On contrary.
Pumping losses is the work the the engine does to pump air in. The intake system is under a vacuum drawing air in. The pumping loss is square of the engine speed and can rob the engine roughly 18% of it's power. This can be felt if you let off the throttle, downshift without throttle or even go down a hill in gear.
Adding a turbocharger heats the air up and pressurizes the intake system. Let's say on a nice day of 70*F, boosting at 6 PSI at sea level.
The temperature after the turbo will be:
Tout = Tin + ((Tinx(-1x(Pout/Pin)^0.263))/n)
Where:
Tout - Temperature after turbo in rankine (R=*F+460)
Tin - Temperature before turbo in rankine
Pout - Pressure after turbo, absolute pressure ... ie ..you have 10lb of boost on the gauge.. add atmosphereic to get absolute
Pin - Pressure before turbo, often slight vacuum, absolute pressure
n - is the efficiency of the turbo... look at the turbo compressor map to determine where it falls in the efficiency range. Most average around 70%
plug in 70*F, 20.7 psia (6 psi boost), .7 for (n as in 70%) and you get a Tout of 158*F
Now, plug it into the density ratio equation to determine the density after the turbo.
DR = (Tin/Tout)*(Pout/Pin)
Same before, remember temperatures are in Rankines and pressures are absolute. DR comes out to be 1.24.
This means that the density of the air after the turbo is 1.24 more than the density than the inlet. Dout = Din * 1.24...
However, since the engine needs to be accomindated for the higher inlet temperatures the ignition timing is adjusted to compensate. The power output is the same even with the slight increase of air.
What's left is the pressure. That helps the engine by having to do less work, and recover lost power explained below.
Just doing an energy analysis on the engine or thermodynamics. The engine experiences a low pressure cycle, negative work, and a high pressure cycle, positive work. Add them together yields net work or what you see at the flywheel. The negative work is... pumping loss.
This is a general Pressure-Volume (P-V) diagram for an actual(opposed to ideal) 4 - stroke engine:
To further explain this diagram, the area inside loop is work, top minus bottom. It represents the 4 stroke in a single rpm in the range. Top side of the loop is compression, combustion and expansion. While the bottom is exhaust and intake.
This is an even more detailed general P-V Diagram:
You can get a general idea at each phase what internally is happening inside the engine. Meaning pressure increasing as volume is shrinking during compression. Pressure growing at combustion. And most noticeably, intake pressures falling below atmosphereic pressure. This takes work to create the vacuum, which means your engine is making less power to suck air in.
Notice that if intake did not fall below atmosphereic pressure that the area of the low pressure cycle would be smaller? And therefore, net work..power at the flywheel... would be larger.
And that's why a pressure increase actually helps the engine recover it's power.
I will not say a rear mount turbo cannot make more positive power. But it's all dependent on inlet temps.
Cheers.
