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tech talk by
Robert Bergeron
Many owners regard their
modern outboard motor as a sealed and sacred piece of machinery which
should never be violated. These individuals think that even turning a
single screw on an outboard power plant will cause it to malfunction.
On the other end of the
spectrum, there are owners who believe that no matter how many carbs
they add, how much they “cut” the heads, how badly they butcher the
porting, or how high they bring the rpm, power will always be better
than it was stock. Of course, any resulting problems are then promptly
blamed on those “stupid factory engineers!” Obviously, neither of these
notions is correct. In the following article, I’ll explain some of the
engineering “facts-of-life” that apply to all 2 cycle outboards. These
fundamental principles should help outboard hot-rodders understand what
can and cannot be expected from their engine modification projects, and
hopefully prevent disappointing and expensive mistakes.
DISPLACEMENT (in ci) x BMEP (in psi) x RPM
NET BRAKE HP = -------------------------------------------------------------------
396,000
INTERNAL DRAG (in)
This ominous looking
equation represents the theoretical power output capability of any 2
cycle outboard engine. Since four important categories of variables
control the results of this formula, their affect on the engine’s power
curve should be clearly understood before you attack your engine with
wrenches and grinder.

INTERNAL DRAG: Friction
and pumping losses inside any reciprocating engine are obviously
undesirable power reducing parasites. Unfortunately it is very unlikely
that there can be significant reductions in either of these drag
factors. Internal friction results primarily from the pistons rings
which are, of course, necessary for cylinder sealing. Lower tension
rings or single ring pistons can reduce the drag problem but there is a
point of diminishing return if cylinder sealing is lost. Pumping losses
in the engine are an unavoidable result of moving air in through the
carburetors, pumping it up to pressure, and exhausting it out the ports.
Even more unfortunate to the performance minded engine builder, is that
all these losses grow with any increase in rpm, BMEP, or displacement.
(Bad news, already!)
DISPLACEMENT: Total
cylinder displacement is probably the most powerful variable in the
formula. Because increasing displacement (either by bore or stroke
enlargement) yields an almost directly proportional increase in power
over the entire rpm band of the engine, it is typically the outboard
design engineer’s favorite method of increasing the power of his engine.
Since a broad power curve is essential for a general purpose production
outboard, modification like displacement increases, which improve power
over the entire rpm range of the engine, are the most suitable.
Unfortunately,
significant increases in cylinder displacement (over 5%) are usually
possible only at the drawing board stage of motor development. For
example, the backyard engine builder will find it virtually impossible
to increase the stroke of his outboard. Normally, there is no extra room
in the crankcase for any additional crank swing, the porting layout will
not lend itself to any stroke change, pistons and/or rods will not be
available, and local crank shops normally will not be equipped to
properly stroke a hardened roller bearing outboard crankshaft.
Likewise, a major
increase in bore size is also usually unfeasible. Again, the lack of
cylinder wall liner thickness, and piston and ring availability thwarts
most big bore plans. Although some independent companies do offer sleeve
kits or services, in most cases, increasing the displacement should only
be done by a factory. Also, even though a displacement increase almost
always results in some power increase, it must be remembered that as
cylinder volume is enlarged, internal drag increases, while BMEP and rpm
capability are reduced. (There is no free lunch!)
BMEP: Brake Mean
Effective Pressure in psi, is a fancy sounding expression for the
average pressure existing in the engine’s cylinder during a power
stroke. It is an excellent indicator of the engine’s effectiveness in
making power from its displacement at any given rpm. The total effects
of volumetric efficiency (how close the engine comes to pumping its
actual displacement with each stroke), combustion chamber design,
compression ratio, ring seal, mixture dilution, air/fuel ratio, ignition
timing, heat loss, fuel, etc. are all contributing factors towards the
BMEP developed in the cylinder. While it is not mandatory to understand
the engineering methods for calculating the BMEP of an engine, it is
important to realize the importance these figures will play when
determining that engine’s power curve.
Find a way to increase
the BMEP of an engine and you’ll have increased its power. But since
factory engineers have already worked long and hard to develop porting
and tuning specifications that will yield high BMEP figures over most
production engines designed power band, it will be quite unlikely that
any appreciable improvements can be made by the independent hot-rodder
over the entire stock power curve (compression ratio increases aside).
It then becomes the job
of the engine modifier to effectively alter the stock specifications to
increase the BMEP in a selected, narrow portion of the rpm band.
Successfully accomplishing this typical requires a good deal of
experimentation using airflow test equipment, engine dynamometers, etc.,
and actual on water testing – or at least a clear set of instructions
from someone who has already done such testing on your particular model
engine. Boaters that approach this task armed with only high hopes and
“intuition” have ruined countless engines.
As an example of the
gains (and problems) associated with raising the BMEP an outboard
engine, let’s take a crack modifying a hypothetical 145 ci production
outboard developing 200 Hp at 5,000 rpm. I’ve drawn a solid line in
Graph #1 to represent this engine’s stock power curve. The engine has a
BMEP of approximately 105 psi at 5,000 rpm. We’ll start our
modifications of this imaginary engine with a substantial increase in
compression ratio, say from 9.0:1 to 12.5:1 (theoretical full volume
compression ratio). We could reasonably expect the power to rise along
the dashed line’s curve in Graph #1. You see that we have increased
power at all rpm’s of the engine for a peak power of 213 Hp at 5,000 rpm
and a BMEP of 112 psi at that rpm. That’s great you say, let’s raise the
compression some more!
Unfortunately, every
modification has limitations and accompanying side effects. Although
increasing compression ratio can often improve power over a wide rpm
range (like a displacement increase), it creates serious piston and
combustion chamber overheating problems if carried to extremes. We have
already modified our motor from an easy going pump gas model, to a mill
that will promptly melt a piston with less than 100-octane aviation gas
in the tank. Raising, the compression ratio much higher would only
result in power losses from detonation, and possibly a holed piston. In
fact, if future modifications are made which further increase the BMEP,
the compression ratio may actually have to be reduced just to stay
within the thermal limits of currently available piston and ring
materials. (There’s still no free lunch!)
Now let’s try a group of
the standard racer’s tricks to improve volumetric efficiency (breathing
of the engine). We’ll avoid the possibility of porting the engine
incorrectly by allowing the factory racing team to port this imaginary
motor to their racing engine specifications. While it’s there, we’ll
have them hang a few extra carbs as well, since it’s just like their
race engine, now it will really scream! Right?
Back at the dyno, we see
that this modification has raised the power to 225 Hp at 5,500 rpm with
a BMEP of 108 psi (see the dash dot dash line in Graph #1). Better, but
not what we expected. Look at the low rpm end of our engine’s horsepower
graph! What happened?
Almost any major
improvement made in volumetric efficiency at high rpm will be
accompanied by a loss of volumetric efficiency at lower rpm’s and of
course a proportional loss of BMEP and horsepower. There are some
exceptions but you can be pretty sure that factory engineers know most
of these tricks and have already incorporated them into your engine’s
stock design.
Well you say, “I still
have an extra 25 Hp over the stock engine, so who cares about the low
rpm range anyway?” You will, the first time you try to out accelerate a
buddy’s stock engine! With only a small improvement in peak power to
compensate for power loss at lower rpm’s this motor will still be
getting on plane when most races are over. (Don’t worry though, things
get better!)
RPM: It seems everyone
has their own notion about what constitutes peak power rpm. Some believe
it is the point where the connecting rods start poking expensive holes
in the side of their “Wonder Motor,” while others think that it is the
original rpm recommended by their owner’s manual, even though the motor
has been ported, fuel injected, etc. Actually, peak power rpm is the
engine speed at which the BMEP (which eventually starts going down as
rpm continues to go up), multiplied by the rpm, gives the highest
results, and therefore the highest horsepower. Revving the engine beyond
that point produces less power, not more. (Another dead end in our power
search? No!)
Here is where all those neat little race tricks, which only
improved the BMEP in the upper rpm range, can be put to good use. Let’s
go back to our imaginary engine in Graph #1. By raising the rpm of the
stock engine, which had a power peak at 5,000 rpm, to 7,600 rpm as shown
in Graph #2 (solid line) we see the BMEP has fallen to 48 psi and the
power has fallen to 140 Hp. We indicated before, that this would happen
past peak power rpm. But assuming we made the correct porting
modifications, as we did with the “race version” of the imaginary
engine, to keep the BMEP at about 100 psi of 7,600 rpm (well within
reasonable expectations) we would have increased the power to 288 Hp at
7,600 rpm (see dashed line in Graph #2). A further increase in BMEP or
rpm would raise peak power even more. Although such improvements would
result in a decrease in the BMEP (and Hp) at lower rpm’s as we
previously noted, the increased new upper rpm range would allow for a
lower unit gear reduction or propeller pitch reduction to “hide” such
loss of low rpm power. This is how most of the outboard manufacturers
have managed to increase usable power in increasingly smaller
displacement engines over the last few years. They have raised the BMEP
of the engine to increase high rpm power and then moved the operating
rpm band upward to regain the lost low end torque.
Many of the recent
advances in power output, displacement increases aside, have come from
developments in piston and ring design (allowing higher BMEP figure
before thermal failure) and improvements in crank-train components
(allowing higher continuous operating rpm). High rpm coupled with good
BMEP is the “trick” to factory racing engine performance. This same
power formula can be used by individual outboard hot-rodders to
carefully plan their modifications to fully utilize the thermal and rpm
capabilities of any production power-head. Power outputs of over 2 Hp
per cubic inch are possible from some of the present production V6
outboards. Next time around I will cover the nuts and bolts of
extracting some of that power from your outboard. |