- Joined
- Jan 20, 2022
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- 93
Especially on Shared Sump motor bikesI actually notice engine smoothness “kicks in” per se after the oil is good and settled in, once it’s been run for a few days.
Yes we all obsess over our cars![]()
Especially on Shared Sump motor bikesI actually notice engine smoothness “kicks in” per se after the oil is good and settled in, once it’s been run for a few days.
Yes we all obsess over our cars![]()
I take that point But its not that important. If you feel its better - its is better to you.Not based on any standard or repeatable test criteria.
What's funny about this post is that I agree with your points written here.I take that point But its not that important. If you feel its better - its is better to you.
Arguing this sentiment with JoelB a while back, the design of experiment to measure the engine noise would be much more involved than what one might casually think . It would take more than a sound level meter set to DB- A weighting to get usable data, wen the experiment is all sorted, the resulting data must be properly interpreted an reported; Data can be misused to disabuse.
Think of audio equipment measurement . Repeatable data required by FTC for power rating and distortion.
THD has been used for decades. Funny thing, it tells you not a wit about the sound of the amp when it is less than a few percent and, any unit with solid design and in good operation operation and not overdriven easily measures less than 2 percent.
Super low distortion was touted as the primary goal for a great amplifier.
Well it appears that the means to that end (global negative feedback application) made the amps sound MUCH worse and caused rise of other distortion that was not measured.
So great specs to advertise, a repeatable test procedure, but measuring and touting the wrong thing.
In life there is good art and bad art, good music and bad music, good science and bad science.
What you're missing is the directional nature of these forces. The force due to the expansion of the ring is negligible in comparison to the force applied on top of the piston by the gas pressure multiplied by the sine etc. of the angle involved to get the resultant component. Here is the full analysis of the forces:
https://www.researchgate.net/public...e_approach_in_engine_design_analysis/download
I didn't read the whole thing, but note that the connecting rod is not perpendicular, and this results in a huge lateral force component on the piston. That force is going to be much larger than the force applied on the thin ring by the gas pressure.
Here are the relevant figures and the accompanying test. The piston has a "thrust" side and an "antithrust" side, resulting from the angle of the connecting rod. The thrust side is where the connecting rod pushes the piston against the wall and the antithrust side is where it pulls it away from the wall during the power stroke. The piston–wall clearance becomes minimum on the thrust side during the power stroke, whereas it becomes minimum on the antithrust side during the suction stroke.
It is interesting to examine force variation in the piston during its motion. In Fig. 14 the forces due to combustion gas force Fₚ and the inertia force
Fᵢ acting on the piston during its downward motion during the suction stroke are shown. These two forces have to be balanced by the force Fᴿ acting on the connecting rod. Even though vertical component Fᵈ on the connecting rod is balanced by Fₚ and Fᵢ, the horizontal component Fₛ has to be balanced by the thrust reaction from the cylinder wall. Viscous friction force acting at the piston–wall interface is given as Fᶠ.
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Forces acting on the piston during successive strokes
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Viscous force and the clearance (film thickness) variation at thrust side
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Viscous force and clearance (film thickness) variation in antithrust side
There is an effect, yes, but it's pretty small as seen in the figures. However, the effect on the friction seems large.Ref: https://www.researchgate.net/public...ngines/link/5d9b09d0a6fdccfd0e7f3b22/download
View attachment 96364F
Figure 1
On Page 7:
"The combustion gases flow into the crevices between piston ring, piston grooves and the cylinder liner as the cylinder pressure rises. The generated contact pressure for the piston ring is determined by the trapped mass behind the ring (i.e. the control volume B)."
View attachment 96365
Figures 3a and 3b
From Page 10:
"The piston compression ring undergoes hydrodynamic regime of lubrication for a large part of the engine cycle. Asperity interactions occur at piston reversals (particularly at the top dead centre) due to a reduction in lubricant entrainment into the conjunction. The associated friction indicates that boundary interactions take place at the top dead centre in the combustion (power) stroke (Fig. 3b). Contact pressure is distributed more uniformly for the flexible ring and there is a rise in the minimum lubricant film thickness. Therefore, boundary friction is marginally mitigated with a flexible ring."
View attachment 96366
Figure 6a
From Page 10:
"Mixed regime of lubrication occurs during piston reversals and especially during the combustion stroke due to the reduced sliding velocity and increased contact load, resulting in the reduction of the minimum film thickness (Fig. 6a)."
"A sudden reduction in the film thickness appears during the maximum cylinder pressure."
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My comments: This study seems to be very through and detailed IMO. It specifically addresses the combustion pressure effect on the top ring which increases the ring face force to cylinder, and how that effects the film thickness at TDC power stroke.
Also, the studies I've seen don't seem to address the effect of the combustion on the level of lubrication film on the cylinder wall. The combustion has to burn away some oil film which makes the environment for the top piston ring even more harsh in terms of getting adequately lubricated. I think of of the studies referenced before in this thread make a mention that their study/model didn't account for that "lack of lubrication" factor.
The bottom line is that the combustion pressure has a large effect on the film thickness and lubrication of the top compression ring on the power stroke. This is why the top ring and the top area of the cylinder wears the most (ie, cylinder taper and ring groove at TDC) compared to the rest of the cylinder and the 2nd compression ring and oil control rings. The top compression ring IMO is probably the most abused component in an ICE. Many times, the ring(s) will wear out much faster (resulting a a loss of compression) than the rod, crank or cam journal bearings.
Moreover, any expansion of the rings would actually increase the minimum oil-film thickness (MOFT), not decrease it. That is because the eccentricity (wobbling) is reduced when the rings expand, and the MOFT is inversely proportional to the eccentricity (wobbling), as more wobbling squeezes out the oil film more.
Nevertheless, these are theoretical calculations, and I doubt that the authors bothered to factor the ring expansion into them.
What figures are you referring to?There is an effect, yes, but it's pretty small as seen in the figures. However, the effect on the friction seems large.
The ratio of the force applied by the gas pressure onto the ring to the thrust force applied on the ring by the connecting rod will be on the order of:
face area of the ring / top-surface area of the piston / sine of the angle from vertical of the connecting rod
This ratio should be pretty small.
I don't agree, because the fact is that the ring floats in the ring groove. While the piston gets slammed against the cylinder to take up the small piston to wall clearance during a power stoke (actually happens on all strokes), the rings will simply readjust themselves in the ring groove. Once the piston makes that initial impulse tilt and hits the cylinder wall, the piston tilting movement stops. Probably happens in a few milliseconds.
There is a film of oil of course between the piston and cylinder wall, it was discussed in the one paper Gokhan posted a link to. Of course the piston skirts hit and rub on the cylinder walls ... look at the wear marks on any piston (example below) and you can see where they rub.First of all, this is a great discussion.
I have not heard of the piston hitting the cylinder wall before. One might think that would cause damage to the cylinder walls within a short period of time. I had always thought the rings were the only contact with the cylinder wall.
Having said that, are the pistons actually hitting the cylinder wall itself or is there a oil film or tribofilm that is there to avoid metal to metal?
3(a) and (b).What figures are you referring to?
Look at this figure below. It is a simple static-equilibrium problem. Something must counter-support the lateral force of the connective rod, and this is not an instantaneous force—the angle of the connective rod is nonzero for most of the cycle. If the ring is not counter-supporting, it must be the piston itself, but that would cause more wear I would think. Moreover, this lateral con-rod force is much larger than the force applied by blowby on the ring. My guess is that the ring is almost completely pushed in on the thrust side but floats on the antithrust side.As mentioned more below, the rings float in the piston groove, so how can the side load on the piston cause the rings to see more load when they will move in their ring groove if the piston is forced against the cylinder wall.
On the contrary, according to Figure 3(a), MOFT is larger when there is blowby vs. when there is no blowby. This larger MOFT with blowby is resulting in less friction with blowby vs. without blowby if you look at the inset in Figure 3(b).Obviously the top ring gets hit with a lot of combustion pressure which forces the face harder against the cylinder wall, which causes more ring friction (and causes reduced MOFT too as shown in the other study) ... that's why the top ring and top of the cylinder wear. Friction means increased wear, which is caused by a combination of higher forces and reduced lubrication (less film thickness).
Re: Comments on your bolded text: 1st one - Of course it's the piston itself hitting the cylinder wall (due to rocking in the bore) that is supporting the piston forces from stroke motion. As said multiple times, the rings float in their grooves. The rings on the thrust side can compress all the way into their grooves to the point where the piston in the ring groove area is rubbing on the cylinder wall, along with the rings. The rings float and don't really support the piston in any way. Piston dynamics is all about the piston rubbing on the bore, as discussed in the paper your figure above came from. 2ne one - Yes, the rings obviously can be pushed into their grooves all the way if the piston tilt is extreme. Watch the video I posted in post #90 - they show piston contact to the wall in the ring area and even above the rings on the circumference of the dome area.Look at this figure below. It is a simple static equilibrium problem. Something must counter-support the lateral force of the connective rod, and this is not an instantaneous force—the angle of the connective rod is nonzero for most of the cycle. If the ring is not counter-supporting, it must be the piston itself, but that would cause more wear I would think. Moreover, this lateral con-rod force is much larger than the force applied by blowby on the ring. My guess is that the ring is almost completely pushed in on the thrust side but floats on the antithrust side.
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The gas blow-by is probably giving a gaseous film between the ring face and cylinder wall, which helps reduce friction. Fact is, all this info from the studies referenced show that the oil film is reduced throughout the power stroke when there is no gas blow-by, and it's pretty easy to see that it's from the combustion pressure effect on the back side of top ring as shown in Figure 1 in post #86 and Figure 3a in post #88.On the contrary, according to Figure 3(a), MOFT is larger when there is blowby vs. when there is no blowby. This larger MOFT with blowby is resulting in less friction with blowby vs. without blowby if you look at the inset in Figure 3(b).
So, you're basically saying that the rings carry almost no load and the piston skirt does all the hard work of supporting the lateral force of the connective rod. I would have to see a study to believe that.Re: Your bolded text comments. 1st one - Of course it's the piston itself hitting the cylinder way (due to rockng in the bore) that is supporting the piston forces from stroke motion. As said mulitple times, the rings float. The rings on the thrust side can compress all the way into their grooves so the piston in the ring groove area is rubbing on the cylinder wall also, along with the rings. The rings float and don't really support the piston in any way. Piston dynamics is all about the piston rubbing on the bore, as discussed in the paper your figure above came from. 2ne one - Yes, the rings are obviously can be pushed into their grooves all the way if the piston tilt is extreme. Watch the video I posted in post #90.
Look at Figure 3(a) again. It is contradicting what you're saying. When the blowby is included, MOFT is increased, not reduced like you claim.The gas blow-by is probably giving a gaseous film between the ring face and cylinder wall, which helps reduce friction. Fact is, all this info from the studies show that the oil film is reduces throughout the power stroke, and it's pretty easy to see that it's from the combustioin pressure effect on the top ring as shown in Figure 3a in post #88. I've seen nothing that says the thinning effect on the oil film thickness during the power stroke is due to the dynamics of the piston assembly. Like said in post #88, if you rotated the engine at some constant RPM, the oil film thickness vs piston position curves would all look the same for all four stokes. Throw in combustion on the power stroke and you can see the effect on the oil film thickness on the top ring.
Of course the piston rubbing on the cylinder wall it carrying all the side load induced by the piston stroke. Have you ever held a piston assembly in your hands and looked closely at it? Tell me how rings that float in/out of their grooves can support the piston when the piston is up tight against the wall and the rings are pushed all the way into their groove to be even with the piston surface. The rings can't support any more force than beyond their spring tension against the wall ... that's why the piston can tilt in the bore and rub on the wall if the piston skirt to cylinder clearance is excessive, just like discussed in the video I linked in post #90.So, you're basically saying that the rings carry almost no load and the piston skirt does all the hard work of supporting the lateral force of the connective rod. I would have to see a study to believe that.
I think it's actually Figure 3b, with the little exploded window inside the graph showing more friction detail around TDC. Blow-by gas at the highest pressure at TDC could certainly cause the ring friction to do down because a layer of gas could lift the ring face off the wall somewhat. Figure 3b is showing ring friction, not MOFT. In figure 3a, the oil film thickness is basically the same throughout the power stroke regardless of which ring it is.Look at Figure 3(a) again. It is contradicting what you're saying. When the blowby is included, MOFT is increased, not reduced like you claim.
I think we are both right here. This paper has some data:Of course the piston rubbing on the cylinder wall it carrying all the side load induced by the piston stroke. Have you ever held a piston assembly in your hands and looked closely at it? Tell me how rings that float in/out of their grooves can support the piston when the piston is up tight against the wall and the rings are pushed all the way into their groove to be even with the piston surface. The rings can't support any more force than beyond their spring tension against the wall ... that's why the piston can tilt in the bore and rub on the wall if the piston skirt to cylinder clearance is excessive, just like discussed in the video I linked in post #90.
I think it's actually Figure 3b, with the little exploded window inside the graph showing more friction detail around TDC. Blow-by gas at the highest pressure at TDC could certainly cause the ring friction to do down ... Graph 3b is showing ring friction, not MOFT. In figure 3a, the oil film thickness is basically the same throughout the power stroke regardless of which ring it is.
Think about it. If there is a high pressure gas blowing by the ring then there must also be a relatively large gap between the ring face and cylinder wall that leaks some combustion pressure. It was on a "flexible" ring too, so that may allow more blow-by. If oil can occupy that space or not (they don't really say or explain the ring blow-by data) then maybe that's why the film thickness is higher. I think that was "model data" too, which might have something to do with it.
Anyway, the bottom line is there is plenty of other information that supports that combustion gas pressure pushing on the back side of the top ring during the power stroke effects the top ring film thickness, friction and wear. I really haven't seen anything that says otherwise.
I think we are both right here. This paper has some data:
I wouldn't give any credibility to your postulate about the blowby directly lubricating the ring. The oil and the tribological films do the lubrication—not the blowby.
It looks like the blowby is flowing behind the rings in their model according to Figure 5.Quick scan of that paper, and a quick comment on the ring blow-by after scanning that paper. They describe the "blow-by/blow-back" as gas that gets past the rings through the back side of the ring pack - see Figure 5. They don't show any reference to the blow-by going past the ring face and cylinder wall that I can see.
So in the study I reference, they don't really describe exactly what the "blow-by" refers to, or show any figure describing exactly what they mean. You would think that if high pressure gas was actually blowing past the ring face and the cylinder wall that the pressure on the back side of ring would be counter acted and force on the back of the ring negated somewhat, which would reduce the force pushing the ring outward, and thereby increasing the film thickness (and reducing friction) because of less ring force squeezing out oil between its face and wall. Any gas blow-by pressure on the face side of the ring will cancel out some pressure on the backside of the ring. If the ring was perfectly sealed between the ring face and wall (zero ring face blow-by gas pressure), then all the combustion gas pressure would act to force the ring face against the wall, thereby reducing MOFT and increasing friction.
Also look at Figure 7 in your link reference (see page 11).
"Calculated combustion pressures acting on ring face profiles are presented in Figure 7. The pressure values are highly influences by ring clearances and also liner deformations. Pressure acting on first ring face is very similar to combustion pressure in a combustion chamber."
Just as I noted above, if the pressure on the ring face is very high right around TDC during combustion, the gas force on the back side of the ring is essentially cancelled for a short time, and that would mean less ring expansion force and higher MOFT between the ring face and cylinder wall. As the piston moves downward, then the ring starts sealing better between the ring face and wall.
Anyway ... good find on that last paper ... will digest in more detail later, and maybe comment more on your post #96 if I find something. In the middle of doing my taxes, and looks like I owe $$.![]()
Wanted to comment on this. Even if there is that much combustion pressure behind the top ring making it expand with that much force, it's still possible for the piston to tilt enough (if the piston skirt to wall clearance is excessive) for the area of the ring pack to rub on the cylinder. it also depends a lot on the piston design. That means the ring(s) would have to be totally flush with the piston surface at that point.I think we are both right here. This paper has some data:
https://cyberleninka.org/article/n/583816
For a 75 mm ⌀ × 1 mm ring, an 11 MPa of pressure corresponds to a 2,600 N of force. This force is being applied on the ring from the inside of it by the blowby pressure as you said, and it is the force that is counter-supporting the lateral force of the connective rod as I said (action–reaction principle). Without the blowby pressure, the ring would be entirely pushed into the groove to support the 2,600 N (580 lbf) of lateral force applied by the connective rod.
I agree ... I'm always up for a civil technical discussion, and it does also become a learning experience because we have to go dig up all the technical references to debate viewpoints.This discussion veered quite off from the effect of the base-oil viscosity and VII on the lubrication of the valvetrain and piston rings, but we've learned quite a bit. I say you should believe that the shear rates in the valvetrain and at the rings can be as quite high as the Shell paper I posted earlier reported.![]()