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Trends and Limits of Two-Stage Boosting Systems for Automotive ...

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Section 1.2 Chapter 1<br />

Conventional thermomechanical limits such as maximum cylinder pressure,<br />

exhaust manifold temperature <strong>and</strong> pressure, compressor outlet temperature,<br />

etc. . . become rapidly limiting factors. Modifying their levels represents major<br />

investments not only in new engine parts but as well in complete validation<br />

processes to guarantee engine reliability. So it is important to analyze how<br />

these limits restrain the downsized-downspeeded engine per<strong>for</strong>mance <strong>and</strong> when<br />

substantial benefits can be achieved. Another limiting factor is the small turbine<br />

size requirement to fulfill the high specific torque density at low engine<br />

speeds. Nowadays, very small turbines are not present in the automotive market<br />

as turbine efficiency significantly decreases with turbine diameter [348].<br />

When combustion efficiency improvements through higher gas density in the<br />

cylinders are lower than pumping losses deterioration caused by the small turbine<br />

design, limitations appear in the utilization <strong>of</strong> turbocharging technologies.<br />

Reaching this point, if other solutions like mechanical or electrical assistances<br />

cannot efficiently provide the required boost pressure, downsized-downspeeded<br />

techniques cease to be efficient. These limits have there<strong>for</strong>e to be defined to<br />

quantify the maximum CO2 benefits that can be raised by these techniques.<br />

The right design <strong>and</strong> coupling <strong>of</strong> the boosting system to the internal combustion<br />

engine have capital importance to obtain the best overall per<strong>for</strong>mance.<br />

Chargers characteristics, components <strong>and</strong> control valves specifications have to<br />

be carefully optimized to match a given engine size <strong>and</strong> to fulfill as optimum<br />

as possible project objectives. Doing such optimization process experimentally<br />

would be very expensive <strong>and</strong> <strong>of</strong> little efficiency. That is why a correct<br />

combination <strong>of</strong> experimental techniques <strong>and</strong> simulation tools is required. Generally,<br />

wave action models are used <strong>for</strong> engine per<strong>for</strong>mance prediction [119,<br />

134]. Through numerical methods, they solve the unsteady, non-linear <strong>and</strong><br />

non-homentropic gas flow equations assuming one-dimensional flow in intake<br />

<strong>and</strong> exhaust piping system. Nevertheless as they predict engine per<strong>for</strong>mance<br />

from a specific boosting system configuration, they need a lot <strong>of</strong> iterations to<br />

per<strong>for</strong>m matching calculations <strong>and</strong> are too time-consuming. With the complexity<br />

arising from multistage architectures, large parametric studies have to<br />

be carried out to optimize the large number <strong>of</strong> parameters, to underst<strong>and</strong> the<br />

important interactions between systems <strong>and</strong> to check influences <strong>of</strong> particular<br />

designs. Their computational costs are there<strong>for</strong>e inappropriate to undertake<br />

these studies especially under current fast engine development process.<br />

Furthermore, when turbochargers <strong>and</strong> engine architecture are not completely<br />

defined, few intake <strong>and</strong> exhaust lines geometrical data are usually available.<br />

Without in<strong>for</strong>mation such as intake manifold runners diameters, pipe lengths,<br />

10

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