Intercoolers for Diesels

“Intercoolers” cool the air charge from the turbocharger compressor before it enters the engine, but why is this so wonderful? Probably more important than the decrease in air temperature that’s achieved (but that is still useful and important in its own right), is the increase in air charge density that can be achieved by charge cooling.

Air will get hotter when compressed - and hot air is less dense than cool air. So you have a lower mass of air in a certain volume when it’s hot than when it’s cool. The real aim of charge compressing and cooling is to increase the mass of air that is put into the engine’s cylinders.

Remember that air has mass and the number of oxygen molecules available to combust the fuel is directly related to the mass of air in the engine’s cylinders. If we have a fixed volume of air, say 1 Litre, the density of the air is the mass of air contained in that Litre. In the case of air at 15 C and normal atmospheric pressure (about 14.7 psi absolute or about 1.0 bar absolute) the density is 1.225 g/L. As the volume of an engine’s cylinders is fixed, the only way to increase the mass of the air charge in them is to increase it’s density. So first we compress the air. If our turbocharger increases the air to 2.0 Bar absolute (about 30 psi Abs) and the air temperature is still 15 C, the density would be around 2.45 g/L. BUT (and this is the big BUT), if the temperature is greater than our original 15 C the density will be less than 2.45 g/L.

A cooler, denser air charge means we have a greater mass of air available to combust fuel and the more power we ultimately get from our engine. Generally it will also run cooler and be more fuel efficient. So, the answer is to cool the air charge. And the cooler we can get that air, the better.

Factory Air-to-Air Charge Coolers

Many factory air-to-air charge coolers are placed on top of the engine, with a hole in the bonnet (hood) and an air scoop to collect and direct air flow through the cooler core. This is known as a “top mounted” location for obvious reasons.

Aftermarket Air-to-Air Charge Coolers

The other common location, and one with some inherent advantages in my opinion, is “front mounted” where the cooler is at the front of the vehicle, behind the grill and either in front of or beside the coolant radiator. Aftermarket air-to-air charge coolers are usually front mounted as there will not often be room to add a top mounted installation.

Aftermarket Air-to-Water Charge Coolers

Some aftermarket manufacturers are now producing air-to-water devices which can, in theory at least, be mounted just about anywhere. They are often a cylindrical device with large charge air inlet and outlet stubs at each end and smaller coolant hose connections to the outer casing.

These coolers generally have their own closed coolant circuit which in turn needs a small water-to-air radiator to ‘cool the coolant’, as it were. This then needs to be placed in a good, cool airflow. They also typically require a small electric pump to circulate the coolant. This all adds to the cost and complexity of the installation but the charge cooler itself is usually much smaller than an equivalent air-to-air cooler and they can produce excellent results.

Instead of the theory of operation and mathematical explanations regarding heat transfer co-efficients, effective surface areas etc., we’ll look at the effects of charge cooling.

The pressure, temperature and volume of a fixed mass of gas are related by a rule of physics called the Ideal Gas Equation:

PV/T = Constant,

where P = absolute pressure, V = volume and T = absolute temperature.

All it really says is that if you change any one of these parameters, at least one of the others will change too.

Another way to write this is: P1V1/T1 = P2V2/T2,

where, say, P1, V1 & T1 describe our ambient air entering the air cleaner and P2, V2 & T2 describe the air coming out of our turbocharger compressor.

You might think that, as it’s called the “ideal” gas equation, it doesn’t really apply in the real-world but at the low-ish pressures and temperatures we’re talking about, it’s pretty accurate. [Though for super-high pressure steam boilers in power stations, for example, the mathematics can get quite a bit trickier.]

Now, we’ll modify the Ideal Gas Equation a bit to suit our purposes. [Any theoretical physicists out there, please just come along with us for a while, OK?]

As mentioned earlier, the equation applies to a fixed mass of gas. In our case let’s say this is the mass of air drawn in through the air cleaner of our engine in one second, while we’re driving at full throttle and heavy load. The volume of our air is related to the mass of our air by the equation:

V = m/d, where m = mass (grams) and d = density (grams/Litre),

and so, if we replace “V” in our equation, we get: P1m1/T1d1 = P2m2/T2d2.

As the mass of air leaving our turbocharger is the same as the mass of air entering it, m1 = m2 and our equation becomes:

P1/T1d1 = P2/T2d2

We can rearrange this to:

d2 / d1 = post-turbocharger density/pre-turbocharger density = P2/P1 x T1 /T2.

Before we go on, we do need to clarify our pressure and temperature measurements. We discussed the concept of absolute pressure in the first article of the series, that is, pressure above an absolute vacuum. So, to convert from gauge pressure (or boost pressure) to absolute pressure, we need to add 14.7psi or 1.0Bar.

A similar thing applies to temperature. Zero degrees Celsius is obviously not as cold as anything can even get. In fact, that temperature is -273.15°C or Absolute Zero. To convert from Celsius temperature to absolute temperature, we need to add 273.15 to the Celsius temperature.
The units of absolute temperature are Kelvin (K), so 0°C is the same as +273.15K and 25°C is 298.15K etc.

Absolute pressure and absolute temperature are the units we need to make use of our gas equations.

Figures from actual measurements on my vehicle when towing a 2tonne+ caravan up a mountain range:

P1 = 1.00Bar Abs, T1 = 23°C = ~296K and

P2 = 1.98Bar Abs, T2 = 184°C = ~457K.

P2 = 1.98Bar Abs, T2 = 184°C = ~457K.

Our re-arranged equation gives us:

d2 / d1 = post-turbocharger density/pre-turbocharger density = 1.98/1.00 x 296/457 = 1.283

This means our turbocharger has increased the density of the air charge to ~28% above the ambient air. It is a long way short of the 98% increase we might have expected by looking only at the boost pressure to ambient pressure ratio (1.98/1.00 = 1.98).

Now let us have a look at the figures for the air entering the engine, after having passed through the vehicle’s standard intercooler.

P3 = 1.98 Bar Abs; T3 = 91°C = ~364K. The intercooler has dropped the air temperature by a massive 93°C ! Even better news is the air charge density we have recovered:

d3 / d2 = post-intercooler density/pre-intercooler density = 1.98/1.98 x 457/364 = 1.256

So we have now increased our air charge density by another ~26% by cooling it through the intercooler.

(The boost pressure before and after the intercooler is assumed to be the same. It was measured only after the intercooler)

Now the total increase in density is:

d3 / d1 = post-intercooler density/pre-turbocharger density = 1.98/1.00 x 296/364 = 1.61

or ~61% higher than the ambient air density.

Now we’re talking some serious improvement in performance, as long as we increase the fuel supply along with this increased air charge.

The first chart shows the vehicle encountering a steep climb from a steady cruise. The boost pressure (Black dashed line) quickly increases from about 0.3 Bar to about 1.0Bar (the wastegate setting), indicating full load. Notice that the Turbo Air Outlet temperature (Red line = charge cooler inlet) increases almost instantaneously with boost. However, the Manifold Air Inlet temperature (Blue line = charge cooler outlet) increases slowly over about 30 or 40 seconds.

This is because the several kilograms of aluminium forming the charge cooler (and it’s interconnecting pipes and hoses) form a fairly large heat sink. That is, they absorb much of the heat from the charge air before they themselves become hot and begin radiating that heat to the ambient air flow.

From about the 60 second mark, the manifold air temp actually drops a little. I believe this is due to a couple of effects. The now-hot charge cooler is now effectively transferring heat to the ambient air and the vehicle speed has probably increased a little, further improving the heat transfer. Click on the table chart below to see a larger version.

The second chart shows the opposite effect when the load is reduced. In this case, the engine comes off full load at the 380 second mark and slows to a stop at about 400 seconds. Again, the Turbo Air Outlet temperature falls almost in line with the boost pressure. The Manifold Air Inlet temperature falls at a much slower rate as the charge cooler “heat sink” gives up its accumulated heat to both the ambient air and some to the now much cooler charge air.

What Does it Mean?

Well, for short bursts of full load acceleration (traffic light ‘drags’ or performance testing?), just about any charge cooler will do quite a bit of good as it removes heat from the charge air via its heat sink effect. However, once the vehicle has been at full load for some time (tens of seconds+), the actual heat transfer efficiency of the charge cooler becomes more important.

Sustained full load operation means the charge cooler has to be effective at transferring the heat to the ambient air, either directly by an air-to-air cooler or via the coolant circulating system in an air-to-water cooler. Otherwise the actual engine charge air temperature will continue to rise toward that of the turbo outlet. Among other things, this must increase the load on the engine cooling system and increase the exhaust gas temperature.

Preferences

This is why I much prefer front mounted air-to-air coolers. Regardless of the vehicle speed (and especially when operating in low gears at full load, such as heavy sand driving or towing up steep gradients), the engine’s standard viscous and/or electric fans will keep up a strong flow of ambient air through the cooler. Top mounted coolers on the other hand, often rely solely on the vehicle’s forward motion to create air flow through the cooler. At low speeds this may be negligible and, at standstill, these coolers will often be acting as air heaters, absorbing the high temperatures from the engine bay and transferring this to the otherwise cool charge air.

Benefits

Despite their cost and complexity, air-to-water charge coolers have the potential to give the very best performance. Firstly, they have a much larger heat sink effect for short term loads, due to the much higher thermal mass of the water jacket around the cooler core. Secondly, if all is correctly sized and operating properly, they have the potential to very effectively transfer large quantities of heat from the cooler core to the ambient air via their own radiator, which is usually front mounted.