Laser Ignition System For IC Engine.

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Acknowledgement
I would like to take this opportunity to express our deep sense of
gratitude and respect to our project Guide Prof. V. B. Labhane, Lecturer in Mechanical
Engineering. It was great privilege to get this constant inspiration and guidance to complete
project in every respect.
I also extend word of thank to Prof.H.G. Fakatkar , Head of
Mechanical Engineering and to all our department Teaching and Non- Teaching Staff
members, who each time, stood behind to support and help us.
I am thankful to beloved, Prof.R.M.Jalnekar for providing all
necessary facilities and encouraging us throughout the project work.
I am highly obliged to our parents and entire friends group providing the way in difficult
times.
Suraj P. Darokar
(132160)

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List Of Figures
List Of Tables
Sr. No. Description Page No.
1. Technical Data Of Solid State Laser 13
2. Technical Key Data Of Test Engine 14
3. Estimated basic cost and performance requirements for
a laser spark plug
34
Sr. No. Description Page No.
1.3 Conventional SI System Of IC Engine 9
1.4 Processes In Laser Ignition 11
2.2 C/S Of The Engine Made For Laser Ignition 13
2.4 Working Of Lis With ND-Yag Laser 15
3.1.1.a Pressure History In Combustion Bomb With Lower Pulse 18
3.1.1.b Pressure History In Combustion Bomb With Higher Pulse 19
3.1.2 Schlieren Photographs Of Laser Ignition 20
3.2.2 Cold start performance with soiled combustion bomb
window
22
3.2.3.a Misfire Rate & Comparison of optics 24
3.2.3.b Influence of the energy on burn off performance 24
3.2.3.c Comparison Laser Energy Of Optics 25
3.2.3d Comparison Of Energy Density Of Optics 25
6.a Effects Of Chamber Pressure On Emin For Laser Ignition 29
6.b Pressure Traces After The Combustion Initiation By Laser 30
6.c Cylinder Pressure Traces At Two Different Air/Fu 31
6.d COV Of IMEP At Three Different Ignition Timing 32

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Nomenclature
i. IMEP - Indicated Mean Effective Pressures
ii. COV – Coefficient Of Variation
iii. SIS – Spark Ignition System
iv. LIS – Laser Ignition System
v. IC Engine – Internal Combustion Engine
vi. µs - Nano Second
vii. Mj – Milli-Joule
viii. Mpa – Mega Pascal
ix. MPI – Multi Photon Ionization
x. DOHC - Double-Overhead-Camshaft
xi. PPM - Particles Per Million
xii. CH4 - Methane
xiii. CO2 - Carbon Dioxide
xiv. NO X - Oxides Of Nitrogen
xv. λ - Air/Fuel Equivalence Ratio
xvi. MEP - Mean Effective Pressure
xvii. Is - Build-Up Intensity
xviii. Es - Build-Up Energy
xix. MPE - Minimum Pulse Energy For Ignition

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Content
Sr. No Description Page No
i. Acknowledgment 1
ii. List Of Figures & Tables 2
iii. Nomenclature 3
iv. Abstract 5
v. Introduction 6
1. What Is Laser? 7
1.1 How Does A Laser Work? 7
1.2 Types Of Laser 8
1.3 Alternative Ignition Systems 8
1.4 Laser Ignition 10
2. Experimental 12
2.1 Laser Ignition And Concurrent Schlieren
Photography In A Combustion Bomb
12
2.2 Laser Ignition In An Internal Combustion Engine 12
2.3 Laser Testing 14
2.4 How LASER Ignition Works? 14
2.5 Why LASER Ignition? 15
3. Result & Discussion 17
3.1.1 Laser Ignition Of Hydrogen/Air Mixtures 17
3.1.2 Laser Ignition Of Biogas/Air Mixtures 19
3.2 Engine Tests 21
3.2.1 Optics Deposits And Self-Cleaning Effect 21
3.2.2 Laser Self-Cleaning With Deposits Caused By The
Combustion Process
21
3.2.3 Laser Self-Cleaning With “Worst Case” Deposits 22
3.2.4 Properties Of The Optical Window 26
4. Comparison Of LI system with SI system
5. Advantages & Disadvantages of LIS
6 Application Of LIS
7. Future Scope & Current Status 27
8. Conclusion 28
9. References 29

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Abstract
Motive : To test the fuel consumption and emissions of IC engine with use of laser
ignition system and optimize the engine performance.
Method : Test data is collected from experiments conducted by various organizations. The
performances of IC engines with laser ignition were compared in terms of indicated mean
effective pressures (IMEP), mass burn fraction duration and coefficient of variation (COV)
of IMEP, and COV of peak pressure location..
Key Result : Ignition-delay times are smaller and pressure gradients are much steeper
compared to conventional spark plug ignition. Laser ignition reduces the fuel consumption
by several percents. NOx emission can be reduced by significant amount.
Conclusion : On the whole it is concluded that on adequate development, LIS can bring a
revolution in IC engines replacing the conventional spark plugs. The most encouraging
result come out from this study is 20% exhaust reduction as compared to the conventional
spark plug. Also Laser ignition reduces the fuel consumption by several percents and can
effectively burn leaner mixtures. Considering the advantages associated with LI system
research should be accelerated.

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Introduction :
Laser ignition Laser ignition is an alternative method for
igniting compressed gaseous mixture of fuel and air. The method is based on laser devices
that produce short but powerful flashes regardless of the pressure in the combustion
chamber. Usually, high voltage spark plugs are good enough for automotive use, as the
typical compression ratio of an Otto cycle internal combustion engine is around 10:1 and in
some rare cases reach 14:1. However, fuels such as natural gas or methanol can withstand
high compression without self ignition. This allows higher compression ratios, because it is
economically reasonable, as the fuel efficiency of such engines is high. Using high
compression ratio and high pressure requires special spark plugs that are expensive and
their electrodes still wear out. Thus, even expensive laser ignition systems could be
economical, because they would last longer. Laser plugs have no electrodes and they can
potentially last for much longer.

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1. What is laser?
A laser is a device that emits electromagnetic radiation through a process of optical
amplification based on the stimulated emission of photons. The term ‘laser’ is
an acronym for Light Amplification by Stimulated Emission of Radiation. The emitted
laser is unique in its high degree of spatial and temporal coherence.
Spatial Coherence means a fixed phase relationship between the electric fields at different
locations across the beam. Typically it is expressed through the output being a narrow
beam which is diffraction-limited, also known as a "pencil beam." Laser beams can be
focused to very tiny spots, achieving a very high irradiance.
Temporal coherence means a strong correlation between the electric fields at one location,
but different times.
1.1 How does a laser work?
Lasers are monochromatic, meaning they are very orderly forms of light
that have only one wavelength and one direction. It all starts with the electrons. By sending
energy to a system we can achieve what is known as population inversion. This means that
there are more electrons in the excited states than those in the lower energy states. As one
electron releases energy (a photon), the other electrons strangely seem to communicate with
each other and also begin releasing photons. This chain reaction of releasing photons is
called stimulated emission. The problem now is that these photons are released in random
directions. In order to make sure this energy is all forced in the same direction, mirrors are
strategically placed within a laser to direct the photons. The photons are directed by
bouncing back and forth between the mirrors, hitting each other and causing more
stimulated emission. So, by having Population Inversion, Stimulated Emission, Strategic
Planting of Mirrors. We get Monochromatic, Directional, and Coherent light.
1.2 Types of laser :
i. Gas
a. A Helium-Neon (HeNe) used mostly for holograms such as laser printing.
ii. Chemical

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a. Lasers that obtain their energy through chemical reactions. Used mostly for
weaponry.
iii. Dye
a. Uses organic dye as the lasting medium, usually in the form of a liquid
solution. Used in medicine, astronomy, manufacturing, and more.
iv. Solid-state
a. Uses a gain medium that is a solid (rather than a liquid medium as in dye or
gas lasers). Used for weaponry
v. Semiconductor
a. Also known as laser diodes, a semiconductor laser is one where the active
medium is a semiconductor similar to that found in a light-emitting diode.
b. Applications include telecommunication and medicine.
1.3 Alternative ignition systems
The protection of the resources and the reduction of the CO2 emissions
with the aim to limit the greenhouse effect require a lowering of the fuel consumption of
motor vehicles. Great importance for the reduction lies upon the driving source. Equally
important are the optimization of the vehicle by the means of a reduction of the running
resistance as well as a low-consumption arrangement of the entire power train system. The
most important contribution for lower fuel consumption lies in the spark ignition (SI)
engine sector, due to the outstanding thermodynamic potential which the direct fuel
injection provides. Wall- and air-guided combustion processes already found their way into
standard production application and serial development, whereas quite some fundamental
engineering work is still needed for combustion processes of the second generation.
Problems occur primarily due to the fact that with conventional spark ignition the place of
ignition cannot be specifically chosen, due to several reasons. By the means of laser
induced ignition these difficulties can be reduced significantly.
The combination of technologies (spray-guided combustion process and
laser induced ignition) seems to become of particular interest, since the ignition in the fuel
spray is direct and thus the combustion initiation is secure and non-wearing. The engine

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tests in this paper are on laser ignited, spray-guided combustion. Another approach is laser
ignition of a homogeneous mixture. Within the scope of this paper, laser ignition in
homogeneous fuel/air mixtures was investigated in a combustion bomb without turbulence.
In other alternative ignition systems than laser ignition are reviewed. Laser
ignition, microwave ignition, high frequency ignition are among the concepts widely
investigated. In this article the basics of applied laser ignition, will be illustrated and it
potential compared to a conventional ignition system. The figure Shows the working.
Fig. 1.3. Conventional Spark Ignition System Of IC Engine.
1.4 Laser ignition
Laser ignition, or laser-induced ignition, is the process of starting
combustion by the stimulus of a laser light source. Basically, energetic interactions of a
laser with a gas may be classified into one of the
following four schemes as described in :
i. thermal breakdown

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ii. non-resonant breakdown
iii. resonant breakdown
iv. photochemical mechanisms
In the case of thermal interaction, ignition occurs without the
generation of an electrical breakdown in the combustible medium. The ignition energy is
absorbed by the gas mixture through vibrational or rotational modes of the molecules;
therefore no well-localized ignition source exists. Instead, energy deposition occurs along
the whole beam path in the gas. According to the characteristic transport times therein, it is
not necessary to deposit the needed ignition energy in a very short time (pulse). So, this
ignition process can also be achieved using quasi continuous wave (cw) lasers.
Another type, resonant breakdown, involves non-resonant multi-
photon dissociation of a molecule followed by resonant photo ionization of an atom. As
well as photochemical ignition, it requires highly energetic photons (UV to deep UV
region). Therefore, these two types of interaction do not appear to be relevant for this study
and practical applications.
In these experiments, the laser spark was created by a non-
resonant breakdown. By focusing a pulsed laser to a sufficiently small spot size, the laser
beam creates a high intensity and high electric fields in the focal region. This results in a
well localized plasma with temperatures in the order of 106 K and pressures in the order of
102 MPa as mentioned in . The most dominant plasma producing process is the electron
cascade process: Initial electrons absorb photons out of the laser beam via the inverse
bremsstrahlung process. If the electrons gain sufficient energy, they can ionize other gas
molecules on impact, leading to an electron cascade and breakdown of the gas in the focal
region. It is important to note that this process requires initial seed electrons. These
electrons are produced from impurities in the gas mixture (dust, aerosols and soot particles)
which are always present. These impurities absorb the laser radiation and lead to high local
temperature and in consequence to free electrons starting the avalanche process. In contrast
to multi photon ionization (MPI), no wavelength dependence is expected for this initiation
path. It is very unlikely that the first free electrons are produced by multi photon ionization

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because the intensities in the focus (1010 W/mm2) are too low to ionize gas molecules via
this process, which requires intensities of more than1012 W/mm2.
An overview of the processes involved in laser-induced ignition
covering several orders of magnitude in time is shown in Fig. 1. Laser ignition encompasses
the nanosecond domain of the laser pulse itself to the duration of the entire combustion
lasting several hundreds of milliseconds. The laser energy is deposited in a few
nanoseconds which leads to a shock wave generation. In the first milliseconds an ignition
delay can be observed which has a duration between 5 – 100 ms depending on the mixture.
Fig. 1.4. Scope of timescales of various processes involved in laser-induced ignition: The
lengths of the double arrowed lines indicate the duration ranges of the indicated processes

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2. Experiment
This section describes the experimental setup. Laser ignition experiments
were carried out in a constant volume vessel (0.9 l) and an internal combustion engine. The
constant volume vessel, also termed the combustion bomb, was used to conduct basic
studies of laser ignition in homogeneous fuel/air mixtures. The sustainable fuels hydrogen
and biogas were used. The biogas was obtained from a municipal water purification plant. It
was composed of 50.5% CH4, 31.7% CO2 and 80 ppm H2S. Schlieren photography was
used for accompanying optical diagnostics. The engine, a one-cylinder research engine, was
deployed for the investigation of spray guided combustion initiated by a laser. Gasoline
was used as a fuel here. The focus of sustainability is on laser ignition for enhanced
combustion and efficiency.
2.1 Laser ignition and concurrent Schlieren photography in a combustion bomb
The laser ignition experiments in the constant volume vessel were
carried out with hydrogen and biogas. The experimental setup and tests with methane are
outlined in. A pulsed Nd:YAG laser with pulse energies from 1 to 50 mJ was used for the
ignition tests. Table 1 lists the specifications of the laser. Schlieren photography was
conducted in the plane of the focal spot of the igniting laser. Perpendicularly to the igniting
laser beam, a collimated light beam from a flash lamp (1 μs pulse duration) was shone
through the combustion vessel. As the diffraction index of light depends on the type and
mass density of a gas, areas with different temperatures or different pressures have different
diffraction indices. So a parallel beam of light is diffracted at differences of temperature
and pressure and the diffraction angle is proportional to the first derivate of these
parameters . The experimental setup for the Schlieren experiments is outlined in.
2.2 Laser ignition in an internal combustion engine
A one-cylinder research engine was used as a test engine. The research
engine was equipped with a four-valve DOHC cylinder head with a spray-guided
combustion system of AVL List GmbH . In a double-overhead-camshaft (DOHC) layout,
one camshaft actuates the intake valves, and one camshaft operates the exhaust valves.

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Gasoline was used as a fuel. Engine test runs were carried out with two different
approaches. First, a plane window was inserted into the cylinder head of the engine. A
focusing lens was placed in front of that window in order to focus the laser beam down into
the combustion bomb (“separated optics”). Second, a more sophisticated window was
deployed. A lens like curvature was engraved directly into the window. By using such a
special window, no further lens was required (“combined optics”). This is depicted
schematically in Fig.2.2.
Fig 2.2. Schematic cross section of the engine for laser ignition test runs. Two window/lens
configurations were tested: Fig. 2.2(a) shows the separated optics, Fig. 2.2(b) the combined
optics.
Table No – 1: Technical data of the laser. A solid-state laser was used here.
One-cylinder research engine
Four-valve cylinder head
Spray-guided combustion process
Multi-hole injector
Stroke 85 mm
Bore 88 mm
Displacement volume 517 cm3
Compression ratio ε 11.6

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Table No – 2: Technical key data of the test engine. A spray-guided research engine
running on gasoline was used.
Flash lamp pulsed Nd:YAG laser
Manufacturer Quantel Quantel S.A.
Type Brilliant
Wavelength 1064 nm or 532 nm
Pulse energy 1-50 mJ
Pulse duration 6 ns
Max. beam performance 10 W
Power consumption 1 kW
Beam diameter 6 mm
2.3 Laser Testing:
i. A one-cylinder research engine was used as a test engine.
ii. The research engine was equipped with a four-valve DOHC cylinder head with a
spray-guided combustion system of AVL List GmbH.
iii. Engine test runs were carried out with two different approaches:
First, a plane window was inserted into the cylinder head of the engine. A focusing lens
was placed in front of that window in order to focus the laser beam down into the
combustion bomb (“separated optics”). Second, a more sophisticated window was
deployed. A lens-like curvature was engraved directly into the window. By using such a
special window, no further lens was required (“combined optics”).
From the point of view of components development, the main goal is the
creation of a laser system which meets the engine-specific requirements. Basically, it is
possible to ignite mixtures with different types of lasers.
2.4 How LASER ignition works?
The laser ignition system has a laser transmitter with a fiber-optic cable powered
by the car’s battery. It shoots the laser beam to a focusing lens that would consume a much
smaller space than current spark plugs. The lenses focus the beams into an intense pinpoint
of light, and when the fuel is injected into the engine, the laser is fired and produces enough
energy (heat) to ignite the fuel.

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Below is a diagram of the laser arrangement:
Fig.2.4. Working Of Laser Ignition System with ND-YAG LASER.
2.5 Why LASER ignition?
i. Regulations on NOx emissions are pushing us toward leaner air/fuel ratios (higher
ratio of air to fuel).
a. These leaner air/fuel ratios are harder to ignite and require higher ignition
energies. Spark plugs can ignite leaner fuel mixtures, but only by increasing
spark energy. Unfortunately, these high voltages erode spark plug electrodes
so fast, the solution is not economical. By contrast, lasers, which ignite the
air-fuel mixture with concentrated optical energy, have no electrodes and are
not affected.
ii. Natural gas is more difficult to ignite than gasoline due
to the strong carbon to hydrogen bond energy.
a. Lasers are monochromatic, so it will be much easier to ignite natural
gases and direct the laser beam to an optimal ignition location.
iii. Because of the requirement for an increase in ignition energy, spark plug life will
decrease for natural gas engines.

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a. Laser spark plug ignition system will require less power than traditional
spark plugs, therefore outlasting spark plugs.
iv. Ignition sites for spark plugs are at a fixed location at the top of the combustion
chamber that only allows for ignition of the air/fuel mixture closest to them.
a. Lasers can be focused and split into multiple beams to give multiple ignition
points, which means it can give a far better chance of ignition.
b. Lasers promise less pollution and greater fuel efficiency, but making small,
powerful lasers has, until now, proven hard. To ignite combustion, a laser
must focus light to approximately 100 giga watts per square centimeter with
short pulses of more than 10 milli joules each.
c. Japanese researchers working for Toyota have created a prototype laser that
brings laser ignition much closer to reality. The laser is a small (9mm
diameter, 11mm length) high powered laser made out of ceramics that
produces bursts of pulses less than a nanosecond in duration.
d. The laser also produces more stable combustion so you need to put less fuel
into the cylinder, therefore increasing efficiency.
e. Optical wire and laser setup is much smaller than the current spark plug
model, allowing for different design opportunities.
v. Lasers can reflect back from inside the cylinders relaying information such as fuel
type and level of ignition creating optimum performance.
vi. Laser use will reduce erosion.

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3. Result & Discussion :
3.1.1. Laser ignition of hydrogen/air mixtures
Given fig. depicts a pressure history of combustions for different mixtures
(λ) at an initial chamber temperature of 473 K and an initial pressure of 1 MPa. Comparable
pressure histories could be seen for higher initial pressures. λ is the so called air/fuel
equivalence ratio: λ < 1 signifies a fuel-rich mixture, whereas λ > 1 describes a fuel-lean
mixture. Between λ = 2.5 and 3.6 (14.4% and 10.4% H2) an oscillating pressure history
could be observed having a frequency in the lower kHz region which is the resonant
frequency of the combustion bomb . The oscillating combustion process is called knocking,
which means that the combustion propagates not only by a spherical flame front, starting
from the plasma but also that the mixture explodes at different locations in the end-gas
(unburned gas) as an effect of self ignition conditions . With “rich” hydrogen-air mixtures
(λ < 3.6) the flame propagates at a specific instant during the combustion time with sonic
velocity through the gas and produces high pressure and temperature values in the end-gas
region leading to auto ignition . This auto ignition process produces shock waves which are
reflected from the chamber walls and end in oscillations which can be observed in Fig3.1.1.
a. for a λ between 2 and 3.6. Knocking is very disadvantageous for engine applications.
Pressure histories for a constant gas mixture (λ = 3.5) and constant initial temperature (T =
473 K) but different initial filling pressures are plotted in Fig.3.1.1.b. The main result of
this diagram is that with higher initial pressures the minimum pulse energy for ignition
(MPE) is decreasing. Further on, it can be seen that with higher initial pressures, which
means higher energy contents in the combustion bomb, the peak pressures increases. Gas
mixtures with λ = 3.5 represent the leaner boundary where knocking starts, as depicted in
Fig. 3.1.1.b. Especially at this boundary knocking occurred
Only at lower filling pressures. With higher initial filling pressures no knocking could be
Observed. Richer gas mixtures only have a knocking combustion with no dependency on
the filling pressure. Figures are shown on next page.

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Fig.3.1.1.a. Pressure history in the combustion bomb after ignition applying minimum pulse
energy for ignition (MPE); λ = 1.8 - 5; initial temperature = 473 K, initial pressure = 1
MPa; If the air/fuel equivalence ratio (λ) is increasing (leaner mixtures), the peak pressure
is decreasing but the total combustion time is increasing.

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Fig.3.1.1.b Pressure history in the combustion bomb after ignition applying minimum pulse
energy for ignition (MPE); λ = 3.5, initial temperature = 473 K, initial pressure = 1 – 4.2
MPa; For higher initial pressures the peak pressure, ignition delay and total combustion
time is increasing but the minimum pulse energy for ignition (MPE) is decreasing.
3.1.2. Laser ignition of biogas/air mixtures
Biogas is CO2-neutral and can act as a promising alternative fuel having
a high availability. The two most common sources of biogas are digester gas and landfill
gas. Bacteria form biogas during anaerobic fermentation of organic matters. The
degradation is a very complex process and requires certain environmental conditions.
Biogas is primarily composed of CH4 (50-70%) and CO2 (25-50%). Digester gas is
produced at sewage plants during treatment of municipal and industrial sewage. Landfill
gas is obtained during decomposition of organic waste in sanitary landfills. When using

20
biogas as fuel one must also pay attention to several harmful ingredients such as H2S
polluting e.g. the catalytic converter of the engine or blocking the window of the laser (see
later for issues related to the window). With respect to laser ignition, biogas was compared
to methane. Fuel-lean biogas/air mixtures exhibit a slower combustion process resulting in
lower peak Pressure and flame emission compared to methane-air mixtures of similar air to
fuel Equivalence ratio. The reason for these results could be due to the presence of CO2 in
the biogas which reduces the burning velocity due to obstructing the flame propagation
during combustion. SO2 may also be responsible for the decreased burning rate of the
biogas/air mixtures reducing mainly the O-radical concentration to equilibrium state due to
the recombination of the O-radicals. In Fig.3.1.2.a, images of the developing flame kernel
in laser ignited biogas/air mixtures are depicted (see below). More details on laser ignition
of biogas/air mixtures can be found in.
Fig.3.1.2 Schlieren photographs of laser ignition, laser entering from the left side. The
images are 11.6 mm long and 9.15 mm high. Top row: Laser-induced spark and shock wave
in 25 bar air; From left to right: 500 ns, 1000 ns, 2000 ns, 3000 ns. Middle row: Laser-
ignition of H2/air mixtures at 25 bar, lambda 6.0; From left to right: 100 μs, 200 μs, 300 μs,
1000 μs. Bottom row: Laser-ignition of biogas/air mixtures at 25 bar, lambda 1.8; From left
to right: 100 μs, 900 μs, 1800 μs, 15000 μs.

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3.2 Engine tests
Engine tests were conducted to investigate the optical window with respect to
i. Durability of the optics (vibrations)
ii. Minimum ignition energy
iii. Wear and fouling properties of the inner window surface
The engine tests were conducted with gasoline. Whereas the focus of the previous tests and
ongoing work in a static combustion bomb was on the understanding of the ignition
process, the aim of the engine tests was to investigate the durability of the optical window.
3.2.1 Optics deposits and self-cleaning effect
As stated above, laser ignition is based on the principle of optical breakdown and thus it is
essential to provide the necessary intensity which is approximately 1011 W/cm2 in the
focus. The energy emitted from the laser is attenuated by reflections on the surface of the
window and the lens and by absorption in the lens, in the combustion-chamber window and
in the deposits on the windows. The transmission of typical windows in the infrared is
approximately 90%; the reflections on the surfaces further reduce the energy. Adding it up,
when the laser beam passes through a window or a lens, the losses amount to approximately
15%. The laser self-cleaning effect was studied with deposits from the “true” combustion
process, and also with artificially applied deposits.
3.2.2 Laser self-cleaning with deposits caused by the combustion process
Fig. 3.2.2. shows the cold start performance of the engine with a soiled window. Here, the
deposits stemmed from a real combustion process inside the engine. These deposits, which
were caused by the combustion process, were built up during the tests with a conventional
spark plug. Thereby the combustion-chamber window was installed in
Different load points, the engine running mode being homogeneous, for about 20 hours. As
it can be seen in Fig. 3.2.2., the window was soiled with a dark and opaque layer of
combustion deposits after these 20 hours. In the simulated cold-start test with a stratified
engine running mode with 1000 rpm (rotations per minute) and pMEP = 1 bar, the pMEP
course was recorded for each cycle, as shown in Fig. 3.2.2. (MEP = mean effective

22
pressure). The first ignition and injection impulse occurred at cycle 10. The first laser
impulse already ignites the mixture. The following ignition impulses resulted in a running
without misfire. After the test (100 cycles) the window was disassembled and, as visible in
Fig. 3.2.2., all deposits were removed in the beam passage area.
Fig.3.2.2. Cold start performance with soiled combustion bomb window – deposits because
of engine-related combustion process.
3.2.3 Laser self-cleaning with “worst case” deposits
In order to study the effect of the laser on a heavily soiled window, it was chosen to
artificially apply a layer of dirt onto the window. This artificially applied soiling on the
combustion-chamber side of the window represents a kind of “worst case scenario”.
For doing so, a mixture of Diesel soot and waste oil at a ratio of 1:5 was produced and, with
a thickness of 1 mm, applied to the combustion-chamber window and afterwards dried. Fig.
3.2.3.a shows the clear influence of the laser energy on the self-cleaning effect of the optics.
Up to a build-up energy of the threshold energy ES, an engine operation without misfire is
possible with a separated optics configuration, presupposed that a corresponding pulse
number for the burning-off of the window is shot. This build-up energy ES is significantly

23
higher in combined optics when aiming to reach a misfire rate of 0%. The relative laser
energy was replaced by the actually occurring relative energy intensity I on the combustion
chamber side of the window in Fig. 3.2.3.b.
An engine operation without misfire with both optics configurations, i.e. separated and
combined optics (see Fig 3.2.3.c.), is possible as of a build-up intensity of IS. In separated
optics this build-up intensity IS corresponds to the build-up energy of ES. However, the
minimum intensity for keeping the combustions-chamber window clean during the engine
running is IS/2. The minimum ignition energy when the engine running is stationary is
determined by the intensity level of self-cleaning at the optics, and not by the engine-related
working process. In the whole engine operating map a secure ignition and self-cleaning of
the optics can be guaranteed with the laser energy ES. For cold start applications, the laser
energy should thus be raised momentarily in order to burn off possible deposits at the
optics. Fig.3.2.3.c. shows the laser energy for the different window configurations (compare
Fig. 2.2). Both the minimum ignition energy (left bar) and the laser energy for a 20 hour
test run (right bar) are shown. As it can be clearly seen, the combined optics are more
favorable than the separated optics with respect to required laser energy. The energy density
at the window is a major criterion for the ablation of combustion bomb deposits. During
cold start, heating up and in the case of existing deposits only a high laser energy density
can ensure the ablation effect at the location of the laser. The energy density is therefore an
important determinant on the reliability of a future laser ignition system. As it can be seen
from Fig. 3.2.3.d, the energy density is by an order of magnitude higher for the separated
optics than for the combined optics for the chosen configuration. The separated optics
scheme leads to a higher energy density at the window. Especially in the case of cold start
or unexpected deposits, this setup should be more reliable than the combined optics. As can
be seen from Fig.3.2.3.c. and Fig. 3.2.3.d, there is a trade-off between low laser energy
requirements (combined optics) and system reliability (separated optics). From an engine
manufacturer’s point of view, system reliability comes first, which translates into higher
required laser energies and hence higher system costs.

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Fig.3.2.3.a. Misfire rate dependent on the relative laser energy in a simulated cold start test,
comparison of the optics, worst case deposits.
Fig.3.2.3.b. Influence of the energy intensity I at the combustion bomb window on the burn
off performance and the misfire rate, worst case deposits.

25
Fig.3.2.3.c. Laser energy for ignition as a function of different window configurations. The
separated optics, i.e. a focusing lens before a window, is less favorable than a combined
optics, i.e. a window with integrated lens curvature, with respect to the minimum ignition
energy.
Fig.3.2.3.d. Energy density at the window. It is higher for the separated optics. The higher
the energy density, the better ablation works. The separated optics scheme should therefore
be more reliable than the combined optics.

26
3.2.4 Properties of the optical window
Potential window materials evidently have to be transparent for the laser radiation. The
laser used in these tests was a Nd:YAG laser at 1064 nm. The near infrared spectral region
is a common wavelength region for laser suitable for laser ignition test runs. So infrared
transparent windows are good candidates for a future laser ignition system.
The second, no less important prerequisite is that the window withstand the high energy
density of the laser. The shorter the focal length of the lens, the higher generally the laser
light intensity of the passing laser beam becomes at the window surface. Third, the window
must show a weak inclination to deposits and aid laser self-cleaning. Combustion bomb
deposits can either be organic (up to 300°C) or inorganic in nature. When they form on the
window, they increasingly block the incoming laser light up to a point where no breakdown
can be produced any more. For instance, laser ignition tests of methane/air mixtures in an
engine had to be aborted after 1.25 hours because of excessive combustion product build-
up. ZnSe was used in that study. The formation of deposits on the window depends on the
temperature, the fuel and the engine oil.
The laser light also interacts with deposits. By a process called laser cleaning or ablation,
deposits are removed by the laser light. The contrary can also happen, i.e. that the laser
fosters the formation of deposits at the location where it enters the combustion chamber.
Generally, ablation overweighs so that a kind of self-cleaning effect as shown above is
achieved by the laser. Sapphire, quartz and ZnSe are among potential window materials in a
future laser ignited engine. reviews the major infrared transparent substrates suitable for
window fabrication.

27
4. Comparison Of LI system with SI system:
Fig. 4.a. Ignition of a/f mixture with LI system
Fig. 4.b. Ignition Of a/f mixture with SI system
ignition reliability of laser ignition
A/F rel ( )
1,40 1,50 1,60 1,70 1,80 1,90 2,00 2,10 2,20 2,30
pinit(bar)
10
15
20
25
30
35
40
0,00
0,25
0,50
0,75
1,00
ignition reliability of spark plug ignition
A/F rel ( )
1,40 1,50 1,60 1,70 1,80 1,90 2,00 2,10 2,20 2,30
pinit(bar)
10
15
20
25
30
35
40
0,00
0,25
0,50
0,75
1,00

28
5. Advantages & Disadvantages of LIS
Advantages
i. Lasers promise less pollution
ii. The laser also produces more stable combustion so you need to put less fuel into the
cylinder, therefore increasing efficiency.
iii. Optical wire and laser setup is much smaller than the current sparkplug model,
allowing for different design opportunities.
iv. Lasers will reduce erosion.
v. easier possibility of multipoint ignition.
vi. shorter ignition delay time and shorter combustion time.
vii. absence of quenching effects by the spark plug electrodes.
viii. Lasers can reflect back from inside the cylinders relaying information such as fuel
type and level of ignition creating optimum performance.
Disadvantages
i. high system costs
ii. concept proven, but no commercial system available yet.

29
6. Laser Ignition Applications
An observed advantage of the laser ignition over the electric spark
ignition method is the reduction of the Emin as the charge pressure is increased. For
example, a nine-fold decrease in Emin was observed as pressure was raised from 1 to 10
bars for methane/air mixture, see Fig. 6.a. Kopecek et al. (2000) showed that the use of
optimized optics and laser systems can reduce the required minimum laser pulse energy for
the ignition to where the application of the laser becomes reasonable. A minimum useful
focal spot size of 20 μm was found to be independent of the laser wavelength.
Fig. 6.a. Effects of chamber pressure on Emin for laser ignition. Kopecek et al. (2000).
Use of lasers for ignition purposes at three different wavelengths in a
constant volume bomb was demonstrated by Ma et al. (1998) and results were compared
with those obtained by an electric spark system. Lower combustion times and higher early
flame speeds were measured for the laser ignition system. Figure 6.b. shows a comparison
of the pressure traces when combustion is initiated by different ignition methods. They also
showed that equivalence ratio, initial temperature, initial pressure, and ignition location
were all significant in determining the combustion duration, peak heat release, peak

30
pressure, and flame speed, whereas ignition energy was not. Finally, laser ignition exhibited
smaller cycle-to-cycle
variations during the early combustion phase than those with the electric spark plug.
Fig. 6.b. pressure traces after the combustion initiation by laser (three wavelengths) and
electric
discharge with spark plug. Maetal. (1998).
One of the earliest application of the laser ignition in a gasoline
engine was demonstrated by Dale et al. (1978). They reported that the laser ignition was
able to ignite a leaner mixture and that the pressure rise time was shorter compared to an
electric ignition unit. However, the smaller pressure rise time led to a higher emission of the
nitric oxide (NO). In particular, the use of laser increased the peak cylinder pressure by 5%
and 15%, without the exhaust gasrecirculation (EGR) and with 16% EGR, respectively.
Additionally, they found that the CO and HC emissions were comparable for the two
ignition systems. Figure 6.c. shows samples of their reported results. It indicates the so-
called tradeoff between the specific fuel consumption and NO emissions for the two
ignition systems. It is clear that for a given level of NO emission, the laser ignition system
offers a superior fuel economy than the spark plug system. Regarding the window fouling,
the authors reported that carbon deposit build-up made it necessary to remove the window
for cleaning every 30 to 75 minutes of operation.

31
One of the most promising near-term applications of the laser
ignition is for large lean-burn natural gas engines. Regulations on NOx emissions have
continued to force operation of natural gas engines to leaner air/fuel ratios. Engine
operation under the lean fuel/air mixtures using a spark plug ignition is limited because of
the misfire and unstable operation.
Fig.6.c. Cylinder pressure traces at two different air/fuel (A/F) mass ratios for laser and
standard (STD) ignition systems. Dale et al. (1978).
Additionally, ignition of the lean mixture is difficult and conventional systems require high
ignition energies. High energies are usually achieved through an increased ignition coil
energy. However, this measure tends to rapidly burn out even the precious metal spark
plugs

32
utilized in stationary engines for power generation. Also, natural gas is more difficult to
ignitethan gasoline due to the strong C-H bond energy. Considering the foregoing, and the
recent availability of small-sized high-power solid-state rugged lasers, the near-future use
of the laser ignition in this application is promising. Figure 6.d. shows the coefficient of
variation (COV) of the indicated mean effective pressure (IMEP) from a single-cylinder
lean-burn natural gas engine using two ignition, systems (electric and laser) for power
generation, see McMillan et al. (2003). A much lower COV 7 values are seen with the laser
especially when the ignition timing is retarded to 15 degrees before top dead center
(BTDC). Similarly, 0-to-10% mass burn duration was also reduced with laser ignition
indicating accelerated combustion in the early development phase. In this study, a Q-
switched Nd;YAG laser with 10 ns pulse is used at 1064 nm with 60 to 180 mJ/pulse of
energy. They reported no issues with vibration or with combustion products fouling the
sapphire window installed on the engine for the laser beam.
Fig.6.d. Coefficient of variation of the IMEP at three different ignition timing. Results are
shown for three different equivalence ratios (phi). McMillan et al. (2003).

33
7. Future Scope & Current Status
From the perspective of dwindling oil resources laser ignition system
is good as it reduces the fuel consumption. From the environmental point of view it is very
significant since it considerably reduces the emission. Seen as the current best alternative
to conventional sparkplug ignition system.
Some of leading institutes and organizations researching and came
with adaptive results are
i. University of Liverpool in collaboration with Ford Motor Company
ii. National Energy Technological laboratory, United States of America
iii. Colorado State University,
iv. National Institutes of Natural Sciences-Japan, etc.
The leading automobile companies that are developing laser
ignition system for their vehicles are:
i. Ford Motor Company
ii. Mazda.
Practical Laser Sparkplug Requirements
The simplest and least costly laser ignition design architecture would consist of a compact
high peak power laser transmitter head, and a sapphire window/lens delivery system. The
sapphire window is a well proven and reliable method of providing a transparent bulkhead
seal on high pressure combustion chambers such as gas engine cylinder heads and the
breeches of 155mm howitzers. BMLIS (Breech Mount Laser Ignition System) lasers,
mounted directly on to the breech of large cannons, have over the last 20 years proven to be
more reliable than fiber optic laser beam delivery systems . In these laser applications the
laser window “self cleaning” or “burning free” effect is well known . This is a laser
ablation effect where ignition residue that collects on the window surface is blown free and
clear of the optical aperture with each laser pulse.

34
Many BMLIS, ARES and ARICE researchers are reaching the same conclusions about the
attractiveness and dependability of direct fire laser ignition designs. Estimated basic cost
and performance requirements for a practical laser spark plug are listed in table 3.
Table 3. Estimated basic cost and performance requirements for a laser spark plug
Mechanical Laser and mounting must be hardened against shock and vibration
Environmental Laser should perform over a large temperature range
Peak Power Laser should provide megawatts raw beam output
Average Power 1-laser per cylinder requires 10Hz for 1200rpm engine operation
Lifetime 100 million shots – good, 500 million shots - better
Cost(ARES) Laser cost less than $3,000 each (100M pulse life ~ break even)
Cost (Auto) Laser cost less than $600 each
The cost values shown for the natural gas engine laser spark plug
are based upon the estimated operational costs of an 800 Kilowatt 16-cylinder Waukesha
engine operating at 1200rpm with 16 lasers (one for each cylinder). At 1200 rpm the laser
operates 24 hours a day, 365 days a year at 10 Hz (1200 rpm/2 strokes/ 60sec/min) for a
total of approximately 315M pulses per year. The natural gas fuel consumption cost
estimation for this engine is based upon $10MMBtu, $65.00/hr equal to approximately
$569,000 per year [10]. Replacement of a standard spark plug with a laser spark plug
provides an estimated 40% increase in fuel efficiency. Under these conditions, the laser
spark plug requires $46.00/hr in fuel consumption. This translates into cost savings of
approximately $174,000 per year. Laser replacement cost (materials only) is estimated at
$144,000 (16 x $3000 each) x 3 times per year with an estimated 100M pulse lifetime. This
spark plug cost analysis indicates that laser lifetime is a key issue with regard to the
development of an economically viable (read practical) laser spark plug.
We may also envision smaller and less costly laser spark plugs for
use in common automobile and truck engines. These applications may make use of very
small low cost single emitter laser diodes to significantly reduce the laser spark plug
component cost. Diode laser pumps are the most costly element employed in traditional
side and end pumped DPSS Lasers. The diode lifetime is the limiting factor in the laser
lifetime.

35
8. Conclusion:
In this work, laser-induced ignition of hydrogen/air and biogas/air mixtures was
investigated experimentally in a static combustion bomb. An enhanced ignition source can
make a strong contribution to sustainability in internal combustion engines. Schifrin
photography was applied to gain information on the shock wave propagation and early
flame kernel development. Results and trends from the literature, predominantly existing in
the ambient pressure regime, could be verified. It was found for the laser ignition tests with
hydrogen that with higher initial pressures the minimum pulse energy for ignition (MPE)
decreases. That behaviour was also found for methane. Fuel-lean biogas/air mixtures
exhibit a slower combustion process resulting in lower peak pressure and flame emission
compared to methane-air mixtures of similar air to fuel equivalence ratio. The applicability
of the laser induced ignition as a future ignition system for combustion engines with spray-
guided combustion process could be proved with the basic research. The lowest required
ignition energy in a stationary engine running mode is defined by the intensity level of the
self-cleaning effect at the optics and not by the engine-related working cycle. In order to
prevent deposits on the optics by the combustion process, a certain build-up intensity IS has
to be available on the combustion bomb side of the window in order to ensure an engine
operation without misfire. The energy intensity necessary to keep the burnt off optics clean
during the normal engine operation is, however, lower. Half the build-up intensity IS has
proven to be sufficient in order to prevent deposits. From the point of view of components
development, the main goal is the creation of a laser system which meets the engine-
specific requirements. Basically, it is possible to ignite mixtures with different laser
systems. The concept with the greatest development potential regarding efficiency and
miniaturization is the diode pumped solid-state laser.

36
9. References:
i. http://www.laserist.org/Laserist/showbasics_laser.html
ii. http://www.wikihow.com/Laserign+principle/icengine
iii. http://www.dtic.mil/cgi-
bin/GetTRDoc?Location=U2&doc=GetTRDoc.pdf&AD=ADA427076
iv. http://www.maik.rssi.ru/full/lasphys/05/7/lasphys7_05p947full.pdf
v. http://www.carbontrust.co.uk/SiteCollectionDocuments/Grant%20Funded%20Proje
cts/075,%20076,%20077%20projects/076-
207%20University%20of%20Liverpool%20final%20PDF%20locked.pdf
vi. http://www.laserist.org/Laserist/showbasics_laser.html
vii. http://affleap.com/laser-ignition-system-to-replace-spark-plugs/

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