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Originally Posted by FL_Gator
(Post 23321626)
I think the proposed explanation is that the deformation of the tire under weight is consistent for the entire revolution, thus the reduced radius is consistent for the entire revolution and therefore the effective circumference loaded is less than an unloaded circumference.
Edit: note that "patch" below refers to the contact patch (the part of the tire that is touching the road). Note that the result you are looking for is the horizontal distance the center of the axle moves with a full rotation of the wheel. This is related to the patch radius (the distance of the axle to the ground directly under it). With a load, the patch radius is smaller than the tire radius. The axle is rotating around an "imaginary" circle that has the patch radius. That is, this circle would be the size of the wheel if the wheel was perfectly rigid (no patch deformity). The (C) distance the axle moves horizontally in a full rotation is equal to the (C) circumference of the patch circle. (Imagine the patch radius below rotating full circle.) https://cimg8.ibsrv.net/gimg/bikefor...2e9b83c09e.png The only number that matters is the vertical patch radius. You really only need to measure this number (accurately). That's kind of hard to do. So, people measure the roll-out distance instead (which is the circumference of the patch-radius circle). What is going on elsewhere with the tire (the tire radius) doesn't matter at all. (The tire radius isn't strictly constant anyway.) ====================================================================== Note that the actual radius to use is the "rolling" (or effective) radius but it's hard to explain what is going on with that. (This was somewhat clarified below.) The rolling radius would be forward of the contact patch and (generally?) would be larger than the patch radius but smaller than the tire radius. |
Originally Posted by alpineboard
(Post 23321623)
The distance length of the circumference does not change when loaded, it stays the same, as when unloaded.
When going from an unloaded state to a loaded state, the radius changes at this contact point area, but the vital idea to keep in mind is that one complete revolution equals one circumference distance length of forward travel distance. Opinions welcome please thank you. If the radius changes (due to different loads, mostly), the circumference changes. With a higher load, the bicycle moves a shorter distance with each full rotation of the wheel. The "circumference" (the path of the outer edge) of the tire doesn't change but it doesn't matter what that number is (as long as the patch radius is the same). |
Originally Posted by njkayaker
(Post 23322690)
Sort of.
Note that the result you are looking for is the horizontal distance the center of the axle moves with a full rotation of the wheel. This is related to the patch radius (the distance of the axle to the ground directly under it). With a load, the patch radius is smaller than the tire radius. The axle is rotating around an "imaginary" circle that has the patch radius. That is, this circle would be the size of the wheel if the wheel was perfectly rigid (no patch deformity). The (C) distance the axle moves horizontally in a full rotation is equal to the (C) circumference of the patch circle. (Imagine the patch radius below rotating full circle.) https://cimg8.ibsrv.net/gimg/bikefor...2e9b83c09e.png The only number that matters is the vertical patch radius. Your theory is incorrect. The effective radius of a tire is less than the unloaded radius, but greater than the loaded ("patch") radius that you show. You really only need to measure this number (accurately). That's kind of hard to do. So, people measure the roll-out distance instead (which is the circumference of the patch-radius circle). |
Originally Posted by tomato coupe
(Post 23322782)
Your theory is incorrect. The effective radius of a tire is less than the unloaded radius, but greater than the loaded ("patch") radius that you show.
"Tire radius" (in my illustration) is the radius of the part of the tire that isn't at the patch on a loaded wheel. Tire radius (loaded) > patch radius (loaded). As I said and as the illustration shows. This tire radius (loaded) is going to be very close to tire radius (unloaded). But we don't care about these numbers at all (we only care about the patch radius),
Originally Posted by tomato coupe
(Post 23322782)
Actually, measuring the "patch" radius in your diagram is trivial
Originally Posted by tomato coupe
(Post 23322782)
-- it's the distance from the center of the hub to the ground.
Originally Posted by tomato coupe
(Post 23322782)
If you measure it and the roll-out distance of a tire, you'll quickly find that the effective radius of the tire is greater than the loaded radius, and the difference increases as the tire is more heavily loaded.
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Originally Posted by njkayaker
(Post 23322792)
???
"Tire radius" (in my illustration) is the radius of the part of the tire that isn't at the patch on a loaded wheel. Tire radius > patch radius (as the illustration shows). This radius is going to be very close to the radius of an unloaded wheel ??? It seems it would be harder to load the bike and take that measurement. You'd probably need two people. ?? I said this. ??? This is what the illustration is showing. The effective radius of the tire is irrelevant. Only the patch radius matters. |
Originally Posted by tomato coupe
(Post 23322807)
I think we're in agreement based on with what you're saying, but your diagram shows something different.
No, it doesn't (the illustration is correct). Tire radius (loaded) > Patch radius (loaded). <<== what we are both saying. The circle (with the tire radius) is larger than the circle with the patch radius. The illustration shows the two circles (the patch circle is smaller and inside the tire radius circle). |
Originally Posted by njkayaker
(Post 23322813)
????
No, it doesn't (the illustration is correct). Tire radius (loaded) > Patch radius (loaded). <<== what we are both saying. The circle (with the tire radius) is larger than the circle with the patch radius. The illustration shows the two circles (the patch circle is smaller and inside the tire radius circle). |
Originally Posted by tomato coupe
(Post 23322845)
Quite honestly, I can't follow your reasoning, because I can't figure out what your definition of "patch radius" is.
Look at the illustration. It's the vertical distance from the center of the wheel to the ground. It's pointing directly at the part of tire that is being compressed.
Originally Posted by tomato coupe
(Post 23322782)
The effective radius of a tire is less than the unloaded radius, but greater than the loaded ("patch") radius that you show.
Originally Posted by tomato coupe
(Post 23322782)
Actually, measuring the "patch" radius in your diagram is trivial -- it's the distance from the center of the hub to the ground
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Originally Posted by njkayaker
(Post 23322847)
???
Look at the illustration. It's the vertical distance from the center of the wheel to the ground. It's pointing directly at the part of tire that is being compressed. Unloaded radius > effective radius > loaded (patch) radius |
Let us agree on a few things, one complete revolution of the rim equals one complete revolution of the tire.
If you cut the tire circle at one point and lay it flat on the ground in a straight line, like a belt, one complete revolution of the circle equals one full length of this belt, this does not change, ever, squish or no squish. This distance does not change if it gets squished under load or no squish under no load. One rev of the wheel equals one circumference distance. Assume there is not any slip during squish load footprint. I fully realize there other variables going on, at the squish load spot, compression, temperature, ect, but all these are irrelevant until the understanding of the belt theory is understood. Am def willing and able to hear all opinions about this subject. |
Let us agree on a few things, one complete revolution of the rim equals one complete revolution of the tire.
If you cut the tire circle at one point and lay it flat on the ground in a straight line, like a belt, one complete revolution of the circle equals one full length of this belt, this does not change, ever, squish or no squish. This distance does not change if it gets squished under load or no squish under no load. One rev of the wheel equals one circumference distance. Assume there is not any slip during squish load footprint. I fully realize there other variables going on, at the squish load spot, compression, temperature, ect, but all these are irrelevant until the understanding of the belt theory is understood. Am def willing and able to hear all opinions about this subject. |
Originally Posted by tomato coupe
(Post 23322859)
With that definition, your theory is incorrect. The effective radius of the tire is larger than what you're calling the "patch" radius, and it is related to the tire circumference (or roll-out) by the familiar L = 2 * pi * radius.
Unloaded radius > effective radius > loaded (patch) radius
Originally Posted by tomato coupe
(Post 23322859)
Unloaded radius > effective radius > loaded (patch) radius
I suspect it's more like: "Tire radius (loaded) approximately equal to tire-radius (loaded) > loaded (patch) radius." (But we don't care about either tire radius. We only care about the patch radius.) |
Originally Posted by alpineboard
(Post 23322864)
Let us agree on a few things, one complete revolution of the rim equals one complete revolution of the tire.
If you cut the tire circle at one point and lay it flat on the ground in a straight line, like a belt, one complete revolution of the circle equals one full length of this belt, this does not change, ever, squish or no squish. This distance does not change if it gets squished under load or no squish under no load. It's important to keep in mind that the loaded tire isn't a circle. It's a deformed circle (there's a flat part at the bottom). It's also important to be clear that circumference is an attribute of an actual circle (or ellipse).
Originally Posted by alpineboard
(Post 23322864)
One rev of the wheel equals one circumference distance.
There are two circumferences to keep mind of: (1) the circle with the tire radius and (2) the circle with the "patch radius" (the vertical distance between the center of the wheel and the ground). (The tire perimeter is a third thing to keep in mind.) The circumference that matters is the second one. This is the 2*(vertical distance) * Pi circle. The vertical distance varies with the load (it's shorter with heavier loads). Thus. the circumference varies with load (as does the horizontal distance travelled). (The tire perimeter is irrelevant.) Look at my illustration.
Originally Posted by alpineboard
(Post 23322864)
Let us agree on a few things, one complete revolution of the rim equals one complete revolution of the tire.
Originally Posted by alpineboard
(Post 23322864)
I fully realize there other variables going on, at the squish load spot, compression, temperature, ect, but all these are irrelevant
until the understanding of the belt theory is understood. Tanks are an extreme example of what is going on. The distance travelled in a rotation is the circumference of the circle with the radius of the wheel axis to the round (not the track length). The tire perimeter is like the track: it doesn't matter how long it is. https://cimg9.ibsrv.net/gimg/bikefor...9aca4ee24c.png =============================================== (1) Consider what the deal would be if you removed the tire and just ran on a raw rim. Note that this would be what would happen if you had an extreme load (or no air in the tire). In this case, the horizontal distance would be equal to the circumference of the rim. (2) Now, imagine running on a raw rim that was as big as the wheel with a fully-inflated tire. Or on the same rim but with a solid tire that doesn't compress. In this case, circle and circumference is larger, which means the horizontal distance would be larger than case (1). So, the circumference of a real wheel is going to be between case (1) and case (2). The circumference will be smaller with more load or less pressure. |
Again, a simple roll out test, one loaded and one unloaded will give the answer. Of course that might not be as fun as several pages of physics arguments.
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I’m going to start a new thread as a tangent to this one: How many Angels can dance on the contact patch of a 28mm tire, loaded, or unloaded.
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Originally Posted by merlinextraligh
(Post 23323223)
Again, a simple roll out test, one loaded and one unloaded will give the answer. Of course that might not be as fun as several pages of physics arguments.
Is the contact patch compressed horizontally due to the torque exerted by the rider? |
Originally Posted by njkayaker
(Post 23322870)
:rolleyes: I said this multiple times! The illustration clearly shows it!
https://cimg3.ibsrv.net/gimg/bikefor...468cc5e9c5.jpg |
Originally Posted by merlinextraligh
(Post 23323223)
Again, a simple roll out test, one loaded and one unloaded will give the answer. Of course that might not be as fun as several pages of physics arguments.
Originally Posted by znomit
(Post 23323311)
Does the tyre compress less at speed? There is work done deforming the tyre.
Is the contact patch compressed horizontally due to the torque exerted by the rider? |
Originally Posted by tomato coupe
(Post 23323513)
The following diagram shows the relationship between the three radii, where Ru = unloaded radius, Rl = loaded radius, and Re = effective radius. Your illustration shows the effective radius and the "patch" radius as being the same. They are not, in general.
https://cimg3.ibsrv.net/gimg/bikefor...468cc5e9c5.jpg What’s the definition of the “effective radius” there? Cos based on the image alone it’s “distance from hub to an arbritrary dotted line”. Does PC=CA? And if so, why? |
Originally Posted by choddo
(Post 23323550)
OK this is physics arguments :thumb:
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Originally Posted by tomato coupe
(Post 23322005)
Is there a practical reason why you need better accuracy?
An errorless cyclocomputer would have been a game changer. With GPS you just obey the GPS. Every turn is easy like a T. Admittedly something is lost when navigation becomes effortless, but alas sometimes GPS fails and one is forced to a backup method. Which can be fun in its own way. |
Ok I think I understand what tomato coupe is saying but I think he’s wrong for weights in bike territory as opposed to cars.
Figure 8.12 of this suggests the effective radius actually being smaller than the patch radius for weights below 1200N (about 120kilos) https://www.sciencedirect.com/topics...rolling-radius |
Originally Posted by tomato coupe
(Post 23323513)
The following diagram shows the relationship between the three radii, where Ru = unloaded radius, Rl = loaded radius, and Re = effective radius.
https://www.sciencedirect.com/topics...%20the%20wheel.
Originally Posted by tomato coupe
(Post 23323513)
Your illustration shows the effective radius and the "patch" radius as being the same. They are not, in general.
So, you are saying the actual radius to use is somewhat larger than the patch radius. So, sure, what I said was not quite correct. It's still explains closely-enough why the unloaded radius is wrong (too large). So, you are correct but explained it very poorly. How different is this effective radius from the patch radius? =========================== So, to be clear... The actual radius to use for measuring distance per rotation is called the "effective" or ("rolling") radius. You can't really measure it directly, which is why one does a roll-out measurement. https://www.tractorbynet.com/forums/...2#post-4599241 Talking about the loaded (patch) radius is a simplification. I think it's a useful simplification: it would be impossible to talk about the effective (rolling) radius without being clear about the loaded radius. =========================== Note that the effective radius is different between "free rolling" and "driven" wheels. So, there are situations where the effective radius can be smaller than the loaded (patch) radius. (This might not be the case when bicycling.) https://liu.diva-portal.org/smash/get/diva2:1762057/FULLTEXT01.pdf While driving, the driven wheels will get a driving torque. This torque will lead to tire slip, which will make the wheel speed larger than if no slip occurred. This will push up the center of rotation and decrease the effective rolling radius, making it smaller than the loaded rolling radius [7]. If instead the vehicle is braking, the wheels will skid and the wheel speed is smaller than if no skid occurred [7]. This means that the center of rotation will be pushed down and the effective rolling radius will be greater than the unloaded radius. |
Originally Posted by choddo
(Post 23323552)
Can just about read that. A higher quality image would have helped.
What’s the definition of the “effective radius” there? Cos based on the image alone it’s “distance from hub to an arbritrary dotted line”. Does PC=CA? And if so, why?
Originally Posted by choddo
(Post 23323571)
Ok I think I understand what tomato coupe is saying but I think he’s wrong for weights in bike territory as opposed to cars.
Originally Posted by choddo
Figure 8.12 of this suggests the effective radius actually being smaller than the patch radius for weights below 1200N (about 120kilos)
https://www.sciencedirect.com/topics...rolling-radius |
Originally Posted by downtube42
(Post 23323567)
Indeed, one of the biggest improvements in going from cyclocomputer + cue sheet to GPS for long distance navigation, is eliminating the need for math in your head. Cue sheet says turn right at 47.18 miles, from which you have to subtract 0.62 in your head due to error, and remember the result before the turn comes. Then let's say there's another turn at 47.29, which is pretty quick so you have to decide ahead of time whether to remember 0.11 and add that upon turning, or subtract 0.62 again and remember two results, or just hope there's only one road in close proximity. Keeping in mind the 0.62 becomes 0.63 after a bit, now try that short on sleep on day two or three. Then add rain, with required efforts to keep the cue sheet dry. The best is when the cue says turn at T in the road, in which case you give the brain a break and ride to the T.
An errorless cyclocomputer would have been a game changer. With GPS you just obey the GPS. Every turn is easy like a T. Admittedly something is lost when navigation becomes effortless, but alas sometimes GPS fails and one is forced to a backup method. Which can be fun in its own way. |
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