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Author Topic: I need a Bill Nye the Science Guy  (Read 1166 times)

Nodsleinad

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I need a Bill Nye the Science Guy
« on: June 04, 2008, 05:59:52 AM »
How can one measure the Coefficient of Friction of a Bowling Ball?

Thanks - Nod
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Edited on 6/4/2008 2:00 PM
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1MechEng

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Re: I need a Bill Nye the Science Guy
« Reply #1 on: June 04, 2008, 02:13:22 PM »
Static or kinetic COF?
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Dan
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Engineering * Bowling = a fun and practical application of rotational kinematics.

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Dan

Nodsleinad

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Re: I need a Bill Nye the Science Guy
« Reply #2 on: June 04, 2008, 02:14:14 PM »
It will be for a bowling ball  So i guess Kinetic?  For the coverstock

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1MechEng

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Re: I need a Bill Nye the Science Guy
« Reply #3 on: June 04, 2008, 02:26:45 PM »
Juggernaut is on the right track (no pun intended).
On edit - Juggernaut's post has disappeared. Wonder where it went?!

From Wikipedia:
quote:
Static friction and kinetic friction

Friction forces are categorized as either static or kinetic. The coefficient of static friction ìs, characterizes friction when no movement exists between the two surfaces in question, and the kinetic coefficient ìk, characterizes friction where motion occurs. While static and kinetic friction differ in value (the coefficient of static friction typically being greater than that of kinetic friction), both result from the electric force acting on microscopic irregularities in two adjacent surfaces. It should be noted the friction force depends mostly on the resultant force acting on the body, while the motion of the body only influences the distinction between static or kinetic. While it is easier to visualize friction in terms of motion, its dependence is on the Resultant Force acting on a body.

The static friction force must be overcome by an applied force before an object will move. The maximum possible friction force between two surfaces before sliding begins is the product of the coefficient of static friction and the normal force: Fmax = ìsN. It is important to realize that when there is no sliding occurring, the friction force can have any value from zero up to Fmax. Any force smaller than Fmax attempting to slide on surface over the other will be opposed by a frictional force of equal magnitude and opposite direction. Any force larger than Fmax, will overcome the force of static friction and cause sliding to occur. The instant that sliding occurs, kinetic friction is applicable, and static friction is no longer relevant.

When the Resultant Force acting along the plane of a surface increases in value, a proportional increase in Static Friction Force results, up to a maximum value Fmax. Since this is the maximum value which Static Friction can take for any particular material, a further increase in the Resultant Force will produce motion. A lower value of friction, kinetic friction, replaces static friction for the duration of the movement.

When one surface is sliding over the other, the friction force between them is always the same, and is given by the product of the coefficient of kinetic friction and the normal force: F = ìkN. The coefficient of static friction is larger than the coefficient of kinetic friction: it takes more force to make surfaces start sliding over each other than it does to keep them sliding once started.

These empirical relationships are only approximations: they do not hold exactly. For example, the friction between surfaces sliding over each other may depend to some extent on the contact area, or on the sliding velocity. The friction force is electromagnetic in origin: atoms of one surface "stick" to atoms of the other briefly before snapping apart, causing atomic vibrations, and thus transforming the work needed to maintain the sliding into heat. It should also be noticed that the coefficient changes slightly along a surface and that the coefficient is simply an approximation. However, despite the complexity of the fundamental physics behind friction, the relationships are accurate enough to be useful in many applications.



Thus, coeffs. of friction are empirical (that is to say - statistically derived from recorded measurements) in nature. As a result, they are, at best, only very good approximations.

To answer your post, you would need to find or create a test surface and drag the bowling ball over it. This test surface would ideally be very hard, very tough, and machined to a known surface roughness in order to prevent wear and allow its use in multiple tests. It should also be level, flat, clean, and at a constant temperature. You could test the static coeffs. (before movement of the ball), and kinetic coeffs. (once the ball is moving at a constant test speed). You could also test the rolling friction of the ball, if the test surface was long enough, flat enough, and level enough.

Hope this helps!



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Dan
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Engineering * Bowling = a fun and practical application of rotational kinematics.

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Edited on 6/4/2008 2:27 PM
Dan

Juggernaut

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Re: I need a Bill Nye the Science Guy
« Reply #4 on: June 04, 2008, 02:31:21 PM »
OOOOPS.  

  Was editing my post and hit the wrong dang button .  

   Oh well, 1mecheng has it going on anyway.  The gist of what i said was that, to measure variable factors, such as friction of different coverstocks, you must make all other factors known, leaving the friction the only variable.

  When you have done this, you can rate the differences between the friction/resistance encountered.

  Before you could come up with numbers comparable to those used by the USBC, you would have to run your test under those same criteria and use their scale of resistance to calculate the COR numbers.
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Edited on 6/4/2008 2:34 PM
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