Scientific American Supplement, No. 447, July 26, 1884 — John Shaqi
Scientific American Supplement, No. 447, July 26, 1884Various
Science
Scientific American Supplement, No. 447, July 26, 1884
Various
Science -- Periodicals
In the first place, the rider is placed over the main wheel, as in the
bicycle, but much further forward. There are around him, on or near the
ground, four little wheels, two before and two behind, supported in a
manner the ingenuity of which calls for the utmost admiration. Turning
the steering handle not only causes the front and rear pairs to turn
opposite ways, but owing to their swiveling about an inward pointing
axis, the machine is compelled to lean over toward the inside of the
curve; not only is this the case, but each pair rises and falls with
every inequality of the road, if the rider chooses that they run on the
ground; but he can, if he pleases, arrange that in general they ride in
the air, any one touching at such times as are necessary to keep him on
the top of the one wheel, on which alone he is practically riding. He
can, if he likes, at any time lift the main wheel off the ground and run
along on the others only. The very few machines of the kind which I have
seen have been provided with foot straps, to enable the rider to pull as
well as push, which is a great advantage when climbing a hill, but this
is on every machine except the Otto, of which I shall speak later,
considered a dangerous practice.
Some of the objections to the bicycle to which I have referred were
sufficient to prevent many, especially elderly men, from dreaming of
becoming cyclists. So long as the tricycle was a crude and clumsy
machine, there was no chance of cycling becoming a part, as it almost is
and certainly soon will be, of our national life. The tricycle has been
brought to such a state of perfection that it is difficult to imagine
where further progress can be made.
Perhaps it will be well to mention what is necessary in order that a
three-wheeled machine may be made to roll freely in a straight line, and
also round curves. At all times each wheel must be able to travel in
its own plane in spite of the united action of the other two. To run
straight, the axes of all the wheels must obviously be parallel. To run
round a curve, the axis of each must, if continued, pass through the
center of curvature of the curve. If two wheels have a common axis, the
intersection of the two lines forming the axes can only meet in one
point. To steer such a combination, therefore, the plane of the third
wheel only need be turned. If the axis of no two are common, then the
planes of two of the wheels must be turned in order that the three axes
may meet in a point.
Not only does free rolling depend on the suitable direction of the
planes of the wheels, each wheel must be able to run at a speed
proportional to its distance from the point of intersection of the three
axes, i.e., from the ever-shifting center of curvature.
Public-domain text, read in full here on John Shaqi.
Reviews
Reviews
No reviews yet
Be the first to share your thoughts on this work.
Join the Discussion
Join the discussion
Sign in to leave a comment or review.
Sign InorCreate an account