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Moment of Inertia Print E-mail

Weight is not the whole story

Moment of Inertia is white-coat, taped-glasses technical jargon for “rotating weight”. For cyclists, it is as closely related to performance as weight, and should be heavily considered when choosing big components that spin, like wheels.

More specifically, Moment of Inertia (denoted by the engineering community) is a measure of resistance to change of angular velocity. It is a function both of weight (or mass) and how the weight (or mass) is distributed. It takes more torque to accelerate an object (like a wheel) with a large moment of inertia than an object with a smaller moment of inertia. In this sense, moment of inertia is like mass; it takes more force to make something massive move faster. However, even if two rotating objects have the same weight, the one with the smaller moment of inertia takes less torque to accelerate. That is why Cane Creek wheels accelerate so quickly: they are not just lightweight, they also have a low moment of inertia because of the patented nipple at the hub design and lower spoke count.

So clearly, this moment of inertia thing is a big deal. Let’s work out the details. Newton’s
second law of motion states:

fig_01.jpg 
That is, the sum of the forces on a body is equal to the mass of the body times the acceleration of the body. However, this only applies to rectilinear motion, i.e. to things that are not spinning. A cyclist might think of this equation as follows:
I can generate a certain amount of force, therefore if my bike weighs less I have a greater acceleration. Greater acceleration means I get to the finish line sooner, I get to work faster, and I can finally outrun that angry dog!

If nothing on your bike was spinning, this would be the end of the story. Since rolling bicycles are much faster than sliding bicycles, there is more to this story. Newton’s second law also applies to rotational motion. For rotating objects it states:

fig_02.jpg

where τ = torque, I = moment of inertia, α = angular acceleration. In words, torque equals
Moment of Inertia times angular acceleration. A cyclist might think of this equation as
follows:
I can generate a certain amount of torque, therefore if my wheels have a lower moment of
inertia, I can make them accelerate faster. More acceleration means I can get to the
finish line sooner, I get to work faster, and I can finally outrun that angry rabid dog!
To tie these two concepts together, we can use the fact that on a bicycle there is a
fundamental relationship between acceleration and angular acceleration. Specifically, 
fig_03.jpg  
which comes from the fact that bicycle wheels do not slip on the ground as they roll. In the above equation, r  is the radius of the inflated tire. Using this relationship, and a small assumption about how chain force is transmitted to the hub (see Advanced MOI ), allows us to obtain the following more insightful equation. 

fig_04.jpg

With this equation a cyclist is finally in a position to think clearly.

I can generate a certain amount of force. To increase my acceleration, I need low weight AND low moment of inertia! If my bike is light and my wheels have low moment of inertia, I can cross the finish line first, sleep in late since I can get to work so quickly, and after that angry rabid dog sees how fast I am, he’ll never chase me again!

As can be seen, moment of inertia is just as important as mass. Indeed the quantity 

fig_05.jpg

is often referred to as “equivalent mass”, since it is a true measure of how force is related to acceleration when the force acts on bodies that both translate and rotate.   Cane Creek has addressed this fundamental property with our patented wheel design.

 

By combining the best rims technologies and the best spokes with our proprietary low moment of inertia nipple at the hub design, Cane Creek wheels get you there faster.


The story does not end there. The same “equivalent mass” concept that relates force to acceleration also applies to deceleration. Consequently, Cane Creek wheels not only accelerate faster, they also require less force to stop. To the rider this translates into less force at the brake levers and decreased stopping distances. A cyclist can interpret this as:

Since my Cane Creek wheels stop faster with less effort, I can stay at speed longer without worrying about overcooking the corner, I can have a fighting chance to avoid T-boning that SUV that just turned in front of me, and I can stop short of smashing that cute little puppy.

As though better acceleration and deceleration are not enough, the low moment of inertia design of Cane Creek wheels make turning and cornering easier. Since the same physics apply to turning and cornering as apply to accelerating and decelerating, less force is required at the handlebars to change the direction of the bike. 

For more details on this analysis, a complete derivation of the equations, and some arguments on energy saved due to lower moment of inertia, please see Advanced MOI

 
 
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