| Let's establish a few facts first,
straight from the discipline of contemporary Physics.
No header/exhaust system is ideal for all applications.
Depending on their design and purpose, all exhaust/header
systems compromise something to achieve something else. Before
performing header or other exhaust modifications to increase
performance, it is critical to determine what kind of
performance you want. Do you want max low RPM power for chugging
around town casually like a Harley? Not likely if you ride a BSA!
Do you want max mid-range power for ease of passing while
cruising down an Interstate highway? Do you want max peak-RPM
power for top speed and/or bragging rights? Maybe you just want
an exhaust that looks cool. Or do you want the best of all
worlds? In the latter case, a well-designed aftermarket exhaust
system is where you'll find it.
If you are wowed only by peak HP numbers on a dyno chart,
consider the following: For a vehicle to cover "X" distance as
quickly as possible, it is not the highest peak power generated
by the engine that is most critical. It is the highest average
power generated across the distance that typically produces the
quickest time. When comparing two power curves on a dynamometer
chart (assuming other factors remain constant), the curve
containing the greatest average power is the one that will
typically cover the distance in the least time. This fact is
what makes the nature of the power band important. You don't
want to give up powerful mid-range performance just to have the
highest peak power numbers--that's only good for bragging rights
and will kill your acceleration because most time spent
accelerating is in the mid-range, not at peak-power RPM.
Actually, we want both (maximum mid-range power and maximum peak
power), don't we? I'll answer for you--YES!
In the strictest technical sense, an exhaust system cannot
produce more power on its own. The potential power of an engine
is determined by the amount of fuel available for combustion.
More fuel must be introduced to increase potential power.
However, the efficiency of combustion and engine pumping
processes is profoundly influenced by the exhaust system. A
properly designed exhaust system can reduce engine pumping
losses. Therefore, the primary design objective for a high
performance exhaust is (or should be) to reduce engine-pumping
losses, and by so doing, increase volumetric efficiency. The net
result of reduced pumping losses is more power available to move
the vehicle. As volumetric efficiency increases, potential fuel
mileage also increases because less throttle opening is required
to move the vehicle at the same velocity. This is where the old
bugaboo of back-pressure rears it's ugly, mythical head. Much
controversy and confusion surround the issue of exhaust
back-pressure which, in other terms, is a pumping loss. Many
performance-minded people (including some "professionals") who
are otherwise well-enlightened still cling tenaciously to the
old cliché "You need some back-pressure for best performance."
WRONG--period > if your definition of "best" performance is
"maximum power throughout the power band".
For virtually all high performance purposes:
back-pressure in an exhaust system increases engine-pumping
losses and thereby decreases maximum engine power. Are we
clear about this?
Here is something to chew on: Theoretically, in a normally
aspirated state of tune without special fuel or oxygen-rich
additives, an engine’s maximum power potential is directly
proportional with the volume of air it flows. This means that an
engine of 750 cc has the same maximum power potential as an
engine of 1000 cc that is if they both flow the same volume of
air. In this example, the power band characteristics of the two
engines will be quite different but the peak attainable power is
essentially the same. In view of this reality, I have amended
the old hot rod proverb "There's no substitute for cubic inches"
"except there is more efficiency!"
Many "performance" people resist some of these notions but
their resistance does not change reality nor the laws of
physics.
Are you still awake? Okay, let's establish a few Rules of
Thumb.
1- Longer header tubes tend to
increase power below the engine’s torque peak and shorter header
tubes tend to increase power above the torque peak.
2- Large diameter headers and
collectors tend to limit low-range power and increase high range
power. Conversely, small diameter headers and collectors tend to
increase low-range power and limit high-range power.
3- "Balance" or "equalizer" tubes
between the header tubes tend to flatten the torque peak(s) or
widen the power band.
4- Stainless headers do not transfer
heat to the ambient air as fast as mild steel headers. Keeping
more of that heat "inside" the header pipes and aids exhaust
flow because the exhaust gas is more energetic and it reduces
the amount of heat flowing across the engine (and across you).
The objective of most engine modifications is to maximize
air and fuel flow into, and exhaust flow out of the engine. The
inflow of an air/fuel mixture is a separate issue, but it is
directly influenced by exhaust flow, particularly during valve
overlap (when both valves are open for "X" degrees of crankshaft
rotation). Gasoline requires oxygen to burn. By volume, dry,
ambient air at sea level contains about 21% oxygen, 78% Nitrogen
and trace amounts of other gases. Since oxygen is only about 1/5
of air’s volume, an engine must intake 5 times more air than
oxygen to get the oxygen it needs to support the combustion of
fuel. If we introduce an oxygen-bearing additive such as nitrous
oxide, or use an oxygen-bearing fuel such as nitro methane, we
can make much more power from the same displacement because both
additives bring more oxygen to the combustion chamber to support
the combustion of more fuel. If we add a supercharger or
turbocharger, we get more power for the same reason and more
oxygen is forced into the combustion chamber.
Perhaps the most important aspect of exhaust flow is the
issue of flow volume vs. flow velocity. This also happens to
apply equally to intake events.
An engine needs the highest flow velocity possible for
quick throttle response and torque throughout the low-to-mid
range portion of the power band. The same engine also needs the
highest flow volume possible throughout the mid-to-high range
portion of the power band for maximum performance. This is where
a fundamental conflict arises. For "X" amount of exhaust
pressure at an exhaust valve, a smaller diameter header tube
will provide higher flow velocity than a larger diameter tube.
Unfortunately, the laws of physics will not allow that same
small diameter tube to flow sufficient volume to realize maximum
potential power at higher RPM. If we install a larger diameter
tube, we will have enough flow volume for maximum power at
mid-to-high RPM, but the flow velocity will decrease and
low-to-mid range throttle response and torque will suffer (the
"back-pressure" myth probably arises from a misunderstanding of
these factors). This is the primary paradox of exhaust flow
dynamics and the solution is usually a design compromise that
produces an acceptable amount of throttle response, torque and
horsepower across the entire power band.
| |
|
|
| Guess what? There's more. It's
called scavenging and it's complicated.
Inertial scavenging and wave scavenging are
different phenomenon but both impact exhaust system
efficiency and affect one another. Scavenging is simply
gas extraction. These two scavenging effects are
directly influenced by tube diameter, length, shape and
the thermal properties of the tube material (stainless,
mild steel, titanium, etc.). When the exhaust valve
opens, two things immediately happen. An energy wave, or
pulse, is created from the rapidly expanding combustion
gases. The wave enters the header tube (or manifold)
traveling outward at a nominal speed of 1,300 - 1,700
feet per second (this speed varies depending on engine
design, modifications, etc., and is therefore stated as
a "nominal" velocity). This wave is pure energy, similar
to a shock wave from an explosion. Simultaneous with the
energy wave, the spent combustion gases also enter the
header tube and travel outward more slowly at 150 - 300
feet per second nominal (maximum power is usually made
with gas velocities between 240 and 300 feet per
second). Since the energy wave is moving about 5 times
faster than the exhaust gases, it will get where it is
going faster than the gases. When the outbound energy
wave encounters a lower pressure area such as a larger
collector pipe, muffler or the ambient atmosphere, a
reversion wave (a reversed or mirrored wave) is
reflected back toward the exhaust valve with little loss
of velocity.
The reversion wave moves back toward the exhaust
valve on a collision course with the exiting gases
whereupon they pass through one another, with some
energy loss and turbulence, and continue in their
respective directions. What happens when that reversion
wave arrives back at the exhaust valve depends on
whether the exhaust valve is still open or closed. This
is a critical moment in the exhaust cycle because the
reversion wave can be beneficial or detrimental to
exhaust flow, depending upon its arrival time at the
exhaust valve. If the exhaust valve is closed when the
reversion wave arrives, the wave is again reflected
toward the exhaust outlet and eventually dissipates its
energy in this back and forth motion. If the exhaust
valve is open when the wave arrives, its effect upon
exhaust gas flow depends on which part of the wave is
hitting the open exhaust valve.
A wave is comprised of two alternating and
opposing pressures. In one part of the wave cycle, the
gas molecules are compressed. In the other part of the
wave, the gas molecules are rarefied. Therefore, each
wave contains a compression area (node) of higher
pressure and a rarefaction area (anti-node) of lower
pressure. An exhaust tube of the proper length (for a
specific RPM) will place the wave’s anti-node at the
exhaust valve at the proper time for it’s lower pressure
to help fill the combustion chamber with fresh incoming
charge and to further extract spent gases from the
chamber via vacuum effect. This is wave scavenging or
"wave tuning".
From these cyclical engine events, one can deduce
that the beneficial part of a rapidly traveling
reversion wave can only be present at an exhaust port
during portions of the power band since it's relative
arrival time changes with RPM. This makes it difficult
to tune an exhaust system to take advantage of reversion
waves which is one reason why there are various
anti-reversion schemes designed into some header systems
and exhaust ports. These anti-reversion devices are
designed to weaken and disrupt any detrimental reversion
waves (when the wave's higher-pressure node impedes
scavenging and intake draw-through). Such anti-reversion
schemes include merge collectors, truncated cones/rings
built into the primary tube entrance and exhaust port
ledges.
Unlike reversion waves that have no mass, exhaust
gases do have mass. And since they are in motion, they
also have inertia (or "momentum") as they travel outward
at their comparatively slow velocity of 150 - 300 fps.
When the gases move outward as a gas column through the
header tube, a decreasing pressure area is created in
the pipe behind them. It may help to think of this lower
pressure area as a partial vacuum and one can visualize
the vacuous lower pressure "pulling" residual exhaust
gases from the combustion chamber and exhaust port. It
can also help pull fresh air/fuel charge into the
combustion chamber. This is inertial scavenging and it
has a major effect upon engine power at low-to-mid range
RPM.
If properly timed with RPM and firing order, the
low pressure that results from gas inertia can
spill-over into other primary tubes, via the collectors,
and aid the scavenging of other cylinders in that bank.
There are other factors that further complicate
the behavior of exhaust gases. Wave harmonics, wave
amplification and wave cancellation effects also play
into the scheme of exhaust events. The interaction of
all these variables is so abstractly complex that it is
difficult to fully grasp. I am not aware of any absolute
formulas/algorithms that will produce a perfect exhaust
design. Even factory super-computer exhaust designs must
undergo dynamometer and track testing to determine the
necessary tube adjustments for the desired results.
We all are the benefactors of all this technical
information. Be glad that there are bright minds in the
world whom sort it out for us. |
|