On Mon, 15 Oct 2007 16:32:10 -0700, Jim Thompson
On Mon, 15 Oct 2007 16:23:39 -0700, John Larkin
[snip]
No,he's right;those wheel spinners use low friction bearings,and any
crud will stop them.
So, you won't do the math either.
John
Math without practical experience is useless.
Practical experience without math is amateur guesswork.
John
John, I think you've got yourself out on a limb, on the wrong side of
the saw ;-)
I think it's you who has to put some numbers to it.
...Jim Thompson
I already did. And Guy confirmed it.
John
Macon?? That's almost as good as having "...bored..." do it ;-)
I think you need a pendulum of _substantial weight_ so that it
_doesn't rotate, but acts as a "pinning" point for the piston(s). What
weight does it take for a 1/2" piston working against 30PSI, and what
are the respective arm lengths?
If someone is going to get a bit creative and make a spinner-powered
tire pump, why not make the piston diameter 1/8 inch? That takes .37
pound. For that matter, how about 1/16 inch? That takes a bit over .09
pound of force.
Now, let's say you have .3 G braking and a ring-shped flywheel "spinner"
of diameter 60% of that of the tire. More like a big ring than "bling",
but this is for function and angineering calculations - it could
concievably be "blinged up" afterwards.
Ring with points accelerating (even if negatively) by .18 G only needs
to weigh a little over half a pound to have such
acceleration/decelleration provide enough force to push a 1/16 inch
diameter column of air 30 PSI above atmosphere.
For that matter, the flywheel could have a half pound outer rig welded
to it but have some point closer to the axle drive the pump. And there is
such a thing as gears.
Let's say the pump has a stroke of 1 inch, a bore of 1/16 inch diameter,
meaning volume of about 1/325 cubic inch. Let's say that a 35 to zero
braking at .3 G occurs 4 times a day, a 25 to zero braking occurs 6 times
a day and a 55 to 20 MPH braking occurs twice a day, 6 days a week. (Of
course I am pulling numbers out of a hat, probably on the conservative
side, for "typical driving".)
This adds up to 55 seconds a day if braking at .3 G, with average speed
reduction of 30 MPH per braking. I would consider the available kinetic
energy from the flywheel to be 1/2 times its mass (if in form of a ring)
times square of speed reduction of braking. So I would use half this 30
MPH braking figure for effective flywheel speed for calculating average
RPM of a pump shaft during braking.
I am guessing a fairly typical tire has a circumference of 6 feet - I am
feeling a little too lazy just now to go to the parking lot with a tape
measure. But 15 MPH and 6 feet means 3.67 revolutions per second. Times
55 seconds of braking a day, is 201-202 revolutions. Even if the pump has
only one cycle per cycle of flywheel outrunning the tire, that is 201-202
strokes. This is roughly 5/8 cubic inch of air for 1/16 inch diameter
bore, 1 inch stroke.
If the flywheel output to the pump is only 1.5 or so inches from the
centerline of the axle, a half pound ring flywheel, it will deliver enough
force to push a 1/8 inch diameter column of air 30 PSI above atmosphere.
That means 2.5 cubic inches a day. If the pump has so much drag with a
small bore to need force double or triple that required just to push the
air, make the flywheel a ring of 1 to 1.6 pounds.