<!DOCTYPE article PUBLIC "-//NLM//DTD JATS (Z39.96) Journal Archiving and Interchange DTD v1.0 20120330//EN" "JATS-archivearticle1.dtd">
<article xmlns:xlink="http://www.w3.org/1999/xlink">
  <front>
    <journal-meta />
    <article-meta>
      <title-group>
        <article-title>Detailed Analysis of Mixture and Combustion of Diesel Jets by Laser Induced Fluorescence Techniques</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>G. Bruneaux</string-name>
          <email>gilles.bruneaux@ifp.fr</email>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>Engine System Analysis Department IFP</institution>
          ,
          <country country="FR">France</country>
        </aff>
      </contrib-group>
      <abstract>
        <p>The evolution of Diesel engines in the last decades has been driven by the stringent pollution legislation and increasing environmental concern. In this context the Diesel engine appears like a very good candidate due to its naturally high efficiency. However, in order to further reduce engine out pollutant and green house gases to the required limits, a detailed study of the fuel-air mixing and combustion processes is necessary. An investigation of those processes by Laser Induced Fluorescence (LIF) techniques is presented. The mixing process is studied by tracer LIF, enabling a statistical analysis of the mixture structure and of the effect of injection parameters. The combustion process is studied by simultaneous formaldehyde, Poly-Aromatic-Hydrocarbons (PAH) and OH LIF, giving access to detailed information on the combustion process. A strong coupling is observed between the two processes.</p>
      </abstract>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>-</title>
      <p>mass concentration field is illustrated in Figure 1
for a set of injection conditions.</p>
    </sec>
    <sec id="sec-2">
      <title>Introduction</title>
      <p>High Pressure Direct Injection (HPDI) has
established itself as a proven technology which
allows the efficient reduction of engine-out emissions
in DI Diesel engines. But although HPDI is
becoming a standard, the consequences of this new
technology on mixing and combustion processes
inside the combustion chamber have yet to be
further understood because the physical
phenomena involved are extremely complex, in particular
since the two processes occur on overlapping time
scales and therefore a strong coupling is
happening.</p>
      <p>
        For a detailed investigation of the physical
processes occurring in the combustion chamber,
optical diagnostics are the best candidates since
they are the only way to obtain two dimensional
quantitative measurements inside the combustion
chamber. Various techniques are available for the
study of mixing[
        <xref ref-type="bibr" rid="ref1 ref2">1,2</xref>
        ] and combustion processes[
        <xref ref-type="bibr" rid="ref3">3</xref>
        ],
each one having its advantages and limitations.
Among them, Laser Induced Fluorescence (LIF) is
a complete and powerful tool giving access to
detailed qualitative and quantitative information on
the mixing and combustion processes. Examples
of application of these techniques are presented
here.
      </p>
    </sec>
    <sec id="sec-3">
      <title>Mixing process</title>
      <p>
        Tracer LIF is appropriate for the study of the
mixing process since it can provide
twodimensional quantitative information appropriate
for statistical analysis. The first step of the
application of tracer LIF to the measurement of fuel
distribution in the jet is to develop a method to obtain
normalized fuel mass concentration fields. In ref.[
        <xref ref-type="bibr" rid="ref4">4</xref>
        ]
such a methodology was developed based on the
knowledge of the injected mass at a given instant
and taking into account laser sheet profile shape,
beam steering effect corrections, and the effect of
temperature on the LIF signal. The resulting fuel
[kg/m3]
      </p>
      <p>Figure 1 : Schematics of tracer LIF images
configuration and palette connecting image colors and fuel mass
concentrations.</p>
      <p>2.5
] 2
,[
m
rag 1.5
o
it
s
eh 1
m
u
l
o
V0.5</p>
      <p>A
B
F
A
B
0
0 1 2 3 4 5</p>
      <p>Vapor fuel mass concentration, [kg/m3]</p>
      <p>A statistical analysis of the mixture fields
obtained by tracer LIF was carried out and is
illustrated in Figure 2. It showed that the Diesel jet
mixture can be separated in two distinctive zones:
the mixing zone on the upstream sides, where air
entrainment due to shear turbulence dominates the
jet dynamic, and the stagnation zone at the tip
where the jet pushes away the dense surrounding
gases. The latter is characterized by a lower
mixing rate since small scales turbulence are missing.</p>
      <p>Such analysis was then carried out to
investigate the effect on the mixing process of different
injection parameters such as injection pressure
(illustrated in Figure 3), nozzle hole diameter,
injection duration.</p>
    </sec>
    <sec id="sec-4">
      <title>Combustion process</title>
      <p>The combustion of Diesel jets is a complex
process involving different steps from auto-ignition
to the stabilization of a diffusion flame, and
different regimes of combustion (premixed, diffusion,
soot formation...).</p>
      <p>
        In order to carry out a detailed analysis of the
different combustion regions, a simultaneous
formaldehyde, PAH and OH LIF technique was
developed and applied to the Diesel jet configuration
[
        <xref ref-type="bibr" rid="ref5">5</xref>
        ]. The technique allows to obtain simultaneous
information on the different regions of the
combustion zone: the low temperature zones with
formaldehyde, the fuel-rich high temperature zones with
PAH and the fuel-lean high temperature zones with
OH.
      </p>
      <p>Figure 4 shows a typical combined image
obtained with this technique during the diffusion
limited combustion. A detailed analysis of the
structure of those images was carried out in order to
identify the different regions of combustion and
understand the evolution of the process, in
particular the transition from premixed auto-ignition to
diffusion controlled combustion.</p>
      <p>The results were then synthesized by a
conceptual model of Diesel jet combustion illustrated in
Figure 5.</p>
      <p>One important result that came out of those
investigations is the clear connection between the
mixture and combustion structures, as well as for
the transition from auto-ignition to diffusion limited
combustion than for the structure of the diffusion
flame itself.</p>
    </sec>
    <sec id="sec-5">
      <title>Perspectives</title>
      <p>
        The study of mixture and combustion processes
of Diesel jets by LIF clearly brought up the
advantage of using such techniques for this kind of
complex investigation. Furthermore, this kind of
research can clearly benefit in the future from the
improvement of LIF technique. Indeed in recent
years, a lot of efforts has been made to obtain
more quantitative information with LIF[
        <xref ref-type="bibr" rid="ref6">6</xref>
        ], in
particular for measurements of temperature.
      </p>
      <p>Also, it will be interesting in the future to use the
LIF techniques presented here to study more
complex configurations. For instance multiple injection
strategies are a promising technology to further
reduce engine out emission, and a more detailed
analysis of the physical phenomena involved
during those strategies will certainly help the
optimization process of Diesel combustion systems towards
cleaner engines.</p>
    </sec>
  </body>
  <back>
    <ref-list>
      <ref id="ref1">
        <mixed-citation>
          1 Espey,
          <string-name>
            <given-names>C.</given-names>
            ,
            <surname>Dec</surname>
          </string-name>
          ,
          <string-name>
            <given-names>J. E.</given-names>
            ,
            <surname>Litzinger</surname>
          </string-name>
          ,
          <string-name>
            <given-names>T. A.</given-names>
            ,
            <surname>Santavicca</surname>
          </string-name>
          ,
          <string-name>
            <given-names>D. A.</given-names>
            ,
            <surname>Quantitative</surname>
          </string-name>
          2-
          <string-name>
            <given-names>D</given-names>
            <surname>Fuel Vapor</surname>
          </string-name>
          <article-title>Concentration Imaging in a Firing D.I. Diesel Engine Using Planar Laser-Induced Rayleigh Scattering</article-title>
          , SAE
          <volume>940682</volume>
          ,
          <year>1994</year>
          .
        </mixed-citation>
      </ref>
      <ref id="ref2">
        <mixed-citation>
          2 Bruneaux,
          <string-name>
            <surname>G.</surname>
          </string-name>
          ,
          <article-title>Liquid and Vapor Spray Structure in High Pressure Common Rail Diesel Injection</article-title>
          ,
          <source>Atomization and Sprays</source>
          , vol
          <volume>11</volume>
          , issue
          <volume>5</volume>
          ,
          <fpage>pp533</fpage>
          -
          <lpage>556</lpage>
          ,
          <year>2001</year>
          .
        </mixed-citation>
      </ref>
      <ref id="ref3">
        <mixed-citation>
          3 Dec,
          <string-name>
            <surname>J.,</surname>
          </string-name>
          <article-title>A conceptual Model of DI Diesel Combustion Based on Laser-Sheet Imaging</article-title>
          ,
          <source>SAE paper 970873</source>
          ,
          <year>1997</year>
          .
        </mixed-citation>
      </ref>
      <ref id="ref4">
        <mixed-citation>
          4 Bruneaux,
          <string-name>
            <surname>G.</surname>
          </string-name>
          ,
          <article-title>Mixing Process in High Pressure Diesel Jets by Normalized Laser Induced Exciplex Fluorescence - Part I: Free Jet</article-title>
          ,
          <string-name>
            <surname>SAE</surname>
          </string-name>
          <year>2005</year>
          -
          <volume>01</volume>
          -2100,
          <year>2005</year>
          .
        </mixed-citation>
      </ref>
      <ref id="ref5">
        <mixed-citation>
          5 Bruneaux
          <string-name>
            <surname>G.</surname>
          </string-name>
          ,
          <article-title>Combustion Structure of Free and Wall Impinging Diesel Jets by Simultaneous Laser Induced Fluorescence of Formaldehyde, PAH</article-title>
          and
          <string-name>
            <surname>OH</surname>
          </string-name>
          ,
          <source>International Journal of Engine Research</source>
          , volume
          <volume>9</volume>
          , issue 3,
          <year>2008</year>
          .
        </mixed-citation>
      </ref>
      <ref id="ref6">
        <mixed-citation>
          6 Schulz,
          <string-name>
            <given-names>C.</given-names>
            ,
            <surname>Sick</surname>
          </string-name>
          ,
          <string-name>
            <surname>V.</surname>
          </string-name>
          ,
          <article-title>Tracer-LIF diagnostics: Quantitative measurement of fuel concentration, temperature and air/fuel ratio in practical combustion situations</article-title>
          ,
          <source>Prog. Energy Combust Sci</source>
          .
          <volume>31</volume>
          ,
          <fpage>75</fpage>
          -
          <lpage>121</lpage>
          (
          <year>2005</year>
          ).
        </mixed-citation>
      </ref>
    </ref-list>
  </back>
</article>