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multistage cylinder tip load

  • Thread starter Thread starter AngeloB
  • Start date Start date
I'll be like the "sphinx", answering with a question:

what stress is present in the material when the pressure cylinder arrived at the maximum extension and supports in elevation the load?
 
for pasteurman
the piston of the last stem is diam.63
therefore indicative
p= 900/((pi/4)*6.3^2)= about 29 bar
 
apart from the last section "full" of the cylinder, under equilibrium conditions and at the maximum extension, the walls of the hollow cylinders, are subjected to a "normal" stress nothing since it is the pressure oil column that supports everything "pushing" the two bottoms.
Obviously the walls will be subject to a circumferential tension not anything caused by the pressure.

beyond the equilibrium condition, that is, with pressure greater than that necessary to balance the load, the walls of the hollow sections are subjected to traction and not compression.

Therefore, a possible check at peak load, should be made only on the last part of the piston, the full one.

Is he coming back?
 
If I understand correctly you mean that where there is pressure oil there is no peak load.
and something I thought about, but there was no way to prove it.
doing the verification, not considering the plumbing aspect, thinking the rods blocked "mechanically" I think I'm on the security side.
 
Yes, where the material is "teso" there is no danger of instability to cover.
to prove it uses the eq. cardinals of the static to a sistama made by two solo telescopic elements.
Say hi.
 
apart from the last section "full" of the cylinder, under equilibrium conditions and at the maximum extension, the walls of the hollow cylinders, are subjected to a "normal" stress nothing since it is the pressure oil column that supports everything "pushing" the two bottoms.
Obviously the walls will be subject to a circumferential tension not anything caused by the pressure.

beyond the equilibrium condition, that is, with pressure greater than that necessary to balance the load, the walls of the hollow sections are subjected to traction and not compression.

Therefore, a possible check at peak load, should be made only on the last part of the piston, the full one.

Is he coming back?
I understand that.
But I would like to make an observation: In my opinion the seals and seals of the plunger and the stem are a point that could be easily deformable. In other words, even if the stem and shirt remain straight, they could still form a break with the edge placed at the point where the stem enters the cylinder. at this point the static scheme changes and I do not think that it is enough for the internal pressure to prevent instability. What do you say?
 
I don't want to, but you have an incorrect static pattern in mind.

think of a simple cilider; when the oil pressure exceeds the value necessary to lift the load and cylinder is at its maximum extension, it turns out that:

- the stem is compressed
- the shirt (or cylinder) is tense
- the cylinder case is compressed

I attach a sketch.
Hi.
 

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  • cilindro.webp
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I don't want to, but you have an incorrect static pattern in mind.

think of a simple cilider; when the oil pressure exceeds the value necessary to lift the load and cylinder is at its maximum extension, it turns out that:

- the stem is compressed
- the shirt (or cylinder) is tense
- the cylinder case is compressed

I attach a sketch.
Hi.
I understood the static scheme, maybe I explained badly in making observation.
I don't have much knowledge of oleodynamics.

My perplexity lies in the fact that, from the reasoning you have exposed, it seems that it is possible to build cylinders with very long and slim lines, because only the last vent is subject to peak load.
your reasoning line and is certainly right, but I would say that you do not consider any other phenomenon that could affect the maximum length of these multi-swire cylinders. I therefore thought of the effect that can have seals and seals when the cylinder is completely extended. I think about the limit case, with garnishes with a lot of game, which may not guarantee that the stem and shirt remain coaxial.
 
Perhaps the misunderstanding lies in the hinges that are in the head and tail to the cylinder. in the scheme are ideal hinges and without friction.
cannot be born bending under these conditions and therefore there is no risk of loss of coaxiality for intermediate shirts since they are stretched and not compressed.

the last seal is the one that determines the value to be assigned to the free length of inflection "lo"

in the calculation of stability for the spherical utim (compressed because full), you can consider the free length of inflection as if:

- the seal was a hinge.
- the load attack a vertical cart.

look at the table and see when it is "the" free length of inflection.

Hi.
 
Has anyone ever faced such analytical problem?

i.e. having a telscopic cylinder or a beam with non-continuous section loaded axially and verify whether the chosen section is sufficient to avoid the transfer for peak load?

to me it seems that there is something that allows to calculate the lungh of free inflection for every part, but I do not remember where and especially if I did not dream of it. . .
 
Has anyone ever faced such analytical problem?

i.e. having a telscopic cylinder or a beam with non-continuous section loaded axially and verify whether the chosen section is sufficient to avoid the transfer for peak load?

to me it seems that there is something that allows to calculate the lungh of free inflection for every part, but I do not remember where and especially if I did not dream of it. . .
You need this one I've attached. verifiable in cnr uni 10011 (retired in 2004) and eurocode 3.

Let's say that having a different section multistage cylinder you could do the overlap of the effects, analyze each piece of spherical and calculate the single shift. then join the bands until you find the total.

or calculate average section and consider it unique beam.

Remember that there are adequate oversized coefficients.
 

Attachments

  • cdpunta.webp
    cdpunta.webp
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You need this one I've attached. verifiable in cnr uni 10011 (retired in 2004) and eurocode 3.

Let's say that having a different section multistage cylinder you could do the overlap of the effects, analyze each piece of spherical and calculate the single shift. then join the bands until you find the total.

or calculate average section and consider it unique beam.

Remember that there are adequate oversized coefficients.
I would simply consider the whole stem of size equal to the smallest/periculous section (and then it would go oversize the whole) and then I would go to apply the "usual" verification of which you have returned a branch.. .

what do you mean by overlaying effects?

If you mean what I think I know there would be doubts/problems to assign to each section the coefficient "mu"...:confused:
 
I would simply consider the whole stem of size equal to the smallest/periculous section (and then it would go oversize the whole) and then I would go to apply the "usual" verification of which you have returned a branch.. .

what do you mean by overlaying effects?

If you mean what I think I know there would be doubts/problems to assign to each section the coefficient "mu"...:confused:
by reasoning above are all with the 3rd scheme with mu=1 because it is considered that at stem out in pressure you get a recess due to the pressure of the greater section than the next while the upper section free iterato for n sfli. then you can reason differently but first caught could be so. as much as the whole unique beam with schema 3. I'm pointing out if you have a simulator modeler like swx cosmos set the point load analysis and you're appropriate as further verification.
 

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