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Re: Centripetal F from friction



OK, let approach the same problem from the other end. The
radius R is given and I want to know by how much should
the front wheel (or wheels) be turned to follow the circle at
a given speed.

The angle iz zero when R is infinity; R decreases when the
angle (between the planes of front and back wheels) becomes
larger. Driving experience tells me that there is only one
answer for a given car on a uniform horizontal surface.

I know that the resultant of frictional forces acting on all
wheels must be equal to centripetal force. Suppose the
speed and the mass of the vehicle are given. Then I can
calculate the centripetal force needed as Fc=m*v^2/R. At
what angle should the front wheels (or wheel) be turned to
generate this force? The distances between the wheels are
presumably known. Specify other details, if necessary.
I have no idea how to solve this problem.

Hugh Haskell wrote:

At 22:28 -0500 10/31/01, Ludwik Kowalski wrote:

Is this OK?
A tricycle is moving along a straight line on a horizontal floor.
All three wheels are parallel. Then the front wheel is turned
by 10 or 20 degrees and the path becomes circular. The wheels
roll without sliding or skidding. What is the radius of the path?

My guess is that R does not depend on the speed. To estimate
the radius I would replace (on my drawing only) the back
wheels by a single wheel in the middle. Then I would say
that the plane of the back wheel is tangent to the circle and
the plane of the front wheel is tangent to the circle. Knowing
the distance between the centers of two wheels I can trace
the circle and determine R (or derive a formula for R). Would
this produce a good prediction? Probably not. Why not?

I think that a tricycle would be easier to analyze than a bicycle
because the is no tilting.

Assuming no tilting, and you have stated that the tires do not slip
or skid. Then you cannot predict the radius of the circle, because
the friction that is providing the centripetal force is static
friction, whose law is an inequality. So as you go around the circle,
you can go at any radius or any speed as long as the centripetal
force necessary is less than the maximum possible static friction
force between the wheels and the floor.

What you can do is predict the minimum radius for a given speed, or a
maximum speed for a given radius. Just plug in the maximum friction
force for the surfaces and solve for the missing item.

Its the same if you allow tilting, only figuring out the friction
force is a bit more tricky.

An almost as interesting problem that is solvable is to find the
turning radius for an airplane in balanced flight at a given speed
and given angle of bank. Turns out to be independent of the mass of
the airplane. Complicating factor: when you bank the plane the amount
of lift available to maintain the plane's altitude decreases, since
it is always perpendicular to the wings (assume no dihedral for
simplicity). Hence in order to maintain altitude, and airspeed, you
have to add power, because you need to raise the nose a bit to
increase the lift of the wings, which slows down the aircraft. If you
are going to slow for the angle of bank, the airplane can stall. Fun
to do at altitude, but really scary if it happens as you turn onto
your final approach during landing when you are only a couple of
hundred feet up.

I'm sure John D. can tell you of at least one instance where a
student did it to him. Probably only one, though, since that is a
lesson that you learn very well the first time-if you survive. I'm
sure that was the kind of stall that little girl who was trying to
solo across the country a couple of years ago, when she spun in soon
after takeoff from Cheyenne, Wyo. Turning when you are low, slow and
heavy can get you into really big trouble very fast, especially if
you are inexperienced.