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1
Internal Combustion Engines
Lecture-18
Ujjwal K Saha, Ph.D.
Department of Mechanical Engineering
Indian Institute of Technology Guwahati
Prepared under
QIP-CD Cell Project
2
Combustion in CI Engine
Combustion in a CI engine is quite different
from that of an SI engine. While combustion in
an SI engine is essentially a flame front moving
through a homogeneous mixture, combustion
in a CI engine is an unsteady process
occurring simultaneously in many spots in a
very non-homogeneous mixture controlled by
fuel injection.
Air intake into the engine is unthrottled, with
engine torque and power output controlled
by the amount of fuel injected per cycle.
3
Only air is contained in the cylinder during
compression stroke, and a much higher
compression ratios (12 to 24) are used in CI
engines.
In addition to swirl and turbulence of the
air, a high injection velocity is needed to
spread the fuel throughout the cylinder and
cause it to mix with the air.
Fuel is injected into the cylinders late in
the compression stroke by one or more
injectors located in each cylinders.
Injection time is usually about 200 of
crankshaft rotation (150 bTDC and 50 aTDC).
4
Cylinder pressure as a function
of crank angle for a CI engine.
A : point of fuel injection
B : point of ignition
C : end of fuel injection
AB : delay period
5
Combustion in CI Engine
In a CI engine the fuel is sprayed directly into the
cylinder and the fuel-air mixture ignites spontaneously.
These photos are taken in a RCM under CI engine
conditions with swirl air flow
0.4 ms after ignition 3.2 ms after ignition
3.2 ms after ignition Late in combustion process
1cm
6
In Cylinder Measurements
This graph shows the fuel injection flow rate, net heat release
rate and cylinder pressure for a direct injection CI engine.
Start of injection
Start of combustion
End of injection
7
Four Stages of Combustion in CI Engines
Start of
injection
End of
injecction
-10 TC-20 10 20 30
8
Combustion in CI Engine
The combustion process proceeds by the following stages:
Ignition delay (ab) - fuel is injected directly into
the cylinder towards the end of the compression
stroke. The liquid fuel atomizes into small drops
and penetrates into the combustion chamber.
The fuel vaporizes and mixes with the high-
temperature high-pressure air.
Premixed combustion phase (bc) –
combustion of the fuel which has mixed with
the air to within the flammability limits (air at
high-temperature and high-pressure) during
the ignition delay period occurs rapidly in a
few crank angles.
9
Combustion in CI Engine – contd.
Mixing controlled combustion
phase (cd) – after premixed
gas consumed, the burning
rate is controlled by the rate
at which mixture becomes
available for burning. The
rate of burning is controlled in
this phase primarily by the
fuel-air mixing process.
Late combustion phase (de) – heat release may
proceed at a lower rate well into the expansion
stroke (no additional fuel injected during this phase).
Combustion of any unburned liquid fuel and soot is
responsible for this.
10
CI Engine Types
Two basic categories of CI engines:
i) Direct-injection – have a single open
combustion chamber into which fuel is
injected directly
ii) Indirect-injection – chamber is divided into
two regions and the fuel is injected into the
“pre-chamber” which is connected to the
main chamber via a nozzle, or one or more
orifices.
11
CI Engine Types – contd.
• For very-large engines (stationary power
generation) which operate at low engine speeds
the time available for mixing is long so a direct
injection quiescent chamber type is used (open or
shallow bowl in piston).
• As engine size decreases and engine speed
increases, increasing amounts of swirl are used to
achieve fuel-air mixing (deep bowl in piston).
• For small high-speed engines used in automobiles
chamber swirl is not sufficient, indirect injection is
used where high swirl or turbulence is generated in
the pre-chamber during compression and
products/fuel blowdown and mix with main
chamber air.
12
Types of CI Engines
Direct injection:
quiescent chamber
Direct injection:
swirl in chamber Indirect injection: turbulent
and swirl pre-chamber
Orifice
-plate
Glow plug
13
Direct Injection
quiescent chamber
Direct Injection
multi-hole nozzle
swirl in chamber
Direct Injection
single-hole nozzle
swirl in chamber
Indirect injection
swirl pre-chamber
14
Combustion Characteristics
Combustion occurs
throughout the chamber
over a range of
equivalence ratios
dictated by the fuel-air
mixing before and
during the combustion
phase.
In general most of the
combustion occurs under
very rich conditions
within the head of the jet,
this produces a
considerable amount of
solid carbon (soot).
15
Ignition Delay
Ignition delay is defined as the time (or crank angle
interval) from when the fuel injection starts to the onset
of combustion.
Both physical and chemical processes must take place
before a significant fraction of the chemical energy of
the injected liquid is released.
Physical processes are fuel spray atomization,
evaporation and mixing of fuel vapour with cylinder air.
Good atomization requires high fuel-injection pressure, small
injector hole diameter, optimum fuel viscosity, high cylinder
pressure (large divergence angle).
Rate of vaporization of the fuel droplets depends on droplet
diameter, velocity, fuel volatility, pressure and temperature of
the air.
16
Physical processes are fuel spray atomization,
evaporation and mixing of fuel vapour with
cylinder air.
Chemical processes similar to that described
for auto-ignition phenomenon in premixed fuel-
air, only more complex since heterogeneous
reactions (reactions occurring on the liquid fuel
drop surface) also occur.
Ignition Delay
17
Fuel Ignition Quality
The ignition characteristics of the fuel
affect the ignition delay.
The ignition quality of a fuel is defined
by its cetane number CN.
For low cetane fuels the ignition delay is
long and most of the fuel is injected
before autoignition and rapidly burns,
under extreme cases this produces an
audible knocking sound referred to as
“diesel knock”.
18
Fuel Ignition Quality
For high cetane fuels the ignition delay
is short and very little fuel is injected
before auto-ignition, the heat release
rate is controlled by the rate of fuel
injection and fuel-air mixing – smoother
engine operation.
19
Cetane Number
The method used to determine the ignition
quality in terms of CN is analogous to that
used for determining the antiknock quality
using the ON.
The cetane number scale is defined by
blends of two pure hydrocarbon reference
fuels.
By definition, isocetane (heptamethylnonane,
HMN) has a cetane number of 15 and cetane
(n-hexadecane, C16H34) has a value of 100.
20
Cetane Number
In the original procedures a-
methylnaphtalene (C11H10) with a
cetane number of zero represented the
bottom of the scale. This has since been
replaced by HMN which is a more stable
compound.
The higher the CN the better the
ignition quality, i.e., shorter ignition
delay.
21
The method developed to measure CN uses a
standardized single-cylinder engine with
variable compression ratio
The operating condition is:
Inlet temperature (oC) 65.6
Speed (rpm) 900
Spark advance (oBTC) 13
Coolant temperature (oC) 100
Injection pressure (MPa) 10.3
Cetane Number Measurement
22
With the engine running at these
conditions on the test fuel, the
compression ratio is varied until
combustion starts at TC, ignition delay
period of 13o.
The above procedure is repeated using
blends of cetane and HMN. The blend that
gives a 13o ignition delay with the same
compression ratio is used to calculate the
test fuel cetane number.
Cetane Number Measurement – contd.
23
Cetane vs Octane Number
The octane number and cetane number
of a fuel are inversely correlated.
Gasoline is a poor diesel fuel and vice versa.
24
Factors Affecting Ignition Delay
Injection timing – At normal engine conditions the
minimum delay occurs with the start of injection
at about 10-15 BTC.
The increase in the delay time with earlier or later
injection timing occurs because of the air
temperature and pressure during the delay
period.
Injection quantity – For a CI engine the air is not
throttled so the load is varied by changing the
amount of fuel injected.
25
Increasing the load (bmep) increases the
residual gas and wall temperature which results
in a higher charge temperature at injection
which translates to a decrease in the ignition
delay.
Intake air temperature and pressure – an
increase in ether will result in a decrease in the
ignition delay, an increase in the compression
ratio has the same effect.
Factors Affecting Ignition Delay – contd.
26
(gauge)
Factors Affecting
Ignition Delay
27
Factors Affecting Delay Period (DP)
1. Compression Ratio: DP decreases with
increase of CR.
2. Engine Speed: DP decreases with increase
of engine speed.
3. Power Output: DP decreases with increase
of power output.
4. Fuel Atomization: DP decreases with fineness
of atomization.
5. Fuel Quality: DP decreases with higher
cetane number.
6. Intake Temp. & Pressure: DP decreases with
increase of Temperature and pressure.
28
Effect of
Ignition
Delay
29
Knock in CI Engines
Knock in SI and CI engines are fundamentally
similar. In SI engines, it occurs near the end of
combustion; whereas in CI engines, it occurs
near the beginning of combustion.
Knock in CI engines is related to delay
period. When DP is longer, there will be more
and more accumulation of fuel droplets in
combustion chamber. This leads to a too rapid
a pressure rise due to ignition, resulting in
jamming of forces against the piston and rough
engine operation. When the DP is too long, the
rate of pressure rise is almost instantaneous
with more accumulation of fuel.
30
Knock in SI and CI Engines
31
1.1. Crouse WH,Crouse WH, andand Anglin DLAnglin DL, (1985), Automotive Engines, Tata McGraw Hill.
2.2. Eastop TD,Eastop TD, andand McConkey A,McConkey A, (1993), Applied Thermodynamics for Engg.
Technologists, Addison Wisley.
3.3. Fergusan CR,Fergusan CR, andand Kirkpatrick ATKirkpatrick AT,, (2001), Internal Combustion Engines, John
Wiley & Sons.
4.4. Ganesan VGanesan V,, (2003), Internal Combustion Engines, Tata McGraw Hill.
5.5. Gill PW, Smith JH,Gill PW, Smith JH, andand Ziurys EJZiurys EJ,, (1959), Fundamentals of I. C. Engines, Oxford
and IBH Pub Ltd.
6.6. Heisler H,Heisler H, (1999), Vehicle and Engine Technology, Arnold Publishers.
7.7. Heywood JB,Heywood JB, (1989), Internal Combustion Engine Fundamentals, McGraw Hill.
8.8. Heywood JB,Heywood JB, andand Sher E,Sher E, (1999), The Two-Stroke Cycle Engine, Taylor & Francis.
9.9. Joel R,Joel R, (1996), Basic Engineering Thermodynamics, Addison-Wesley.
10.10. Mathur ML, and Sharma RP,Mathur ML, and Sharma RP, (1994), A Course in Internal Combustion Engines,
Dhanpat Rai & Sons, New Delhi.
11.11. Pulkrabek WW,Pulkrabek WW, (1997), Engineering Fundamentals of the I. C. Engine, Prentice Hall.
12.12. Rogers GFC,Rogers GFC, andand Mayhew YRMayhew YR, (1992), Engineering Thermodynamics, Addison
Wisley.
13.13. Srinivasan S,Srinivasan S, (2001), Automotive Engines, Tata McGraw Hill.
14.14. Stone R,Stone R, (1992), Internal Combustion Engines, The Macmillan Press Limited, London.
15.15. Taylor CF,Taylor CF, (1985), The Internal-Combustion Engine in Theory and Practice, Vol.1 & 2,
The MIT Press, Cambridge, Massachusetts.
References
32
1. http://www.mne.psu.edu/simpson/courses
2. http://me.queensu.ca/courses
3. http://www.eng.fsu.edu
4. http://www.personal.utulsa.edu
5. http://www.glenroseffa.org/
6. http://www.howstuffworks.com
7. http://www.me.psu.edu
8. http://www.uic.edu/classes/me/ me429/lecture-air-cyc-web%5B1%5D.ppt
9. http://www.osti.gov/fcvt/HETE2004/Stable.pdf
10. http://www.rmi.org/sitepages/pid457.php
11. http://www.tpub.com/content/engine/14081/css
12. http://webpages.csus.edu
13. http://www.nebo.edu/misc/learning_resources/ ppt/6-12
14. http://netlogo.modelingcomplexity.org/Small_engines.ppt
15. http://www.ku.edu/~kunrotc/academics/180/Lesson%2008%20Diesel.ppt
16. http://navsci.berkeley.edu/NS10/PPT/
17. http://www.career-center.org/ secondary/powerpoint/sge-parts.ppt
18. http://mcdetflw.tecom.usmc.mil
19. http://ferl.becta.org.uk/display.cfm
20. http://www.eng.fsu.edu/ME_senior_design/2002/folder14/ccd/Combustion
21. http://www.me.udel.edu
22. http://online.physics.uiuc.edu/courses/phys140
23. http://widget.ecn.purdue.edu/~yanchen/ME200/ME200-8.ppt -
24. http://www.bae.uky.edu
Web Resources

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CI engine

  • 1. 1 Internal Combustion Engines Lecture-18 Ujjwal K Saha, Ph.D. Department of Mechanical Engineering Indian Institute of Technology Guwahati Prepared under QIP-CD Cell Project
  • 2. 2 Combustion in CI Engine Combustion in a CI engine is quite different from that of an SI engine. While combustion in an SI engine is essentially a flame front moving through a homogeneous mixture, combustion in a CI engine is an unsteady process occurring simultaneously in many spots in a very non-homogeneous mixture controlled by fuel injection. Air intake into the engine is unthrottled, with engine torque and power output controlled by the amount of fuel injected per cycle.
  • 3. 3 Only air is contained in the cylinder during compression stroke, and a much higher compression ratios (12 to 24) are used in CI engines. In addition to swirl and turbulence of the air, a high injection velocity is needed to spread the fuel throughout the cylinder and cause it to mix with the air. Fuel is injected into the cylinders late in the compression stroke by one or more injectors located in each cylinders. Injection time is usually about 200 of crankshaft rotation (150 bTDC and 50 aTDC).
  • 4. 4 Cylinder pressure as a function of crank angle for a CI engine. A : point of fuel injection B : point of ignition C : end of fuel injection AB : delay period
  • 5. 5 Combustion in CI Engine In a CI engine the fuel is sprayed directly into the cylinder and the fuel-air mixture ignites spontaneously. These photos are taken in a RCM under CI engine conditions with swirl air flow 0.4 ms after ignition 3.2 ms after ignition 3.2 ms after ignition Late in combustion process 1cm
  • 6. 6 In Cylinder Measurements This graph shows the fuel injection flow rate, net heat release rate and cylinder pressure for a direct injection CI engine. Start of injection Start of combustion End of injection
  • 7. 7 Four Stages of Combustion in CI Engines Start of injection End of injecction -10 TC-20 10 20 30
  • 8. 8 Combustion in CI Engine The combustion process proceeds by the following stages: Ignition delay (ab) - fuel is injected directly into the cylinder towards the end of the compression stroke. The liquid fuel atomizes into small drops and penetrates into the combustion chamber. The fuel vaporizes and mixes with the high- temperature high-pressure air. Premixed combustion phase (bc) – combustion of the fuel which has mixed with the air to within the flammability limits (air at high-temperature and high-pressure) during the ignition delay period occurs rapidly in a few crank angles.
  • 9. 9 Combustion in CI Engine – contd. Mixing controlled combustion phase (cd) – after premixed gas consumed, the burning rate is controlled by the rate at which mixture becomes available for burning. The rate of burning is controlled in this phase primarily by the fuel-air mixing process. Late combustion phase (de) – heat release may proceed at a lower rate well into the expansion stroke (no additional fuel injected during this phase). Combustion of any unburned liquid fuel and soot is responsible for this.
  • 10. 10 CI Engine Types Two basic categories of CI engines: i) Direct-injection – have a single open combustion chamber into which fuel is injected directly ii) Indirect-injection – chamber is divided into two regions and the fuel is injected into the “pre-chamber” which is connected to the main chamber via a nozzle, or one or more orifices.
  • 11. 11 CI Engine Types – contd. • For very-large engines (stationary power generation) which operate at low engine speeds the time available for mixing is long so a direct injection quiescent chamber type is used (open or shallow bowl in piston). • As engine size decreases and engine speed increases, increasing amounts of swirl are used to achieve fuel-air mixing (deep bowl in piston). • For small high-speed engines used in automobiles chamber swirl is not sufficient, indirect injection is used where high swirl or turbulence is generated in the pre-chamber during compression and products/fuel blowdown and mix with main chamber air.
  • 12. 12 Types of CI Engines Direct injection: quiescent chamber Direct injection: swirl in chamber Indirect injection: turbulent and swirl pre-chamber Orifice -plate Glow plug
  • 13. 13 Direct Injection quiescent chamber Direct Injection multi-hole nozzle swirl in chamber Direct Injection single-hole nozzle swirl in chamber Indirect injection swirl pre-chamber
  • 14. 14 Combustion Characteristics Combustion occurs throughout the chamber over a range of equivalence ratios dictated by the fuel-air mixing before and during the combustion phase. In general most of the combustion occurs under very rich conditions within the head of the jet, this produces a considerable amount of solid carbon (soot).
  • 15. 15 Ignition Delay Ignition delay is defined as the time (or crank angle interval) from when the fuel injection starts to the onset of combustion. Both physical and chemical processes must take place before a significant fraction of the chemical energy of the injected liquid is released. Physical processes are fuel spray atomization, evaporation and mixing of fuel vapour with cylinder air. Good atomization requires high fuel-injection pressure, small injector hole diameter, optimum fuel viscosity, high cylinder pressure (large divergence angle). Rate of vaporization of the fuel droplets depends on droplet diameter, velocity, fuel volatility, pressure and temperature of the air.
  • 16. 16 Physical processes are fuel spray atomization, evaporation and mixing of fuel vapour with cylinder air. Chemical processes similar to that described for auto-ignition phenomenon in premixed fuel- air, only more complex since heterogeneous reactions (reactions occurring on the liquid fuel drop surface) also occur. Ignition Delay
  • 17. 17 Fuel Ignition Quality The ignition characteristics of the fuel affect the ignition delay. The ignition quality of a fuel is defined by its cetane number CN. For low cetane fuels the ignition delay is long and most of the fuel is injected before autoignition and rapidly burns, under extreme cases this produces an audible knocking sound referred to as “diesel knock”.
  • 18. 18 Fuel Ignition Quality For high cetane fuels the ignition delay is short and very little fuel is injected before auto-ignition, the heat release rate is controlled by the rate of fuel injection and fuel-air mixing – smoother engine operation.
  • 19. 19 Cetane Number The method used to determine the ignition quality in terms of CN is analogous to that used for determining the antiknock quality using the ON. The cetane number scale is defined by blends of two pure hydrocarbon reference fuels. By definition, isocetane (heptamethylnonane, HMN) has a cetane number of 15 and cetane (n-hexadecane, C16H34) has a value of 100.
  • 20. 20 Cetane Number In the original procedures a- methylnaphtalene (C11H10) with a cetane number of zero represented the bottom of the scale. This has since been replaced by HMN which is a more stable compound. The higher the CN the better the ignition quality, i.e., shorter ignition delay.
  • 21. 21 The method developed to measure CN uses a standardized single-cylinder engine with variable compression ratio The operating condition is: Inlet temperature (oC) 65.6 Speed (rpm) 900 Spark advance (oBTC) 13 Coolant temperature (oC) 100 Injection pressure (MPa) 10.3 Cetane Number Measurement
  • 22. 22 With the engine running at these conditions on the test fuel, the compression ratio is varied until combustion starts at TC, ignition delay period of 13o. The above procedure is repeated using blends of cetane and HMN. The blend that gives a 13o ignition delay with the same compression ratio is used to calculate the test fuel cetane number. Cetane Number Measurement – contd.
  • 23. 23 Cetane vs Octane Number The octane number and cetane number of a fuel are inversely correlated. Gasoline is a poor diesel fuel and vice versa.
  • 24. 24 Factors Affecting Ignition Delay Injection timing – At normal engine conditions the minimum delay occurs with the start of injection at about 10-15 BTC. The increase in the delay time with earlier or later injection timing occurs because of the air temperature and pressure during the delay period. Injection quantity – For a CI engine the air is not throttled so the load is varied by changing the amount of fuel injected.
  • 25. 25 Increasing the load (bmep) increases the residual gas and wall temperature which results in a higher charge temperature at injection which translates to a decrease in the ignition delay. Intake air temperature and pressure – an increase in ether will result in a decrease in the ignition delay, an increase in the compression ratio has the same effect. Factors Affecting Ignition Delay – contd.
  • 27. 27 Factors Affecting Delay Period (DP) 1. Compression Ratio: DP decreases with increase of CR. 2. Engine Speed: DP decreases with increase of engine speed. 3. Power Output: DP decreases with increase of power output. 4. Fuel Atomization: DP decreases with fineness of atomization. 5. Fuel Quality: DP decreases with higher cetane number. 6. Intake Temp. & Pressure: DP decreases with increase of Temperature and pressure.
  • 29. 29 Knock in CI Engines Knock in SI and CI engines are fundamentally similar. In SI engines, it occurs near the end of combustion; whereas in CI engines, it occurs near the beginning of combustion. Knock in CI engines is related to delay period. When DP is longer, there will be more and more accumulation of fuel droplets in combustion chamber. This leads to a too rapid a pressure rise due to ignition, resulting in jamming of forces against the piston and rough engine operation. When the DP is too long, the rate of pressure rise is almost instantaneous with more accumulation of fuel.
  • 30. 30 Knock in SI and CI Engines
  • 31. 31 1.1. Crouse WH,Crouse WH, andand Anglin DLAnglin DL, (1985), Automotive Engines, Tata McGraw Hill. 2.2. Eastop TD,Eastop TD, andand McConkey A,McConkey A, (1993), Applied Thermodynamics for Engg. Technologists, Addison Wisley. 3.3. Fergusan CR,Fergusan CR, andand Kirkpatrick ATKirkpatrick AT,, (2001), Internal Combustion Engines, John Wiley & Sons. 4.4. Ganesan VGanesan V,, (2003), Internal Combustion Engines, Tata McGraw Hill. 5.5. Gill PW, Smith JH,Gill PW, Smith JH, andand Ziurys EJZiurys EJ,, (1959), Fundamentals of I. C. Engines, Oxford and IBH Pub Ltd. 6.6. Heisler H,Heisler H, (1999), Vehicle and Engine Technology, Arnold Publishers. 7.7. Heywood JB,Heywood JB, (1989), Internal Combustion Engine Fundamentals, McGraw Hill. 8.8. Heywood JB,Heywood JB, andand Sher E,Sher E, (1999), The Two-Stroke Cycle Engine, Taylor & Francis. 9.9. Joel R,Joel R, (1996), Basic Engineering Thermodynamics, Addison-Wesley. 10.10. Mathur ML, and Sharma RP,Mathur ML, and Sharma RP, (1994), A Course in Internal Combustion Engines, Dhanpat Rai & Sons, New Delhi. 11.11. Pulkrabek WW,Pulkrabek WW, (1997), Engineering Fundamentals of the I. C. Engine, Prentice Hall. 12.12. Rogers GFC,Rogers GFC, andand Mayhew YRMayhew YR, (1992), Engineering Thermodynamics, Addison Wisley. 13.13. Srinivasan S,Srinivasan S, (2001), Automotive Engines, Tata McGraw Hill. 14.14. Stone R,Stone R, (1992), Internal Combustion Engines, The Macmillan Press Limited, London. 15.15. Taylor CF,Taylor CF, (1985), The Internal-Combustion Engine in Theory and Practice, Vol.1 & 2, The MIT Press, Cambridge, Massachusetts. References
  • 32. 32 1. http://www.mne.psu.edu/simpson/courses 2. http://me.queensu.ca/courses 3. http://www.eng.fsu.edu 4. http://www.personal.utulsa.edu 5. http://www.glenroseffa.org/ 6. http://www.howstuffworks.com 7. http://www.me.psu.edu 8. http://www.uic.edu/classes/me/ me429/lecture-air-cyc-web%5B1%5D.ppt 9. http://www.osti.gov/fcvt/HETE2004/Stable.pdf 10. http://www.rmi.org/sitepages/pid457.php 11. http://www.tpub.com/content/engine/14081/css 12. http://webpages.csus.edu 13. http://www.nebo.edu/misc/learning_resources/ ppt/6-12 14. http://netlogo.modelingcomplexity.org/Small_engines.ppt 15. http://www.ku.edu/~kunrotc/academics/180/Lesson%2008%20Diesel.ppt 16. http://navsci.berkeley.edu/NS10/PPT/ 17. http://www.career-center.org/ secondary/powerpoint/sge-parts.ppt 18. http://mcdetflw.tecom.usmc.mil 19. http://ferl.becta.org.uk/display.cfm 20. http://www.eng.fsu.edu/ME_senior_design/2002/folder14/ccd/Combustion 21. http://www.me.udel.edu 22. http://online.physics.uiuc.edu/courses/phys140 23. http://widget.ecn.purdue.edu/~yanchen/ME200/ME200-8.ppt - 24. http://www.bae.uky.edu Web Resources