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#673 | |
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The FA20 uses dual AVCS (on both intake and exhaust cams). But that's essentially the same as VVTI. One profile with an oil pressure actuated cam gear to advance or retard the cam's timing. |
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#674 |
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Because of the D4S system I'd guess this is more Toyota ECM than Subaru..
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#675 | |
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The other concern is that the ECU and sensors support the higher speed and the resultant I/O. I would guess that you're probably fine because you're not going to jet engine speeds or anything. Really it wouldn't surprise me if the tables and everything were setup for that kind of speed increase just because they would have over speed and endurance tested the engine beyond what will be fielded and probably just set the software and hardware up to handle that without significant modification. |
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#676 |
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#678 |
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Is the situation that the ratio that gets slightly less friction also has less peak acceleration? Because then you can get a mass reduction with going to a lighter connecting rod. And then slightly lighter crank counter-weights, slightly lighter crank damper, etc...
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#679 | ||
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That is, if you do not change the displacement. One thing I know, based on the calculation of mean piston speed, is that if you want to get high-rev, you need to reduce the stroke so that your rod will not break under high-rev. Motocycle and F-1 engine with high rev but pretty small stroke. However, I do not know the benefit of going with a longer rod (or shorter for that matter). Can someone explain it?
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#680 |
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Draw a diagram, you'll quickly see what's going on. Draw a circle with diameter equal to the stroke, then draw a circle with radius equal to the rod length.
An infinitely long rod would make the piston follow sinusoidal motion. A finite length rod will behave differently near the top and bottom of the stroke. The linear acceleration of the piston is higher in the top half of the stroke with a short rod, and slower in the bottom half of the stroke, while a longer rod has lower acceleration in the top half and greater in the lower half (roughly speaking). Perhaps the more obvious difference though is the difference in the angle between the piston motion and the rod. At a greater angle, the force on the side of the piston is greater. Since the piston skirts and rings are responsible for half the total friction/fluid pumping loss in the engine, there is an appreciable decrease in friction with a longer rod, given the same masses everywhere. A longer rod probably weighs a little bit more though... Here are some pictures that may help: http://en.wikipedia.org/wiki/Piston_motion_equations My question is, what is the primary reason for going to a longer rod length? |
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#681 |
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^ Just throwing stuff out there. What about combustion pressure and leverage differences?
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#682 | |||
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However, if you chart the crank angle vs piston position, you see a sinusoidal graph. Is there any correlation with rod length? It seems to me that by increasing rod length the curve is moved upward on this diagram (re. chart shown in the wiki link). The amplitude is changed when you change the crank diameter (stroke). Quote:
So without considering the increase weight of longer rod, with the same piston head and stroke, the engine with longer rod will have less rotating angle, i.e. less work required to rotate the rod. Thus the total work required to move the piston to rotate the engine is less compared with the one with shorter rod. However, with increase weight of longer rod, the total *work* required to move the piston would increase due to the higher weight. The question becomes: would the effect of reduced rotating angle at the piston side, thus less work to rotate rod, *greater* than the penalty of increase weight of the rod? ![]() On the other hand, based on the formula shown in the WIKI page, I did an quick Excel spreadsheet to show the difference with different rod lengths. With a 6" rod and 2" radius (half stroke), the rotating angle = 38.94 degree, and the absolute maximum values of velocity shown is 2.11 at 75 degree (I was using 15 degree increment). The theoretical maximum velocity should happen at 73.17615 degree. The maximum angular acceleration happens at 0/360 degree with -2.67. If I change the rod length to 7 inch with the same 2" radius, the rotating angle becomes 33.2031 degree, and the absolute maximum velocity is 2.08 at 75 degree with maximum angular acceleration at 2.57. So with these values, one can argue that by increasing the rod length, the maximum angular velocity and acceleration is reduced so that less stress to the rod "if the mass of the rod does not change". However since longer rod = more weight with the same material, one should be careful not to make quick statement simply based on one or two factors.
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#683 |
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I refuse to think about leverage differences, too complicated :P I prefer to just assume that metals have low hysteresis and that crank bearings have lower friction coefficient than piston skirts. Maybe someone can provide empirical evidence here.
I suspect combustion pressure is the biggest difference. A long rod gives more time between any given distance travelled around TDC, so your peak pressure is higher because more of the charge is burned by TDC, and the charge starts burning further up the compression stroke, so the piston doesn't push against a burning charge for as long. The net effect should be like an increased compression ratio in terms of cycle efficiency, without a higher physical compression. Want.FRS, look at the Wikipedia article I linked you. In that case, a picture is probably worth a thousand words. The piston's path is "linear", but its motion is quasi-simple-harmonic (aka sinusoidal) with respect to time. The rod adds some complexity to this, most obviously decreasing it around TDC. The Wikipedia article varies stroke and keeps rod length constant, if you change the rod length instead, you'll see that it's increasing BDC peak acceleration. The reason is the piston's postion at a given crank angle is the vertical distance between a circle of radius = stroke/2 and a tangent circle of radius =rod length, vertical meaning perpendicular to the common tangent of said circles. An infinitely long rod would make the piston's motion perfectly sinusoidal. The rod transmits any force to the piston at the angle it makes with the piston's travel. The force on the side of the piston is completely determined by rod angle and force that the rod transmits. Increased force on a sliding surface increases frictional force. Last edited by serialk11r; 03-08-2012 at 05:20 PM. |
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#684 | ||
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And, what is the relationship of increasing acceleration around TDC of a piston with its motion with respect to time? In fact, with longer rod and everything else the same, the acceleration around TDC is *decreased*, not increase as you said.
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#685 | ||
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And what does that have anything to do with this: Increased force on a sliding surface increases frictional force. When one applied force to an object on a sliding surface, if the object is not moving, the applied force is equal to the friction. When you increase force, provided that the object is not moving, the friction increase. Once you break loose the static friction, the object moves and then it is governed by its dynamic friction, which is less than static friction. The force applied needs to be greater than this dynamic friction to keep object moving or the object will slow down. This is basic physics. What does this have to do with increasing rod length?
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#686 | |
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Oh sorry, just noticed, the first post does point out a valid mistake, sorry about that, now it's fixed. Crank angle and time are interchangeable at constant speed, please don't get nitpicky now. And sorry I couldn't resist being smart on that last comment, but please... Last edited by serialk11r; 03-08-2012 at 05:04 PM. |
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