Rainer Vogt, Ulf Kirchner and Matti Maricq, · 1.4E+10 2.1E+10 PN / # s-1 and speed / km h-1 soot...

15
Rainer Vogt, Ulf Kirchner and Matti Maricq, Ford Forschungszentrum Aachen GmbH, Süsterfeldstr. 200, D-52072 Aachen, Germany Ford Motor Company, Dearborn, USA Particle number emissions are measured with two instruments according to the upcoming European emission regulations for light-duty diesel passenger vehicles and compared to data from other methods, including the current regulatory total particulate matter (PM) mass, photo-acoustic soot sensor (PASS) and engine exhaust particle sizer (EEPS). At the very low emission levels of diesel particulate filter (DPF) equipped vehicles, the solid particle number data correlate well with soot mass and with particle number measured by EEPS, if only those particles belonging to the accumulation mode are considered in the latter case. PN differences of >100% between tests of the same vehicle are observed. Comparison of the two PN instruments and the photoacoustic soot sensor show that these are systematic differences which originate primarily with the vehicle and not from instrument uncertainties. After accounting for this, a repeatability of <8% and a reproducibility of <27% are estimated for the particle number method. A large body of new vehicle data is presented from tests carried out immediately after production. The data show that nearly all vehicles would be below the anticipated Euro-5/Euro-6 particle number limit. The observed variability is significant and needs further investigation.

Transcript of Rainer Vogt, Ulf Kirchner and Matti Maricq, · 1.4E+10 2.1E+10 PN / # s-1 and speed / km h-1 soot...

Page 1: Rainer Vogt, Ulf Kirchner and Matti Maricq, · 1.4E+10 2.1E+10 PN / # s-1 and speed / km h-1 soot [mg/m^3] PN [#/s] NEDC speed [km/h] 0 km/h 70 km/h 140 km/h. Research & Advanced

Rainer Vogt, Ulf Kirchner and Matti Maricq, Ford Forschungszentrum Aachen GmbH, Süsterfeldstr. 200, D-52072 Aachen, Germany Ford Motor Company, Dearborn, USA Particle number emissions are measured with two instruments according to the upcoming European emission regulations for light-duty diesel passenger vehicles and compared to data from other methods, including the current regulatory total particulate matter (PM) mass, photo-acoustic soot sensor (PASS) and engine exhaust particle sizer (EEPS). At the very low emission levels of diesel particulate filter (DPF) equipped vehicles, the solid particle number data correlate well with soot mass and with particle number measured by EEPS, if only those particles belonging to the accumulation mode are considered in the latter case. PN differences of >100% between tests of the same vehicle are observed. Comparison of the two PN instruments and the photoacoustic soot sensor show that these are systematic differences which originate primarily with the vehicle and not from instrument uncertainties. After accounting for this, a repeatability of <8% and a reproducibility of <27% are estimated for the particle number method. A large body of new vehicle data is presented from tests carried out immediately after production. The data show that nearly all vehicles would be below the anticipated Euro-5/Euro-6 particle number limit. The observed variability is significant and needs further investigation.

Page 2: Rainer Vogt, Ulf Kirchner and Matti Maricq, · 1.4E+10 2.1E+10 PN / # s-1 and speed / km h-1 soot [mg/m^3] PN [#/s] NEDC speed [km/h] 0 km/h 70 km/h 140 km/h. Research & Advanced

Research & Advanced Engineering

1

Investigation of EURO-5/6 Level

Particle Number Emissions of

European Diesel Light Duty

Vehicles

Rainer Vogt, Ulf Kirchner and Matti Maricq

Ford Motor Company

Aachen/Dearborn

14th ETH Conference, Zürich, August 1-4th, 2010

Page 3: Rainer Vogt, Ulf Kirchner and Matti Maricq, · 1.4E+10 2.1E+10 PN / # s-1 and speed / km h-1 soot [mg/m^3] PN [#/s] NEDC speed [km/h] 0 km/h 70 km/h 140 km/h. Research & Advanced

Research & Advanced Engineering

2

Introduction

Solid particle number (PN) counting required in upcoming European

emission regulation for light-duty diesel: evaporation of volatiles and

dilution of sample from CVS tunnel.

PSP: Particle

Sample

Probe

PTT: Particle

Transfer

Tube

PCF: Particle

Classifier

PND: Particle

Number

Diluter

Page 4: Rainer Vogt, Ulf Kirchner and Matti Maricq, · 1.4E+10 2.1E+10 PN / # s-1 and speed / km h-1 soot [mg/m^3] PN [#/s] NEDC speed [km/h] 0 km/h 70 km/h 140 km/h. Research & Advanced

Research & Advanced Engineering

3

Experimental Setup

• Diesel passenger car 1.6 L w DPF

• New European drive cycles (NEDC) after DPF regeneration /

conditioning.

• In addition to regulated components (CO, HC, NOx, total PM

mass): Two fully calibrated PN instruments in parallel plus

micro soot sensor (MSS). All sampling from full flow CVS.

• Use of calibrated PN instruments: average Particle

Concentration Reduction Factors (PCRF) for 30, 50 and 100

nm. Counter desensitized for small particles, 50% detection

efficiency for 23 nm particles according to upcoming European legislation.

Page 5: Rainer Vogt, Ulf Kirchner and Matti Maricq, · 1.4E+10 2.1E+10 PN / # s-1 and speed / km h-1 soot [mg/m^3] PN [#/s] NEDC speed [km/h] 0 km/h 70 km/h 140 km/h. Research & Advanced

Research & Advanced Engineering

4

PN compared to Soot Mass

All three parallel methods (2x PN and soot mass) show consistent trend.

0.00

0.02

0.04

0.06

0.08

0.10

A1 A2 A3 A4 A5 B1 B2 B3 B4

Test Number

PA

SS

So

ot

Mass [

mg

/km

]

0.0E+00

3.6E+10

7.2E+10

1.1E+11

1.4E+11

1.8E+11

Part

icle

Nu

mb

er

[km

-1]

Soot mg/km

FFA-PMP #/km

AVL489 #/km

first tests after

DPF regeneration

and conditioning

Page 6: Rainer Vogt, Ulf Kirchner and Matti Maricq, · 1.4E+10 2.1E+10 PN / # s-1 and speed / km h-1 soot [mg/m^3] PN [#/s] NEDC speed [km/h] 0 km/h 70 km/h 140 km/h. Research & Advanced

Research & Advanced Engineering

5

Regression Analysis of PN vs. Soot

Very good (R2>0.98) correlation of PN with soot; 1 mg soot corresponds to ~2 x 1012 particles.

y = 1.81E+12x

R2 = 9.82E-01

0.0E+00

2.0E+10

4.0E+10

6.0E+10

8.0E+10

1.0E+11

1.2E+11

1.4E+11

1.6E+11

0.00 0.01 0.02 0.03 0.04 0.05 0.06 0.07 0.08

Soot Mass [mg/km]

Pa

rtic

le N

um

be

r [k

m-1

]

PN [ km^-1]

Linear (PN [ km^-1])

Page 7: Rainer Vogt, Ulf Kirchner and Matti Maricq, · 1.4E+10 2.1E+10 PN / # s-1 and speed / km h-1 soot [mg/m^3] PN [#/s] NEDC speed [km/h] 0 km/h 70 km/h 140 km/h. Research & Advanced

Research & Advanced Engineering

6

Emission Time Traces (1)

Strong decrease of soot and PN emissions after ~200 s, more

than engine out decrease => increasing filter efficiency.

High efficiency level, initial ~99.7% increase to >99.9%

0.0

0.1

0.2

0.3

0 200 400 600 800 1000 1200

time / s

mg

so

ot

/ m

3

0.0E+00

7.0E+09

1.4E+10

2.1E+10

PN

/ #

s-1

an

d s

peed

/ k

m h

-1

soot [mg/m^3]

PN [#/s]

NEDC speed [km/h]

0 km/h

70 km/h

140 km/h

Page 8: Rainer Vogt, Ulf Kirchner and Matti Maricq, · 1.4E+10 2.1E+10 PN / # s-1 and speed / km h-1 soot [mg/m^3] PN [#/s] NEDC speed [km/h] 0 km/h 70 km/h 140 km/h. Research & Advanced

Research & Advanced Engineering

7Emission Time Traces (2)

CO

2 [

%]

0

5

10

15

20

Sp

eed

[km

/h]

-120

-60

0

60

120

To

tal N

um

ber

[Part

./cm

³]

0

2

4

6

8

EEPS

Part

icle

Siz

e D

p [

nm

]

1

10

100

1000

dN

/dlo

g(D

p)

[#/c

m³]

0

Pa

rtic

le S

ize

Dp

[n

m]

CO

2

8.0x106

6.0x106

4.0x106

2.0x106

0.0

0

0

100

200

300

400

500

600

700

800

900

1000

1100

1200

Time [s]

• Euro-4 DPF vehicle

• tailpipe sampling with FPS and EEPS

M. Bergmann et al., ETH Conference 2008; Atmospheric Environment 43, 1908-1916 (2009)

=> some PN measurable during cold start

=> very low PN during remainder

almost no nucleation mode particles

Page 9: Rainer Vogt, Ulf Kirchner and Matti Maricq, · 1.4E+10 2.1E+10 PN / # s-1 and speed / km h-1 soot [mg/m^3] PN [#/s] NEDC speed [km/h] 0 km/h 70 km/h 140 km/h. Research & Advanced

Research & Advanced Engineering

8

Solid vs. total PN

Total PN measured by TSI Engine Exhaust Particle Sizer (EEPS) ishigher than solid PN >23 nm as expected.

Best match for EEPS >40 nm: different measurement principle, no specific calibration.

0.0E+00

2.0E+11

4.0E+11

6.0E+11

8.0E+11

1.0E+12

1.2E+12

1.4E+12

1.6E+12

1.8E+12

T1 T2 T3 T4

Test Number

Part

icle

Nu

mb

er

[#/k

m]

0

2E+11

4E+11

6E+11

8E+11

1E+12

1.2E+12

1.4E+12

1.6E+12

1.8E+12FFA-PMP #/kmAVL489 #/kmEEPS #/kmEEPS >40 nm #/kmEEPS >23 nm #/km

Page 10: Rainer Vogt, Ulf Kirchner and Matti Maricq, · 1.4E+10 2.1E+10 PN / # s-1 and speed / km h-1 soot [mg/m^3] PN [#/s] NEDC speed [km/h] 0 km/h 70 km/h 140 km/h. Research & Advanced

Research & Advanced Engineering

9Particle mass vs. PN

• Non-DPF vehicles: very good correlation of PM mass with PN.

• DPF vehicles: correlation overwhelmed by artifacts of filter methods (~0.5 mg/km). Good correlation for soot, same slope as non-DPF => similar particles (size, density).

y = 1.81E+12x

R2 = 9.82E-01

y = 2.17E+12x

R2 = 9.72E-01

1.0E+09

1.0E+10

1.0E+11

1.0E+12

1.0E+13

1.0E+14

0.00 0.01 0.10 1.00 10.00 100.00

PM or Soot Mass [mg/km]

Part

icle

Nu

mb

er

[km

-1]

PN vs. SootPN vs. PM massDISI PN vs. PMLinear (PN vs. Soot)Linear (PN vs. PM mass)

soot & PM of the same 9 tests

1 mg =

~2 x 1012

particles

Non-DPF

vehicles

(13 tests)

DPF vehicle (9

tests, each with

PM mass and

soot measured

by a PASS)

Page 11: Rainer Vogt, Ulf Kirchner and Matti Maricq, · 1.4E+10 2.1E+10 PN / # s-1 and speed / km h-1 soot [mg/m^3] PN [#/s] NEDC speed [km/h] 0 km/h 70 km/h 140 km/h. Research & Advanced

Research & Advanced Engineering

10

Testing Variability

• Testing of new, conditioned vehicles at the production plant.

• Large variability of different vehicles of same type and model.

Even for the same vehicle >10% difference at 2nd test.

• Effect of vehicle or method? Error analysis required.

0.0E+00

1.0E+11

2.0E+11

3.0E+11

4.0E+11

5.0E+11

6.0E+11

7.0E+11

8.0E+11

1 1 2 3 4 5

Test Number

PN

[#/k

m]

0.0E+00

1.0E+11

2.0E+11

3.0E+11

4.0E+11

5.0E+11

6.0E+11

7.0E+11

8.0E+11

10 20 30 40 50

same vehicle type and modelvehicle tested twice

Page 12: Rainer Vogt, Ulf Kirchner and Matti Maricq, · 1.4E+10 2.1E+10 PN / # s-1 and speed / km h-1 soot [mg/m^3] PN [#/s] NEDC speed [km/h] 0 km/h 70 km/h 140 km/h. Research & Advanced

Research & Advanced Engineering

11

Error Estimation I: Repeatability

Error propagation of inputs in formula to calculate PN results:

Main contributions to repeatability identified:

• PNC flow. Daily measurements over several months: ±2%.

• Repetition of PCRF calibration, i.e. stability of PN dilution: ± 5%.

CVS volume(∆V/V) 1%

distance (∆d/d) 0.2%

PNC counting accuracy (∆k/k) 0%

PNC flow (∆C/Cs) 2%

PCRF uncertainty, daily (∆fr/fr) 5%

Volatile particles 0%

CVS tunnel background 0.02% - 0.2%

total repeatability ± 8%

Repeatability (one CVS / PN instrument)

d

fCkV rsN

610××××

=

Page 13: Rainer Vogt, Ulf Kirchner and Matti Maricq, · 1.4E+10 2.1E+10 PN / # s-1 and speed / km h-1 soot [mg/m^3] PN [#/s] NEDC speed [km/h] 0 km/h 70 km/h 140 km/h. Research & Advanced

Research & Advanced Engineering

12

Error Estimation II: Reproducibility

Main contributions to reproducibility:

• PNC flow. Daily measurements of 2 instruments: ±5%.

• PNC counting accuracy. Difference between 2 instruments,

which are within legal limits: ±10%.

• PCRF uncertainty. Comparison of 2 instruments with real diesel exhaust size distribution

- instrument “at the limit”, 70%, 80% and 100% penetration

- “low losses” instrument, 90%, 95% and 100% penetration for

particle sizes 30, 50 and 100 nm, respectively: ±10%.

CVS volume(∆V/V) 1%

distance (∆d/d) 0.2%

PNC counting accuracy (∆k/k) 10%

PNC flow (∆C/Cs) 5%

PCRF uncertainty (∆fr/fr) 10%

Volatile particles 1%

CVS tunnel background 0.02% - 0.2%

total reproducibility ± 27%

Reproducibility (several CVS facilities / PN instruments)

Page 14: Rainer Vogt, Ulf Kirchner and Matti Maricq, · 1.4E+10 2.1E+10 PN / # s-1 and speed / km h-1 soot [mg/m^3] PN [#/s] NEDC speed [km/h] 0 km/h 70 km/h 140 km/h. Research & Advanced

Research & Advanced Engineering

13

Summary and Conclusions I

• PN differences of >100% between tests of the same vehicle.

• Comparison of two PN instruments and correlation to a

photoacoustic soot sensor at extremely low emission levels

(<0.08 mg/km): differences are mostly variability of the vehicle.

• Estimations for PN method repeatability: ~8% and reproducibility

~27%. Good numbers for aerosol measurements.

• Following regeneration the DPF efficiency increases from 99.7%

to 99.97% relative to the same vehicle without a DPF.

Formation of a soot cake is a likely explanation, but needs

further investigation.

• Solid PN emissions of newly manufactured DPF Diesel vehicles

showed test to test variability with a CoV up to 110%. This

needs to be taken into account when emission standards are discussed.

Page 15: Rainer Vogt, Ulf Kirchner and Matti Maricq, · 1.4E+10 2.1E+10 PN / # s-1 and speed / km h-1 soot [mg/m^3] PN [#/s] NEDC speed [km/h] 0 km/h 70 km/h 140 km/h. Research & Advanced

Research & Advanced Engineering

14

Summary and Conclusions II

• Good correlation observed between PN emissions and soot mass, which corresponds to 2 x 1012 particles per mg.

• Correlation of solid PN to soot mass extends from DPF

equipped to non-DPF vehicles. This is consistent with soot as dominant component of modern, oxidation catalyst equipped,

light duty diesel vehicles and a uniformly high filtration efficiency

of DPFs versus particle size.

• The upcoming European legal limit of 6 x 1011 particles/km

corresponds to 0.3 mg/km soot, which is over an order of

magnitude more stringent than the PM mass limit of 4.5 mg/km.

• Comparison of solid PN emissions to the accumulation mode

particles measured with an EEPS shows that nucleation

particles are effectively removed by the regulation compliant

solid particle count instruments.

• Please also see Kirchner et al. SAE 2010-01-0789