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The bearings and the shaft. Since
both shaft and inner bearing ring are normally made out
of steel, no thermal expansion problem occur. However it
is of high importance that the inner ring is prevented
from creeping, and wearing the shaft.
In all commercial engines the inner ballrace ring is
retained on the shaft by a more or less heavy
interference fit, or worse, by a sliding fit (Rossi,
Super Tigre, K & B).
A tight fit, like in the Nelson, makes putting the shaft
in and out a specialists job (same advice as before!) and
it also calls for high clearance bearings.
Bearings with normal clearance won't accept interference
fits of more than 0.001 - 0.002 mm interference on the
shaft without loosing their play.
Sliding fits on highly stressed T.R. engines will cause
all sorts of distortion and vibration problems,
increasing friction and eventually ending up with a cold
forged, oval shaft.
In quite a few cases we found remarkable, if temporary,
improvement just Loctiting the shaft to the bearings!
In
the FMV the construction shown in fig. 3 is used. A bush
clamped between the inner rings of the bearings by
tightening the prop nut will prevent both inner rings
from turning. For this reason we can easily use a
non-hardened shaft (material DIN 100Cr6, En 31 (G.B.), E
52100 (U.S.A.), the same as our front housing and
bearings), with 0.001 - 0.002 mm interference fit on the
bearings. This bush is quite common in "real"
machinery and has been used for many years in Russian
TR-motors. It can be adjusted to such a length that the
bearings are set to give the desired axial play to the
shaft.
3.3
Axial and radial play of the shaft.
Apart
from turning the crankshaft can, and probably will, move
(or better vibrate) in axial and radial direction.
These vibrations are directly induced by the ignitions of
the engine and are strongly influenced by the play of the
ballraces. They will increase the friction, heat
generation and wear of the bearings.
In
ball bearing technique it is normal to control the play
of bearings by "preloading" them. This means,
that in the case of a shaft supported by two bearings,
both axial and radial play are controlled by setting the
inner and outer rings at slightly different distance (See
fig. 4 and fig. 5).
fig. 4 Preloading ball
bearing

If
di=do, axial and radial play is equal to that of
one ball-bearing (~0,08 mm in our case)
If di is chosen smaller than do, axial and radial
play decrease. If, in our case, di=do-0.08 no
play is left
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fig 5a

Shaft and
bearings in an aluminium crankcase.
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fig.5b

Curves
of relationship between axial and radial
clearance for Nelson bearings
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fig.5 Axial and
radial clearance of the bearing in an aluminium
crankcase (example: Nelson)
Starting
from zero clearance at T=20 °C we find from
curves, similar to fig .1b and fig 5b, that at
T=80 °C:
Æ1 increases 4mm, so axial clearance
will be 0.08 mm.
Æ2 increases 3.5mm, so axial clearance
will be 0.06 mm.
The different expansion of the crankcase (length
l) and the shaft will preload the bearings for
about 0.02 mm (for l=30 mm) over this temperature
range.
An axial clearance of the shaft of 0.05 results.
Axial load in front direction will be taken by
the main bearing, in rear direction by the front
bearing.
A not "free" feeling shaft at 20 °C
(zero clearance) is necessary in a Nelson to keep
down clearances at running temperatures.
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Our bearings when new, have an
axial play of 0.06 - 0.08 mm.
We found this little too much, causing setting and
overheating problems as well as fast wear of ball
bearings. By shimming, we make the bush between the inner
rings about 0.03 mm shorter than the distance between the
outer rings, resulting in 0.03 - 0.05 mm axial play. This
seems to be a good compromise and will stay constant over
a large temperature range in an all steel set-up.
The
reasons that no less play can be used safely, are the
following:
- During
running the inside of the motor (shaft) will
always be warmer than the outside (front housing)
simply because there's cold air outside and
there's no other way for the generated heat to
go.
Therefore the inner ring is expanded and radial
play (being around 0.003 mm in our case) will
decrease by 0.001 mm with every 10° C rise of
temperature difference.
This effect, helped by a too well cooled front
housing, committed quite some bearing ravages in
our Rossi front-exhaust, the test-bed for many
experiments with steel front housing. That's why
in the FMV model direct cooling to the front
housing is prevented by using a spinner (see fig.
16)
- Play
is necessary to allow the shaft to bend during
ignition. Calculations show that about 0.4°
rotation at crank pin location occurs.
With
an aluminium front housing controlling radial play by
means of axial preloading is nearly impossible. This is
because the bearing play induced by the radial expansion
of the house will be much greater than the play reduction
due to the lengthening of the house for a given
temperature variation.
Setting
a preload for running temperature will ruin the bearing
when the engine is cold. In well fitted engines, like the
Nelson, preloading is controlled by the interference fit
of the bearings and the different expansion of the
crankcase and the shaft, just giving the right radial and
axial play at running temperature. (See fig.5).
3.4
Locating and sealing of the crankshaft, lubrication of
the front bearing.
Because
of the limited axial movement of both ends of the conrod
it was essential that the middle of the crank pin was
located exactly (within 0.01 mm) on the center line of
the cylinder.
The measurements were carried out with the equipment
drawn in fig. 6.
From fig. 6 it is clear that, by measuring the distance
difference to the dummy con-rod with the dial gauge in
top and bottom position, the perpendicularity between the
shafts-axis and the cylinder axis can be checked with the
required accuracy of about 0.05°
The axial play of the shaft can be checked with the dial
gauge on the crankweb by pushing and pulling the shaft
softly.
fig 6

Measuring
equipment to find the distance between the centre
line of the cylinder and the rear plane of the
crankweb.
Part A fits closely in the cylinder hole and has
a pin (Æp), being concentric with the cylinder.
The pin is the "dummy conrod".
The dial gauge , held in B, gives two readings,
one for the crankweb and the second for the dummy
conrod
The distance between the centre of the cylinder
and the crankweb can be easily calculated,
knowing Æp.
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In the case of the FMV the
position of the shaft is set by putting a separate part
into the front housing (See fig. 3)
The thickness of the rear ring determines the exact
position of the shaft.
This part also gives the sealing around the shaft.
A
difficult point has always been the clearance necessary
around the shaft to prevent touching. Since we want the
clearance as small as possible to prevent excess fuel
leaking through the front, calculations were made of the
radial movement of the shaft at different places caused
by the ignition of the motor.
Fig. 7 shows the approximate movements, for an 8 mm shaft
and 8-19-6 mm and 7-14-3,5 mm bearings.
With a stronger shaft and bearings like the Nelson and
Bugl have, these movements will be slightly less, but
still of the same order of magnitude.
fig. 7

Radial
movements of the shaft during ignition. Figures
are not exact because peak pressures in
combustion chamber are not known exactly. Point
of no movement is independent of actual forces.
(Note that a bell valve fixed to the crank pin
will move appr. 0.15 mm)
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In any case it will be clear,
that the best point of sealing the shaft is between the
rear 1/3 and half the ball bearing center distance, where
the movements are smallest. This is unlike most
commercial RV-engines having the sealing right in front
of the main bearing.
A
clearance of 0.06 - 0.08 mm in diameter between the
sealing ring and the bush around the shaft over a length
of about 10 mm has proved to prevent any touching and
gives barely enough leakage
to keep the front bearing wet (1 or 2 drops per tank).
This lubrication is forced by average crankcase pressure
through the small gap around the shaft.
In most other engines this guidance of lubrication
doesn't exist, because after passing the sealing there's
no controlled way for the fuel to reach the front
bearing.
3.5 Balancing.
Since
we always found that vibrations (think of a not fully
tightened pan), cause losses in performance, economy and
consistency, we are convinced that keeping the dynamic
forces, (the cause of vibrations) down to minimum is one
of the ways to make a better engine.
A great deal is known about balancing, one of the things
being that it is impossible to balance a single cylinder
engine completely, without bringing the reciprocating
masses down to zero (except by using auxiliary rotating
counterweight). One logical way of improvement is to
lighten piston and con-rod as much as possible.
Is
there any other reason, that aluminium pistons work so
well??
The
normal way to "balance" single cylinder
two-stroke racing engines is to counterbalance the shaft
in such a way that first order horizontal and vertical
reciprocating forces are equally strong, which means that
the dynamical first order forces are minimized. (See fig
8 for explanation.)
fig. 8

Unbalance
in a 1 cylinder engine
Minimizing
total unbalance forces of first order is done by
making horizontal and vertical components of
unbalance equal, in formula.
Mass
moment left crankweb - mass moment right side
crankweb (incl. crank pin) -r*0.5 mc= 0.5 *r*(mp+0.5mc)
mp = mass piston
mc = mass conrod
r = 0.5 stroke
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In the presently marketed 2,5 cc engines with iron
pistons only 15 - 20% of the piston's weight is balanced.
In ABC or AAC engines this is up to 30 - 35%.
To
get the FMV up to 50% balance with a Meehanite piston two
things were necessary: firstly the piston weight should
go down as much as possible, secondly a counterweight was
put into the crankshaft.
the piston construction is to be described later, the
hollowing and filling of the crankweb is drawn in fig. 9.
The counterweight is made out of tungsten-carbide with a
density of 15.1 gram/cm^3. (about 1.5 times that of
lead).
A standard type cast iron piston, including pin, about 2
grams heavier than ours, would have made a counterweight
out of gold or platinum necessary. Financial problems
then forced us to design a super light piston. With AAC
piston/liners expected to come this year, the problem of
balancing will be solved more easily and with better
result, with only a small counter weight in the shaft.
(By the way, the FMV shaft with counterweight and bushing
is as heavy as a standard Rossi RV shaft).
fig 9

Crankweb of the F.M.V.
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