<?xml version="1.0" encoding="UTF-8"?><?xml-stylesheet type="text/xsl" href="static/style.xsl"?><OAI-PMH xmlns="http://www.openarchives.org/OAI/2.0/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/ http://www.openarchives.org/OAI/2.0/OAI-PMH.xsd"><responseDate>2026-09-21T23:19:24Z</responseDate><request verb="GetRecord" identifier="oai:www.repository.cam.ac.uk:1810/309271" metadataPrefix="uketd_dc">https://api.repository.cam.ac.uk/server/oai/request</request><GetRecord><record><header><identifier>oai:www.repository.cam.ac.uk:1810/309271</identifier><datestamp>2024-06-26T13:52:57Z</datestamp><setSpec>com_1810_213729</setSpec><setSpec>com_1810_256065</setSpec><setSpec>col_1810_219485</setSpec></header><metadata><uketd_dc:uketddc xmlns:uketd_dc="http://naca.central.cranfield.ac.uk/ethos-oai/2.0/" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:dcterms="http://purl.org/dc/terms/" xmlns:uketdterms="http://naca.central.cranfield.ac.uk/ethos-oai/terms/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:doc="http://www.lyncode.com/xoai" xsi:schemaLocation="http://naca.central.cranfield.ac.uk/ethos-oai/2.0/ http://naca.central.cranfield.ac.uk/ethos-oai/2.0/uketd_dc.xsd">
   <dc:title>Laser diagnostics of soot in hydrocarbon diffusion flames</dc:title>
   <dc:identifier xsi:type="dcterms:DOI">10.17863/CAM.56369</dc:identifier>
   <dc:creator>Tian, Bo</dc:creator>
   <dcterms:abstract>Driven by the demand for soot-free combustion, laser-based diagnostic techniques&#xd;
on soot have been developing since the late 1980s. One of these techniques is line-of-&#xd;
sight extinction, which is a fast, low-cost, and quantitative method to investigate&#xd;
the soot volume fraction in flames. However, the extinction-based technique&#xd;
suffers from relatively high measurement uncertainty due to a low signal-to-noise&#xd;
ratio, as the single-pass attenuation of the laser beam intensity is often insufficient. &#xd;
Multipass techniques can increase the sensitivity, but may suffer from a low&#xd;
spatial resolution. To overcome this problem, in the present study, we have developed&#xd;
a high spatial resolution continuous wave laser-cavity extinction (CW-LCE)&#xd;
technique to measure the soot volume fraction from low-soot producing flames.&#xd;
A laser beam cavity is realised by placing two partially reflective concave mirrors&#xd;
on either side of the laminar diffusion flame under investigation. This con guration&#xd;
makes the beam convergent inside the cavity, allowing a spatial resolution&#xd;
within 200 um, whilst increasing the absorption by an order of magnitude. Three&#xd;
different hydrocarbon fuels are tested: methane, propane and ethylene. The measurements&#xd;
of soot distribution across the flame show good agreement with results&#xd;
using laser-induced incandescence (LII) in the range of the soot volume fraction&#xd;
from 20 ppb to 15 ppm. The system is further applied to the measurement of soot&#xd;
volume fraction pro les of a series of nitrogen-diluted methane diffusion flames.&#xd;
The results of CW-LCE agree well with LII. The effect of fuel dilution on soot is&#xd;
interpreted by using a numerically calculated flow velocity and temperature  eld.&#xd;
It is found that a previous one-step model for soot formation may underestimate&#xd;
the suppression effect by dilution. This is because diluent addition may shift the&#xd;
location of the sooting region away from the high temperature region, shortening&#xd;
the residence time for surface growth of soot particles. The effect of each factor&#xd;
(thermal, dilution, residence time) responsible for soot reduction is isolated and&#xd;
quantitatively compared.&#xd;
&#xd;
The size of soot particles is another important aspect of comprehensive soot&#xd;
measurement, and to address this aspect, a planar two-dimensional two-colour&#xd;
time-resolved laser-induced incandescence (2D-2C-TiRe-LII) method is developed&#xd;
and employed to investigate the soot formation in a series of standard ethylene&#xd;
and methane laminar diffusion flame. The time resolution of the 2D-LII signal&#xd;
is realised by shifting the delay time of the ICCD cameras. A two-colour con-&#xd;
 guration is applied to measure the peak temperature of soot particles after the&#xd;
laser pulse, rather than use the energy balance equations to compute the peak&#xd;
temperature, which may introduce signi cant uncertainty. By combining with&#xd;
the CW-LCE technique, both a soot particle volume fraction and a particle size&#xd;
distribution map of the flame are obtained, using a minimum error approach.</dcterms:abstract>
   <uketdterms:institution>University of Cambridge</uketdterms:institution>
   <dcterms:issued>2016-11</dcterms:issued>
   <dc:type>Thesis</dc:type>
   <uketdterms:qualificationlevel>doctoral</uketdterms:qualificationlevel>
   <uketdterms:qualificationname>PhD</uketdterms:qualificationname>
   <dc:language>en</dc:language>
   <dcterms:isReferencedBy xsi:type="dcterms:URI">https://www.repository.cam.ac.uk/handle/1810/309271</dcterms:isReferencedBy>
   <dc:identifier xsi:type="dcterms:URI">https://apollo8-f-pro.lib.cam.ac.uk/bitstreams/28b1c64a-7741-45f4-aae0-e96afd287539/download</dc:identifier>
   <uketdterms:checksum xsi:type="uketdterms:MD5">ed558da333e4928e7555a6b098d82576</uketdterms:checksum>
   <dcterms:license>https://apollo8-f-pro.lib.cam.ac.uk/bitstreams/7840ae1a-6e7e-4068-9e16-9cbcc1d7e20b/download</dcterms:license>
   <uketdterms:checksum xsi:type="uketdterms:MD5">87eda9de84448d1f82354d60eee3eb5f</uketdterms:checksum>
   <dc:rights>https://www.rioxx.net/licenses/all-rights-reserved/</dc:rights>
   <dc:subject>hydrocarbon</dc:subject>
   <dc:subject>flames</dc:subject>
</uketd_dc:uketddc>
</metadata></record></GetRecord></OAI-PMH>