moving to the left, how do you calculate its force?
Is F=ρgHS?
(*The friction force doesn't have to be calculated.)

jsshui.jpg
 
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  • #2
The easiest approach is via conservation of energy. Figure out how much water moves from where to where as function of the displacement, that gives you the force.

You can also note that S1, S2, S always have a fixed relative orientation. The water between them doesn't matter, moving that around doesn't change anything either. Only what happens at S1 matters.
vxiaoyu18 said:
Is F=ρgHS?
No.
 
  • #3
The pressure of the water in the tube will drive the piston to the left. If F=ρgHS it's wrong, what's right?
 
  • #4
1. Because S1 and S2 are coupled, the volume of water common to S1, S2 and S is fixed.
2. The area of S2 exposed to atmosphere cancels an equal area of S exposed to the atmosphere.
3. Only the area of S1 remains, moving with S2 and S.
4. So the force F is being applied directly to S1 only.
5. Eliminate redundant pistons S2 and S, along with the common pool.
6. Connect force F directly to S1. Analyse that.
 
  • #5
Baluncore said:
1. Because S1 and S2 are coupled, the volume of water common to S1, S2 and S is fixed.
2. The area of S2 exposed to atmosphere cancels an equal area of S exposed to the atmosphere.
...
I used to do the same thing, F=ρgHS1, some people didn't agree with my results, so they came here to consult physics experts.
 
  • #6
vxiaoyu18 said:
F=ρgHS1
That is correct.
 
  • #7
The sign of F will depend on convention. F = - ρ⋅g⋅H⋅S1

redraw.jpg
 
  • #8
Baluncore said:
The sign of F will depend on convention. F = - ρ⋅g⋅H⋅S1
Thank you. I can see what you mean.
Now I'm wondering, if S1 = S2 = S, is the piston at rest?
 
  • #9
mfb said:
That is correct.
Thank you.
 
  • #10
vxiaoyu18 said:
Now I'm wondering, if S1 = S2 = S, is the piston at rest?
The areas S1, S2 and S of the pistons is fixed by design.
The balance of forces decides acceleration and motion.
 
  • #11
What will be the force F when the system is at equilibrium, before the piston even begins to move to the left? I get ##-\rho g H S_1##
 
  • #12
vxiaoyu18 said:
Now I'm wondering, if S1 = S2 = S, is the piston at rest?
If S1=S2=S then the area S1 will move slower than S and your force will be different. This setup is very different from what you had before.
 
  • #13
mfb said:
That is correct.
Except for the sign.
 
  • #14
tu1.jpg

1,F =-ρgHS1
 
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  • #15
tu2.jpg

2,F = 0
 
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  • #16
tu3.jpg

3,F =-ρgSH2
 
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  • #17
tu4.jpg

4,F =-ρgS(H1+H2)
 
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  • #18
Is 1 minus 4 all right? :wink:
I am looking for a structure that can be implemented: S=S1=S2, F=-ρgSH; when S=2S1, F=-2ρgSH.
 
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  • #19
vxiaoyu18 said:
https://www.physicsforums.com/attachments/254780
1、F=ρgHS1
Your sign is incorrect. F is negative. Haven’t you ever sucked up on a straw?
 
  • #20
Chestermiller said:
Your sign is incorrect. F is negative. Haven’t you ever sucked up on a straw?
I'll correct it. Thanks for your advice.
 
  • #21
Chestermiller said:
Except for the sign.
Depends on the sign convention, and on the question if F is the force acting on the piston from the water or an external force holding the piston in place.
vxiaoyu18 said:
2,F = 0
No, the force won't be zero in figure 2.
vxiaoyu18 said:
3,F =-ρgSH2
That is not correct either. The piston S2 moves if S moves.

#4 is correct.
 
  • #22
mfb said:
Depends on the sign convention, and on the question if F is the force acting on the piston from the water or an external force holding the piston in place.
F is the force acting on the piston from the water.
 
  • #23
mfb said:
No, the force won't be zero in figure 2.
If it's not equal to 0, how do you calculate it?
 
  • #24
mfb said:
That is not correct either. The piston S2 moves if S moves.
Figure 3. Suppose I add a tension meter and pull S piston at rest, then how to calculate the tension meter data?
 
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  • #25
A homework forum is not the place to rediscover a technical solutions to an unspecified problem using trial and error techniques. Would it not be simpler to first understand hydraulic cylinders, specify the fluid transfer requirement, then design a minimum solution.

The field of “hydraulic regeneration” is not magic. It is well understood and has been used by industry for some time.
https://www.hydraulicspneumatics.co...84332/book-2-chapter-17-regeneration-circuits
 
  • #26
I didn't have a deep understanding of this problem, so I assumed some examples to calculate and see what the result would be. Only by mastering the correct method of physical calculation can I develop and utilize this technology efficiently.
 
  • #27
mfb said:
Depends on the sign convention, and on the question if F is the force acting on the piston from the water or an external force holding the piston in place.
The figure seems to clearly show that F is the external force oriented to the left on the outside face of the piston. What am I missing?
 
  • #28
You're not missing anything. The source of motivation is the pressure of the water.
 
  • #29
One of my engineer friends told me before: To calculate the water pressure, we must pay attention to the position of the inlet and outlet. Only when there is flow can there be water pressure. The height between the inlet and outlet is the height of water pressure. I used this method to analyze figure 1. Water enters from S and comes out from the bottom of S1 with a height of H, so F=-ρgHS. At the same time, since S and S2 move synchronously, the water between S and S2 keeps a fixed volume in the pipe and does not change, so F=0. Finally I worked out that F=-ρgHS.
 
  • #30
Figure 1, if there is no fixed shafts between S1 and S2, from S and S2 water flows out from the bottom of the S1, then S and S1 at the bottom of the nozzle pressure between F1 = -ρgHS, the S2 and S1 at the bottom of the nozzle pressure is F=-ρgHS2, so the existence of fixed shafts brought inside environment and complicated changes, the key problem is the pipe of the synchronization between S and S2 in the sports meet will not cause F resistance.
 
  • #31
As far as I am concerned, the inflow and outflow of water refers to the outflow of water from the tube to the place in contact with air, S and S1 meet this condition, while S and S2 do not meet this condition, because the water at the mouth of S2 has no contact with air.
 
  • #32
I think I've figured out how to do it, and I can do it very quickly with PASCAL's law. 1. F=-ρgSH; 2. F=-(1/2)ρgSH; 3. F=-(1/2)ρgS(H1+H2); 4. F =-ρgS(H1+H2).
 
  • #33
Baluncore said:
2. The area of S2 exposed to atmosphere cancels an equal area of S exposed to the atmosphere.
I can't understand what you said here. I'm not sure if it's because I misunderstood the translation.
If S2 and S are equal to the air contact surface, how to understand figure 2? Does it also result in F =-ρgHS1?
 
  • #34
Chestermiller said:
Except for the sign.
You told me what the answer was, but you didn't tell me how it was calculated. There are several possible ways to compute this answer, and I don't know which one is the most accurate and can be applied to other graphs, so I assumed a few graphs and tried to learn how to compute it from more calculations.
 
  • #35
vxiaoyu18 said:
I can't understand what you said here. I'm not sure if it's because I misunderstood the translation.
If S2 and S are equal to the air contact surface, how to understand figure 2? Does it also result in F =-ρgHS1?
@Baluncore is saying to consider the area S as made of two areas S1' and S2' side by side, the first of area S1 and the second of area S2. The pressure on S2' is the same as that on S2, and they have the same area, so the forces on them are equal and opposite, so cancel.
 
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