Shimmy Analytics:
It appears as if all trikes and quads have
a natural tendency to shimmy unless the proper damping provisions are included
in their design. The purpose of this
section is to quantify what effects the speed that such a shimmy sets in and
its amplitude and how the various design parameters affect the outcome. With this knowledge at hand, you can
determine what effect changing the weight of the wheels or their size, or the
stiffness of the suspension will have on the shimmy properties before you
complete your design choices.
Primary Resonant System:
You can think about this along the
following lines. The outrigger wheels
are essentially like a dumbbell in that they represent two masses (tires, rims
and hubs), each independently sitting on a spring (the torsion suspension unit)
suspended at the ends of a connecting frame.
As one wanders down the road, the rotating wheels bounce alone, jiggling
this dumbbell at a frequency that steadily increases with speed. At a particular speed, the unit will be
jiggled at its “natural frequency”. That
is a special frequency where each cyclic jiggle will add energy to the system amplifying
the resulting jiggling motion. Above or
below this frequency (speed) the motions are naturally damped and minimal.

We are all familiar with pushing a child on
a swing. The swing will have a natural
cyclic motion depending on the weight of the child and the length of the swing
support. If one pushed at just the right
rate (when the swing is at the end of its cycle), the child can be pushed
higher and higher with each added shove.
This is adding energy at the same rate as the natural frequency of the
system. If one decides to push as some
other rate, the swing will actually absorb the energy but slow down. Wikipedia has several good entries on this
natural frequency phenomenon. (http://en.wikipedia.org/wiki/Natural_frequency)

The formula for the suspension’s natural frequency:
K is the “spring
constant” that measures the force necessary to move the outrigger wheel a
certain distance when load is applied.
If you recall, the torsion suspension unit I initially used was rated at
250 lbs per wheel and at this load, the wheel’s axle rotated approximately 2.5
inches. It was necessary to be certain
that at least this fender clearance was provided. The spring constant is therefore: 250lbs/2.5 inches = 100 lbs per inch. To use this in the equation it must be
expressed as pounds per foot thus K = 1200 lbs per foot.
M represents the mass (weight) of the wheel suspended at the extremity
of the outrigger frame by the suspension.
This would be the tire + wheel rim + hub. This is what will be bouncing along the
road. For my 13 inch wheel, the tire and
wheel rim weigh 33 lbs and the hub weighed another 6 lbs for a total of 39
lbs. To use this in the equation, it
must be expressed as mass by dividing the weight by the gravitational constant
“g“ = 32.174 feet per second2.
The resulting units are called slugs (English humor I assume). Thus M as used in the equation becomes 39
lbs/32.174 feet per second2.
M = 1.21 slugs.
When
one combines all of the numbers in the formula above, it turns out that the
natural frequency (f0) of
the outrigger suspension is approximately 5 cycles per second.
f0 = 5 cps.
It
now remains to determine at what speed
the system would be jiggled at 5 cycles per second. I used 13 inch wheels which have an outside
diameter (D) of 24 inches (2
feet). The circumference of the wheel
is therefore C= πD which calculates
to be 3.14 x 2 = 6.28 feet. The wheels
will therefore advance 6.28 feet with every revolution (cycle). At the natural frequency of 5 cycles per
second, the wheels would advance 5 x 6.28 = 31.4 feet per second which equals
21.4 miles per hour.
This result almost exactly matches the actual riding experience
where the notch shimmy originally set in at 22 mph.
The
formula for Shimmy Velocity (in
mph.) is: Vs = 0.1784 f0 D where the natural frequency (f0) is expressed in
cycles per second and the outside diameter of the wheel (D) is measured in inches.
Before
proceeding further, it should be noted that we have just related several design
choices to the speed at which a shimmy would be expected to occur. The design choices are:
·
Wheel outside diameter (diameter
D)
·
Wheel weight (mass M)
·
Suspension stiffness (spring
constant K)
In
general, one would like the natural frequency and the related shimmy speed to
be as high as possible since for an equal energy input, the amplitude of the
disturbance will naturally diminish with increased frequency. The smaller the amplitude of the
oscillations, the more effective a damper will be. How is this best accomplished?
From
the proceeding calculations, you could conclude that the shimmy speed appears
to be directly proportional to the outside diameter (D) of the wheel you choose.
As a rule of thumb, the outside diameter is approximately 1.8 times the
wheel size (i.e. a 13 inch wheel has a
24 inch outside diameter).
Unfortunately, increasing tire diameter also tends to increase the total
wheel weight which reduces the natural frequency f0 thereby offsetting
some of the gain being sought. Thus, the
ideal wheel would appear to be large in diameter and very light in weight. Motorcycle wheels, unlike trailer wheels,
tend to have this property. I leave it
to you to decide how attractive such a wheel choice might be.
The
last design choice to deal with is the stiffness of the suspension (spring
constant K). If one reduces the spring constant, making
for a much softer ride, the effect would be to reduce the suspension natural
frequency and the shimmy speed by the square root of the change. The softer ride is certainly desirable
however, the lowered natural frequency and correspondingly lower shimmy speed
is undesirable. When I truncated the
torsion suspension by physically cutting it down from 10.5 inches to only 6
inches long, I effectively reduced the spring constant of the suspension (K) by approximately 43%. The
formula would predict that the new shimmy velocity would now be 16.2 mph.
This exactly matches the new riding experience where the notch
shimmy tendency now sets in at 16 mph!

I
was pleased to have achieved the softer ride that I sought; however, it came
with a price. The lower the natural
frequency, the greater the amplitude of the shimmy motion that must be damped. The adjacent graph shows that the shimmy
amplitude increased by approximately 30% when the shimmy speed decreased from
21.4 mph to 16.2 mph. The front fork
damper is still effective but it must now work harder to suppress the motion.
As
you can see, the shimmy speed is likely to be between 15 mph and 22 mph
for the practical range of choices available to the designer. Exactly where you come out depends on the
combination of M, K and D that you chose in your own design. There is no free lunch as desirable features
work against one another … ah, such is life!
You
should note that the distance between the outrigger wheels (the width of the outrigger unit) does
not figure into the suspension’s
natural frequency (f0) determination
assuming the outrigger frame is rigid.
As discussed later, the width does affect the total quad assembly’s own
natural frequency (fx).
It
was very interesting (and predictable) to note that the original notch shimmy
speed of 22 mph. did not change when I
put the outrigger wheels on my second bike (Honda Shadow). Logically this should be expected since the
fundamental features (M, K and D) that determine the suspension’s natural
frequency are a property of the outrigger assembly itself, not the motorcycle.
Some
builders have chosen to move the outrigger wheels forward or aft of the rear
wheels axle in an effort to avoid shimmy problems. Based on the fundamentals however, I doubt
that moving the outrigger wheels in this manner would have much effect on the
onset of the natural frequency induced notch shimmy. I will include results from the builders at a
later date.
Lateral Motions:

Before
addressing the lateral motion, it is necessary to look at the front suspension
properties. As illustrated in the
adjacent sketch, the front fork is ahead of the steering axis which in turn passes
through the steering head and meets the ground ahead of the wheel’s contact
point. The distance from these two
ground points is the “trail” which is normally from 4 to 6 inches. The tilt back angle of the steering axis is
the rake angle. The greater the rake
angle, the larger the trail. The larger
the trail, the greater the tendency to steer in a straight line as is characteristic
of a chopper.

The
important point is that if the steering head (along with the steering axis) is laterally
pushed to the right, the front wheel will be turned to the right since the
wheel twists about its contact point with the ground. The front wheel is turned by this motion and
the amount of torque exerted on the wheel depends on the size of the trail
dimension which is in effect the lever arm of the lateral force. The motion would apply a larger torque to the
front wheel that had a large trail and less torque to a wheel with a small
trail. In the academic extreme, the
motion would apply no torque
to a wheel with zero trail.
As
a consequence, a quad with large trail would have heavy steering in that it
would wish to continue in a straight line, but would be shimmy prone as lateral
motion of the chassis would exert more torque on the front wheel.
The
next sketch illustrates the plan-view or lateral aspect of the shimmy (wobble) problem
which relates to the undamped motion at the steering head. The pivot point of the front wheel is at its contact
point with the pavement. The rear pivot
point is at the contact point of the motorcycle’s rear (center) wheel.
When
the bike is at the proper speed to excite the vertical oscillation of the
outrigger wheels, some of that energy will find its way into the lateral
swaying dimensions of the system. The
motorcycle chassis, the steering head plus steering axis and the outrigger assembly
form one integral unit as they oscillate from right to left causing the
steering head to be pulled right and left at the quad’s own natural frequency (fx).
It
stands to reason that the lateral force
applied to the steering head during these motions, will be proportional to the width
of the outrigger wheel assembly.
The wider the assembly, the more chassis torque will be generated from
the disturbance emanating at the outboard wheel locations. Trikes typically have about a four foot wide
track while the outrigger I originally built has a little over five feet. There obviously is virtue in keeping the outrigger as
narrow as possible from a shimmy dynamics point of view.
The
front wheel pivots about its contact
point with the pavement. Therefore,
the front wheel will be turned right to left as the chassis swings right to
left. The result is a lateral shimmy at
the quad’s
natural frequency (fx) which will in
general, be lower than the suspension’s natural frequency f0. You can roughly determine the quad’s overall natural
frequency by simply sitting in the saddle and oscillating the handle bars until
the quad settles into a continuous rocking jiggling motion. Use a stopwatch and see how many seconds it
takes for say 50 cycles of oscillation and calculate the natural frequency in
cycles per second. After softening the
suspension, my quad has a natural frequency of about 2 cycles per second per
the jiggle test.
The
final shimmy motion that one will experience results from a combination of
these two frequencies. It appears as if
the suspension’s 4 to 5 cycle per second natural frequency (f0) determines the velocity
at which the notch shimmy will set in while the natural frequency of the entire
quad (fx) will be the frequency at which the front end will actually
shimmy or wobble (around 2 cycles per
second). The adjacent diagram
illustrates the effect of combining the quad’s own low natural frequency (blue
curve) with the suspension’s higher natural frequency to get the final total
assembly shimmy behavior (red curve).
You can see that the peaks tend to retain the low frequency character of
the quad’s own natural frequency (fx).

As
the handlebars are turned, the bike very easily twists from side to side even
at rest. There is normally very little
resistance to this steering type of motion.
In other words, there is little or no damping in the lateral dimension. High performance sport bikes have addressed this
problem by building in mechanical or electronically controlled dampers of
various types and many commercial trikes use similar dampers in their design. Most trike conversions also employ a
mechanical damper.
The
greater the “trail”, the more exaggerated the front end lateral shimmy motion
will be. A chopper would be a poor
starting point for a trike conversion from a shimmy perspective. The greater the front end “rake angle”, the
larger will be the trail distance from
the contact point to the steering axis.
Cruising bikes generally have about a 30 degree rake while sport bikes
have somewhat less and dirt bikes even less.
When ridden as a motorcycle, a large chopper-like rake angle results in
a bike that is very stable and tracks the road well. However, the steering feels “heavy” in that
the bike wants to naturally continue in a straight line. However, any lateral oscillations of the
chassis increase the torque applied to the front wheel making it more prone to
a shimmy.
Since
we are dealing with a Trike+Plus having the “on-off” feature, it is undesirable and impractical to tamper
with the basic motorcycle’s front end configuration. A far better solution is to simply install an
adjustable strength damper as I mentioned earlier in the section on shimmy
problems. The effects of the damper on
the bike’s handling characteristics are minimal while the effect on damping
shimmy motions is substantial. As I
ride, I am still aware of the notch shimmy speed but the effect is so suppressed
that it is not of concern. When I cut
the torsion suspension tube to soften the ride, I reduced the notch shimmy
speed from 22 mph. to 16 mph. which slightly increased the amplitude of the
motion but it remained of no practical concern.
My Conclusion:
·
Manipulating the outrigger design choices (suspension
stiffness, wheel size and weight) will change the velocity at which the
tendency to shimmy will set in but is unlikely to eliminate that tendency. The notch shimmy speed is likely to be
between 15 and 22 mph. The higher, the
better.
·
The notch shimmy will oscillate the front end at the entire
quad’s natural frequency (about 2 cycles per second).
·
The severity of the shimmy motion will depend on the outrigger’s
own natural frequency, the motorcycle’s front wheel trail distance and the
outrigger’s width … higher natural frequency, less motion … less
trail, less motion … narrower outrigger width, less motion.
·
The most practical
solution to the shimmy tendency is to install an adjustable strength damper at
the front fork. This is easily done, very
effective and relatively inexpensive ($50).
If the natural frequency and shimmy speed become too low, a more robust
damper may be necessary to avoid sensing the inherent tendency.
