Do steel lugged bikes go faster downhill than carbon fiber bikes?
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Gravity is a force, with a constant rate of acceleration working on the mass of the rider + bike (F=ma). When mass is larger, the force is larger, and acceleration won't reach zero until that larger force is balanced out by a larger force of friction of the air (wind resistance) and the bearings. So terminal velocity is higher, and up to that point acceleration remains higher for the heavier rider (since wind resistance is going to be pretty similar between any two riders on road bikes at the same speed).
Last edited by mikeinroch; 07-16-12 at 08:48 AM.
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Galileo proved many centuries ago that the acceleration of gravity is independent of mass.
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Theoretically, if the ramp was short enough, that might be true. Practically speaking, the reason why a steel bike is faster than a carbon bike on a descent is because it weighs more. There is another reason that sometimes applies that was not given by the OP. When I am climbing, I try and conserve energy and use it on the descent. Skinny people try and blast up the hill and rest on the descent. We are both playing to our strengths, which brings us back to the first point.
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Galileo proved many centuries ago that the acceleration of gravity is independent of mass.
In a vacuum. Only in a vacuum. Add air, and the heavier object's greater momentum will accelerate it faster than a light one.
In the atmosphere, a heavier man will accelerate faster down a hill and have a higher terminal velocity than a light one. Frontal area grows more slowly than the volume for a given shape, so it doesn't slow the heavier man down as much as his extra mass speeds him up.
Gravity hasn't changed: only the presence of an atmosphere makes a heavy rider faster than a light one.
I kind of like the steel bike/magnetism theory.
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Wind resistance and rolling resistance matter - but unless you have something really wrong they're not going to vary a great deal between one person and another.[/QUOTE]Sort of true but if the wind resistance doesn't increase with a heavier rider he will reach a higher terminal velocity before the forces due to gravity are balanced with wind resistance.
Gravity is a force, with a constant rate of acceleration working on the mass of the rider + bike (F=ma). When mass is larger, the force is larger, and acceleration won't reach zero until that larger force is balanced out by a larger force of friction of the air (wind resistance) and the bearings. So terminal velocity is higher, and up to that point acceleration remains higher for the heavier rider (since wind resistance is going to be pretty similar between any two riders on road bikes at the same speed).
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As for a bike with a theoretically non-existent rider, I believe tires make more of a difference than anything else in downhill speed. So don't worry about the frame.
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However, wind resistance will contribute a negative acceleration (i.e. a deceleration) that does depend on mass. Deceleration due to wind drag is proportional to 1/mass, which means it will slow down heavy riders less.
So, gravity accelerates all equally, but heavy riders are slowed down less by the wind, and therefore have a larger net acceleration downhill.
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I am no physicist, so I can't cite the correct rules, but I believe everyone is hung up on the wrong rules. The Pinewood Derby Rule of Physics says "All other things being equal, the heavier car wins" For those unfamiliar with the Pinewood Derby, it is an annual competition for Cub Scouts. They make their own small wooden cars and race them against other Scouts down a ramp. There is a weight limit of 5 oz. I was in charge of the competition in my sons Pack for three years. I observed over and over that a car that weighed 4.9 oz had no chance of winning.
In that same regard, I have seen over and over skinny people pass me on the uphill and me fly by them on the downhill. Everybody agrees reduced weight is very important to climbing, but cant seem to agree the opposite is also true.
In that same regard, I have seen over and over skinny people pass me on the uphill and me fly by them on the downhill. Everybody agrees reduced weight is very important to climbing, but cant seem to agree the opposite is also true.
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I think the term everyone is looking for is "inertia". Inertia is affected by mass. The more inertia you have, the less affected you are by resistance. Think about the amount of breaking power that would be required to stop a loaded freight truck going 55mph vs a Fiat going 55mph. The heavier bike/rider going downhilll is going to be less affected by road and wind resistance.
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Btw, p=mv would tell you how much damage a heavy and a light rider would cause if they smashed into a wall at the bottom of a hill. It doesn't explain why the heavy rider would reach the wall at the bottom of the hill first.
P.s. It is worth noting that riders on steel, lugged bikes tend to have a greater mass-to-surface area ratio. So, yes, in the practical sense, steel lugged bikes go downhill faster.
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Last edited by gaucho777; 07-16-12 at 04:27 PM.
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Why do people keep trying to prove their point by arguing things that only apply in a vacuum? We don't ride in a vacuum, people. In the world we live in, net force is greater in the heavier rider, the bike and rider position being equal, period.
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I'm not sure, but I've seen lighter cars win the Pinewood Derby. Not often, but all things being equal, the ones at 4.9oz generally are the fastest.
Last edited by RobbieTunes; 07-16-12 at 04:37 PM.
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You may be closer to the truth than you realize (now that the Higgs boson has been detected).
The fundamental particles of the universe that physicists have identified—electrons, neutrinos, quarks, and so on—are the "letters" of all matter. Just like their linguistic counterparts, they appear to have no further internal substructure. String theory proclaims otherwise. According to string theory, if we could examine these particles with even greater precision—a precision many orders of magnitude beyond our present technological capacity—we would find that each is not pointlike but instead consists of a tiny, one-dimensional loop. Like an infinitely thin rubber band, each particle contains a vibrating, oscillating, dancing filament that physicists have named a string. -Brian Greene
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For a number of years now, work has been proceeding to bring perfection to the crudely conceived idea of a machine that would not only supply inverse reactive current for use in unilateral phase detractors, but would also be capable of automatically synchronizing cardinal grammeters. Such a machine is the "turbo-encabulator." Basically, the only new principle involved is that instead of power being generated by the relative motion of conductors and fluxes, it is produced by the medial interaction of magneto-reluctance and capacitive directance.
The original machine had a base plate of prefabulated amulite, surmounted by a malleable logarithmic casing in such a way that the two spurving bearings were in direct line with the pentametric fan. The latter consisted simply of six hydrocoptic marzelvanes, so fitted to the ambifacient lunar waneshaft that side fumbline was effectively prevented. The main winding was of the normal lotus-0-delta type placed in panendermic semiboiloid slots in the stator, every seventh conductor being connected by a nonreversible tremie pipe to the differential gridlespring on the "up" end of the grammeters.
Forty-one manestically spaced grouting brushes were arranged to feed into the rotor slipstream a mixture of high S-value phenylhydrobenzamine and 5% remanative tetryliodohexamine. Both of these liquids have specific pericosities given by P=2.5Cn6.7 where n is the diathetical evolute of retrograde temperature phase disposition and C is Chlomondeley's annular grillage coefficient. Initially, n was measured with the aid of metaploar refractive pilfrometer (for a description of this ingenious instrument, see Reference 1), but up to the present, nothing has been found to equal the transcendental hopper dadoscope (2).
Electrical engineers will appreciate the difficulty of nubing together a regurgitative purwell and a supramitive wennelsprock. Indeed, this proved to be a stumbling block to further development until, in 1942, it was found that the use of anhydrous nangling pins enabled a kryptonastic boiling shim to the tankered.
The early attempts to construct a sufficiently robust spiral decommutator failed largely because of a lack of appreciation of the large quasi-piestic stresses in the gremlin studs; the latter were specially designed to hold the roffit bars to the spamshaft. When, however, it was discovered that wending could be prevented by a simple addition to the living sockets, almost perfect running was secured.
The operating point is maintained as near as possible to the h.f. rem peak by constantly fromaging the bitumogenous spandrels. This is a distinct advance on the standard nivel-sheave in that no dramcock oil is required after the phase detractors have been remissed.
Undoubtedly, the turbo-encabulator has now reached a very high level of technical development. It has been successfully used for operating nofer trunnions. In addition, whenever a barescent skor motion is required, it may be employed in conjunction with a drawn reciprocating dingle arm to reduce sinusoidal depleneration.
The original machine had a base plate of prefabulated amulite, surmounted by a malleable logarithmic casing in such a way that the two spurving bearings were in direct line with the pentametric fan. The latter consisted simply of six hydrocoptic marzelvanes, so fitted to the ambifacient lunar waneshaft that side fumbline was effectively prevented. The main winding was of the normal lotus-0-delta type placed in panendermic semiboiloid slots in the stator, every seventh conductor being connected by a nonreversible tremie pipe to the differential gridlespring on the "up" end of the grammeters.
Forty-one manestically spaced grouting brushes were arranged to feed into the rotor slipstream a mixture of high S-value phenylhydrobenzamine and 5% remanative tetryliodohexamine. Both of these liquids have specific pericosities given by P=2.5Cn6.7 where n is the diathetical evolute of retrograde temperature phase disposition and C is Chlomondeley's annular grillage coefficient. Initially, n was measured with the aid of metaploar refractive pilfrometer (for a description of this ingenious instrument, see Reference 1), but up to the present, nothing has been found to equal the transcendental hopper dadoscope (2).
Electrical engineers will appreciate the difficulty of nubing together a regurgitative purwell and a supramitive wennelsprock. Indeed, this proved to be a stumbling block to further development until, in 1942, it was found that the use of anhydrous nangling pins enabled a kryptonastic boiling shim to the tankered.
The early attempts to construct a sufficiently robust spiral decommutator failed largely because of a lack of appreciation of the large quasi-piestic stresses in the gremlin studs; the latter were specially designed to hold the roffit bars to the spamshaft. When, however, it was discovered that wending could be prevented by a simple addition to the living sockets, almost perfect running was secured.
The operating point is maintained as near as possible to the h.f. rem peak by constantly fromaging the bitumogenous spandrels. This is a distinct advance on the standard nivel-sheave in that no dramcock oil is required after the phase detractors have been remissed.
Undoubtedly, the turbo-encabulator has now reached a very high level of technical development. It has been successfully used for operating nofer trunnions. In addition, whenever a barescent skor motion is required, it may be employed in conjunction with a drawn reciprocating dingle arm to reduce sinusoidal depleneration.
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^I have heard from reliable sources that work on the turbo-encabulator was thwarted by the powerful dramcock oil industry lobby.
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Also, getting that close to a cyclist whose ability and intentions you don't know is a good way to effect a face/ground interface. If your front wheel touches his/her rear wheel, you're most likely going down. Be careful out there!
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