**Intercooler Design Discussion**

**This write up was posted by Ed Baker on
www.turbobuicks.com. **

**The original author is John Estill, and the original,
complete write up can be found at
http://www.gnttype.org/techarea/turbo/intercooler.html . **

** This synopsis is an interesting, but simple, read for
those who want a real understanding of the subject and not those ads that claim
a bunch of baloney.**

An intercooler is a heat exchanger. That means
there are two or more fluids that don't physically touch each other but a
transfer heat or energy takes place between them.

At wide open throttle and full boost the hot compressed air coming from a
turbocharger is probably between 250 and 350 deg F depending on the particular
turbo, boost pressure, outside air temperature, etc.. We want to cool it down,
which reduces its volume so we can pack more air molecules into the cylinders
and reduce the engine's likelihood of detonation.

How does an intercooler work? Hot air from the turbo flows through tubes inside
the intercooler. The turbo air transfers heat to the tubes, warming the tubes
and cooling the turbo air. Outside air (or water) passes over the tubes and
between fins that are attached to the tubes. Heat is transferred from the hot
tubes and fins to the cool outside air. This heats the outside air while cooling
the tubes. This is how the turbo air is cooled down. Heat goes from the turbo
air to the tubes to the outside air.

There are some useful equations which will help us understand the factors
involved in transferring heat. These equations are good for any heat transfer
problem, such as radiators and a/c condensers, not just intercoolers. After we
look at these equations and see what's important and what's not, we can talk
about what all this means.

Equation 1

The first equation describes the overall heat transfer that occurs.

Q = U x A x DTlm

Q is the amount of energy that is transferred.

U is called the heat transfer coefficient. It is a measure of how well the
exchanger transfers heat. The bigger the number, the better the transfer.

A is the heat transfer area, or the surface area of the intercooler tubes and
fins that is exposed to the outside air.

DTlm is called the log mean temperature difference. It is an indication of the
"driving force", or the overall average difference in temperature between the
hot and cold fluids. The equation for this is:

DTlm = (DT1-DT2) * F

ln(DT1/DT2)

where DT1 = turbo air temperature in - outside air temperature out

DT2 = turbo air temperature out - outside air temperature in

F = a correction factor, see below

Note:

The outside air that passes through the fins on the passenger side of the
intercooler comes out hotter than the air passing through the fins on the
drivers side of the intercooler. If you captured the air passing through all the
fins and mixed it up, the temperature of this mix is the "outside air
temperature out".

F is a correction factor that accounts for the fact that the cooling air coming
out of the back of the intercooler is cooler on one side than the other.

To calculate this correction factor, calculate "P" and "R":

P = turbo air temp out - turbo air temp in

outside air temp in - turbo air temp in

R = outside air temp in - outside air temp out

turbo air temp out - turbo air temp in

This overall heat transfer equation shows us how to get better intercooler
performance. To get colder air out of the intercooler we need to transfer more
heat, or make Q bigger in other words. To make Q bigger we have to make U, A, or
DTlm bigger, so that when you multiply them all together you get a bigger
number. More on that later.

Equation 2

We also have an equation for checking the amount of heat lost or gained by the
fluid on one side of the heat exchanger (i.e., just the turbo air or just the
outside air):

Q = m x Cp x DT

Q is the energy transferred. It will have the exact same value as the Q in the
first equation. If 5000 BTU are transferred from turbo air to outside air, then
Q = 5000 for this equation AND the first equation.

m is the mass flow rate (lbs/minute) of fluid, in this case either turbo air or
outside air depending on which side you're looking at.

Cp is the heat capacity of the air. This is a measure of the amount of energy
that the fluid will absorb for every degree of temperature that it goes up. It
is about 0.25 for air and 1.0 for water. Air doesn't do a great job of absorbing
heat. If you put 10 BTU into a pound of air the temperature of it goes up about
40 degrees. If you put 10 BTU into a pound of water, the temperature only goes
up about 10 degrees! Water is a great energy absorber. That's why we use water
for radiators instead of some other fluid.

DT is the difference in temperature between the inlet and outlet. If the air is
200 deg going in and 125 deg coming out, then DT = 200 - 125 = 75. Again, on the
cooling air side the outlet temperature is the average "mix" temperature.

If you know 3 of the 4 main variables on one side of the exchanger (the amount
of heat transferred, the inlet and outlet temperatures, and the fluid's flow
rate) then this equation is used to figure out the 4th. For example, if you know
the amount of heat transferred, the inlet temperature, and the flow rate you can
calculate the outlet temperature. Since you can't measure everything, this
equation is used to figure out what you don't know.

Caveat

These equations are all for steady state heat transfer, which we probably don't
really see too much under the conditions that we are most interested in - drag
race! Cruising on the highway you would definitely see steady state. Perhaps at
the big end of the track you may see it too, I don't know. The material of the
intercooler itself will rise in temperature when you hit full throttle,
absorbing more heat than what these equations would lead you to believe. For
example, at steady state idle the intercooler body may be at 100 deg F. At
steady state full throttle it may be 175 deg F. The energy it takes to heat it
up to that temperature comes from the turbo outlet air, and so the cooling of
that air is what is removed by both the flowing outside air and the absorption
of the intercooler body. How long does it take to get to the new steady state?
Beats me, but the graphs I've seen of intercooler outlet temperatures over the
course of a quarter mile run lead me to believe that it is approached before you
get to the end of the quarter mile, since the intercooler outlet temperatures
reached a steady level.

So, now that we've got these equations, what do they really tell us?

The difference between the intercooler outlet temperature and the outside air
temperature is called the approach. If it is 100 degrees outside and your
intercooler cools the air going into the intake manifold down to 140 degrees,
then you have an approach of 40 degrees (140 - 100 = 40). To get a better
(smaller) approach you have to have more area or a better U, but there is a
problem with diminishing returns. Lets rearrange the first equation to Q/DTlm =
U x A. Every time DTlm goes down (get a better temperature approach) then Q goes
up (transfer more heat, get a colder outlet temperature), and dividing Q by DTlm
gets bigger a lot faster than U x A does. The upshot of that is we have a
situation of diminishing returns; for every degree of a better approach you need
more and more U x A to get there. Start with a 30 deg approach and go to 20 and
you have to improve U x A by some amount, to go from 20 to 10 you need to
increase U x A by an even bigger amount.

I would consider an approach of 20 degrees to be pretty good. In industrial heat
exchangers it starts to get uneconomical to do better somewhere around there,
the exchanger starts to get too big to justify the added expense. The only
practical way of making the DTlm bigger on an existing intercooler is to only
drive on cold days; if you buy a better intercooler you naturally get a better
DTlm.

You can transfer more heat (and have cooler outlet temps) with more heat
transfer area. That means buying a new intercooler with more tubes, more fins,
longer tubes, or all three. This is what most aftermarket intercoolers strive
for. Big front mounts, intercooler and a half, etc... are all increasing the
area.

A practical consideration is the fin count. The area of the fins is included in
the heat transfer area; more fins means more area. If you try to pack too many
fins into the intercooler the heat transfer area does go up, which is good, but
the cooling air flow over the fins goes down, which is bad. Looking at the 2nd
equation, Q=m*Cp*DT, when the fin count is too high then the airflow ("m")
drops. For a given Q that you are trying to reach then you have to have a bigger
DT, which means you have to heat up the air more. Then that affects the DTIm in
the first equation, making it smaller, and lowering the overall heat transfer.
So there is an optimum to be found. Starting off with bare tubes you add fins
and the heat transfer goes up because you're increasing the area, and keep
adding fins until it starts to choke off the cooling air flow and heat transfer
starts going back down. At that point you have to add more tubes or make them
longer to get more heat transfer out of the increased area.

Make U go up. You can increase the U by adding or improving "tabulators" inside
the tubes. These are the fins inside the tubes which cause the air to swirl
inside the tube and makes it transfer its heat to the tube more efficiently. One
of the best ways to increase the U is to clean the tubes out. Oil film inside
the tubes acts as an insulator or thermal barrier. It keeps heat from moving
from the air to the tube wall. This is expressed in our equation as a lower U.
Lower U means Lower Q's which mean hotter turbo air temperatures coming out of
the intercooler.

Air-to-water. If we use water as the cooling medium instead of the outside air,
we can see a big improvement for several reasons: Water can absorb more energy
with a lower temperature rise. This improves our DTIm, makes it bigger, which
makes Q go up and outlet temps go down. A well designed water cooler exchanger
also has a much bigger U, which also helps Q go up. And since both DTIm and U
went up, you can make the area A smaller which makes it easier to fit the
intercooler in the engine compartment. Of course there are some practical
drawbacks. The need for a water circulation system is one. a big one is cooling
the water down after it is heated, which means another radiator. This leads to
another problem; You heat the water and cool it down with the outside air. You
can't get it as cool as the outside air, but maybe you can get it within 20
degrees of it. Now you are cooling the turbo air with water that is 20 degrees
hotter than the outside air, and you can only get within 15 degrees of that
temperature so coming out of the intercooler you have turbo air that is 35
degrees hotter than the outside. You could have easily done that with an air to
air intercooler. But if you put ice water in your holding tank and circulate
that, then maybe the air temp coming out of the intercooler is 15 degrees above
that or 45 to50 degrees. But after the water warms up you're back to the hot air
again. Great for racing but not as good for the street.

Lower the inlet temperature. The less the turbo has to work to compress the air
the lower the temperature the air coming out of the turbo is. This actually
hurts DTIm, but the cooler going in the cooler coming out. You can work the
turbo less by running lower boost, by improving the pressure drop between the
air filter and the turbo, or by having a more efficient compressor wheel. You
can also reduce the pressure drop in the intercooler, which allows you to run
the same boost in the intake manifold while while having a lower turbo discharge
pressure. If you can drop the turbo outlet pressure by 2 psi, or raise the turbo
inlet pressure by 1 psi, that will drop the turbo discharge temperature by about
16 degrees. If the turbo air is going into the intercooler 16 degrees colder
then it may come out only 10 degrees colder than before, but that is still
better than it was.

Pressure Drop

Another aspect of intercoolers to be considered is pressure drop. The pressure
read by a boost gauge is the pressure in the intake manifold. It is not the same
as the pressure that the turbocharger itself puts out. To get a fluid, such as
air, to flow there must be a difference in pressure from one end to the other.
Consider a straw that is sitting on the table. It doesn't having anything moving
through it until you pick it up, stick it in your mouth, and change the pressure
at one end (either by blowing or sucking). In the same way the turbo outlet
pressure is higher than the intake manifold pressure, and will always be higher
than the intake pressure, because there must be a pressure difference for the
air to move.

The difference in pressure required for a given amount of air to move from turbo
to intake manifold is an indication of the hydraulic restriction of the
intercooler, the up pipe, and the throttle body. Let's say you are trying to
move 255 gram/sec of air through a stock intercooler, up pipe, and throttle body
and there is a 4 psi difference that is pushing it along (I'm just making up
numbers here). If your boost gauge reads 15 psi, that means the turbo is
actually putting up 19 psi. Now you buy a PT-70 and slap on some Champion heads.
Now you are moving 450 gm/sec of air. At 15 psi boost in the intake manifold the
turbo now has to put up 23 psi, because the pressure drop required to get the
higher air flow is now 8 psi instead of the 4 that we had before. More flow with
the same equipment means higher pressure drop. So we put on a new front mount
intercooler. It has a lower pressure drop, pressure drop is now 4 psi, so the
turbo is putting up 19 psi again. Now we add the 65 mm throttle body and the
pressure drop is now 3 psi. Then we add the 2.5" up pipe, and it drops to 2.5
psi. Now to make 15 psi boost the turbo only has to put up 17.5 psi. The
difference in turbo outlet temperature between 23 psi and 17.5 psi is about 40
deg (assuming a constant efficiency)! So you can see how just by reducing the
pressure drop we can lower the temperatures while still running the same amount
of boost.

I have seen some misunderstandings regarding intercooler pressure drop and how
it relates to heat transfer. For example, one vendor's catalog implies that if
you had little or no pressure drop then you would have no heat transfer. This is
incorrect. Pressure drop and heat transfer are relatively independent, you can
have good heat transfer in an intercooler that has a small pressure drop if it
is designed correctly. It is easier to have good heat transfer when there is a
larger pressure drop because the fluid's turbulence helps the heat transfer
coefficient (U), but I have seen industrial coolers that are designed to have
less than 0.2 psi of drop while flowing a heck of a lot more air, so it is
certainly feasible.

Pressure drop is important because the higher the turbo discharge pressure is
the higher the temperature of the turbo air. When we drop the turbo discharge
pressure we also drop the temperature of the air coming out of the turbo. When
we do that we also drop the intercooler outlet temperature, although not as
much, but hey, every little bit helps. This lower pressure drop is part of the
benefit offered by new, bigger front mount intercoolers, by bigger up pipes; and
by bigger throttle bodies. You can also make the turbo work less hard by
improving the inlet side to it. K&N air filters, free flowing MAF pipes,
removing the MAF itself when switching to an aftermarket fuel injection system,
these all reduce the pressure drop in the turbo inlet system which makes the
compressor work less to produce the same boost which will reduce the turbo
discharge temperature (among other, and probably greater, benefits).

What about my Intercooler?

Wondering if your intercooler is up to snuff? The big test: measure your
intercooler outlet temperature! When I did this I got a K type thermocouple, the
thin wire kind, slid it under the throttle body/up pipe hose and down into the
center of the up pipe, and went for a drive. On an 80 to 85 deg day I got a WOT
temperature of 140 deg, for a 55 to 60 deg approach. That tells me that I need
more intercooler. If I can get the temperature down to 100 deg, the air density
in the intake manifold goes up by 7%, so I should flow 7% more air and
presumably make 7% more hp. On a 350 hp engine that is 25 hp increase. On a 450
hp engine that's a 30 hp increase. Damn, where's my check book…

Another check is pressure drop. Best way to check it is to find a pressure
differential gauge, which has 2 lines instead of the single line a normal
pressure gauge has. It checks the difference between the 2 spots it is hooked up
to, as opposed to checking the difference in pressure between the spot it is
hooked up to and atmospheric pressure, which is how a normal pressure gauge
works.

Hook one line of the gauge to the turbo outlet and one to (preferably) the
intercooler outlet. The turbo outlet/intercooler inlet pressure is easy, just
tee into the wastegate supply line off the compressor housing. It would be nice
to get the intercooler outlet pressure directly, but there's no convenient spot
to hook up to. Hooking into the intake manifold (such as via the line to the
boost gauge) is quite convenient, but gives the total pressure drop: intercooler
+ up pipe + throttle body. That'll give you a pretty good idea though.

Instead of the differential pressure gauge you could use 2 boost gauges, one in
each spot, but then you have to worry about whether both gauges are calibrated
the same, try to read both at the same time while driving fast, etc AND you may
spring (i.e., ruin) the gauge on the turbo outlet since when you close the
throttle you get a big pressure spike that your normal boost gauge never sees.

If you find more than 4 or 5 psi difference between the intercooler inlet and
intake manifold (and I'm just giving an educated guess here, you'd probably want
to refer to one of the intercooler manufacturers for a better number) then I
would suspect that a larger, lower pressure drop intercooler would offer you
some gains.

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