real-time exhaust particle measurements with a high ......3.7.2015 12 • arffman et al., 2012, the...

12
Real-time exhaust particle measurements with a high-resolution low-pressure cascade impactor P. Karjalainen 1 , A. Arffman 1 , T. Murtonen 2 , P. Aakko 2 , L. Pirjola 3 , S. Niemi 4 , J. Keskinen 1 , T. Rönkkö 1 1 Tampere University of Technology 2 VTT Technical Research Centre of Finland Ltd 3 Helsinki Metropolia University of Applied Sciences 4 University of Vaasa

Upload: others

Post on 26-Nov-2020

1 views

Category:

Documents


0 download

TRANSCRIPT

Page 1: Real-time exhaust particle measurements with a high ......3.7.2015 12 • Arffman et al., 2012, The influence of nozzle throat length on the resolution of a low pressure impactor -

Real-time exhaust particle measurements with a high-resolution

low-pressure cascade impactor

P. Karjalainen1, A. Arffman1, T. Murtonen2, P. Aakko2, L. Pirjola3, S. Niemi4, J. Keskinen1,

T. Rönkkö1

1Tampere University of Technology 2VTT Technical Research Centre of Finland Ltd

3Helsinki Metropolia University of Applied Sciences 4University of Vaasa

Page 2: Real-time exhaust particle measurements with a high ......3.7.2015 12 • Arffman et al., 2012, The influence of nozzle throat length on the resolution of a low pressure impactor -

Contents

• Motivation • Instrument design • Calibration • Vehicle/engine measurements

– Heavy-duty diesel engine – Diesel passenger car – Gasoline passenger car

• Conclusions

3.7.2015 2

Page 3: Real-time exhaust particle measurements with a high ......3.7.2015 12 • Arffman et al., 2012, The influence of nozzle throat length on the resolution of a low pressure impactor -

Motivation

• Electrical detection combined to a cascade impactor provides a real-time measurement technique of aerodynamic particle size distribution (ELPI; Keskinen et al., 1992)

• Current ELPI: wide size range but low channel resolution in the sub-100 nm particle size range (4 channels), and particle bounce

• Aim is to maximize the nanoparticle resolution of ELPI by confining the measurement size range to ~ 5 – 200 nm (typical for exhaust aerosols)

• This is achieved by introducing a new HRLPI cascade impactor for ELPI

3.7.2015 3

Page 4: Real-time exhaust particle measurements with a high ......3.7.2015 12 • Arffman et al., 2012, The influence of nozzle throat length on the resolution of a low pressure impactor -

Design considerations of HRLPI

• Short throat length slit nozzles (Arffman et al., 2012) steep cut-curves and minimized overlap of kernel functions

• Separate pressure reduction inlet possible to adjust correct impactor upstream pressure + smaller fine particle losses

• Low jet velocities by using high slip correction regime minimized particle bounce probability

• Sensitivity vs. pumping capacity: low sample flow rate compensation with an efficient charger

3.7.2015 4

Page 5: Real-time exhaust particle measurements with a high ......3.7.2015 12 • Arffman et al., 2012, The influence of nozzle throat length on the resolution of a low pressure impactor -

HRLPI components

3.7.2015 5

• Impactor fits to ELPI body • 10 impactor stages and a filter stage • Sample flow rate 1.1 lpm • Operation pressure 40 mbar • Pressure reduction with a separate inlet:

atmospheric 40 mbar • Size range ~ 5 – 200 nm • Lowest cutpoint stage 7.7 nm, largest

cutpoint 142 nm • A miniature corona charger

Unipolar charger (+ optional trap)

Connection to ELPI electrometers

(Arffman et al., 2014)

HRLPI impactor stage

Page 6: Real-time exhaust particle measurements with a high ......3.7.2015 12 • Arffman et al., 2012, The influence of nozzle throat length on the resolution of a low pressure impactor -

• Electrical calibration method (Keskinen et al., 1999) • Monodisperse particles through a DMA or SCAR instrument (Yli-Ojanperä et al., 2010)

Calibration results

3.7.2015 6

Pn Collection efficiency

Kernels Bounce probability

(Arffman et al, 2015)

da (nm)

dmob (nm)

• High steepness

• Minor cross talk

Page 7: Real-time exhaust particle measurements with a high ......3.7.2015 12 • Arffman et al., 2012, The influence of nozzle throat length on the resolution of a low pressure impactor -

Laboratory tests

3.7.2015 7

DEHS DEHS and NaCl

Through a DMA

• Cutpoint concept: C = I/PneQ

dp (nm) dp (nm)

Page 8: Real-time exhaust particle measurements with a high ......3.7.2015 12 • Arffman et al., 2012, The influence of nozzle throat length on the resolution of a low pressure impactor -

Heavy-duty nonroad diesel engine (Tier 4i)

3.7.2015 8

All particles Nonvolatile particles

Sampling: porous tube diluter, ageing chamber, ejector diluter, (thermodenuder), instruments

Page 9: Real-time exhaust particle measurements with a high ......3.7.2015 12 • Arffman et al., 2012, The influence of nozzle throat length on the resolution of a low pressure impactor -

100 200 300 400 500 600

101

102

HRLPI

d a (nm

)

0

5x 106

100 200 300 400 500 600

101

102

EEPS

d mob

(nm

)

0

5x 106

Diesel passenger car, w/o aftertreatment, US06 cycle

3.7.2015 9

100 200 300 400 500 6000

50

100

time (s)

spee

d (m

ph)

Soot + condens.

Engine braking (Rönkkö et al. 2014)

da < dmob

Page 10: Real-time exhaust particle measurements with a high ......3.7.2015 12 • Arffman et al., 2012, The influence of nozzle throat length on the resolution of a low pressure impactor -

GDI passenger car, UDC part of EUDC

10 To do… Real-time particle density analysis by combining EEPS and HRLPI results

Page 11: Real-time exhaust particle measurements with a high ......3.7.2015 12 • Arffman et al., 2012, The influence of nozzle throat length on the resolution of a low pressure impactor -

Conclusions

• HRLPI is designed to operate in the typical particle size range of vehicle exhaust aerosols

• Sharp cut-curves succesfully implemented to a cascade impactor

• Lowest impaction stage cutpoint 7.7 nm • Bounce probability minimal • Increasing native resolution keeps de-convolution and

interpretation of results simple • Real-time exhaust particle density analysis is possible

when aerodynamic and mobility particle size distributions are measured simultaneously (e.g. HRLPI & EEPS)

3.7.2015 11

Page 12: Real-time exhaust particle measurements with a high ......3.7.2015 12 • Arffman et al., 2012, The influence of nozzle throat length on the resolution of a low pressure impactor -

Thank you!

3.7.2015 12

• Arffman et al., 2012, The influence of nozzle throat length on the resolution of a low pressure impactor - an experimental and numerical study, J. Aerosol Sci, 53, 76-84

• Arffman et al., 2014, High-Resolution Low-Pressure Cascade Impactor, J. Aerosol Sci. 78, 97–109 • Arffman et al., 2015, The critical velocity of rebound determined for sub-micron silver particles with a

variable nozzle area impactor, J. Aerosol Sci., 86, 32-43 • Keskinen et al., 1992, Electrical Low Pressure Impactor, J. Aerosol Sci. 23, 353-360 • Keskinen et al., 1999, Electrical calibration method for cascade impactors, J. Aerosol Sci., 30, 1, 111-116 • Rönkkö et al., 2014, Vehicle Engines Produce Exhaust Nanoparticles Even When Not Fueled. Environ. Sci.

Technol. 48, 2043-2050 • Yli-Ojanperä et al., 2010, Towards traceable particle number concentration standard: Single charged

aerosol reference (SCAR), J. Aerosol Sci. 41, 719-728 • Yli-Ojanperä et al., 2010, Improving the Nanoparticle Resolution of the ELPI, Aerosol Air Qual. Res., 10,

360-366

References

Acknowledgements Exhaust particle experiments have been executed in TREAM and CLEEN MMEA research projects with financial and material support from AGCO Power Oy, CLEEN Oy, Dinex Ecocat Oy, Ab Nanol Technologies Oy, Neste Oil Oyj and Tekes.