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HBRP Publication Page 1-9 2020. All Rights Reserved Page 1
Research and Applications of Thermal Engineering
Volume 3 Issue 2
A Review of HCCI Engine Using Alternative Fuels
Manish Kumar1, Piyush Jasooja
2
1Assistant Professor,
2 Graduate
Department of Mechanical Engineering, Bhilai Institute of Technology, Durg, India
*Corresponding Author
E-mail Id:[email protected]
ABSTRACT
In today’s day and age, automotive as an industry is actively exploring alternative
combustion phenomenon’s to substitute Spark Ignition (SI) and Compression Ignition (CI)
systems for Internal Combustion (IC) engines. With a distinctive set of features,
Homogeneous Charge Compression Ignition (HCCI) engines hold a promising position as a
feasible alternative, as besides low emissions of Nitrogen Oxides (NOx) and soot, HCCI also
ensures plausible merits of high volumetric efficiency. In principle, the combustion auto-
ignites at multiple spots once the mixture has reached its chemical activation energy as there
is no spark plug or injector to assist the combustion. The important challenges encountered
in developing HCCI engines are: (i) Uncontrolled combustion and Self-ignition of the
working fluid with fuel,(ii) the maximum pressure at high load operations,(iii) To rectify the
problem of cold starting,(iv) reaching the emission standards and (v) to control the
phenomenon of knocking. At low engine speeds, a probable early auto-ignition can lead to
knocking, while at high engine speeds, delay auto-ignition would make HCCI susceptible to
misfire. The emission levels are greatly reduces by hydrogen but renders reduced power.
However, lower NOx, CO and particulate matter (PM) emissions levels can be achieved by
combining hydrogen with diesel in dual-fuel mode, and the efficiency of the engine can be
increased. HCCI engines performance (i.e. emissions levels, brake thermal efficiency and
combustion phasing) is usually predicted by numerical methods, which are cost effective
compared to entirely relying on empirical data.
Keywords:-HCCI, Energy, Biofuels, Emission Standards, Alternative fuels
INTRODUCTION
An incorporation of characteristics of the
conventional gasoline and diesel engines is
made possible in HCCI. The nomenclature
is derived from the composition of influx
charge and the combustion process,
namely, HCSI in case of gasoline engines
(a union of homogeneous charge (HC)
and spark ignition (SI)) and SCCI in case
of modern direct injection diesel engines
(a union of stratified charge (SC)
and compression ignition (CI)). During
last decades, the two main concerns have
become prominent in the energy
generation and transportation sectors,
namely the increasing energy demand
coupled with the lim3ited availability of
oil reserves and the detrimental
environmental effect produced by their
exploitation to deliver energy and motion.
One major detrimental effect of the use of
fossil fuels is related to the environmental
impact from their use for energy
production and transportation. The fuel
combustion in internal combustion engines
produces – among others – CO2, a major
greenhouse gas that is known to contribute
to the global warming effect. The
production of CO2 is not the primary
concern, as the combustion of most fuels
leads to its production, but the fact that in
the case of fossil fuels, the CO2 emitted
cannot be reconverted to the original fuel
by any short-term, natural – and therefore
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Research and Applications of Thermal Engineering
Volume 3 Issue 2
energy neutral – process.
In an effort to gradually replace fossil
fuels, research has been guided towards
seeking alternative fuels to gradually
substitute conventional ones. Biofuels,
among them have gained increasing
attention due to their atypical qualities of
being renewable in nature and reducing the
net CO2 emissions. Furthermore, even
conventional diesel and gasoline engines
have utilized Biofuels as either neat fuels
or as supplements.
Moreover, besides the conventional
combustion modes, a relatively new
concept has been developing during the
last two decades, i.e. homogeneous charge
compression ignition combustion (HCCI).
In HCCI combustion, a mixture of fuel and
air is introduced into the combustion
chamber early during compression or
during the intake stroke. The mixture is
compressed and auto ignites at the point
where the local thermo- and fluid-dynamic
conditions are favourable [1]. The main
advantage of the HCCI concept relative to
conventional combustion modes is the
significant reduction of NOx emissions and
the absence of soot in the exhaust.
Moreover, the fast combustion usually
encountered and the unthrottled operations
are prone to yield high indicated thermal
efficiency. However, HC and CO
emissions are usually high due to bulk
quenching at low loads and wall
quenching and crevice flows at higher
loads [2].
Added to these unfavourable attributes of
HCCI is the inability to directly control the
combustion phasing in HCCI engines. This
is a major obstacle preventing the
implementation of the HCCI concept.
HCCI ignition relies heavily on chemical
kinetics and largely depends on the fuel
used. In an effort to control ignition and
the combustion rate, thereby expanding the
HCCI operation over a wide range of
load–engine speed, various means have
been used, such as variable compression
ratio, variable valve timing, variable inlet
temperature, internal or external EGR,
direct fuel injection, etc. [2].
The SI and CI engine have divergent
processes to achieve HCCI combustion in
an IC engine, while feeding the manifold
with premixed air-fuel mixture or by an
early infusion into the Direct Injectors (DI)
would result in a successful HCCI
combustion in the former, the CI
arrangement would require a rather higher
compression to attain an auto-ignition as a
consequence of notably higher degrees of
temperature. Anyhow, the limited
operating range of HCCI engines has been
a cause of constant concern as it has
detrimental effects on the engine, such as
knocking at high loads and speeds due to
enormous heat and pressure released and
misfire at low loads. [22].
A promising method for the combustion
control seems to be the use of alternative
fuels and fuel blends, depending on the
characteristics of the engine (compression
ratio, etc.) and the operating conditions [2–
4]. The main concept is that fuels with
different auto-ignition tendencies can be
blended at varying proportions to regulate
the ignition point at various load–speed
regions [26]. This is a fortunate evolution
since the fuels used in the blends may as
well be biofuels. Thus, hydrogen [4],
ethanol, ethers and biodiesel have been
used in HCCI engines, either as neat fuels
or in blends.
PERFORMANCE COMPARISON
Fuels Used in HCCI Engine An early or a chemically energetic auto-ignition causing an increase in the rate of combustion and in-cylinder pressures can potentially impair the Engine. For an auto-ignition, the reactants of the fuel air mixture should have sufficient concentrations and temperature required for ignition, as once triggered, auto-
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ignition occurs at an alarming rate. Using of any fuel which is highly volatile and easily mix with air before ignition, can be operated in HCCI engine [5]. As HCCI engines are largely governed by chemical kinetics, the important is that to deduct the fuel’s self-combustion point to establish smooth engine operation, i.e.; free from knocking and misfiring. Every fuel have different auto ignition point. The intake temperatures required for various fuels to auto-ignite at different compression ratios when operating in HCCI mode [5] is depicted in Figure 1. It can be seen that methane needs a high initial pressure, temperature and compression ratio to self-ignition. The auto-ignition point decreases when the number of carbon atoms in the hydrocarbon increases, as shown in Figure 1, where methane has the fewest possible carbon atoms, while iso-octane has the most of those shown. The lack of well-defined combustion initiator in HCCI engines undermines the ability of a direct control over combustion resulting in an uncontrolled or rather difficult control relative to other combustion engines. In regards with ignition in conventional engines, the gasoline engine uses a spark in combination with a premixed charge of fuel and air whereas the diesel engine is reliant on the injection of fuel into the pre-
compressed air. Unlike SI or CI engines, where definitive control measures for combustion timing are in place, the HCCI engine experiences combustion as and when sufficient temperature and pressure is achieved by the compression of homogeneous fuel and air mixture. Three blends of unleaded gasoline, a Primary Reference Fuel (PRF) blend of 95% iso-octane and 5% n-heptane (95RON), methanol and ethanol were used in a study [22] to ascertain the difference between alcohols and hydrocarbons on HCCI combustion. The findings suggested that although the RONs of all the gasoline were poles apart, there was still some resemblance in their behaviour. While alcohols achieved highest thermal efficiencies, the emission levels were minimal for NOx followed by further lower in methanol. As derived from an experimental study, the fuels with octane numbers having greater differences can be used to obtain higher values of torque. In this study, a high octane homogeneous air/fuel mixture (propane or hydrogen) was infused with a low octane fuel (n-heptane) right before the intake valve. Nonetheless, due to its poor self-ignition tendency, a part of the high-octane fuel does not participate in oxidation reactions resulting in increased hydrocarbon emissions [23].
Fig.1:-Intake temperature required for fuels to operate under HCCI mode with varying
compression ratios, reproduced from [20]
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Table 1:-Natural gas emissions levels compared to oil and coal (Pounds per billion Btu of
energy) [20] Pollutant Natural gas Oil Coal
Carbon dioxide 117,000 164,000 208,000
Carbon monoxide 40 33 208
Nitrogen oxides 92 448 457
Sulphur dioxide 0.6 1122 2591
Particulates 7.0 84 2744
Mercury 0.000 0.007 0.016
From Table 1, the rate of production of
pollutant, Carbon dioxide is observed to be
1.4 and 1.75 times higher than natural gas
in case of crude oil and coal respectively.
Additionally, Natural gas is more readily
available than crude oil, with a cost that
has been competitive for a while now [3].
Though, suffers reduced power output in
HCCI engines, it is able to operate as an
independent fuel in an IC engine with
fairly lower HC and CO emissions[4]. Its
higher auto-ignition point (about 810 K)
ensures a significant precedence over
diesel–natural gas operation by
simultaneously maintaining the high CR of
a diesel engine and lowering emissions. As
claimed by Duc and Wattanavichien [6],
engines can operate at a high CR due to
the high octane number of methane (about
120). Deriving from the results of a four-
stroke HCCI engine simulation, a less than
400 K intake temperature with 15:1
compression ratio, methane can’t ignite
[7].This is shown in Fig. 1, where auto
ignition of methane will take place only
with an initial temperature is less than 400
K when compression ratio is greater than
18:1.
Knocking is often experienced due to the
unstable nature of the only gas capable of
operating as a single fuel in an HCCI
engine, Hydrogen. Besides a homogeneous
intake charge on being premixed with air,
hydrogen also catalyses the diffusivity of
any gas in air to about 3–8 times faster
than natural gas. With an approximate
three folds higher (119.93 MJ/kg
compared to 42.0035 MJ/kg) net heating
value than diesel, self-ignition temperature
to initiate combustion is as high as (858 K)
for hydrogen. Due to its imperative
instability, hydrogen has been ruled out a
single fuel in an HCCI engine by most
researchers, rather it is being used as an
additive: either to control the ignition
timing or to increase the engine
performance.
Iso-octane, a surrogate fuel for gasoline
and n-heptane, a surrogate fuel for diesel
are used in HCCI engine experiments.
Primarily due to the complexity in
production, and a subsequent high
manufacturing costs, Alcohol-derived
fuels, as shown in Fig. 1, are not widely
used. The fact that alcohol-derived fuels
like biofuels are still subject to worldwide
investigations, is in due consideration of
the consistent clogging issues in the engine
arising by their use. Biofuels, in spite of
the numerous challenges, have managed to
gather eminent consideration as a
potential renewable source from
researchers worldwide.
Peak Pressure and Temperature
Due to the high sensitivity to temperature,
HCCI's auto-ignition and combustion
timing are subjected to being largely
influenced by the intake charge
temperature. In light of these events, its
effects on HCCI combustion on-set have
been widely reported by many researchers.
The use of resistance heaters to vary the
inlet temperature is a rather simple but
quite slow approach of temperature control
method to obtain a cycle-to-cycle
frequency variation. The in-cylinder peak
pressure and temperature are directly
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affected by the variations of heat release
rate during combustion. A directly
proportional relationship can be
established between load quantities (heat
release rate, temperature and pressure) and
the speed of the engine, equivalence ratio,
load, intake pressure, temperature and
energy content of the fuel configurations,
i.e., higher peak pressures are observed at
higher loads and richer mixtures. Table 4
gives an insight into the pattern of variance
among HCCI and conventional CI modes
in terms of the in-cylinder peak pressure
and temperature to evidently decide on the
mode that produces a higher peak.
Although the complete data for maximum
temperature is not reported, a general
conclusion drawn from the table can be the
proportional increase of pressure with rise
in temperature. The lower peak pressures
of HCCI configurations with respect to
conventional CI modes confirm significant
impacts on emission levels for every fuel
configuration. Addition of Hydrogen to
diesel causes a reduction in ignition delay
along with a directly proportional
influence on the peak pressure generation;
higher the addition, higher the peak
pressure [10]. A reasonable inference is
that the highest peak pressure along with
better power and efficiency values are
achieved with the hydrogen fuel
configuration.
Table 2:-In-cylinder peak pressure and temperature comparison for natural gas and
hydrogen in various configurations [8, 21] Mode Max pressure (MPa) Max temperature (K)
HCCI CI HCCI CI
H2 ~8 ~12 - -
NG ~7 ~7.5 ~1300 ~1850
Diesel ~6.1 ~6.6 - ~2300
NG+Diesel ~3 ~5.5 ~1450 -
H2+Diesel ~7 ~7.8 - -
Table 3:-Diesel Properties compared to hydrogen and natural gas. Properties Diesel Hydrogen Natural gas
Main component C12H23 H2 Methane (CH4)
Auto-ignition temperature (K) 553 858 923
Lower heating value (MJ/kg) 42.5 119.93 50
Density (kg/m3) 833-881 0.08 0.862
Molecular weight (g/mol) 170 2.016 16.043
Flammability limits in air (vol%) (LFL-UFL) 0.7-5 4-75 5-15
Flame velocity (m/s) 0.3 2.65-3.25 0.45
Specific gravity 0.83 0.091 0.55
Boiling point (K) 453-653 20.2 111.5
Cetane number 40-60 - -
Octane number 30 130 120
CO2 emissions 13.4 0 9.5
Diffusivity in air (cm2/s) - 0.61 0.16
Min ignition energy (mJ) - 0.02 0.28
Brake Thermal Efficiency
By definition, the brake thermal efficiency
(BTE) of an engine is the brake power
produced by an engine with respect to the
energy supplied by the fuel, but it is
represented as the ratio of brake output
power to input power. According to a
study, [8] the energy ratio of biogas and an
intake temperature of 80 1C, 100 1C and
135 1C, denotes the best BTE for biogas
fuels ranging from 40% to 57%. Anaerobic
fermentation of cellulose biomass
materials [6] was deployed to produce the
principal component of biogas, methane
(460%). 51% biogas and 135 1C intake
temperature were reported to be the best
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energy ratio with diesel and the optimum
efficiency respectively, in HCCI mode,
conclusively, the heat release rate and the
efficiency [8] are inversely proportional to
the energy ratios. However, with the
exception of BTE which was higher for
diesel running in CI mode even when
operated at the optimum biogas energy
ratio. According to a report by Duc and
Wattanavichien [6], diesel single fuel in
either HCCI or non-HCCI mode recorded
higher efficiencies than the biogas-diesel
running in dual-fuel non-HCCI. Hydrogen,
on the contrary, having an increased BTE
by 13–16%, recorded a higher BTE than
pure diesel in non-HCCI mode. reported
An addition of 5% hydrogen lead to a
further increase in BTE from 30.3% to
32% as reported by Szwaja and
GrabRogalinski [9]. The uniformity of
mixing of hydrogen could be the prime
cause of the reported increase of BTE in
hydrogen– diesel mode.
Exhaust Gas Emissions
The lower peak temperature encountered
in HCCI relative to that in SI and diesel
engines is due to the fact that it operates on
lean mixtures, which results in incomplete
burning of fuel near the combustion
chamber walls along with reduced NOx
formation. An oxidising catalyst in the
oxygen-rich exhaust is deployed to
eradicate the high carbon monoxide and
hydrocarbons from the corollary
emissions.
As stringent vehicle emissions quality
standards have started being imposed by
numerous regulatory bodies, such as those
in Europe, the United States (US) and
Japan, emission levels have evolved to be
a major focus in new engine developments
recently. UHC, CO, NOx, and particulates
constitute the composition of emissions
from HCCI engines. Lower emission
levels of NOx and particulate matters and
higher levels of unburnt hydrocarbons
(HC) and carbon monoxide (CO) have
been claimed to have found in HCCI
engines emissions. As the emissions levels
of an engine depend upon operating
conditions of the engine, fuel quality and
the engine design, which are particular to
every engine, it is inappropriate and
ineffective to compare emission levels of
any two engines.
HC, CO and CO2
Among others, two major challenges that
need to be resolved are the higher UHC
and CO emissions in HCCI engines than
the conventional diesel engines as
reported. The low combustion
temperatures trigger incomplete
combustion that in turn leads to the
formation of UHC, consequently resulting
in deposition of fuel in boundary layers
and crevices. Total hydrocarbon
concentration (in parts per million carbon
atoms) is used to specify the level of UHC.
The cold area in any combustion wall
when the piston moves down the cylinder
wall leaving a thin layer of oil, known as
the crevice area, is reported to be the
source of UHC. The ability of diesel
engines to reduce UHC and CO emission
levels, is because of the presence of higher
concentrations of hydrogen and natural
gas, which in gaseous state, will reduce the
wall wetting effect on the cylinder liner.
NOx and particulate matter (PM)
The peak temperature which is a factor of
various parameters such as equivalence
ratio, fuel composition and the initial
temperature of the fuel–air mixture is
responsible for the determination of nearly
all of the NOx formation. Further, as
reported by Tanaka et al. An equivalence
ratio greater than 0.33, results in
significant increase in the NOx levels. The
maximum in-cylinder temperature exceeds
1800 K and produces more NOx when a
higher equivalence ratio is achieved. The
NOx and particulate matters (PM) are
reported to be very low by implementing
high CR engines in HCCI engines, which
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Volume 3 Issue 2
can be further reduced by use of high EGR
rates and reduction in the local
temperature and the oxygen amount in the
cylinder However, a hike in unburned HC
and CO emissions could be a consequence
of insufficient oxygen. An effective way of
reducing the NOx, unburned HC and CO
by the use of internal EGR with VVT was
suggested by Bression et al. as he
experimented with high pressure-loop
EGR, to increase the combustion
temperature without employing coolers
and Variable Valve Timing (VVT).
The NOx level for a dual fuel engine, i.e.,
a blend of diesel (direct injected) and
natural gas (port injected) was found to be
lower than diesel CI engine when operated
for the combustion and exhaust emission
characteristics during an investigation by
Papagiannakis and Hountalas [11].
Addition of hydrogen would further reduce
the NOx. As hydrogen has a higher
temperature and flame speed compared to
natural gas and diesel, the concentration of
NOx between natural gas and hydrogen in
diesel HCCI mode is different due to
different combustion temperatures. The
higher level of NOx emissions from the
combustion of natural gas-hydrogen
mixtures was an after effect of the
combustion temperature and flame speed
of hydrogen which developed with
increase in NOx and hydrogen content in
the mixtures as indicated in a survey of
research papers by A.A. Hairuddin et al.
[12].
The NOx level in biogas–diesel HCCI
engines was inversely proportional to the
biogas energy. A higher homogeneity level
achieved between air and fuels could
possibly be the root cause for this. The
importance of a homogeneous and lean
mixture in eliminating the production of
NOx was repoorted by Van Blarigan [13]
in his study. According to Olsson et al.
[14], combining the NOx levels with
exhaust gas recirculation (EGR) would
further drop the already low NOx levels in
natural gas HCCI engines. The NOx level
even in natural gas–diesel non-HCCI mode
is lower than diesel conventional CI
engines. The absence of carbon in the fuel
sequences to the UHC, CO and CO2 free
emission with the use of hydrogen, yet it
produces NOx. Lower NOx levels were
recorded with the operation of hydrogen as
a single fuel in CI mode as compared to
diesel. Hydrogen addition to diesel in non-
HCCI mode yielded lower NOx emissions
amongst those obtained for all load ranges
compared to diesel in conventional mode
as inferred by Saravanan and Nagarajan
[19] in their study, they further reported
that the formation of NOx depends on
temperature more than the availability of
oxygen. Conclusively, extremely low NOx
emissions levels were observed with
hydrogen–diesel in HCCI mode with no
significant amount of PM.
PM is produced due to liquid fuel
nucleation from port fuel injection as
suggested by Kayes and Hochgreb [15]
according to their mechanism model for
PM. A gas-phase nucleation in fuel-rich
conditions also results in the production of
PM. Due to the substantial effects of air-
to-fuel ratio on PM and burning liquid
fuel, it is advisable to keep the fuel in an
atomized condition as this will
consequently increase the amount of PM
in the exhaust gas emissions. Addition of
hydrogen to a diesel fuelled engine and
heating the inlet [15] can significantly
reduce PM. No significant reduction in PM
was recorded [16] when the engine was
made to run on a dual fuel mode between
diesel and natural gas. However, addition
of hydrogen in reducing the PM emission
levels turned out to be an effective
method.
Knocking
A spontaneously ignition due to some un-
burnt gases ahead of the flame in an SI
engine leads to Engine knock or pinging.
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The propagation of the flame compresses
the gas resulting in the rise in combustion
chamber pressure, this high pressure and
corresponding high temperature causes the
un-burnt reactants to spontaneously ignite.
A shock wave from the end gas region and
an expansion wave into the end gas region
are traversed as a result of this ignition. A
similar ignition process occurs in HCCI,
where the only difference being that the
ignition occurs due to piston compression
more or less simultaneously in the bulk of
the compressed charge instead of part of
the reactant mixture being ignited by
compression ahead of a flame front.
Knocking in SI engines is a phenomenon
where the un-burnt mixture in the
compressed gas ignites before it is reached
by the propagating flame front. An
excessive engine vibration and a pinging
sound heard outside as a result of the
combustion activity are physical
indications of Knocking. Besides, loss of
power, if not controlled, knocking could
lead to severe engine damage and shorten
its life. Knocking is a characteristic of
reciprocating engines. Governed by
chemical kinetics, HCCI engines are rather
prone to knock and with a lack of a fixed
mechanism to control knock in them. The
load range of an HCCI engine is also
confined within limits due to the Knocking
phenomena i.e., upper load limits have to
be applied as high load operations can
easily initiate knock. If the combustion
starts before the piston reaches TDC, it
results in knocking where as if it occurs
after TDC, misfire is observed. To prevent
deterioration of engine performance, it is
imperative to avoid Knocking and misfire
in engine operation as both of them can
significantly contribute to the damage
caused to the engine.
A high natural gas flow rate combined
with a low diesel flow rate in a natural
gas–diesel HCCI engines would lead to a
misfire while the opposite configuration
leads to knocking. An addition of high
amount of hydrogen, is expected to trigger
knocking in HCCI engines operating on
hydrogen–diesel fuels. As confirmed by
Guo et al. [17], it is essential for hydrogen
content to be more than 16% of the energy
ratio for Knocking to take place. He
further registered that hydrogen with mass
fraction less than 15% is necessary to
achieve stable combustion. An unstable
operation for high natural gas
concentrations is observed in an HCCI
engine running on dimethyl ether (DME),
resulting in the knock limit of an in-
cylinder pressure of 9 MPa and a very
limited load range.
Use of Computational Fluid Dynamics
(CFD) simulations with detailed chemical
kinetics lead to this discovery. An
equivalence ratio less than 0.45 and an
intake temperature of 380 K culminated to
knocking as revealed in an investigation of
auto-ignition and combustion of natural
gas HCC engines. Figure 3 illustrates the
area of knocking and misfiring of natural
gas HCCI engines with constant intake
pressure. Natural gas HCCI engines are
incapable of operating at high load
conditions, pertaining to this limitation.
A rapid increase in local pressure caused
by a rapid release of energy in the
remaining unburned mixture results in
Knocking. A combination of hydrogen and
diethyl ether (DEE) at 100% load in
hydrogen–diesel engines will cause a
highly unstable condition for working
resulting in severe knock. Besides a higher
probability of knock onset is anyways
expected with higher hydrogen content. By
observing a rapid instantaneous local
pressure rise in the in-cylinder pressure
variations, the Knocking phenomena can
be detected. The severity of the knock
corresponds to the frequency of the knock,
which is the principle to form the graph.
For a single combustion event in a
hydrogen HCCI engine with a
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compression ratio of 17, the knocking
behaviour can be depicted in Figure 4 by
monitoring its in-cylinder pressure. It can
be seen that from the Figure, that the peak
pressure is higher than the normal in-
cylinder peak pressure without knocking,
which denotes the in-cylinder pressure
suddenly increases to the peak before
following the normal pressure trend. In an
incorrect operating condition, there is an
abnormality where the maximum increase
in pressure for knocking is unpredictable.
Due to the low temperature reactions in the
compression stroke, accumulation of H2O2
decomposition is found with HCCI
ignition, as described by Flowers et al.
[18]. Fuels in the cylinder get rapidly
consume by the enormous amount of OH
radicals formed by the rapid
decomposition of H2O2 into two radicals
once the in-cylinder temperature reaches
1050–1100 K. Incomplete combustion is a
result of reduction in OH concentration in
low temperature regions, which is also
responsible for delaying the high-
temperature oxidation. It is easier to
control knock in SI engines, for instance,
car manufacturers usually install knock
and oxygen sensors in the engine where
the sensors will automatically adjust the
spark timing if the mixture is prone to
generate knocking. Whereas, in HCCI
engines, since there is no such concrete
mechanism to define and control
knocking, a strong dependence is on the
right mixtures and conditions.
Fig.2:-Knocking and misfiring area for natural gas HCCI engines under constant intake
pressure, reproduced from [21]
Fig.3:-Knocking phenomena in a hydrogen HCCI engine for a single combustion event,
reproduced from [9]
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CONCLUSION
CAI/HCCI engines have neither evolved to
phase of development nor to the
economical feasibility mandatory for a
market introduction as yet. The technical
challenges incurred with both gasoline and
diesel HCCI combustion are their limited
operational range and less optimized
combustion phasing, owing to the lack of
direct control over the start of ignition and
the rate of heat release.
To summarize, besides generating better
results for most major quantities, the
hydrogen-diesel combination in HCCI
engines also produce higher efficiency
compared to the single diesel mode and the
natural gas–diesel mode. A reduced fuel
consumption of the engine that could also
match to that of the hybrid engine is
credited to a higher value of BTE. HCCI
seems to be a promising choice of engines
in the near future as using it in a hybrid
configuration would result in a significant
reduction in fuel consumption.
The HCCI engine has low emissions levels
of NOx, soot and particulates. However,
knocking and high levels of unburned HC
and CO emissions are still some of the
unresolved issues of the HCCI engines.
Knocking in an HCCI engine will take
place on addition of hydrogen to diesel-air
mixture once the energy ratio is more than
16%. Since the combustion is no longer
controlled by the injection or the spark
timing, knocking is expected to be
influenced by chemical kinetics in HCCI
engines. Therefore, it is hypothesized that
the knocking in HCCI engines could be
due to the instantaneous initiation of local
combustion resulting in a local high heat
release rate in the region with the highest
OH concentrations in the high temperature
zone, i.e., the highest temperature region.
Further studies have to be performed to
have a resolution for these remaining
issues. The numerical method is far better
than the experimental method to simulate
the combustion behaviour in terms of cost
and time. To this end, a simulation model
to investigate the behaviour needs to be
developed and the numerical findings must
then be validated against empirical data.
The multi-zone numerical method
combined with advanced turbulent mixing
models demonstrates promising results
compared to the single-zone model. To
achieve even greater accuracy than multi-
zone model, CFD model can be used at the
expense of computational cost. But, one
could easily implement the LES or DES
model with CFD.
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