Fatter tires, worth the trouble?
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The largest was around 35 - 40 mm, IIRC. Testing 1 4" tire would be problematic, due to frame compatibility.
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For racers, the extra air resistance is a bigger factor than for typical riders. Their speeds are higher and they've made as many reductions elsewhere as they can. That being said, many of them do race on tires that some here would consider wide, or at least at the upper limits of narrow. [Source 1] [Source 2] There's no reason to believe that the trend of using wider tires won't continue if tire manufacturers start making their best racing tires in larger sizes, and frame manufacturers return to building frames with reasonable tire clearances. Currently, few, if any, racing frames will fit a 35 mm tire.
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lol.
and the funny thing is that the main reason pro teams started switching to 25 mm tires was because they reduce drag on wider toroidal carbon fiber wheels. in other words it's all about CFD modelling and wind tunnel testing and has absolutely nothing to do with the randonerd tire line heine pimps based on biased testing of a handful of non-randomly selected race-level clinchers.
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Not me. I think anything under 35 is skinny. Others upthread, on the other hand …
Of course, what racers use is of little importance to commuters, since we don't have support vehicles follow us around town.
Like I said. For racers, air resistance is a bigger consideration than rolling resistance. The reduced rolling resistance is an added benefit.
Of course, what racers use is of little importance to commuters, since we don't have support vehicles follow us around town.
Like I said. For racers, air resistance is a bigger consideration than rolling resistance. The reduced rolling resistance is an added benefit.
Last edited by Jaywalk3r; 10-17-14 at 10:16 PM.
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In Time Trials, aerodynamics are fairly important, and bikes specifically designed for time trials are more aerodynamic.
In races like the Tour De France, riders don't ride those more aero bikes. Because they spend a lot of their time in packs with other riders where aerodynamics don't have as big of effect because they're drafting behind other riders. Sometimes it's packs of riders competing against each other, sometimes it's in pack with their team mates where they taking turns drafting each other so that everyone benefits. But either way, the effects of aerodynamics are much smaller in racing with a team vs racing with a time trial. If a 42c tire was actually faster, Lance Armstrong would have had one on his bike and simply drafted behind his team mates for at least some of the stages of the Tour De France, you'd think.
Even the reason for going from 23c to 25c isn't clear cut either. They make tires differently than they did 20 years ago, with different manufacturing and slightly different materials. It may have been that change in how tires are made have changed, so that 20 years ago a 23c tire was faster, but in modern tires it is not.
You can read about the numerous tests racers have done to look for any way to gain an advantage - clothing material, meal timing, nutrition, etc etc. Sure, Lance Armstrong was on steroids, but he still had to beat the other top 15 contenders who were also on steroids. They're all looking for any advantage they can get. Bike manufacturers have also created entire new frames for riders to suit their preferences. If fatter tires were actually faster, they'd be riding them in serious races. I don't think the aerodynamics explanation is actually the reason they ride skinny tires. If fatter tires had better rolling resistance but were less aero, you'd still see racers riding them and drafting their team mate on a regular basis.
Last edited by PaulRivers; 10-20-14 at 09:25 AM.
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Just to make one thing clear, regardless of the whic is faster:
When racing, a lot goes down to tactics. You need to be able to CHANGE your speed quickly (mostly accelerate) - so you stay where you want to be within a group. That's where lighter wheels are a benefit - rolling mass's effect is a lot higher than static when changing speed. On a TT race, fatter (hence slightly heavier) tyres wouldn't be that much of a problem - except when climbing, of course. Since most races involve some group competing and some climbing, it is clear why a fat and heavy wheel is not used.
I prefer 28s to 25s or 23s, because they are MUCH more comfortable on rough pavement. I didn't notice any speed loss, not significant anyway. Wouldn't call them faster... but on cobblestones they definitely are - the worse the pavement, the faster fatter tyres are.
When racing, a lot goes down to tactics. You need to be able to CHANGE your speed quickly (mostly accelerate) - so you stay where you want to be within a group. That's where lighter wheels are a benefit - rolling mass's effect is a lot higher than static when changing speed. On a TT race, fatter (hence slightly heavier) tyres wouldn't be that much of a problem - except when climbing, of course. Since most races involve some group competing and some climbing, it is clear why a fat and heavy wheel is not used.
I prefer 28s to 25s or 23s, because they are MUCH more comfortable on rough pavement. I didn't notice any speed loss, not significant anyway. Wouldn't call them faster... but on cobblestones they definitely are - the worse the pavement, the faster fatter tyres are.
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No!!!!
When accelerating a massive body from rest, the force needed for accelerating is proportional to the mass being moved. When applying force to a moving body to counteract a resisting force and maintain constant velocity the force required is exactly equal to the resisting force. Unless the resisting for is dependent on mass (which air resistance is not) then force needed to maintain constant speed is also independent of mass. Air resistance is determined (mostly) by frontal cross-sectional area, and so we big fellows on upright bikes do still bear a bigger burden than are slender brethren riding in a nice tucked position, but it's not because of weight.
When accelerating a massive body from rest, the force needed for accelerating is proportional to the mass being moved. When applying force to a moving body to counteract a resisting force and maintain constant velocity the force required is exactly equal to the resisting force. Unless the resisting for is dependent on mass (which air resistance is not) then force needed to maintain constant speed is also independent of mass. Air resistance is determined (mostly) by frontal cross-sectional area, and so we big fellows on upright bikes do still bear a bigger burden than are slender brethren riding in a nice tucked position, but it's not because of weight.
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You can go play with the numbers here for your own entertainment.
Disregarding drag and assuming a level surface.
This equation makes sense if you look at my FBD posted above:
a = g*sin(theta) - Fdrag/m + Fpedaler/m
The hard part is figuring out what Fdrag is. Air resistance, rolling resistance and other drag forces are fairly complex subjects and the mass has an effect on the rolling resistance and other drag forces. (Also, Fpedaler isn't really the amount of force the pedaler is transmitting into the pedals, but that's another complex subject.)
Disregarding resistances, yes, mass doesn't matter when maintaining velocity. Accounting for resistances... heck if I know.
This equation makes sense if you look at my FBD posted above:
a = g*sin(theta) - Fdrag/m + Fpedaler/m
The hard part is figuring out what Fdrag is. Air resistance, rolling resistance and other drag forces are fairly complex subjects and the mass has an effect on the rolling resistance and other drag forces. (Also, Fpedaler isn't really the amount of force the pedaler is transmitting into the pedals, but that's another complex subject.)
Disregarding resistances, yes, mass doesn't matter when maintaining velocity. Accounting for resistances... heck if I know.
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The formula for drag force is this:
You'll notice that none of those terms is mass, not even the mass of the air. The closest you get is the rho which is the density of the air.
As I said before, this is the force which must be counteracted to achieve constant velocity. If this force is not completely matched, you decelerate and then, as a previous poster pointed out, your "F = ma" does indeed come into play as a more massive body will experience less deceleration for the same difference in force. As long as the forces are balanced, however, mass is not a factor.
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My mistake. I thought you were talking about being able to bunny hop.
Last edited by Jaywalk3r; 10-20-14 at 12:40 PM.
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This is incorrect. Mass times acceleration is the most common formula used in connection with force, and it is always relevant, but there are a good many forces which are not dependent on mass.
The formula for drag force is this:
You'll notice that none of those terms is mass, not even the mass of the air. The closest you get is the rho which is the density of the air.
The formula for drag force is this:
You'll notice that none of those terms is mass, not even the mass of the air. The closest you get is the rho which is the density of the air.
To put up a bunch of letters without defining what the letters stand for is meaningless. If you go and look at the formula, FD is the drag force, v is the speed of the object relative to the fluid, A is the cross section area, CD is the dimensionless drag coefficient, and ρ is the density of the fluid.
A density is expressed as a mass per volume. Notice "mass" is part of the equation. You, as the cyclist, are pushing the air out of the way. Air may be light but it isn't massless. And drag is expressed in newtons, N, which is defined as kg-m/s^2. Since that "kg" stands for kilograms, there is a mass element in the equation, as there is anytime a force is present.
You aren't the first to say that there are "forces" which aren't dependent on mass but I have yet to see an example. From microscopic, molecular forces to universe size forces, mass is always part of the equation. Otherwise it wouldn't be a "force".
As I said before, this is the force which must be counteracted to achieve constant velocity. If this force is not completely matched, you decelerate and then, as a previous poster pointed out, your "F = ma" does indeed come into play as a more massive body will experience less deceleration for the same difference in force. As long as the forces are balanced, however, mass is not a factor.
From the bike's standpoint, you may seem to be moving at a constant velocity but from the air's standpoint, it is accelerating. Since the whole system is dynamic, there is a constant acceleration factor in moving the air out of the way which impacts the motive force provided by the bike. Since the bike is providing force to move the air out of the way and force is related to the mass of the object moving, mass becomes a factor at all points. This is borne out by the way that we describe riding a bicycle. You do work to move the bike down the road. You encounter a drag pushing back at you. You have to use a certain amount of power to maintain your speed. Work, power and drag all involve forces in their description.
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A larger mass requires more force to get it up to the same speed as a smaller mass. The large mass with retain its momentum but any loss in momentum will require more force to get it back to speed. Since aerodynamic drag is always causing a loss in momentum, the amount of force needed to move a large object is always greater. That's why everyone works to reduce the mass of vehicles. The less mass that has to be pushed into the air, the less power it takes to push the air out of the way. An 18 wheeler doesn't have a frontal area that much higher than a car but it requires massive amounts of power to move it and even more power to accelerate it if it slows down. A car requires substantially more power to move the car down the road than a bicycle because of it's larger mass.
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A larger mass requires more force to get it up to the same speed as a smaller mass. The large mass with retain its momentum but any loss in momentum will require more force to get it back to speed. Since aerodynamic drag is always causing a loss in momentum, the amount of force needed to move a large object is always greater.
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To put up a bunch of letters without defining what the letters stand for is meaningless. If you go and look at the formula, FD is the drag force, v is the speed of the object relative to the fluid, A is the cross section area, CD is the dimensionless drag coefficient, and ρ is the density of the fluid.
A density is expressed as a mass per volume. Notice "mass" is part of the equation. You, as the cyclist, are pushing the air out of the way. Air may be light but it isn't massless. And drag is expressed in newtons, N, which is defined as kg-m/s^2. Since that "kg" stands for kilograms, there is a mass element in the equation, as there is anytime a force is present.
You aren't the first to say that there are "forces" which aren't dependent on mass but I have yet to see an example. From microscopic, molecular forces to universe size forces, mass is always part of the equation. Otherwise it wouldn't be a "force".
Part of the problem is that people take the wrong view about aerodynamic "drag". Yes, it is present and, yes, it has consequences. But what is flowing? When you ride a bicycle (or drive a car or fly a plane), the air flows around the vehicle but the air isn't moving. The vehicle is moving. Some motive force has to be put into the vehicle to move it through the air. If the two forces...negative aerodynamic force and positive motive force...are balanced, the overall force of the system is zero and the speed is constant. But you aren't moving through the same packet of air all the time. The forces on the air isn't balanced. As you move, you are moving another packet of air that you are accelerating up to your speed. Each time you encounter a new air particle, you are throwing the system out of balance.
From the bike's standpoint, you may seem to be moving at a constant velocity but from the air's standpoint, it is accelerating. Since the whole system is dynamic, there is a constant acceleration factor in moving the air out of the way which impacts the motive force provided by the bike. Since the bike is providing force to move the air out of the way and force is related to the mass of the object moving, mass becomes a factor at all points. This is borne out by the way that we describe riding a bicycle. You do work to move the bike down the road. You encounter a drag pushing back at you. You have to use a certain amount of power to maintain your speed. Work, power and drag all involve forces in their description.
A density is expressed as a mass per volume. Notice "mass" is part of the equation. You, as the cyclist, are pushing the air out of the way. Air may be light but it isn't massless. And drag is expressed in newtons, N, which is defined as kg-m/s^2. Since that "kg" stands for kilograms, there is a mass element in the equation, as there is anytime a force is present.
You aren't the first to say that there are "forces" which aren't dependent on mass but I have yet to see an example. From microscopic, molecular forces to universe size forces, mass is always part of the equation. Otherwise it wouldn't be a "force".
Part of the problem is that people take the wrong view about aerodynamic "drag". Yes, it is present and, yes, it has consequences. But what is flowing? When you ride a bicycle (or drive a car or fly a plane), the air flows around the vehicle but the air isn't moving. The vehicle is moving. Some motive force has to be put into the vehicle to move it through the air. If the two forces...negative aerodynamic force and positive motive force...are balanced, the overall force of the system is zero and the speed is constant. But you aren't moving through the same packet of air all the time. The forces on the air isn't balanced. As you move, you are moving another packet of air that you are accelerating up to your speed. Each time you encounter a new air particle, you are throwing the system out of balance.
From the bike's standpoint, you may seem to be moving at a constant velocity but from the air's standpoint, it is accelerating. Since the whole system is dynamic, there is a constant acceleration factor in moving the air out of the way which impacts the motive force provided by the bike. Since the bike is providing force to move the air out of the way and force is related to the mass of the object moving, mass becomes a factor at all points. This is borne out by the way that we describe riding a bicycle. You do work to move the bike down the road. You encounter a drag pushing back at you. You have to use a certain amount of power to maintain your speed. Work, power and drag all involve forces in their description.
Nothing you've said here brings the weight of the bicycle or its rider into the drag force calculation.
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That's an impressive bit of hand-waving, but the most you've done is elaborate on the presence of the air's mass in the density term, which I mentioned in my previous message. You're either being intentionally obstinate or you're confused.
Nothing you've said here brings the weight of the bicycle or its rider into the drag force calculation.
Nothing you've said here brings the weight of the bicycle or its rider into the drag force calculation.
Another way to approach the drag equation is to do a "dimensional" analysis. Put in the dimensions for the variables and eliminate them algebraically. What drops out is the mass (from the density), length and time squared. If mass isn't part of the equation, where does it come from? Density definitely contains a mass element.
You said that there are "there are a good many forces which are not dependent on mass." Show some.
A heavy rider with a heavy load isn't going to be faster than a lightweight rider with a light load. Try keeping up on your 50 lb bike with someone on a 15 lb race bike. Even on the flats, you don't have an advantage.
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You seem to be conflating force and the effect of the force. The density of air changes with temperature, but the mass of the air does not. Thinking about this should make clear to you the difference between the drag force depending on air density and the drag force depending on the mass of the air. But you'll probably try to dispute that, so feel free to show me the force diagram you are using to understand aerodynamic drag at a molecular level.
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Consider two steel poles with identical external dimensions, standing side by side. One is hollow and the other is solid. Suppose the wind is blowing orthogonally to the line segment created by the two bases of the poles, such that both poles are fully exposed to the wind.
What you are claiming is that the wind senses that the solid pole is heavier, and thus blows harder against it. That's not how it works. The wind doesn't know the weight of the bicycle/rider system. It applies exactly the same force against both, and exactly the same force is required to overcome that wind to maintain speed.
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Maybe you should take a closer look at the calculator you linked to.
I just went there and left the default values -- notably 0% grade, 75 kg rider, 8 kg bike. Then I went to the graph it produces and saw the at 20.02 km/h the drag force is 6.08 Newtons. Next, I changed the weight of the bike to 800 kg (that's one beefy bike!) while leaving everything else the same. The graph got re-scaled a bit so I couldn't get exactly 20.02 km/h, but at 20.05 km/h it tells me the drag force is 6.10 Newtons.
So I'm pretty sure that the calculator you linked to is telling me that aerodynamic drag force is independent of the weight of the bike.
I just went there and left the default values -- notably 0% grade, 75 kg rider, 8 kg bike. Then I went to the graph it produces and saw the at 20.02 km/h the drag force is 6.08 Newtons. Next, I changed the weight of the bike to 800 kg (that's one beefy bike!) while leaving everything else the same. The graph got re-scaled a bit so I couldn't get exactly 20.02 km/h, but at 20.05 km/h it tells me the drag force is 6.10 Newtons.
So I'm pretty sure that the calculator you linked to is telling me that aerodynamic drag force is independent of the weight of the bike.
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