
If any component can be truly described as the
“heart” of a turbo system, then the APS 350Z system
truly has the biggest heart of all!! Or, should
that be TWO hearts?
Twin, state of the art and water cooled Garrett
twin ball bearing turbochargers deliver ballistic
power with bullet proof turbocharger reliability
- and with a custom APS aerodynamic configuration,
that ballistic power is delivered in an extreme
efficiency and super compact package that is ideally
suited to the 350Z vehicle dynamics. In fact,
with a built engine, how about 800 hp air flow
capacity at just 16 psi of turbocharger boost
pressure!
Given that the engine with stock heads/cams will
produce around 550hp flywheel at this boost, it
can be seen that significant headroom remains
in the available turbocharger capacity.
Or to put it another way, just add the APS Twin
Turbo System for an instant 150 hp adrenalin shot
at only 8 psi of boost pressure - obviously the
turbochargers are extremely efficient and under-stressed
at this power level!
Turbos left and right hand side. Click
each image for a large view
But engineering excellence doesn't just stop
with the turbochargers alone. Along with the APS
cast Ni Resist exhaust manifolds that supply the
maximum amount of exhaust gas energy to each turbocharger,
APS cast Ni Resist High Flow Turbine Outlets scavenge
exhaust gasses and ensure the highest possible
energy transfer from each turbocharger. In addition,
with the optimum internal outlet configuration,
the APS High Flow Turbine Outlets deliver unsurpassed
turbocharger wastegate performance for rock steady
boost pressure.

Demands for improving acceleration response and
for the reduction of so-called turbo lag are popular
amongst performance enthusiasts who wish to take
advantage of the enormous gains in power and torque
delivered by turbochargers. In addition, bullet-proof
reliability is required particularly at high turbocharger
boost pressure levels as well as at extreme exhaust
gas temperatures commonly found in high performance
turbocharged engines.
In order to achieve crisp turbocharger response,
a number of advances in turbocharger design have
been utilized over the past decade. Primarily
through the use of modern metals/ceramics in order
to reduce the mass of the rotating assembly. However,
significant gains have been made by reducing the
friction of the rotating assembly - and this has
meant a departure from traditional turbocharger
designs.
Traditional turbocharger design employs a conventional
plain bearing that runs on a film of oil. This
is known as a floating metal bush.

The diagram above shows the turbocharger
main shaft supported by floating metal bushes.
Oil is fed through the bushes and forms a cushioning
layer between the turbocharger shaft and the supporting
bush. The shaft relies on a constant supply of
fresh, clean oil over a very wide contact area
in order to maintain sufficient clearance from
the bush itself. A similar approach is used to
support the turbocharger main shaft from thrust
loads as well.
Whilst
floating metal designs have served us well in
the past, the frictional forces are relatively
high. This results in sluggish turbocharger response
and can be somewhat fragile in nature under extreme
operating conditions.
Nissan attacked this very issue some 15 years
ago on the GTR Skyline by developing a turbocharger
bearing system that forms the basis of the true
high performance modern turbocharger.
By utilizing robust ball bearings at either side
of the turbocharger main shaft, this did away
with the floating metal and thrust bushes.
APS turbocharger rotating group above is a true
twin ball bearing unit that not only delivers
huge power and torque, but is also extremely robust
and incredibly compact in size.

As seen in the diagram above, the
turbocharger shaft is supported by two ball bearing
assemblies. These again are fed with engine oil,
but no longer rely on a thin film of oil over
a wide area to support the turbocharger shaft.
The result is an outstanding reduction of frictional
torque on the rotating turbocharger assembly in
contrast to the old fashioned floating metal bushes.
The improvement in turbocharger response, particularly
in the lower to mid turbocharger speed range is
phenomenal.

The graph above shows frictional
torque versus turbocharger speed of both old fashioned
designs and modern ball bearing turbochargers.
Clearly evident are the improvements with ball
bearing turbochargers - especially at the low
speed range of under 60,000 RPM where friction
losses are reduced by 40% to 50%. This translates
directly into a quantum leap in turbocharger response.
And best of all for those who wish
to push the limits, ball bearing design turbochargers
provide significantly higher robustness by better
supporting the rotating turbocharger assembly,
as well as better spreading thrust loads over
old fashioned methods.

Whilst turbochargers began to be applied to passenger
cars in the late 1970's in response to the energy
crisis, the first generation passenger car turbochargers
were derived directly from commercial diesel engines.
Engine oil was used to provide both lubrication
and cooling and whilst this was an effective compromise
between cost, durability and performance, in high
engine performance applications durability suffered
through fouling of the turbocharger bearings through
high turbine and bearing temperatures.
By encasing the turbocharger bearings in intricate
water passages, engine coolant is used to significantly
reduce turbocharger bearing temperatures in order
to eliminate the coking and lacquering issues
that fouled old fashioned turbocharger bearings.
Non water cooled turbochargers have no place in
a high performance gasoline engine application
and should be avoided at all costs.

The graph above shows the turbocharger
bearing temperature leading up to engine shutdown
and for 20 minutes following shutdown. The temperature
is displayed relative to the coking threshold
of high quality mineral based oil.
As is clearly evident, the old
fashioned non water cooled turbocharger operates
above the coking threshold when under high load
and experiences a very high temperature increase
through heat soak immediately after engine shutdown.
The APS water cooled turbocharger on the other
hand remains cooler than the coking threshold
at all times and the bearing temperature increase
through heat soak immediately after shutdown
is reduced drastically.
By specifying the latest
in turbocharger designs that incorporate both
water cooling and true twin ball bearing designs,
the APS turbochargers deliver bullet-proof reliability
and durability along with exceptional power
levels and unprecedented no-lag turbocharger
response.

It is no secret that APS is developing a single
turbocharger system for the Nissan 350Z, however
this new offering may create confusion in the
market place regarding the benefits of single
versus twin turbochargers. The following discussion
sets out to explain the strengths of each approach
so that APS customers can make an informed decision
as to which application is appropriate for their
requirements.
Turbochargers demand a good deal
of high energy exhaust gas to drive the turbocharger
turbine. Exhaust gas energy is a function of
the mass flow rate of exhaust gas, gas temperature
and velocity. The higher each of these exhaust
gas parameters, the greater the energy available
to spin the turbines. This means that the exhaust
manifold design and the proximity of the turbocharger
to the exhaust ports is critical in the overall
performance of the turbocharger.
A "V6" configuration
engine such as that found on the 350Z has 3
cylinders on one bank and another 3 on the other
bank. This means that for the optimum turbocharger
operation in terms of turbocharger response
and resultant engine power over the entire RPM
range, a turbocharger must be located in close
proximity to each bank of cylinders - ie twin
turbochargers.
In a twin turbocharger configuration,
each turbocharger is located close to the respective
cylinder bank for the optimum exhaust gas energy
transfer to each turbocharger.
A single turbocharger configuration
on the other hand necessitates the exhaust gasses
from each bank travel a longer distance than
that of twin turbochargers located at each bank.
The total distance travelled is determined by
the placement of the single turbocharger but
in short, exhaust gasses from one bank must
travel across the width of the engine bay and
merge with the gasses from the other bank before
finally entering the turbocharger. This has
a negative impact on the total exhaust gas energy
available to drive the single turbine.
To offset the affect of lower
exhaust gas energy available to drive the single
turbine, the size of the single turbocharger
must be reduced when compared to the total turbocharger
capacity of twin turbochargers in order to achieve
similar low to mid RPM engine performance to
that of a twin turbocharger configuration.
There are 3 different scenarios
to consider:
There will be a crossover point
on the power curve if the single turbocharger
is significantly larger than the twin turbochargers
- and only in case 3 (where the single turbocharger
is larger in total air mass flow rate than the
twin turbochargers). This cross over point will
be at some point around 6500 RPM (best estimate
only).
But getting back to production
specification - a single 60 lb per minute single
ball bearing turbocharger (600 flywheel horsepower
turbo) - its power curve will always be below
that of the twin ball bearing turbochargers
(800 flywheel horsepower total) at the same
boost level. It's virtually impossible to achieve
the same low to mid range power and turbocharger
response from a large single turbocharger in
a V configuration engine.
If the single turbocharger is
matched to produce strong low to mid range performance
(which would be the wise choice) then obviously
the turbocharger specification will need to
be precisely matched to the engine capacity.
Bottom line, a large single turbocharger matched
for strong low to mid range performance on the
Z V6 engine will always have a power ceiling
of around 600 flywheel horsepower (around 500
wheel horsepower).
Regardless of the single turbocharger
size, the real issue pertaining to high horsepower
on a single turbo conversion for the Z is the
very limited space available to package an exhaust
downpipe capable of producing over 500 wheel
horsepower. This is where we see the real limitation
of the single turbo design for the Z in comparison
to the twin turbo approach, unless you're prepared
to cut the body sheet metal and make some fairly
radical mods.
It's all very well to have an
large single turbo, but when it's limited to
around 500 horsepower due to a restrictive exhaust
down pipe, you'll never see the real potential
of the large single turbocharger.
Hopefully this helps to put the
single turbo in perspective - and to give one
an idea of the challenges that are presented
to APS as turbocharger system design specialist.
In our view, a well designed single
intercooled turbo system with a well matched
turbo would be a very streetable package on
the V6 350Z engine up to around 600 flywheel
horsepower. This is a great option for the 350Z
enthusiast who desires engine performance that
is superior to the lower cost supercharger options
- but at a similar price point.
That said, the twin turbochargers
utilized in the APS Intercooled Twin Turbo system
deliver superior low to mid RPM engine power
but with a higher power potential of up to 800
flywheel horsepower (rather than 600 flywheel
horsepower of the single turbocharger configuration).
This of course comes at a higher initial purchase
cost.
APS is committed to delivering
either option to the 350Z performance enthusiast.
To
see more components for the Nissan 360Z Twin Turbo
kit click HERE
If you would like further information
on the APS Intercooled Twin Turbo System for the
Nissan 350 Z, please do not hesitate to contact
Autotech Engineering via email on on sales@autotechengineering.com.au
or by phone on (02)9897 1378