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Combustion Targets for Low Emissions and High Efficiency Tom Ryan September, 2005

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Combustion Targets for Low Emissions and High Efficiency

Tom RyanSeptember, 2005

Three Combustion Modes

Flame Propagation (SI Gasoline)Stoichiometric Combustion Thin Reaction ZoneHigh Temperature and High NOx

Diffusion Burning (Conventional Diesel)Stoichiometric Reaction ZoneThin Reaction ZoneHigh Temperature and High NOxRich Zones at High T Leading to Soot Formation

Homogeneous Reaction (HCCI)Dilute MixturesLow Temperature Reactions and Low NOxHomogeneous Mixture at Low Temperature

Background

Engine Combustion Technologies are Apparently Converging to the same General Characteristics

Delayed Ignition and Rapid Burn RateEngine Technologies are also Converging

Highly BoostedHigh BMEPHigh EGR 0

10

20

30

40

50

60

70

0 60 120 180 240 300 360 420 480 540 600 660 720CRANK ANGLE

PRES

SUR

E (b

ar)

New Combustion Modes

HEDGE, HCCI, CAI, PCCI, LTC, PCI, and CSI are some of the Acronyms used to Describe the Recent Developments for Modified Fuel Reaction Approaches

HEDGE - High Efficiency Dilute Gasoline EngineHCCI - Homogeneous Charge Compression IgnitionCAI - Controlled Auto IgnitionPCCI - Premixed Charge Compression IgnitionLTC - Low Temperature CombustionPCI - Premixed Compression Ignition

CSI - Compression and Spark Ignition

HEDGE, HCCI, CAI, PCCI, LTC, PCI, and CSI

Common Factors include:Thick FlamesPart or all of the Fuel is PremixedAll Use EGRAll have Lower NOx All have Higher HC and CO

Differences Include:Degree of PremixingPM EmissionsOverall Equivalence RatioInitiation of ReactionPurpose/Application

Low EmissionsExhaust Gas Composition and Temperature Control

Best Combustion Phasing - Theoretical vs Practical

Thermodynamically Ideal Cycles Produce Highest Efficiency with Instantaneous Heat Release at TDCPractical Limitations Include

Noise due to Rapid Rates of Heat ReleaseIncreases in Friction due to Higher Bearing Loads and Small dV/dθ EffectsPeak Firing Pressure LimitsPressure Oscillations (maybe Knock)

Typical Advanced Heat Release Rate

CA (Degrees)140 160 180 200

Hea

t Rel

ease

Rat

e (J

/deg

)

-200

20406080

100120140160 Main Reaction

Cool Flame

Approach

Use Cycle Simulation to Determine the Effects of Changing the Heat Release Rate Characteristics on the Emissions and the Efficiency

Mainly Concerned with NOx and BTE

HEDGE Performance PredictionsTools

Alamo Engine (A_E) Phenomenological, Zero Dimensional ModelsGas Exchange

Steady State Emptying & Filling (Checks With Steady State 1D Flow Code)

TCEnergy and Flow Balance for Selected Efficiencies, Wastegating (Vs Engine Speed)

CombustionWatson and Wiebe

FrictionChenn-flynn

AftertreatmentFixed Converter Efficiencies

Assumption for All Calculations

Engine Configuration130X160 mm BoreXStroke16:1 CRTurbocharged

Engine Conditions1800 rpmA/F 24:140% EGR240 kPa MAP

Only Changes, Shape and Timing of the HRR Diagrams

Details on Shape and Timing Effect

Peak Efficiency Occurs in All Cases as 12o ATDCRapid to Slow Heat Release (Duration 10 to 30o) Results in 0.5% Change in BSFCCorresponding IMEP Drop of 0.5%

14.5

14.55

14.6

14.65

14.7

14.75

14.8

14.85

14.9

14.95

15

355 360 365 370 375 380 385

crank angle of main heat release peak [deg]

IME

P [b

ar]

200

202

204

206

208

210

212

214

216

218

220

BSF

C [

g/kW

-hr]

IMEP, narrow profileIMEP, middle profileIMEP, wide profileBSFC, narrow profileBSFC, middle profileBSFC, wide profile

0

0.05

0.1

0.15

0.2

0.25

340 345 350 355 360 365 370 375 380 385 390 395 400

crank angle [deg]

Future Diesel Engines

Areas of Greatest Potential

Fuel ManagementHigh Pressure Injection EssentialInjection Rate Control EssentialAir Utilization Essential Liquid Fuel Wall Interactions must be Avoided

Gas ManagementHigh Density EssentialHigh EGR Levels Essential

Outcome is High Boost PressureUniform EGR Distribution EssentialIntake Cooling is DesirableHigh Efficiency Turbocharger Systems EssentialIn-Cylinder Flow Management Essential

Combustion ChambersMatched to Nozzle Spray CapabilitiesDesign for Maximum Mixing RatesPremixed Combustion Considerations

Surface-to-Volume Ratio MinimizedQuench Volume Minimized

Premise

Lowest Possible Emissions and Highest Efficiency in Diesel Engines Achieved Using:

Ultra High Injection Pressure and Small HolesMassive EGRUltra High BoostWell Designed Pistons and Intake

High Injection Pressure and Small Holes

Fuel Injection - High PressureSwRI Results SAE 2002-01-0494

Single Hole Nozzles 0.086 to 0.18 mm DiaPeak Injection Pressures from 254 to 283 MPaHigher Mixing Rates and Smaller Drops

High Pressure ElectronicUnit Injector Operating on

a Fixed Cam at Constant Speeds

Fuel Injection - High Pressure

Mixing Parameter and Drop Size both Decrease with Smaller HolesPinj Increases with Smaller Holes

1. Mixing Rates Quantified in Termsof SwRI Defined Mixing Parameter

2. Mixing Parameter Defines the Mass of Fuel at Phi Greater Than 1.0 for than 0.6 ms

3. Rich Regions Mean More Soot

Fuel Injection - High Pressure

Small Holes Produce High Pressure, Small SMD, High Mixing Rates and Low Soot Formation Rates

0.144 mm

0.128 mm

0.086 mm

Fuel Injection - High Pressure

High Pressure does not Affect the Jet Penetration Rate in either Evaporating on Non-Evaporating Sprays

SwRI

Small Holes do Affect the Evaporation Rate and the Liquid Length in Evaporating Sprays

Fuel Injection - High Pressure

12% Cam and 0.17 mm Nozzle Give same Duration as Baseline12% Cam and 0.131 mm Nozzle Give Higher Rates

Variable Area Nozzle (0.17 to 0.131 mm) Gives a Significant Improvement

0131 Used for Light Loads0.17 Used for High Loads

Duration, Liquid Length, and Mixing Rate are Important

Constant Injection DurationRequires Higher Pressure when using Small Holes

High Boost

Fuel Injection - High DensityLiquid Length Affected most Strongly by Hole Size and the Ambient Density

Smaller HolesHigher Density

Gas Jet Always Interacts with Combustion Chamber

Wall Jet Mixing Important

Air Motion

Combustion Chamber Design

Fuel Injection - Jet-Wall Interaction

Combustion Chamber Design

Spray Wall Interactions are Unavoidable

Avoid Liquid ImpingementTake Advantage of Jet Break-up and Wall Jet Opportunities

Pilot and Post Injections Change the Bowl Shape and Spray Angle Requirements

Cat uses Pilot at Almost all Conditions

Spray Angle Narrower

Man D20

Cat C9

Cat C15

Volvo D12

ISX

DDC S60

Fuel Injection WallFuel Injection Wall--Wetting IssuesWetting Issues

Background Is Liquid Impingement and Oil Dilution a Concern?

Concerned with both Early Pre- Injection for Emissions and Noise Control and Late Post -Injection Strategies for DPF and LNT Regeneration

Fuel Jet Penetration Increases during Late Injection Due to the Lower Density

Decreasing Pressure and High TemperatureLiquid Fuel can Impinge on the Wall and Some can Adhere and Enter the Lubricant

Approach Developed an empirical based model for estimation of the relative quantity of injected fuel that becomes associated with, or adheres, to the combustion chamber walls

DDC Series 60, 1600 rpm, Pilot

Liquid Mass Fractions at Bore

90oC = 31% Liquid65oC = 37% Liquid40oC = 43% Liquid

Adhering Mass Fraction on Bore is 71%

90oC = 22%65oC = 26% Liquid 40oC = 31%

DDC Pre-Injection Conditions

Time (msec)0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4

Pene

trat

ion

Dis

tanc

e (m

m)

40

50

60

70

80

90

Bore Radius = 65mm

1600 rpm,220 kPa, 90oC Tcoolant

65oC Tcoolant

1600 RPM, 100 kPa, 90oC Tcoolant

65oC Tcoolant

40oC Tcoolant

40oC Tcoolant

OM 611, 1500 rpm, PilotLiquid Mass Fractions at Bore

High Load65oC = 22% Liquid40oC = 34% Liquid

Low Load90oC = 50% Liquid65oC = 64% Liquid40oC = 76% Liquid

Adhering Mass Fraction 71%High Load

65oC = 16% Liquid40oC = 24% Liquid

Low Load90oC = 36% Liquid65oC = 45% Liquid40oC = 54% Liquid

OM 611 Pre-Injection1500 rpm

Time (msec)

0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4

Pene

trat

ion

(mm

)

0

20

40

60

80

100

High Load, 65oC TcoolantHigh Load, 90oC Tcoolant

Low Load, 65oC Tcoolant

High Load, 40oC Tcoolant

Low Load, 90oC Tcoolant

Low Load, 40oC Tcoolant

Bore Radius = 44 mm

Fuel Injection - Pilot and Post

Split Injection Offers Opportunity to Reduce Liquid Length and Liquid ImpingementBenefits for both Pre and Post Injection

First Pilot, 0.17 ms

Second Pilot, 0.17 msMain, 0.45 ms

First Post, 0.17 ms

Second Post, 0.17 ms

Massive EGR

Massive EGR Background - EPA-Ford Data

EPA/Ford MIT Workshop 11/02

Massive EGR Background - Diffusion Burn Engine (Alternative to NOx After treatment)

SwRI Has Extensive Data Base of 8-Mode Data for Cat 3176 2.5 g/hp-hr NOx + HC EngineUse Cycle Simulation to Model Different Levels of EGRAssumed LP Loop EGR After DPFConditions Examined

Baseline - Good Prediction of Existing DataBaseline A/F and Timing + EGR + BoostBaseline Timing + A/F=25:1 + EGR + BoostA/F=15:1 + EGR + Boost + Timing Advance

Massive EGR

NOx

Test Name

Base Variable 25to1 15to1

NO

x (g

/hp-

hr)

0.00.20.40.60.81.01.21.41.61.82.0

BSFC

Test Name

Base Variable 25to1 15to1

BSF

C (g

/kw

-hr)

100

120

140

160

180

200

220

Baseline Engine Around 2 g/hp-hrBSFC Penalty with Variable Due to Back Pressure Increases25:1 A/F Produced Lots of Turbine Energy15:1 A/F Lowered the Air Flow and Boost Requirements

Massive EGR Issue

Cooled EGR

S in the Fuel Raises the Exhaust DewpointConcentration Determines the Concentration of H2SO4 in the Exhaust

NO in the Exhaust Raises the Exhaust Dewpoint

Concentration Determine the Concentration of HNO3 in the Exhaust

H2SO4 in the Exhaust is Directly Related to Fuel S Concentration

Concentation of H2SO4 in ExhaustPhi = 0.5, 0.011 kg/kg Humidity

Exhaust T (K)260 280 300 320 340 360 380 400 420 440 460

Con

cent

ratio

n of

H2S

O4

in E

xhau

st

0

1

2

3

4

5

1000 ppm S

2000 ppm S

5000 ppm S

Concentration of HNO3 in ExhaustPhi=0.5, P=1 atm, 0.011 kg/kg Humidity

Exhaust Temperature (K)260 280 300 320 340C

once

ntra

tion

of H

NO

3 in

Exh

aust

(ppm

)

0

200

400

600

800

500 ppm NO

1000 ppm NO

1500 ppm NO

Exhaust Dew PointPexh = 1 atm, Texh = 40oC

Phi = 0.5, 0.011 kg/kg Humidity

Fuel Sulfur Concentration (% mass)0.00 0.05 0.10 0.15 0.20 0.25

H2S

O4 D

ew P

oint

T (K

)

280

300

320

340

360

380

400

Exhaust Dewpoint Pexh = 1 atm, Texh = 40oC

Phi = 0.5, 0.011 kg/kg Humidity

Concentration of NO in Exhaust (ppm)0 400 800 1200 1600 2000

HN

O3

Dew

poin

t T (K

)

240

260

280

300

320

340

H2SO4 Concentration in ExhaustPhi = 0.5, 0.011 kg/kg Humidity

Fuel Sulfur Concentration (% mass)0.00 0.05 0.10 0.15 0.20 0.25C

once

ntra

tion

of H

2SO

4 in

Exha

ust (

ppm

)

0.00.20.40.60.81.01.21.41.61.82.0

Diffusion Burn Engine Fuel

Conventional Current Diesel Engine Fuel Appetite

Low Aromatics (high H/C Ratio)Lower Flame T and Lower NOxLower Propensity for Soot Formation

High Cetane NumberAdvanced Diesel Engine Fuel Appetite

Mixed Mode (Part Time HCCI and LTC)Low AromaticHigh Cetane Number (at least consistent)

So, Best Diffusion Burn System

Ultra High Injection Pressure and Small HolesMassive EGRUltra High BoostWell Designed Pistons and IntakeHigh Quality Diesel Fuel

Alternative Approaches

Full Time HCCINew Fuel Required

HEDGECould be the Lowest Cost Alternative

Thank You