Toward the Design of an Optimal Recumbent
Preface
Lest I be misunderstood in discussing an "optimal" recumbent bicycle, I should clarify that I intend to mean a recumbent "for the masses", intended primarily for leisurely street and (somewhat) sporty touring considerations. I am not addressing the ultimate land speed record recumbent, not the ultimate recumbent mountain bike.
1.0 - Bicycle Geometry and Stability
The standard "upright" bicycle has reached a degree of near perfection. A well-made touring bicycle
is an object of grace, performing the tasks demanded of it almost effortlessly. The fact that you
can pilot a good bicycle hands free (not recommended) and even control gentle steering through
minor shifts of weight and acceleration are a testament to the fine degree of balance the modern
bicycle has achieved.
The goal of this exposition is to achieve this same degree of natural riding experience in a recumbent.
To understand the difficulties associated with this goal, we need to understand what makes
a standard bicycle behave the way that it does. Three of the major qualities of bicycle geometry
that make a bicycle ride naturally are
We take each of these in turn, and illustrate how they come together to produce a well-balanced machine.
Note: For the mathematically-inclined, see my Bicycle Geometry Mathematics page.
1.1 - Steering Castor
Take any good upright bicycle, hold it in the straight and vertical position,
turn the front wheel slightly, and then push the bicycle forward from the seat.
Notice that the front wheel immediately tends to straighten toward the direction
of motion. This effect is due to what is called positive steering castor, or positive
steering trail, and is evidenced primarily during acceleration. Figure 1 below
illustrates steering castor.
The measure of steering castor, or trail, is given by the displacement
of the steering head point (the extension of the steering tube axis to
the ground) with respect to the wheel contact point with the ground.
(A more accurate measure, from the standpoint of physics, would be
the horizontal component of the displacement from the wheel contact
point to the point on the steering head axis that is orthogonal to the axis,
called the steering trail normal. However, either they are both positive,
or both negative.) Figure 1a illustrates the effect of negative trail - as
the bicycle accelerates forward, a small degree of steering will tend to
become more severe, and the rider would need to exert additional effort
against the direction of steer to keep the wheel tracking along the intended heading.
Figures 1b and 1c both illustrate positive trail, whereby acceleration tends
the straighten the wheel to align with the direction of motion. This effect
exists because a non-spinning wheel does not want to begin spinning on its
own - one must overcome the wheel's rotational inertia to give it rotational
(angular) momentum. The resistance to the gain in angular momentum is
experienced by the wheel as if the ground is trying to drag the wheel toward
the rear. The ground is essentially "grabbing" the wheel at its ground contact
point and pulling it backwards. This will tend to straighten the wheel if the
ground contact point is already behind the steering head point, but will move
it further from straight otherwise.
1.2 - Steering Lift
Refer again to figures 1b and 1c above. Both of these illustrate (good) positive
steering trail, but they have poor steering lift (actually, 1c has negative steering lift,
while 1b will exhibit negative steering lift as the bike is canted into a turn.)
Steering lift refers to the degree to which the bicycle frame (or its center of gravity)
either rises or falls as the wheel is turned. Take a good upright bicycle, hold it in
the straight and vertical position from the frame near the steering tube, and then
turn the wheel 45 degrees. You should notice that the frame has risen slightly,
and that by pushing downward on the frame you will tend to cause the wheel to
straighten and diminish the steering. This effect is due to a combination of two
factors - the steering head angle (often called the rake angle) and the steering
"offset", being the orthogonal distance from the steering axis line to the wheel center.
I will refer to this distance as the "steering radius".
With small but positive steering lift, a rider should feel a slight pressure resisting
the direction of steer. With negative steering lift, as the rider begins a turn, their
own weight will tend to cause the wheel to "steer ahead" of their effort, or over-steer,
and they must exert force against the direction of their intended steer in order to keep
the steer from becoming greater than their intent. Figure 2a illustrates (severe) negative
steering lift. If you attempted to ride such a bike "hands-free", and the wheel begins
to turn, it will suddenly turn violently, despite the fact that this configuration has "great" steering trail.
1.3 - Counter-Canting Steer
To get a sense of counter-canting steer, imagine you are riding at a good speed on a
curved road in a constant and gentle right-hand turn. Naturally, you and the bicycle
are slightly canted (leaning) to the right, toward the direction of the center of your
turning circle, to maintain constant balance. Up ahead, you can see that the road
will soon straighten, and you must prepare to eliminate this lean and bring the
bicycle upright. How do you "un-cant" yourself?
There are two ways to accomplish this. One way is to accelerate, because as you
travel along any circle, increasing your tangential velocity will increase the effective
outward centrifugal force. Another way is to momentarily increase the degree of
rightward steering, as this will cause the bicycle to begin tracking a smaller turning
circle, and (again) increase the effective outward centrifugal force.
But this is not the whole story. Consider a bicycle with "naive" rear-wheel steering
(where the RSR is smaller than the FSR). To maintain the same gentle right-hand
turn described in the previous paragraph, the rear wheel is steered to the left. If the
steering is momentarily increased (the rear wheel is turned further to the left), the
bicycle is indeed "tracking a smaller turning circle", and must eventually produce a
greater outward force. But the immediate effect is that the rear wheel is initially
tracking this new circle to the left, causing the cant of the bicycle to increase rather
than decrease, until the rear of the bike swings around to the far side of this new
turning circle. This is a very unsettling and counter-intuitive effect.
Figure 3 illustrates what is really happening with standard front wheel steer
(where FSR < RSR) and "naive" rear wheel steer (where RSR < FSR).
Figure 3a represents a bicycle in a constant right-hand turn. I have purposely
drawn it so that both the front and rear wheels are tracking the same turning
circle, leaving it ambiguous as to whether this is front wheel or rear wheel steering.
Notice that you find the center of the turning circle at the intersection of the two
vertical planes (green lines) containing the ground contact points of the front and
rear wheels, and each perpendicular to the tracking direction of the respective
wheels. The red line, denoted the "turning arm", connects the center of the turning
circle to the bicycle's center of gravity, and the blue arrow indicates the direction
of the bicycle's current heading (direction of momentum). (If the bike were to hit
"frictionless ice" at this moment, the bike would slide along the blue line.) Note
that the blue momentum line is exactly tangential to the current turning circle,
and perpendicular to the turning "arm".
Figure 3b shows what happens with front wheel steering, if the rider suddenly
increases the amount of rightward steer (and the tires do not slide.) Notice that
not only has the new turning circle gotten smaller, its center has moved *behind*
the red line of the previous turning circle. This means that the bicycle's current
momentum line is no longer tangential to the new turning circle, but is actually
heading *away* from the circle, and away from the tangent heading of the new
turning arm. This effect is what is immediately responsible for lifting the bike up
from its current canting angle, and is what I will define as Counter-Canting Steer.
Importantly, note that suddenly turning the wheel provides the bike a new "tangent heading",
but does not immediately alter the momentum heading.
Figure 3c shows what happens with (naive) rear wheel steering, if the rider
suddenly increases the amount of leftward steer to the rear wheel to force a
"sharper" right turn. Again, the new turning circle has gotten smaller, but now
its center has moved *ahead* of the red line of the previous turning circle.
This means that the bicycle's current momentum line is carrying the bicycle
*into* the new circle (compared to the new tangent heading) rather than
away from it. This is what will cause the bike's canting angle initially to *increase*.
It should be clear from these diagrams that one must have FSR < RSR
(modulo rake angle) in order to have counter-canting steer. Specifically,
with the bike canted into a turn, extend the steering head axis to the ground
and call this the "steering head point". This point also lies on the intersections
of the lines representing the directions of the front and rear wheel tracks.
The line segment connecting the front wheel contact point to the steering
head point, and the segment connecting the rear wheel contact point to the
steering head point, are essentially the "shadows" cast by the FSR and the
RSR upon the ground, if light shines down in parallel to the steering head axis.
It is actually the FSR-shadow that must be shorter than the RSR-shadow
that is required to have counter-canting steer.
Wheel Diameter
Another property that upright bicycles enjoy is the ability to easily
accommodate large wheel diameters on a relatively short wheelbase.
Having large wheel diameters provides two benefits. First, it allows
the bicycle to moderate the jarring effect of small bumps in the roadway,
thus lessening the need for suspension. Figure 4 depicts a 15" and 30"
wheel encountering a 2" curb. Note that upon "impact", the path of the
smaller wheel center must make a larger instantaneous change of trajectory
(red arrow) in order to ride up and over the curb. A second benefit is
added gyroscopic stability at high speed. (If you can find a long, steep,
well-paved and isolated roadway, take a good 26-inch bike to top
speed on a downhill run. As you approach 50-60 MPH, try to
"recklessly" swerve the bike left and right - it is almost impossible.
As far as steering and canting goes, the bike acts like it is moving
through molasses.)
In summary (so far), one can appreciate why the standard upright
bicycle, with its moderate rake angle (as measured from vertical),
its moderate steering offset (FSR) and moderate trail come together
to forge the finely balanced machine that so many people enjoy.
Any bicycle, be it front or rear wheel steer, front or rear wheel drive,
upright or recumbent, cannot stray far from a careful relationship
among these settings and produce a "naturally" rideable machine.
With these considerations (and some others) in mind, let us set forth
to design the "ultimate" recumbent bicycle.
2 - Recumbent Bicycles
2.0 - Recumbent Position Pros and Cons
2.1 - RWD - SWB
One of the first "equations" we can write for recumbents is that RWD = VLC
(very long chain). I consider this to be a largely negative feature (the entire
chain-path must be protected from interference with body and clothing,
and it requires many intermediate and noisy chain-guiding rollers). It is
largely unavoidable with Rear-Wheel-Drive recumbents, both for short
and long wheelbase designs.
2.2 - RWD - LWB
Figure 5d depicts the Long Wheelbase alternative for Rear Wheel Drive.
Here, the pedal crank is maintained at a lower altitude by placing the front
wheel ahead of the pedals.
2.3 - FWD - SWB (FWS)
The solution to "Very Long Chain" is to power the front wheel, as this is the general
location of one's feet in a recumbent position. Unfortunately (for most designs), the
front wheel is also the wheel that is expected to effect steering. The "lateral inflexibility"
of chain drive means that the pedal crank must be kept fixed in, and perpendicular to
the plane of the wheel being driven. Hence, as one steers the front wheel left and right,
the entire pedal system must swing left and right along with the wheel. This places
interesting constraints on front wheel drive bicycle designs.
2.4 - FWD - SWB ("RWS")
But who says you must "ride in the back"? Why not take the front seat?
A radical alternative for Front Wheel Drive design is the Kalle FWD, "Rear Wheel Steer"
design. I quote the words "Rear Wheel Steer" because (as one person wrote) the Kalle
can be thought of as front wheel steer - with the rider positioned on the handle bars.
Note that the position of the steering tube allows the bike to maintain a reasonable
steering geometry. I will call this Rear Wheel Steer, precisely because the rider remains
in fixed alignment to the front wheel (and pedal crank) during a steer, while it is the rear
wheel that moves "out of alignment" with the rider during steer.
2.5 - The Z-Bike
Here, I propose two "radical" modifications to the Kalle FWD-RWS design,
in a design I have designated the "Z-Bike".
The first of these modifications is not terribly radical, and certainly has its own weight-related
downside. Construct the front frame to straddle both sides of the front wheel while remaining
open at the top, allowing the wheel to move up and past the top of the frame for suspension
travel, and allowing the crank to maintain a lower position forward of the front wheel.
This "split frame" (in itself) would not allow for a much larger front wheel, nor a much
lower rider position, as the rider's legs must still reach across the wheel diameter and
allow room for the steering tube. Larger front wheel and lower crank position only
becomes possible when the rider can get closer and "more intimate" with the front
wheel, a generally impossible situation, because there is then no room to place the
steering tube and allow the rear steering assembly to move freely beneath the rider.
With the Z-Bike, the steering tube is replaced by a pair of swiveling arms in a
trapezoidal arrangement (see figure 6). This steering mechanism can be placed
well behind the location of the would-be steering tube, and at various elevations,
yet it will cause the bike to "fold" at a point that approximates the standard
steering tube position - what I will call the "phantom steering tube" or
"phantom steering axis". One can adjust the "phantom" rake angle directly by
the angle in which the steering assembly mounts to the front frame, and can
adjust the "phantom" front steering offset either by the selection of mount point,
or by the length of the swivel arms employed, or even by the ratio between the
separation of the front steering pivots and the rear steering pivots.
Figure 6a illustrates the steering arrangement of a standard upright bicycle,
from a "top view" (actually, from a view that aligns with the steering tube,
depicted as a red circle offset from the front wheel center). The "rear frame"
is depicted in blue, and the horizontal gray line maintains the front and rear
wheel ground contact points. With figure 6b, a 30-degree left steer is shown
(with bike held vertical). Notice that the steering tube has shifted to the right,
and that the rear wheel is actually "steering" about 4 degrees to the right.
This has also resulted in moving the rear wheel forward, shortening the wheelbase
by some fraction of an inch. (Of course, in a "real" 30 degree steer, the bike
would be canted over to the left, and the wheel contact points would move further
apart, actually increasing the effective wheelbase.)
Figure 6c illustrates the Z-Bike steering mechanism, before steering is applied.
Note that the two steering arms (depicted in red) form a trapezoid, as the pivot
points near the front wheel are closer together than those near the rear wheel.
With figure 6d, a 30-degree left steer is shown. The large red circle on the
front wheel indicates where a "standard" steering tube would appear, and is
now the "phantom" steering tube. Note that at 30 degrees of steer, the rear
wheel still steers about 4 degrees to the right, and remains pointing (approximately)
to the phantom steering tube, as if the rear frame was rotating about that point.
(Note also, the "double-bent" shape of the frame during a steer is reminiscent
of the letter "Z", hence the "Z-Bike" name.)
With any solution, new "problems" appear. There are indeed drawbacks to the
Z-bike mechanism. Careful examination of figure 6 would show that, as steering
is increased, the "phantom" steering tube actually drifts backward a bit (increasing
the front steering offset), and the rear wheel has moved several inches closer to
the front of the bike, diminishing the wheelbase and causing steering to increase
the degree of turn effected. (Alternately, one could argue that less "steer" is
needed to effect an equivalently sharp turn for the bicycle as a whole.)
In any case, geometry will show that these effects can be reduced by lengthening
the two steering arms and moving the mechanism back a bit further from the front
wheel, at the expense of lengthening the overall wheelbase.
Another potential drawback to the trapezoid-arms steering system is that it is
very difficult to obtain an effective steering angle of more than about 50 degrees.
Of course, one rarely applies such a sharp steering angle except when practically
at a standstill, or walking the bike, and by then the bike's overall wheelbase will
have been reduced to such an extent that 50 degrees provides for a very small
turning radius, such as one might obtain at 60-65 degrees of steer for a standard bike.
Of course, a more general drawback to the Z-bike design is simply its structural
considerations. Although it affords a rather sleek, "compact" and unified framework,
that framework is still rather substantial, weight-wise. With its additional complexity
comes additional expense – the single thrust-bearing-housed steering tube of a standard
bicycle becomes four such (albeit smaller) tube-assemblies with the Z-Bike, to
accommodate the four pivot-points of the trapezoidal steering mechanism.
In its favor, one could design an adjustable mount point (location and angle) for
the front pivot assembly, along with "replacement" pivot arms of various lengths,
that would easily allow one to create a very wide range of bicycle geometries.
On another positive note, notice that this design allows the pedal crank to be
further ahead of the front wheel, and lower, than with any other FWD design.
Since the chain travel from crank to wheel most be kept relatively constant, a
suitable front suspension (that does not jar the rider's feet) demands that it pivot
very close to the crank. Other FWD designs must place the crank so far above
the front wheel, that such suspension travel moves the wheel more "backwards"
than upwards, an issue that is addressed well in the Z-bike design.
There is one more issue that must be mentioned with all "Kalle" type bicycles.
For all RWD bikes, the front wheel can be steered "very rapidly" to the left or
right if desired, since it is only the front wheel, fork and handlebars that are at play.
However, with the Kalle (and to a lesser extent, all FWD designs) far more mass
exists to be rotated to effect a change of steer. Although we might call Kalle-type
designs "rear wheel steer", we fully expect that as we pull upon the handlebars it will
be the front section (and rider with it) that performs most of the "turning". There is a
danger that, with too much front-loading of weight, together with the angular inertia
presented by the rider, an attempt at a "sudden left-hand steer" might cause the rear
section to slide to the left, rather than stay put and allow the front section to turn left.
Mitigating this potential requires moving the rider back and increasing the "recumbency"
(moving more weight toward the rear), while ensuring that the majority of the rider's
mass remain as close as possible to the steering axis (real or phantom). This (once again)
leads us toward a bit smaller front wheel.
Summary
Having confessed to its variable deficiencies, I feel that the Z-Bike "solves" the
major issues I see with the standard Kalle design (and other recumbent designs in general).
In summary, the Z-Bike accommodates all of the following design goals:
Given the outlined Z-Bike design, there exists room for further innovations
(a variety of specific mechanisms to apply steering force to the trapezoidal
steering system can be developed, for example.) But whatever improvements
exist to be made, I believe they will center around the Z-Bike configuration on
a path to the ultimate sport-touring recumbent.
Additional (Computer-Generated) Images
Below I intend to provide additional images of possible Z-bike implementations. Enjoy!
Here is a detail view of a potential steering mechanism, using a ball-and-socket linkage between the handlebar pivot arm and the trapezoidal steering arm.
It may be counter-intuitive to view this image and SEE the virtual steering axis. One tends to imagine that the bike could fold (rotate)
independently about either the front, or rear steering pivots. However, the trapezoid location of the 4 pivots actually constrains the
steering arms so that they cannot pivot independently, and the bike is thus forced to behave as if a steering tube were present along the
indicated green line.
Here are several images that show the Z-bike in various degrees of steering (and canting.) Each sequence of four images depicts
0, 10, 20 and 30 degrees of steer, in concert with 0, 10, 20 and 30 degrees of front wheel canting (leaning) into a turn.
NOTE: If you download these images and save them to a separate folder, you can view them with (say) Windows Picture and Fax Viewer
(surely the Mac has something similar), and rapidly click the next-image button to get a sense of the bike as its steering is increased.
NOTE: If some images do not appear, you may need to click browser-refresh.
Note: For the mathematically-inclined, see my Bicycle Geometry Mathematics page.
Solution - Eliminate the Steering Tube