A four-stroke single-cylinder research diesel engine (80kW nominal power) was operated on either MGO (FSC = 0.01 S w%) or LS-HFO (FSC = 0.5 S w%) at low engine load (20kW, 25% of nominal power), representing docking maneuvers. Raw exhaust emissions were connected to diluters via heated tubing (constant at 350°C), see Fig. 3. A series configuration of a porous tube diluter and an ejector diluter was employed to achieve a dilution ratio of 1:250. The dilution ratio was determined by measuring the CO₂ concentrations in the raw exhaust, the diluted exhaust, and the dilution air. The dilution ratio was regulated by automatically adjusting the flow rate of the porous tube diluter, while maintaining a constant flow rate for the ejector diluter.
The diluted (1:250) exhaust sample passed through the oxidation flow reactor “Photochemical Emission Aging flow tube Reactor” (PEAR), which was operated at a flow rate of 100 lpm. 25 At these flow conditions, the mean residence time in the PEAR is 70 s. At the entrance to the PEAR 10ppm of ozone was added in addition to water vapor keeping the relative humidity (RH) at approximately 50%. The photochemical aging was controlled through UV-lamp(254nm) intensity, water vapour supply for 50% relative humidity and constant ozone (10ppm) addition in order to obtain atmospheric aging equivalent to 0 to 9 days (supplementary table S7). The photochemical age was determined with d9-butanol decay measured by a Proton-transfer-reaction mass spectrometry (PTR-MS) based on the principle of the “photochemical clock”.26 The Kinsim27–31 model was used to verify the atmospheric relevancy by simulating the chemistry within the PEAR, by determining the RO2 fate to remove speculations on non-tropospheric chemistry occurring in the OFR. (supplementary table S7-9)
An additional ejector diluter was added after the PEAR for a further 10-fold dilution before online instruments, resulting in a total dilution ratio of 1:2500 for aerosol instruments presented here. Aerosol phase measurement were done with High-Resolution Time of Flight Aerosol Mass Spectrometer (HR-ToF-AMS)32 for obtaining the chemical composition of the non-refractory aerosol, aethalometer for BC and a scanning mobility particle sizer (SMPS) for particle number concentration and size distribution. SMPS data was treated with the AIM V. 10.3.1.0 software.
Optically defined black carbon (BC), “equivalent black carbon" (eBC), was quantified by the Aethalometer (AE33-7, Aerosol Magee Scientific), which measures light attenuation through a filter tape at 7 wavelengths (UV–IR, 370–950 nm). Using different corrections, such as multiple-scattering correction and loading compensation, attenuation coefficients were converted to absorption coefficients, and further to black carbon concentrations. A mass absorption coefficient (MAC) was used to quantify light absorption as a mass concentration. Absorption at 880 nm is generally assumed to be only caused by BC. Thus, the equivalent black carbon mass concentrations (\(\:eBC\)) was calculated (Eq. 1)
$$\:eBC=\frac{A\bullet\:\left(\frac{\varDelta\:ATN}{100}\right)}{{F}_{meas}\bullet\:\left(1-\zeta\:\right)\bullet\:\left(1-k\bullet\:AT{N}_{t}\right)*\varDelta\:t\bullet\:C\bullet\:MAC}\:,\:(eq.1)$$
where \(\:A\) is the surface area of the filter spot, \(\:\varDelta\:ATN\) the change of attenuation at 880nm during a time interval \(\:\varDelta\:t\), \(\:{F}_{meas}\) the measured flow rate, \(\:\zeta\:\) the leakage factor (default value 0.01), \(\:k\) the real-time loading compensation parameter3 \(\:AT{N}_{t}\) the attenuation at time \(\:t\) for 880nm, \(\:C\) the multiple-scattering coefficient (here \(\:C\) = 2.80 based on reference absorption measurement by PAX-870 during the campaign), and \(\:MAC\) the mass absorption coefficient (here \(\:MAC\left(880\:nm\right)\) = 5.47 m2/g, based on reference refractory black carbon (rBC) measurement by LII 300 and elemental carbon (EC) measurement by DRI 2015 during the campaign).
AMS data was treated in Tof-AMS Analysis Toolkit 1.65 (squirrel), and HR analysis was performed with ToF-AMS HR Analysis 1.25 (PIKA). Elemental analysis was performed by the Aiken method (aiken et al. 2007) The AMS was equipped to handle particles with an aerodynamic diameter between 42nm and 645nm. With small aerosol diameters, (supplementary table S12), falling outside the size range of the AMS.
Moreover, to the best of our knowledge no information is available on the density of aged aerosol emissions from ships but aging of aerosol emissions from solid fuel combustion demonstrate a particle size dependent increases in effective density with differences between fuels.33 Therefor the mass of the aerosol is determined by the SMPS, with an assumed density of 1,5+-0,2 g/cm3. Composition of the aerosol is then calculated based on AMS and aethalometer as in Eq. 2.
$$\:{EF}_{x}=\left({EF}_{SMPS}-{EF}_{eBC}\right)\text{*}\frac{Con{c}_{x}}{Con{c}_{ams}},\:\:\:(eq.2)$$
Where \(\:{EF}_{X}\) is the emission factor of an aerosol group, \(\:Con{c}_{x}\) is the concentration of the aerosol group measured by the AMS, \(\:{Conc}_{AMS}\) is the total concentration of aerosols measured by the AMS. \(\:E{F}_{SMPS}\) is the emission factor determined by the SMPS and \(\:E{F}_{eBC}\) is the emission factor of eBC determined by aethalometer. Primary organic aerosol (POA) was determined as the organic fraction with no photochemical aging. The SOA fraction was calculated by subtracting the POA from the total OA mass at a given simulated ageeq.3. Organic enhancement factor was calculated as the fractional increase of organics, see supplement equation Eq. 4.
$$\:SO{A}_{x}=O{M}_{x}-POA,\:\:\:\:\:(eq.3)$$
$$\:Or{g}_{enh,x}=\frac{O{M}_{x}}{POA},\:\:\:\:\:(eq.4)$$
Where POA is the total organic mass at 0 days of atmospheric aging and OMx is the total organic mass at X days of atmospheric aging.