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fast tech
/ TECH / TURBOCHARGERS /
fast tech
SUPERSIZE ME
SUPERSIZE ME
BEFORE
STARTING…
The fi rst rule of working on
cars and using tools of any
kind is don’t ever skimp on
decent protection. Goggles,
gloves, ear defenders,
masks and a set of overalls
should be in your garage.
Use them.
When using power tools,
protective gear is essential
— grinders and welders can
make a real mess of your
soft skin and bone if you get
it wrong.
Never work under a car
without supporting it using
axle stands. A car falling on
you is not something you’ll
be laughing about down
the pub.
Turbochargers: big or small? How does a bigger one make the power
difference without a boost pressure increase?
WHO IS STU?
A Level 5-trained fuel-injection
technician, in the past Ford nut Stu’s
worked for a Ford RS dealer, a well-
known fuel-injection specialist and
various tuning companies. Then six
years ago, he joined forces with Kenny
Walker and opened up Motorsport
Developments near Blackpool,
specialising in engine management
live remapping, as well as developing
a range of Evolution chips which are
now sold all over the world.
He’s also the brains behind www.
passionford.com. Started in 2003, it’s
grown rapidly from a few friends and
customers contributing, to one
of the biggest Ford communities on
the web.
Stu’s enviable knowledge of the
workings of modern-day Ford
performance engines means
that he’s just the man to explain
how and why things work, and
most importantly, how they can
be improved!
Having worked as a tuner for over
16 years, Stewart ‘Stu’ Sanderson
is one of the most respected
names in the business.
to-day
work as an engine tuner, I’ve learnt
that there are various concepts that
most car enthusiasts (and some
professionals!) can’t get their heads
around. One of these is turbo sizing.
When I recommend it’s time a
customer increases the size of the
turbo on their engine as part of a
power upgrade package, it’s almost
guaranteed the very fi rst question
asked is, “Does this mean we can
run more boost, Stu?”.
The answer is usually: “While we
could if we wanted to, we aren’t
going to — we’re going to run the
same boost or less, and get much
more power!”
This reply normally leads — via
confused looks — to a discussion
about how a large turbo (Garrett
T4, for example) can produce more
power with a 20 psi intake plenum
pressure, than a much smaller
turbo like a Garrett T3 does at
exactly the same 20 psi intake
plenum pressure.
The facts are quite simple, if not a
little tricky to explain, so let’s look at
a few things shall we?
To make this 170 bhp we are
utilising the air pumping ability
of our 2-litre engine, via its four
500cc cylinders.
These cylinders are drawing in,
through the inlet valves, enough air
and fuel at the correct ratio to burn
safely and, importantly, expelling it
once burnt and processed via the
exhaust valves, to produce a power
at the crankshaft of 170 bhp.
The air processed and power
produced is related to the engine’s
volumetric effi ciency (VE). (See
boxout for how this is calculated.)
So the engine in question is
making its 170 bhp with its nice,
well-designed standard 4-2-1
exhaust system. So, now let’s
redesign this engine and make
it turbocharged.
Starting at the exhaust system,
we’ll remove that 4-2-1 manifold
and stick a Garrett T3 turbo with a
relatively small turbine housing on
it. We’ll then jam close the exhaust
turbine bypass gate (also known as
a wastegate), and weld tight the
compressor wheel so it can’t spin
and pressurise our intake system —
just to see what actually bolting the
turbo on does to our engine.
In essence, we now have the
same, proven 170 bhp engine, but
with a far more restrictive exhaust
due to the turbo’s turbine housing.
Hands up anyone there who
thinks this engine will still make
170 bhp?
I’m sure we are all agreed that by
restricting our exhaust this way we
are now going to be lucky to see
100 bhp! But why does the power
Fitting a turbo actually costs
the engine some power
VOLUMETRIC
EFFICIENCY?
VE is the amount a cylinder fi lls
itself with mixture on the
induction stroke. If a 500cc
cylinder draws in 500cc of air/
fuel on the induction stroke, it
achieves 100 per cent VE.
Words: Stewart Sanderson
FORCE THE ISSUE
The fi rst question I have to ask you
is this: “Are you aware that a
turbocharger is universally
recognised as a form of forced-
induction that initially costs the
engine some power?”
Let’s look at this carefully with
a little tuning scenario. For the sake
of discussion, we’ll take a 1994
RS2000 I4 unit that’s had the
breathing improved by the fi tment
of some sensible camshaft profi les
and a nice porting job on the
cylinder head to produce a healthy
170 bhp.
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DURING my day-
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fast tech
/ TECH / TURBOCHARGERS /
fast tech
this costs us power, is a great
proportion of the energy produced
from the power stroke of each
cylinder burning the charge of fuel
and air is now wasted trying to push
the spent gas out of the previously
active cylinder’s exhaust valve, and
through the tiny turbine housing
into the exhaust before it can draw
in another fresh charge.
We also have some detrimental
knock-on effects from this back
pressure: the friction on components
caused by this pumping loss will
now add heat to our engine, too. This
heat was part of our power stroke’s
energy so is wasted power.
This pumping loss has also
caused a problem with a
phenomenon known as cylinder
scavenging. Scavenging is used
extensively with normally-aspirated
engines, but is reduced to virtually
zero on almost all turbocharged
engines due to the back pressure in
the relatively tiny turbine housing.
This back pressure has now also
decreased the amount of air the
exhaust pulse drew through the
inlet valve at overlap (the point at
which both inlet and exhaust valves
are slightly open), so the maximum
cylinder fi ll (VE) has reduced. Not
The much larger T4 turbo will produce a lot more power at the
same boost, but as it has larger housings, it’s very laggy
A T3 turbo will produce good power at a given boost limit with
relatively low lag, giving good response and driveability
Our turbo’s pressurised air has to
travel through hoses, intercoolers,
throttle bodies and then ultimately
the plenum, before it has fuel added
to it and it travels through the inlet
valve into the awaiting cylinder.
Once combusted and the energy
from this mixture is converted into
crankshaft energy as best it can
be, the piston travels back
upwards with the exhaust valve
open, and the air is expelled into
the turbine housing and exhaust
awaiting a fresh charge through
the inlet valve...
So, how do we make our engine
shift more air and thus create even
more bhp?
The engine will only process
more air if we do one of the
following things:
What did bolting a T4 onto our
engine do? The head hasn’t been
ported or cams fi tted so there’s no
route improvement.
We are running the same boost
pressure as on the smaller turbo, so
there’s no harder push.
So, have we changed the engine’s
VE? We must have!
only that, but the back pressure
created means that some of the
exhaust gas no longer escapes at
all, thus diluting down our next
cylinder of air/fuel with dead (and
extremely hot) gases.
Down goes the engine’s VE
again... things are looking really bad
for our power curve now!
So conversely, as we now have
less airfl ow on overlap, we are going
to start dumping heat through our
exhaust seat and port and are
heating our soft alloy head up. Why?
Simple: designers use scavenging
on overlap as a very simple and
effective way of cooling valve seats,
guides and ports.
How does that work? Well, it’s
simply because when we reach
overlap in our cam timing event,
we have both a cold inlet and
hot exhaust valve open. This gives
the exhaust valve and relative
components time to cool down
from their grievous job only
moments after shifting a mass
of immensely hot air through its
system. So it’s a great relief for
them to sit in some nice cold-
fl owing air for a second and
transfer a bit of excess heat away!
Our fancy new engine design
isn’t looking too hot now is it? Well
actually, it’s getting very hot!
So, hopefully you can now
see why the turbo costs an engine
horsepower just by its very
existence, and if you understand
that, you are now well on your way
to understanding how a bigger
turbo will make more power than
a smaller one with the same
inlet pressure.
T3 V T4
The necessary exhaust back
pressure caused by the turbine
housing assembly is the key
element between the T3 and T4 —
the T4 fl ows far more exhaust gas
than the T3 so pumping losses are
far reduced.
But let’s deal with the delivery of
our air into the engine now, and for
that let’s use the Cosworth four-
cylinder YB power unit.
A T4 produces far more volume of
air at a given pressure from its
compressor housing than a T3 —
that’s universally agreed. And we
agree both turbos have the same job
— to pressurise our engine’s intake
system and keep the air fl owing
through it, mixed with fuel at the
correct ratio, to generate power.
So let’s look at the route of the air
a little closer:
Below. Unlike the manifold on
the left, all the gas on a turbo’d
car has to be forced through that
little square opening you can see
in the turbine housing. It is then
spun so that when it reaches the
turbine wheel, it has a higher ve-
locity than when it left the engine,
creating turbine inlet pressure
Above. In a perfect world,
exhaust gasses would have
no restrictions to cause losses,
like when a 4-2-1 manifold is
fi tted to a NA engine
TECH NOTE
To explain how, I am afraid we have
to get a little bit technical. First, the
Compressor Stage:
On a standard YB, a Garrett T3
equipped with a 50-trim compressor
(2wd Cosworth), running our desired
boost pressure of 20 psi may be
spinning at around 120,000 rpm with
a compressor effi ciency of 70 per
cent (depending on air consumption
at the time of measurement).
A Garrett T4 equipped with a 60-
trim compressor (RS500), running
our desired boost pressure of 20 psi
may be spinning at only 90,000 rpm
with a compressor effi ciency of
drop? What has actually changed
that’s cost us 70 bhp?
LOSE OUT
The answer is that we have
dramatically increased pumping
losses. Pumping losses are the
amount of power used by the
power stroke of a cylinder, to pump
out the exhaust gas from another
cylinder. The harder it is to get the
gas out, the more power is lost in
doing so.
This is the biggest issue with
turbocharged engines. The reason
1. Improve the air’s route into
the cylinders
2. Increase the pressure we push it
in with
3. Improve the volumetric effi ciency
Here you can clearly see the difference in size of the T3
(left) and T4 compressor wheels. The T4 will move a far
greater volume of air thus improving the engine’s VE
CYLINDER
SCAVENGING
This is the extra amount of
waste gas drawn out of the
exhaust valve at top dead
centre (TDC), due to the
presence of a slight depression
that was created by the
evacuation of gas through the
exhaust valve.
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fast tech
T4 can supply it all in its stride, due
to its nice, large compressor.
But we aren’t making more
power simply because the T4
pumped more air at 20 psi, are we?
I have now proven that we are
making more power because this
turbo improved the volumetric
effi ciency of our engine. The
improvements are mainly through
exhaust back pressure reductions,
and an improvement in outlet
temperatures at the compressor
itself. This temperature improvement
is due to a factor known as Adiabatic
Effi ciency (which we’ll discuss in a
future issue).
This is achieved by narrowing
the turbine housing down prior
to it terminating at the turbine
wheel, increasing the compression
of the gas and ultimately releasing
maximum heat — but creating
the maximum back pressure.
A small turbine housing and
wheel will spool the turbo up
quickly, but leave you with lots of
exhaust back pressure and a
torque curve that at high rpm will
drop off very quickly due to the
pumping losses generated at high
rpm when we try and move
maximum volume of air in the least
possible amount of time.
The size of the turbine housing
is expressed in an A/R fi gure, and
in most cases, the smaller the
number, the smaller the housing,
and therefore, the faster the spool
will be and the higher the ultimate
back pressure.
When we increase the turbine
housing A/R, we drop the back
pressure, and in doing so, also drop
energy and velocity at the turbine
wheel, thus slowing the turbine’s
response, which ultimately harms
the compressor’s response and
making the engine’s ‘time to
boost’ worse. Not to mention the
possibility of engine and turbo-
damaging surge.
This lower TIP and corresponding
compressor response has the
effect of moving the engine’s
power band higher, but damaging
low-end torque at the same time.
Turbo choice is a science that
requires an educated amount of
give and take. You cannot yet have
your cake and eat it — at least,
not until variable geometry
turbochargers are ready for us to
start reliably bolting to your petrol
engines. But that’s another story...
The exhaust, or turbine housing as its known will make all the
difference to how a car drives — too big and it will be laggy, too
small and it won’t make big power but will have instant response
BIGGER = BETTER?
Therefore everything about the
bigger turbo is good, isn’t it? So why
don’t we always fi t a huge, great
turbo and benefi t from the greatly
fl owing turbine stages?
Well, that brings me to the
downsides of fi tting a larger turbo...
Where do we lose out with a larger
turbo? And why?
Turbochargers require high
back pressures prior to the turbine
wheel to drive them correctly. This
pressure is referred to as the Turbine
Inlet Pressure (TIP), and
is the fi rst part you must match
when designing a turbocharged
installation on an existing engine.
A normal ratio here will be in the
order of 2:1 (for example, 40 psi
turbine inlet pressure and 20 psi inlet
valve boost pressure). The
way the turbine housing works is
to accelerate the gasfl ow and
concentrate the heat energy, so that
it meets the turbine wheel with more
velocity and heat energy to drive it
hard, thus spinning our compressor
hard and generating the maximum
boost pressure in minimum time.
82 per cent (depending on the
air consumption at the time of
the measurement).
another exhaust back pressure
improvement there at all times,
wastegate open or closed.
Let’s look now at the boost
pressure seen at our intake valves.
Since our exhaust back pressure
is now largely reduced, our cylinder’s
demand for and ability to process
air has increased. We have overlap
effi ciency gains during valve open
events, we have thermal effi ciency
gains in the compressor stage
meaning our air is cooler coming
out of the bigger turbo and thus
denser, and we can suck more air
into the cylinder, mix it with more
fuel and generate more bhp due to
increased cylinder evacuation on
the exhaust event. Result: we are
now processing more air and this
Turbine Stage:
The T4 P trim turbine wheel fl ows a
lot more air than the standard T3
trim rear wheel. But it conversely
takes more energy to spin it to
speed, so the fi rst thing to note is
we have an exhaust gasfl ow
improvement due to a better
fl owing rear wheel.
Secondly, we now have a
wastegate that will open much
sooner and much wider than it
would on the T3 turbo, as less
exhaust volume is required to
spin the turbine and compressor
to generate our required inlet
pressure, due to improvements
made to the effi ciency of both the
turbine and compressor.
At the turbine we now have a
30,000 rpm improvement in
effi ciency at our rated 20 psi inlet
pressure — hey, and that’s another
exhaust back pressure improvement
there, isn’t it?
A nice, wide-open wastegate
is also a by-product of a more
effi cient turbocharger — the
wastegate bypasses the restrictive
turbine housing as a means to
stabilise and regulate boost
pressure. This also makes the
piston and crank’s job of pumping
the exhaust gas from the engine a
little easier again, so the wider the
better please.
Since our T4 is actually using an
altogether bigger turbine housing
area radius (A/R) as well, we have
Even on Cossies, big turbos don’t always make for great road-car
installations, simply because of the increased ‘time to boost’
NEXT MONTH
What’s a compressor map?
Plus how it helps you to
make the correct turbo
choice and avoid surge
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