Factors Impacting EGR Cooler Fouling – Main Effects...

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Page 1 DEER 2010 Emissions Controls Technologies, Part 2 Factors Impacting EGR Cooler Fouling – Main Effects and Interactions 16 th Directions in Engine-Efficiency and Emissions Research Conference Detroit, MI – September, 2010 Dan Styles, Eric Curtis, Nitia Ramesh Ford Motor Company – Powertrain Research and Advanced Engineering John Hoard, Dennis Assanis, Mehdi Abarham University of Michigan Scott Sluder, John Storey, Michael Lance Oakridge National Laboratory

Transcript of Factors Impacting EGR Cooler Fouling – Main Effects...

Page 1DEER 2010

Emissions Controls Technologies, Part 2

Factors Impacting EGR Cooler Fouling –Main Effects and Interactions

16th Directions in Engine-Efficiency and Emissions Research ConferenceDetroit, MI – September, 2010

Dan Styles, Eric Curtis, Nitia RameshFord Motor Company – Powertrain Research and Advanced Engineering

John Hoard, Dennis Assanis, Mehdi AbarhamUniversity of Michigan

Scott Sluder, John Storey, Michael LanceOakridge National Laboratory

Page 2DEER 2010

Benefits and Challenges of Cooled EGR• Benefits

Enables more EGR flow Cooler intake charge temp Reduces engine out NOx

by reduced peak in-cylinder temps

NOx

PM

Increasing EGR Rate

Increasing EGR Cooling

• Challenges More HC’s/SOF More PM More heat rejection More condensation HC/PM deposition in

cooler (fouling) degraded heat transfer and higher flow resistance

After 200 hr. Fouling Test

Page 3DEER 2010

What is EGR Cooler Fouling?

• Deposition of Exhaust Constituents on EGR Cooler Walls Decreases heat transfer effectiveness and increases flow restrictiveness

Page 4DEER 2010

Previous DEER Conferences• DEER 2007

Benefits of an EGR catalyst for EGR Cooler Fouling Reduction• DEER 2008

Overview of EGR Cooler Fouling Literature Search Results of initial controlled fouling experiment

High gas flow velocities reduce exhaust constituent trapping efficiency Low coolant temperatures increase Hydrocarbon condensation An oxidation catalyst is only marginally helpful at eliminating the heavier

Hydrocarbons that are likely to condense in an EGR cooler

• DEER 2009 Further results from controlled fouling experiment Complex interaction between PM and HC HC’s are more likely to increase mass of deposits PM more likely to decrease heat transfer Initial results of 1D EGR Cooler Fouling model

Page 5DEER 2010

DEER 2010• Present results of a large, full factorial DOE including

key factors impacting EGR cooler fouling Gas temperature Coolant temperature Gas flow rate Hydrocarbon concentration Particulate matter concentration

• Use an improved controlled EGR cooler fouling sampler that improves repeatability and accuracy of temperature and flow rate controls

• Experiments are short term (3 hours) and use simplified round Ø ¼” tubes

• Show updated modeling results

Page 6DEER 2010

What Causes EGR Cooler Fouling?

EGR Cooler Fouling

Cooler Design

Shell-and-Tube

Fin-Type

Aspect Ratio

Operating ModeSteady State

Transient

Constituents

PM/SOF

HC

Boundary Conditions

Gas Temps

Coolant Temp

Gas Flow Rate Shutdowns

Chemistry

Reactions

Acids

Page 7DEER 2010

Improved EGR Cooler Fouling Sampler

4X cooled tubes

4X critical flow orifices w/ pre-heating

Thermocouple positioning features added

• Air pre-heating added to eliminate startup transients

Exhaust Gas

Page 8DEER 2010

Improved EGR Cooler Fouling Sampler, cont’d

More consistent positioning of thermocouples leads to close repeatability

of effectiveness data for tube replicates

Less drop off in mass flow rate over time due to heating upstream of critical flow orifice

Tube A

Tube B

Page 9DEER 2010

Test Engine and Conditions

• 2008MY 6.4L Turbo-Diesel• 3 hours steady-state @ 2250 rpm / 300 ft-lbf• 1.5 FSN• 35 ppm C1 HC• 385°C exhaust temperature• CP Chem 2007 ULS Certification Diesel (≈ 47 Cetane)

Heated Line

Flow Control Section

Cooled Removable

Tubes

DPF

To PM/HC Measurement

Optional injector and DPF to achieve “low” PM & “high”

HC levels

Page 10DEER 2010

Experimental Factor Levels

• Average Gas Velocity: 13.5 and 22 m/s via critical flow orifices (chosen to represent range of typical range)

• Gas Inlet Temperature: 220 & 380ºC• Coolant Temperature: 40 & 90ºC• PM Levels: 0.4 FSN ( or 7.5 μg/l via uncatalyzed DPF)

and 1.5 FSN (30 μg/l or natural level)• HC Levels: 35 ppm C1 (natural) and 250 ppm C1

(achieved via downstream diesel fuel injector)• Coating: An “anti-coking” tube coating was also included

as a sixth factor in a fractional factorial DOE

• Note: Factor levels varied “outside of cylinder” to avoid confounding effects. Gas pressure constant ≈ 7 psig.

Page 11DEER 2010

Experimental Structure and Response Variables

• Full factorial DOE with replicates• 32 * 2 replicates / 4 tubes = 16 runs • Response variables include

Absolute heat transfer effectiveness loss

Deposit mass gain Deposit “high level” speciation

Light volatile (fuel HC’s, water) Heavy volatile (oil) Non-volatile (soot, ash, inorganics)

Deposit layer sectioning, microscopy, thickness

ε = = qactual

qmax theoretical

Tgas,in – Tgas,out

Tgas,in – Tcoolant

Page 12DEER 2010

Effectiveness Loss Main Effects

Mea

n of

Eff

ect

Loss

(%

)

22.013.5

10

8

6

4

380220 1.50.4

25035

10

8

6

4

9040

Flow Rate (m/s) Inlet Temp (C) PM (FSN)

HC (PPM) Coolant Temp (C)

Main Effects Plot (data means) for Effect Loss (%)

Higher inlet temperatures more thermophoresis More thermophoresis more PM deposition More PM deposition more effectiveness loss Also, higher flow rate double mass flow higher effectiveness loss

Page 13DEER 2010

Deposit Mass Accumulated Main Effects

Lower coolant temperatures more Hydrocarbon condensation More Hydrocarbon condensation more mass gain Higher PM levels also resulted in higher mass gains, but not higher

flow rate (double mass exposure) and higher inlet temperature! Interesting interactions ….

Mea

n of

Tot

al G

ain

(mg)

22.013.5

28

24

20

16

12380220 1.50.4

25035

28

24

20

16

129040

Flow Rate (m/s) Inlet Temp (C) PM (FSN)

HC (PPM) Coolant Temp (C)

Main Effects Plot (data means) for Total Gain (mg)

Page 14DEER 2010

Interactions

Non-parallel lines indicate an interaction between factors Intersecting lines indicates a strong interaction between factors For example: For total deposit mass accumulated several 2-way and

higher interactions are statistically significant! The physics are complicated!

Flow Rate (m/s)

380220 1.50.4 25035 9040

30

20

10

Inlet Temp (C)

30

20

10

PM (FSN)

30

20

10

HC (PPM)

30

20

10

Coolant Temp (C)

13.522.0

(m/s)RateFlow

220380

(C)TempInlet

0.41.5

(FSN)PM

35250

(PPM)HC

Interaction Plot (data means) for Total Gain (mg)

Flow Rate (m/s)

380220 1.50.4 25035 904012

8

4

Inlet Temp (C)

12

8

4

PM (FSN)

12

8

4

HC (PPM)

12

8

4

Coolant Temp (C)

13.522.0

(m/s)RateFlow

220380

(C)TempInlet

0.41.5

(FSN)PM

35250

(PPM)HC

Interaction Plot (data means) for Effect Loss (%)

Page 15DEER 2010

Light Volatile Mass Accumulated Main Effects

Sources are diesel fuel, other light volatiles. Accounts for ½ mass gain. Some trends as expected (HC concentration, coolant temperature). Others puzzling (half the mass gain with double the exposure)! Key point: Deposit layer thermal conductivity variable & important.

Mea

n of

Lig

ht G

ain

(mg)

22.013.5

15

10

5

380220 1.50.4

25035

15

10

5

9040

Flow Rate (m/s) Inlet Temp (C) PM (FSN)

HC (PPM) Coolant Temp (C)

Main Effects Plot (data means) for Light Gain (mg)

Page 16DEER 2010

Impact of Tube “Anti-coking” Coating

½ fraction factorial with added factor of anti-coking coating. No impact on effectiveness loss. “Center-points” indicate linear

responses. Coating increases mass gain? Responses are not linear between

factor levels.

Mea

n of

Tot

al G

ain

(mg)

30.022.515.0

50

40

30

20

10385.0297.5210.0 30.0018.757.50

250.0142.535.0

50

40

30

20

10906540 YesNo

Flow Rate (lpm) Inlet Temp (C) PM (ug/l)

HC (ppm) Cool Temp (C) Coating

CornerCenter

Point Type

Main Effects Plot (data means) for Total Gain (mg)

Mea

n of

Eff

ect

Loss

%

30.022.515.0

12

10

8

6

4385.0297.5210.0 30.0018.757.50

250.0142.535.0

12

10

8

6

4906540 YesNo

Flow Rate (lpm) Inlet Temp (C) PM (ug/l)

HC (ppm) Cool Temp (C) Coating

CornerCenter

Point Type

Main Effects Plot (data means) for Effect Loss %

Page 17DEER 2010

Cooled Tube Microscopy, Sectioning

205

µm

6 hours, 30 SLPM, High HC, Low Coolant Temp

Metal

Deposit

• Deposit thicknesses were measured by milling the tube metal to ~2 mils and then breaking it open thereby revealing the deposit cross-section.

• From this and the mass measurement, the density of the deposit was determined. • High HC and low coolant temperatures increased the deposit density.

Exposure Time (hr) Flow Rate (SLPM) HC Coolant Temp

Density (g/cc) StDev (g/cc)

0.5 15 High Low 0.069 0.0411 15 High Low 0.104 0.0346 15 High Low 0.077 0.03812 15 High Low 0.054

0.5 30 High Low 0.050 0.0273 30 High Low 0.056 0.0106 30 High Low 0.064 0.016

0.5 30 Low High 0.037 0.0254 30 Low High 0.043 0.00812 30 Low High 0.032

Page 18DEER 2010

Modeling Overview

A schematic of the surrogate tube and the heat transfer model

• Thermophoresis, the only dominant deposition force on soot particles

• No physical verification for deposit stabilization in long exposures

• Possible hypotheses for stabilization: Kinetic theory removal mechanism Variable deposit thermal

conductivity

• Subroutines for EGR properties calculation • Calculating of density, viscosity, thermal

conductivity of a mixture including four components (CO2, H2O, N2, O2 )

• Variable thermal conductivity of deposit layer• Variable sticking and removal coefficients• Radiation, convection, and conduction heat

transfer mechanisms included

Model features: Key Physics:

Page 19DEER 2010

Variable Thermal Conductivity of LayerThe equivalent thermal conductivity is calculated as:

avgTEGRGraphitedeposit kkk 25.05.1)1( ϕϕ +−=

FluidSolidcluster kkk 25.05.1)1( ϕϕ +−=

In our study, the solid can be assumed asGraphite and EGR as the fluid:

Trapped GasSolid Phase

depositkConstant porosity 98%.

porosity=ϕ

Page 20DEER 2010

Short Exposure Time• Different thermo-hydraulic conditions.

• The comparison for soot mass gain along the tubes and the effectiveness drop of thesurrogate tubes after 3 hours (short exposure) are in a reasonable agreement with ORNLdata.

• Comparable results for short exposure times with no removal and variable depositproperties.

Page 21DEER 2010

Long Exposure Time

• Literature: the sticking probability of soot nanoparticles is assumed 100%!

• The removal rate to match the data in first 8 hours is too much for the second phase when deposition stops!

Criterion for removal: Kinetic Energy > Van der Waals Energy

Literature: removal coefficient proportional to drag/ bond force ratio.

• No physical verification yet for removal mechanisms! Matching the data with the proposed kinetic theory.

Page 22DEER 2010

Key Conclusions• Thermophoresis substantiated as key PM deposition

mechanism.• PM is penalizing to heat transfer effectiveness.• HC’s are more penalizing to deposit mass accumulation.• There are several statistically significant interactions between

the key factors impacting cooler fouling.• The physics are complicated.• Capturing deposit layer thermal conductivity changes due to key

factors such as flow velocity, gas temperatures, HC levels, etc. is key to any successful modeling exercise for EGR cooler fouling.

• The deposits in these shorter-term experiments consisted of light volatiles and non-volatiles in roughly equal proportions on average (mass basis).

• The effect of the anti-coking coating is inconclusive.

Page 23DEER 2010

Thanks for Your Attention

• Questions?

Page 24DEER 2010

Heavy Volatile Mass Accumulated Main Effects

Sources are lube oil and partially oxidized productions of combustion Levels are small relative to light volatile and non-volatile. Trends as expected. Higher flow rates, higher PM (SOF), higher HC

levels, lower coolant temperatures.

Mea

n of

Hea

vy G

ain

(mg)

22.013.5

1.8

1.6

1.4

1.2

1.0

380220 1.50.4

25035

1.8

1.6

1.4

1.2

1.0

9040

Flow Rate (m/s) Inlet Temp (C) PM (FSN)

HC (PPM) Coolant Temp (C)

Main Effects Plot (data means) for Heavy Gain (mg)

Page 25DEER 2010

Non-volatile Mass Accumulated Main Effects

Trends as expected … higher flow rates, inlet temperatures and PM levels increase non-volatile mass gain.

Higher HC’s and lower coolant temperatures increase HC condensation … and PM sticking.

Mea

n of

Soo

t Ga

in (

mg)

22.013.5

15.0

12.5

10.0

7.5

5.0380220 1.50.4

25035

15.0

12.5

10.0

7.5

5.09040

Flow Rate (m/s) Inlet Temp (C) PM (FSN)

HC (PPM) Coolant Temp (C)

Main Effects Plot (data means) for Soot Gain (mg)