"Anthony Jones" <
[email protected]> wrote in message
news:
[email protected]...
> DavidR wrote:
>> You apply a force on the pedals, which applies a force on the rim
>> proportional to crank & rim diameters and sprocket ratios to perform
>> whatever accelerate/decelerate manouevre you are doing.
>>
>> Torque is only internal to the mechanism. For example, applying force to
>> the left hand crank puts a torque on the axle transfering the drive
>> across
>> the frame.
> I'm afraid I still don't get how that contradicts what I was saying.
I wasn't really paying attention to what you were saying in detail. I am
not interested in skid stops on a fixer, either for aesthetic or technical
reasons. It's only that the curious use of the word 'torque' jumped out.
> I felt that a description in terms of the torque resulting from the force
> on
> the pedals
....about what axis?
> was clearer than referring solely to 'force' when there are two
> pedals and the forces are in unspecified directions...
You have a crank describing a diameter of about 13 inches. The sprockets
give you an imaginary wheel of about 60 inches diameter. It's also an
imaginary direct drive - think of a penny-farthing. Force on the pedal
gives 13/60 of that force at the rim. That's all that matters in your
experiment.
But...real wheels are not 60 inches. It's most likely 27 inches. Let's
assume you need 54 pound force (for sake of argument), to lock the back
wheel. That's equivalent to the wheel being driven by 48 foot-pound force.
Now try a Brompton which has 16 inch diameter wheels; to lock you will
need exactly the same 54lb force at the rim. That would be developed from a
torque of 20lbf-ft.
Don't you now see that torque is not meaningful?