Nanoparticles - Primary and secondary organic aerosols from a … · 2016. 4. 13. · 1995 2000...

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Primary and Primary and secondary organic aerosols secondary organic aerosols from a diesel car during smog chamber from a diesel car during smog chamber experiments experiments Roberto Roberto Chirico Chirico Laboratory of Atmospheric Chemistry Paul Scherrer Institut, Switzerland [email protected] 13 TH ETH Conference, 22-24 June 2009

Transcript of Nanoparticles - Primary and secondary organic aerosols from a … · 2016. 4. 13. · 1995 2000...

  • Primary andPrimary and secondary organic aerosols secondary organic aerosols

    from a diesel car during smog chamber from a diesel car during smog chamber experimentsexperiments

    Roberto Roberto ChiricoChirico

    Laboratory of Atmospheric ChemistryPaul Scherrer Institut, Switzerland

    [email protected]

    13TH ETH Conference, 22-24 June 2009

  • Why are we interested in aerosol particles ?Why are we interested in aerosol particles ?

    Direct radiative forcingScattering and absorption of solar and infrared radiation Indirect radiative forcingAlteration of the formation and precipitation efficiency of liquid water, ice and mixed-phase clouds

    Health effectRespiratory and carcinogenic effects

    Importance of aerosol size (d < 1µm) and composition (PAHs associated to particles)

    VorführenderPräsentationsnotizenAfter the first 2 interesting talk Ican skipmy first slide but before that I want to add that the aerosols can haave also an health effect..Aerosol particles can have an effect on the climate changes and they can have an health effect and those effects depend on…..Concerning the climate changes up to day there are big uncentanties associated to aerosols

    http://immagini.p2pforum.it/out.php/i234505_13teschio800.jpg

  • Diesel passenger carsDiesel passenger cars

    (ACEA, 2008; EPA, 2002; Automotive Industry Data Newsletter )

    Number of new diesel passenger cars in Europe

    0.16

    0.14

    0.12

    0.10

    0.08

    0.06

    0.04

    0.02

    0.00

    DPM

    [g/k

    m]

    2010200520001995Year

    EURO 1 (1992)

    EURO 2 (1996)

    EURO 3 (2000)

    EURO 4 (2005)

    EURO 5 (2009)

    EURO 6 (2014)

    EU Emission Standards for Diesel Particulate Matter

    VorführenderPräsentationsnotizenAn important source of particles are diesel vehicles

  • Dilution effect on PM massDilution effect on PM mass

    (Robinson et al., Science 2007; Lipsky and Robinson, ES&T 2006)

    Fine particulate mass with initial OM/BC=2 can

    decrease by 50% when dilution ratio is increased

    from 20:1 to 350:1

    Primary Organic Aerosols (POA) contains Semi-

    Volatile Organic Compounds (SVOCs) that

    partially evaporate.

  • Primary and Secondary organic aerosolsPrimary and Secondary organic aerosols

    Primary Organic Aerosols

    High temperature

    Ambient temperatureLow dilution ratio (10-100)

    Ambient temperatureHigh dilution ratio

    (1000-10000)Secondary Organic

    Aerosols

    OH

    O3NO3

    hv

    (Robinson et al., Science 2007)

    POA constituents as non volatileOA mainly present in urban areas

    POA main constituent of OA

    POA constituents as volatile

    Decrease of OA

    Photochemical aging of SVOCs

    Considerable amount of Urban and Regional

    SOAtime < 1 sec

  • Set up for smog chamber experimentsSet up for smog chamber experiments

    Clean air generator

    Smog Chamber

    Heated Diluter (150°C)

    Pressurised air heater (150°C)

    Ambient air Excess air

    Heatedline (150°C)Heated line (150°C)

    EURO 3 Diesel car

    Diluter

    1:84

    1:8

    CO2 Analyzer CO2 Analyzer

    SMPS

    AMS

    CPCAethalometer

    CO, NO, NOx, O3 Analyzer

    60 L/min60 L/min

    7 L/min7 L/min

    DC

    PAS

    Drier

    Dilution factors: 300-1200

    Idle – 60 km/h

  • HRHR--ToFToF--AMS and AMS and AethalometerAethalometer

    (De Carlo et al., Anal. Chem. 2006; Weingartner

    et al., Aerosol Sci. 2003)

    3 5

    3 0

    2 5

    2 0

    1 5

    1 0

    5

    0

    µg/m

    3

    543210T im e a f te r l ig h ts o n (h r s )

    T e m p o r a l e v o lu t i o n O r g a n i c M a t te r ( H R - T o F - A M S ) T e m p o r a l e v o lu t i o n B la c k C a r b o n ( A e th a lo m e t e r )

    Aerosols are internally mixedBC can be used as tracer for chamber wall loss

    [ ])/BC(t)BC(tOM(t) MeasuredOM(t) Estimated 0×=

    VorführenderPräsentationsnotizenThe ecrease of BC is due to wall losses..

  • 6 0

    5 0

    4 0

    3 0

    2 0

    1 0

    0

    µg/m

    3

    543210T im e a fte r lig h ts o n (h rs )

    1 .4

    1 .2

    1 .0

    0 .8

    0 .6

    0 .4

    0 .2

    0 .0

    Characteristic aging experiment Characteristic aging experiment of diesel exhaustof diesel exhaust

    Primary aerosols consist mainly of BC with a low fraction of Organic Matter (OM)Photo-oxidation of gaseous organics produces SOA

    VorführenderPräsentationsnotizenMass absorption efficiency doesn‘t change with time

  • Starting POA concentration assumed constant

    Primary and Secondary organic aerosolsPrimary and Secondary organic aerosols

    60

    50

    40

    30

    20

    10

    0

    µg/m

    3

    543210Tim e after lights on (hrs)

    SO A

    PO A

    BC

  • SOA contribution to total organic massSOA contribution to total organic mass

    After 5 hours of aging SOA is 30-80 % of the Total Organic Aerosols

    100

    80

    60

    40

    20

    0

    % P

    OA

    543210Time after lights on (hrs)

    Idle 60 km/h

    SOA (60 km/h)

    SOA (Idle)

    [ ] 100)/OM(t)POA(t%POA(t) 0 ×=

    VorführenderPräsentationsnotizenNow let‘s have a look at the differences between POA and the OOA….

  • OrganicOrganic

    Aerosol Mass Aerosol Mass SpectraSpectra

    Discrimination between ions with the same nominal mass

    Ions grouped into 4 different organic classes depending on the atom combination

    Average mass spectrum for an ensemble of submicron particles with a time resolution of few seconds

    High resolving power (2000-5000)

    1 4

    1 2

    1 0

    8

    6

    4

    2

    0

    Rel

    ativ

    e In

    tens

    ity (%

    )

    8 07 57 06 56 05 55 04 54 03 53 0m / z

    C H C H O C H N C H O N

    VorführenderPräsentationsnotizenWe can do this because with the AMS we can obtain the MS of the organic aerosols

  • m/zHydrocarbon-like Organic Aerosols

    (Fragmentation pattern similar to that one of long chain hydrocarbons)

    Photochemically Aged Organic Aerosols

    OrganicOrganic

    Aerosol Mass Aerosol Mass SpectraSpectra

    fromfrom

    dieseldiesel

    exhaustexhaust

    m/z

  • OrganicOrganic

    Aerosol Mass Aerosol Mass SpectraSpectra

    fromfrom

    dieseldiesel

    exhaustexhaust

    Higher contribution of the CHO family to the organic aerosols after 5 hours of aging

  • AtomicAtomic

    ratiosratios

    and OM/BC and OM/BC ratiosratios

    O/C and OM/OCH/C

    OM/OC (POA)= 1.28-1.33(60 km/h) (idle)

    VorführenderPräsentationsnotizenfor those people interested in the measurements of organic carbon I think that it is important to say that the om to oc values for POA that I measured were 1.28 and 1.33

  • ConclusionsConclusions

    Fresh aerosols from an Euro 3 diesel car consist mainly of BC (OM/BC=0.2-0.3)

    POA is an Hydrocarbon-like Organic Aerosol

    Diesel cars can contribute to SOA (30- 80% after 5 hrs of aging)

    During the aging Organic Aerosols get more oxidized

    VorführenderPräsentationsnotizenI have started my talk with this picture and I will conclude with this one as well because I think that my conclusions might be interesting for those people involved in the studies of global warming and health effectsIt is important to learn more about the composition of SOA

    http://immagini.p2pforum.it/out.php/i234505_13teschio800.jpg

  • Thanks toThanks to…………..

    M. Heringa, P. M. Heringa, P. DeCarloDeCarlo, T. , T. TritscherTritscher, , E. Weingartner, G. E. Weingartner, G. WehrleWehrle, , R. Richter, A.S.H. R. Richter, A.S.H. PrevotPrevot, , and U. and U. BaltenspergerBaltensperger

  • Thank you for your attentionVielen Dank für Ihre Aufmerksamkeit

    Merci pour votre attention Grazie per la vostra attenzione

    http://www.chrismadden.co.uk

    [email protected]@psi.ch

  • Filling

    the

    chamber in ~15 min

    Euro 3 diesel

    car

    running

    at 60 km per hour

    AgingAging

    of of dieseldiesel

    exhaustexhaust

    in in thethe

    PSI PSI smogsmog

    chamberchamber

  • 200

    150

    100

    50

    0

    09:4505.11.2008

    10:00 10:15 10:30 10:45 11:00dat

    dat

    09:4507.11.2008

    10:00 10:15 10:30

    09:00 09:15 09:30 09:45 10:00

    dat

    Tem p_051108 (60 km/h) Tem p_171108 (idle) Tem p_071108 (60 km/h) Tem p_211108

    200-210 °C

    82 °C

    Exhaust temperatureExhaust temperature

  • Diesel Oxidation CatalystDiesel Oxidation Catalyst

    the oxidation of NO to NO2 is constrained kinetically at low temperatures and thermodynamically at higher temperatures

  • 1.0

    0.8

    0.6

    0.4

    0.2

    0.0

    OM

    /BC

    13 012 01101009080Tem p era tu re e xh au st

    Idlin g m od e600 R PMC on su m ptio n 0.6 l/h

    Direct measurement: Temperature effectDirect measurement: Temperature effect

  • 1 . 2

    1 . 0

    0 . 8

    0 . 6

    0 . 4

    0 . 2

    OM

    /BC

    543210

    A V G _ O M B C _ id le A V G _ O M B C _ 6 0 k m h

    0.80+/-0.36

    0.44+/-0.20

    OM/BCOM/BC

  • Size distributionSize distribution

    2

    3

    4

    56789

    100

    2

    3

    4

    5

    6

    Size

    [nm

    ]

    20151050

    H.A .L .O .(h rs)

    2 .0x10 41 .51 .00 .50 .0

    dN /d logDp

    31-01-2008

    idle

  • 3 .0

    2 .5

    2 .0

    1 .5

    1 .0

    0 .5

    0 .0

    OM

    /BC

    1 6 01 4 01 2 01 0 08 06 04 02 00O rg a n ic lo a d in g

    O n ly 0 6 0 0 -1 8 3 0 in te rv a ls

    O M o v e rB C _ 0 6 0 0 _ 1 8 3 0 O M o v e rB C _ E M P A -S ilk e O M o v e rB C _ S m o g C h a m b e r

    OM/BC OM/BC vsvs

    OrgOrg

  • OM/OC OM/OC vsvs

    O/CO/C

    Diesel fuelsC10-C25 hydrocarbon mixtures

    Lubricating oilsC14-C45 hydrocarbon mixtures

    OM/OC (C10-C45 long chain alkanes) 1.17 -1.19

  • VOC/NOVOC/NOXX

    ratioratio

    2 6 0

    2 4 0

    2 2 0

    2 0 0

    1 8 0

    1 6 0

    1 4 0

    1 2 0

    1 0 0

    8 0

    6 0

    4 0

    2 0

    0

    ppb

    2 01 51 050H . A . L . O . ( h r s )

    O z o n e _ M L N O _ M L N O x _ M L

    OzonePropene

    High NOX

    (~NO) conc. from diesel exhaust

    OH reacts about 5.5 times more rapidly with NO2

    than with an average urban VOC mix

    VOC/NOX

    ratio needs to be increased

    NO2

    NO

    O

    O2

    O3

    sunTermination

    by NOx

    Initiation RO :Photolysis of

    O , Aldehydes, HONO

    x

    3

    OHHNO3

    H

    RCH (OH)2

    RCH O2 2

    HO2

    RCH O2

    RCO

    RCH (ROG)3

    CO

    RCHO

    Terminationby RO + ROx x

    H O2 2RCH OOH2

    ORCO

    RCO2O

    PAN'sHO2+

    + HO2

    +

    NO2

    +O2

    +

    +

    +

    or Addition

    SubstractionH O2

    O2++ O2

    + O2

    CO2

    CO2

    + O2

    H O2

  • HRHR--ToFToF--AMSAMS

    (MS mode)(MS mode)

    (Jayne et al., 2000; De Carlo et al., 2006)

    Turbo Pump (~1E-3 Torr)

    Turbo Pump (~1E-8 Torr)

    Particle Inlet (1 atm)

    AerodynamicLens (2 Torr)

    SAMPLING CHAMBER

    AERODYNAMIC SIZING

    CHAMBER

    Thermal Vaporization

    (600°C)and

    Electron Ionization

    (70 eV)

    Critical orifice(100 µm) DETECTION

    CHAMBER

    QuadrupoleMass Spectrometer

    Chopper (150 Hz)

    e-

  • Composition of diesel emissionsComposition of diesel emissions

    (Schneider et al., ES&T 2005)

    Primary Organic Aerosols (POA)

    100-200 nmagglomerated particles

    consisting of solid carbonaceous material

    with adsorbed organics and sulfates

  • Composition of the organic fractionComposition of the organic fraction

    (Schauer et al., ES&T 1999)

    Hundreds of different organic compounds

    AldehydesKetonesAlkanesPAHs

    TOTAL ORGANICS

    8%

    4%

    1%

    4%

    1%

    0%

    42%10%

    1%

    0%

    29%

    ALKANESALKENESALKYNESMONOCYCLIC AROMATICPAHsHOPANE AND STERANESALDEHYDESKETONESACIDSTOTAL OTHERSUnresolved Complex Mixture

  • Diesel particle number concentrationDiesel particle number concentration

    THE TOTAL PARTICLE NUMBER HAS

    DECREASED WITH NEWER DIESEL

    ENGINES

    (Burtscher, 2005; Kittelson et al., 1998; www.dieselnet.com)

    Older diesel cars

    → high conc of soot particles→ large surface areaNewer diesel cars

    → low conc of soot particles → little surface area → nucleation

    more likely

    PARTICLE NUMBER IN THE NUCLEI MODE HAS

    INCREASED WITH NEWER DIESEL CAR WITH

    PARTICLE TRAP

  • Kelvin effectKelvin effect

    The saturation vapor pressure is defined as the equilibrium partial pressure for a plane (flat) liquid surface at a given temperature. If the liquid surface is sharply curved,

    such as the surface of a small droplet, the partial pressure required to maintain mass equilibrium is greater than that for a flat surface. The curvature of the surface modifies slightly the attractive forces between surface molecules, so that the smaller the droplet, the easier it is for molecules to leave the droplet surface. To prevent this evaporation-that is, to maintain mass equilibrium-

    the partial pressure of vapor surrounding the droplet must be greater than ps.

    For pure liquids, the relationship between the saturation ratio required for equilibrium (no growth or evaporation), called the Kelvin ratio Kr, and the droplet size is given the Kelvin equation

    Kr=pd/ps=exp(4γM/ρRTd)

    γ

    =surface

    tension

    M=molecular

    weight

    Ρ=density

    of the

    droplet

    liquid

    D=Kelvin

    diameter, the

    diameter

    of the

    droplet

    that

    will neither

    grow

    nor

    evaporate

    when

    the

    partial pressure

    of vapor

    at the

    droplet

    surface

    is

    pd

    This

    equation

    defines

    a specific

    saturation

    ratio

    required

    to mantain

    mass equilibrium

    for

    a given

    particle

    size

    d

    WdV

    forces

    = 1/R6

    (Hinds, 1999)

  • Gas-particle partitioning of organics

    Absorption into the aerosol organic matter

    6om

    0Lom

    omP 10pMW

    RT760fKγ

    =

    GasGas--particle partitioningparticle partitioning

    (Pankow, Atm

    Environ 1994)activitypressure,vapor ,MW

    matter organic offraction phase org

    ATSP/F

    PK =

    F (ng/m3) is the particulate-associated concentration of orgTSP is the concentration of the total suspended particulate (µg/m3)A (ng/m3) is the gas-phase concentration of org

    omigi ff ,, =0,,, iLomomiomi pf γχ=Ideal conditions: fi=pi RT

    pmmoli

    Vn

    igi

    760)/( 3, =

    VorführenderPräsentationsnotizenThe gas-particle partitioning of organics can be describe by Absorption into the aerosol organic matter

  • The absorption coeffcient

    (babs

    ) is defined with Beer–Lambert’s law

    where I0

    is the intensity of the incoming light and I the remaining light intensity after passing through a medium with the thickness x. The attenuation (ATN) is typically given as percentage values and is defined by the relationship

    Aethalometers

    measure the light attenuation through a quartz filter matrix where the fiber filter is assumed to act as a perfect diffuse scattering matrix in which the light-absorbing particles are embedded.

    According to the Beer–Lambert’s law, the aerosol absorption coefficient of the filtered aerosol particles bATN (or attenuation coefficient) is defined as

    where A is the filter spot area (m2), Q the volumetric flow rate

    (m3/s)and ΔATN is the change in attenuation during the time interval Δt.It

    is well known that bATN

    may differ significantly from the true aerosol absorption coeffcient

    babs of airborne particles. Therefore, the calibration factors C and R(ATN) are introduced, which can be used to convert aethalometer

    attenuation measurements to “real”

    absorption coefficients:

    Absorption coefficient

    (m-1)

    C and R describe the two effects which change the optical properties of filter embedded particles with respect to the properties of the same particles in the airborne state

    C

    = is greater than unity and is caused by multiple scattering of

    the light beam at the filter fibers in the unloaded filter. This leads to an enhancement of the optical path and thus to enhanced light absorption of the deposited particles. C depends on the λ. It was experimentally determined during smog chamber studies a C = 2.14±

    0.21

    Attenuation coefficient (m-1) of the system composed by filter and particles is measured

    R(ATN) =

    varies with (a) the amount of aerosol particles embedded in the filter and (b) optical properties of the deposited particles. For unloaded filters R is set to unity, i.e. R(ATN = 0) = 1. With the gradual increase in attenuation due to the accumulating particles in the filter the absorbing particles in the filter absorb a higher

    fraction of the scattered light which leads to a reduction of the optical path in the filter (R¡1). As a consequence, generally lower attenuation coefficients are measured for higher filter loadings than for lightly loaded filters (Shadowing effect)The aerosol black carbon mass concentration MBC

    (gm −3) is related to the absorption and attenuation coefficients bywhere σabs

    and σATN

    ≡ σabs

    ·C are the mass specific absorption and attenuation cross-sections (m2 g−1), respectively. σATN

    strongly depends on the aerosol type and age. They depend on λ.σATN

    ≡ σabs

    ·C Mass specific attenuation cross-sections (m2/g). σATN (λ=880 nm)=16.6 m2/g (this

    value

    is

    given

    by

    the

    manual)bATN

    and σATN

    relate light attenuation to BC mass in the case of filter based

    measurement method while babs

    and σabs

    are used for suspended particle in the air

  • Q Q vsvs

    ToFToF

    SpectrometersSpectrometers

    ––

    Time Time resolutionresolution

    6≈VV~

    D

    zeEsmDt

    2=

    A COMPLETE MASS SPECTRUM IS

    ACQUIRED EVERY 12 µs

    A MASS SPECTRUM IS SCANNED OVER A MASS

    RANGE OF m/z 1-300 WITHIN 300ms

    E

    QQ ToFToF

    m/z=100

    Shorter averaging time for representative particle counting statistics

  • UNIVERSAL AND QUANTITATIVE CHEMICAL ANALYSIS

    Positive IonMass

    Spectrometry

    Vaporizer

    e-

    ELECTRON EMITTINGFILAMENT

    R+

    FOCUSED PARTICLE BEAM

    FLASHVAPORIZATION

    OF NON-REFRACTORYCOMPONENTS (NR)

    600 °C ELECTRON IMPACT

    IONIZATION

    Evaporation/ionizationEvaporation/ionization

    chamberchamber

    The term ‘non-refractory’

    (NR) is defined operationally as those species that evaporate rapidly (

  • Water H2

    O H2

    O+

    , HO+

    , O+

    18,

    17, 16Ammonium

    NH3

    NH3+, NH2+, NH+

    17, 16, 15Nitrate HNO3

    HNO3+, NO2+, NO+

    63, 46, 30

    Sulfate

    H2

    SO4 H2

    SO4+, HSO3+, SO3

    + 98, 81, 80

    SO2+, SO+

    64, 48Organic Cn

    Hm

    Oy

    H2

    O+, CO+, CO2+

    18, 28, 44(Oxygenated) H3

    C2

    O+,

    HCO2+, Cn’

    Hm+ 43, 45, ...

    Organic

    Cn

    Hm Cn’

    Hm’+

    27,29,41,43,55,57,69,71...(hydrocarbon)

    Group Molecule/Species

    Ion Fragments

    Mass Fragments

    e-e-

    e-

    e-

    e-

    e-

    Standard electron impact ionization @ 70 eVEasy to quantify Comparable to the NIST MS libraryEasy to separate inorganic and organic componentsSpeciation of organic composition is challenging

    MS Signatures for Aerosol Species IdentificationMS Signatures for Aerosol Species Identification

  • Terminal velocity is obtained when the gravitational force (FG) is equal and opposite to the drag force

    Continuum Regime Aerodynamic Diameter

    for irregular particles ofstandard density, dm > dve

    > da

    Vacuum Aerodynamic Diameter

    dm dm vsvs

    dvadva

  • SensitivitySensitivity

    The V-Mode

    data show detectable signal up to

    m/z 1300

    The lower sensitivity of W-mode

    results in detectable signal up to

    m/z 700

    (De Carlo et al., 2006)

  • (Arey

    et al., 1989; Reisen

    and Arey, 2005; EEA, 2006)

    1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24

    Hour of the day

    No

    scal

    e

    Oxidant

    concentrations

    in urban

    areas

    O3

    conc

    = 80-150 ppbNOX

    conc

    = 30-80 µg/m3(Milano 150 µg/m3)

    NO3

    conc

    = 1×1010

    molecules/cm3

    (nighttime) OH

    conc

    =5-10×106

    molecules/cm3 (summertime)

    Oxidant concentrations and diurnal variationOxidant concentrations and diurnal variation

    ·NO2

    + hν

  • Zhang et al., GRL 2007

    Worldwide

    AMS measurements

    show

    the

    abundance of organics

    in the

    atmospheric

    aerosol

  • Worldwide

    AMS measurements

    show

    the

    abundance of organics

    in the

    atmospheric

    aerosol

    Zhang et al., GRL 2007

  • FractionsFractions

    of BC, OM, NO3, SO4 and NH4 of BC, OM, NO3, SO4 and NH4 and fossil and and fossil and nonnon--fossilfossil

    contributioncontribution

    to EC and OCto EC and OC

    Nearly identical composition

    Black CarbonOrganic massNitrateSulfateAmmonium

    Black CarbonOrganic massNitrateSulfateAmmonium

    Z_meanPM10

    ECbb4% ECfossil

    17%

    OCfossil23%

    OCnonfossil56%

    Z_meanPM10

    ECbb4% ECfossil

    17%

    OCfossil23%

    OCnonfossil56%

    Zürich

    16%30%

    14%

    6%

    34%

    Zürich

    16%30%

    14%

    6%

    34%

    R_mean

    ECbb5%

    ECfossil17%

    OCfossil22%

    OCnonfossil56%

    R_mean

    ECbb5%

    ECfossil17%

    OCfossil22%

    OCnonfossil56%

    7%

    15%

    34%11%

    33%

    Reiden

    7%

    15%

    34%11%

    33%

    Reiden

    Urban background Highway/rural

  • 13%

    60%

    13%

    7%7%

    Zürich (July)

    11%

    32%

    15%

    27%

    1%

    14%

    Zürich (January)

    Black CarbonOrganic massNitrateSulfateAmmonium

    AverageAverage

    compositioncomposition

    in Zin Züürich in rich in summersummer

    and and winterwinter

  • Lanz et al., ACP (2007)

    Organic mass13%

    60%

    13%

    7%7%

    Zürich (July)

    Black CarbonOrganic massNitrateSulfateAmmonium

    OOA: Secondary organic aerosol

    HOA: mostly traffic

    Chemical Chemical compositioncomposition

    in Zin Züürich rich summersummer

    andand

  • Z_meanPM10

    ECbb4% ECfossil

    17%

    OCfossil23%

    OCnonfossil56%

    Zürich (mean)

    Use of AMS analysis :

    - wood burning 38%

    - HOA 7%

    Assumptions :

    -

    only SOA, HOA and wood burning present

    -

    OM/OC=2 for wood burning and SOA and OM/OC=1.2 for HOA

    -

    RESULT : SOAnonfossil: 69% SOAfossil: 31%

    (biomass burning)

    38%

    7%17%

    38% Wood burning

    Traffic

    Secondary(fossil)Secondary(non-fossil)

    81%

    19%

    EC (fossil)

    EC (non-fossil)

    OM

    EC

    CarbonCarbon

    apportionmentapportionment

    usingusing

    14C 14C analysisanalysis EstimationEstimation

    of fossil and of fossil and nonnon--fossilfossil

    SOA SOA contributioncontribution

  • InorganicsInorganics--S.CS.C..

    60 km/h

    date_60 OM/BC CO/NOx CO/CO2 OM/(BC*CO2) NO/NOx

    110408 0.413 0.254652 0.00050322 0.004945473 0.982716109

    71108 0.397 0.025746 0.00010761 0.005113857 0.899252778

    211108 0.18 0.012236 3.1328E-05 0.00149138 0.922717961

    70109 0.201 0.044092 0.00010491 0.001052584 0.938656715

    90408 1.2612 0.691773 0.00152673 0.019011913 0.954776135

    51108 0.5089 0.00078636

    Idle

    date_idle OM/BC_idle CO/Nox_idle CO/CO2_idle OM/(BC*CO2)_idle NO/NOx_idle

    100308 0.176 0.275182 0.00271439 0.003667389 0.900077229

    40408 0.304 0.249277 0.00247813 0.00452191 0.904475671

    171108 0.102 0.232615 0.00248073 0.002273959 0.940398773

  • 1 0 0

    8 0

    6 0

    4 0

    2 0

    0

    org

    9 : 4 5 A M4 / 3 / 2 0 0 9

    9 : 5 0 A M 9 : 5 5 A M 1 0 : 0 0 A M 1 0 : 0 5 A M 1 0 : 1 0 A M

    d a t

    5 0 0

    4 0 0

    3 0 0

    2 0 0

    1 0 0

    0

    BC

    0 . 4

    0 . 2

    0 . 0

    OM

    /BC

    1 . 0

    0 . 8

    0 . 6

    0 . 4

    0 . 2

    0 . 0

    Frac

    tion

    9 : 5 0 A M4 / 3 / 2 0 0 9

    9 : 5 5 A M 1 0 : 0 0 A M 1 0 : 0 5 A M 1 0 : 1 0 A M

    D a t e a n d T i m e

    M F _ P A H M F _ C h l M F _ N H 4 M F _ N O 3 M F _ S O 4 M F _ B C M F _ O r g

    HDDVHDDV

  • 0.4

    0.3

    0.2

    0.1

    0.0

    2:05 PM4/2/2009

    2:10 PM 2:15 PM 2:20 PM 2:25 PM 2:30 PM 2:35 PM

    dat

    2:35 PM4/8/2009

    2:40 PM 2:45 PM 2:50 PM 2:55 PM 3:00 PM 3:05 PM

    dat

    20

    15

    10

    5

    0

    2:00 PM 2:05 PM 2:10 PM 2:15 PM 2:20 PM 2:25 PM 2:30 PM 2:35 PM

    dat

    O MoverBC_090402_1 (HD DV) O MoverBC_090406_3 (HD DV) O MoverBC_090408_3 (Diesel-E3-10 ppm) org_090408_3 org_090402_1 org_090406_3

    60 km/h 90 km/h

    HDDV HDDV vsvs

    Diesel E3 passenger carDiesel E3 passenger car

  • DPM DPM compositioncomposition

    1.0

    0.8

    0.6

    0.4

    0.2

    0.0

    Frac

    tion

    4:00 PM4/16/2009

    4:05 PM 4:10 PM 4:15 PM

    Date and Time

    MF_PAH MF_Chl MF_NH4 MF_NO3 MF_SO4 MF_BC MF_Org

    Diesel Euro 4

    1.0

    0.8

    0.6

    0.4

    0.2

    0.0

    Frac

    tion

    4:40 PM4/8/2009

    4:45 PM 4:50 PM 4:55 PM

    Date and Time

    MF_PAH MF_Chl MF_NH4 MF_NO3 MF_SO4 MF_BC MF_Org

    Diesel Euro 3

  • E4 E4 gasolinegasoline

    carcar

    60

    50

    40

    30

    20

    10

    0

    11:1520.04.2009

    11:30 11:45 12:00

    dat

    60

    50

    40

    30

    20

    10

    0

    10

    8

    6

    4

    2

    0

    Foliennummer 1Why are we interested in aerosol particles ?Diesel passenger cars�Dilution effect on PM massPrimary and Secondary organic aerosolsSet up for smog chamber experimentsFoliennummer 7Characteristic aging experiment �of diesel exhaustFoliennummer 9SOA contribution to total organic massOrganic Aerosol Mass SpectraOrganic Aerosol Mass Spectra from diesel exhaustOrganic Aerosol Mass Spectra from diesel exhaustAtomic ratios and OM/BC ratiosConclusionsThanks to…….Foliennummer 17Foliennummer 18Foliennummer 19Foliennummer 20Foliennummer 21Foliennummer 22Size distributionFoliennummer 24OM/OC vs O/CVOC/NOX ratioHR-ToF-AMS (MS mode)Composition of diesel emissionsComposition of the organic fractionDiesel particle number concentrationKelvin effectFoliennummer 32Foliennummer 33Q vs ToF Spectrometers – Time resolutionFoliennummer 35Foliennummer 36Foliennummer 37SensitivityOxidant concentrations and diurnal variationFoliennummer 40Worldwide AMS measurements show the abundance �of organics in the atmospheric aerosolFoliennummer 42Foliennummer 43Chemical composition in Zürich summer andFoliennummer 45Inorganics-S.C.Foliennummer 47Foliennummer 48DPM compositionE4 gasoline car