Sally E. Pusede, Trevor C. VandenBoer, Jennifer G. Murphy, Milos Z. Markovic, Cora J. Young,

Similar documents
Supplement of SOA formation from the photooxidation of α-pinene: systematic exploration of the simulation of chamber data

Figure S1. Configuration of the CIMS inlet during the KORUS-AQ 2016.

AQRP Project Implementation and evaluation of new HONO mechanisms in a 3-D Chemical Transport Model for Spring 2009 in Houston

Preliminary report: Analyses of tcfp s potential impact on atmospheric ozone

Supplement of Iodine oxide in the global marine boundary layer

A SPARC Success Story: The Role of Halogen Chemistry in Polar Stratospheric Ozone Depletion

Received 8 November 2012; revised 19 December 2012; accepted 24 December 2012; published 31 January 2013.

Supplement of Organic nitrate aerosol formation via NO 3 + biogenic volatile organic compounds in the southeastern United States

Supplementary Material for: A Comparison of the chemical sinks of atmospheric organics in the gas and aqueous phase

Appendix B: Aqueous chemistry and gas-phase halogen chemistry

NF 3 : UV absorption spectrum temperature dependence and the atmospheric and climate forcing implications

On the Satellite Determination of Multilayered Multiphase Cloud Properties. Science Systems and Applications, Inc., Hampton, Virginia 2

Measurements of HONO during OASIS in Barrow, Alaska

Supplemental material

Tropospheric NO 2 column densities deduced from zenith-sky DOAS measurements in Shanghai, China, and their application to satellite validation

Satellite-based estimate of global aerosol-cloud radiative forcing by marine warm clouds

Land Surface Temperature in the EUMETSAT LSA SAF: Current Service and Perspectives. Isabel Trigo

Simulated Radiances for OMI

M-RICh v0.5 MATLAB Rate Integrator for Chemical equations

Trip and Parking Generation Study of Orem Fitness Center-Abstract

Solar UV radiation and microbial life in the atmosphere

frequency R 2 =0.99 y=1.01x modelled O 4 Correspondence to: Yang Wang y=1.02x-1.44

Supplement of Non-methane hydrocarbon variability in Athens during wintertime: the role of traffic and heating

Observations of the effects of temperature on atmospheric HNO3,?ANs,?PNs, and NOx: evidence for a temperature-dependent HOx source

FRAPPÉ/DISCOVER-AQ (July/August 2014) in perspective of multi-year ozone analysis

FINAL REPORT An Assessment of Nitryl Chloride Formation Chemistry and its Importance in Ozone Non-attainment areas in Texas. AQRP Project

Ongoing EPA efforts to evaluate modeled NO y budgets. Heather Simon, Barron Henderson, Deborah Luecken, Kristen Foley

On the Interpretation of Shortwave Albedo-Transmittance Plots

SUPPORTING INFORMATION

Land-cloud-climate Coupling on the Canadian Prairies

TOTAL COLUMN OZONE AND SOLAR UV-B ERYTHEMAL IRRADIANCE OVER KISHINEV, MOLDOVA

2016 EXPLANATION OF OBSERVATIONS BY REFERENCE NUMBER

Α neural network based prediction method for troposheric ducting over the Hellenic region

Coupling Climate to Clouds, Precipitation and Snow

Supplement of Inversion of and

Surface-Atmosphere Exchange of Ammonia in a Non-fertilized Grassland and its Implications for PM 2.5

Ozone production rates as a function of NO x abundances and HO x production rates in the Nashville urban plume

Direct effects of particle precipitation and ion chemistry in the middle atmosphere

Optical Turbulence Model for Laser Propagation and Imaging Applications

Nocturnal loss and daytime source of nitrous acid through reactive uptake and displacement

Supporting Information

Supplement of Observation of isoprene hydroxynitrates in the southeastern United States and implications for the fate of NO x

Supplementary Information for Fatty acid Surfactant. Photochemistry Results in New Particle Formation

CREATE Summer School. Tim Canty

Symposium for the 30 th Anniversary of the Montreal Protocol. The Impact of Laboratory Photochemistry on the Montreal Protocol. James B.

Supplemental Material Table 1

A New Mechanism for Regional Atmospheric Chemistry Modelling. A contribution to subproject CMD. W.R. Stockwell', F Kirchner^ M. Kuhn' and S.

List of Exposure and Dose Metrics

Supplement of Cloud and aerosol classification for 2.5 years of MAX-DOAS observations in Wuxi (China) and comparison to independent data sets

Radiative Climatology of the North Slope of Alaska and the Adjacent Arctic Ocean

Testing and improving OMI DOMINO tropospheric NO 2 using observations from the DANDELIONS and INTEX B validation campaigns

Chapter 3. Materials and Methods

Air temperature environment on the debriscovered area of Lirung Glacier, Langtang Valley, Nepal Himalayas

Chasing Aerosol Particles Down to Nano Sizes

Evaluation of Spatial Gradients and Temporal Trends of Black Carbon in Boston MA. George Allen

Analysis of Data from the 2009 SOOT Experiment

Arctic Halogen Chemistry Part II

Aircraft Observations of the Lower Atmosphere and Surface Exchange Processes. Jennifer Murphy Department of Chemistry, University of Toronto

Chemical sources and sinks of Hg(II) in the remote atmospheric marine boundary layer

Chapter 2 Available Solar Radiation


R. Fröhlich et al. Correspondence to: A. Prévôt

Central Ohio Air Quality End of Season Report. 111 Liberty Street, Suite 100 Columbus, OH Mid-Ohio Regional Planning Commission

ESE / GE 148a: Introduction to Climate. Organizational Details - I

4.5 Comparison of weather data from the Remote Automated Weather Station network and the North American Regional Reanalysis

Learning Objectives. Thermal Remote Sensing. Thermal = Emitted Infrared

Radiation and the atmosphere

and Atmospheric Science, University of Miami, 4600 Rickenbacker Causeway, Miami, FL 33149, USA.

Relation of atmospheric humidity and cloud properties to surface-near temperatures derived from GOME satellite observations

1. The frequency of an electromagnetic wave is proportional to its wavelength. a. directly *b. inversely

Monitoring daily evapotranspiration in the Alps exploiting Sentinel-2 and meteorological data

Chapter 1 Solar Radiation

Lecture 14. Principles of active remote sensing: Lidars. Lidar sensing of gases, aerosols, and clouds.

Griffith Observatory Field Trip Guide

Parking Study MAIN ST

GLAS Team Member Quarterly Report

PMF ANALYSIS OF WIDE-RANGE PARTICLE SIZE SPECTRA COLLECTED ON A MAJOR HIGHWAY ROY M. HARRISON, DAVID C. S. BEDDOWS AND MANUEL DALL OSTO

Lavinia Onel, Alexander Brennan, Freja F. Østerstrøm, Michele Gianella, Lisa Whalley, Gus Hancock, Paul Seakins, Grant Ritchie and Dwayne Heard

Gas/particle partitioning of water-soluble organic aerosol in Atlanta

Determining correction factors for seasonal and regional variability in

Supplementary Figures

Supplementary Appendix

Actinometric measurements of NO 2 photolysis frequencies in the atmosphere simulation chamber SAPHIR

What is PRECIS? The Physical Parameters Boundary Conditions Why the Mediterranean Basin? The Sulfur Cycle & Aerosols Aerosols Impacts Data Analysis

On my honor, I have neither given nor received unauthorized aid on this examination. YOUR TEST NUMBER IS THE 5-DIGIT NUMBER AT THE TOP OF EACH PAGE.

Table of Contents. Page

Spatial bias modeling with application to assessing remotely-sensed aerosol as a proxy for particulate matter

Supplement of Photochemical grid model implementation and application of VOC, NO x, and O 3 source apportionment

Measurements of a potential interference with laser-induced fluorescence measurements of ambient OH from the ozonolysis of biogenic alkenes

ASTR 101L: Motion of the Sun Take Home Lab

Laboratory Exercise #7 - Introduction to Atmospheric Science: The Seasons and Daily Weather

Surface UV Irradiance Obtained by Ozone Monitoring Instrument (OMI) Over Peninsular Malaysia

Supporting Information for. Suppression of OH Generation from the Photo-Fenton Reaction in the Presence of α-pinene Secondary Organic Aerosol Material

9.4. The newly released 5-year Terra-based monthly CERES radiative flux and cloud product. David R. Doelling, D. F. Keyes AS&M, Inc.

BIRA-IASB, Brussels, Belgium: (2) KNMI, De Bilt, Netherlands.

Relative humidity and its effect on aerosol optical depth in the vicinity of convective clouds

Supplement of Studying the vertical aerosol extinction coefficient by comparing in situ airborne data and elastic backscatter lidar

Global Atomic Oxygen Abundance in the Upper Mesosphere and Lower Thermosphere as Measured by SCIAMACHY

1 A 3 C 2 B 4 D. 5. During which month does the minimum duration of insolation occur in New York State? 1 February 3 September 2 July 4 December

G109 Midterm Exam (Version A) October 10, 2006 Instructor: Dr C.M. Brown 1. Time allowed 50 mins. Total possible points: 40 number of pages: 5

Transcription:

SUPPLEMENTAL INFORMATION for An Atmospheric Constraint on the NO 2 Dependence of Daytime Near- Surface Nitrous Acid (HONO) Sally E. Pusede, Trevor C. VandenBoer, Jennifer G. Murphy, Milos Z. Markovic, Cora J. Young, Patrick R. Veres, James M. Roberts, Rebecca A. Washenfelder, Steven S. Brown, Xinrong Ren, Catalina Tsai, Jochen Stutz, William H. Brune, Eleanor C. Browne, Paul J. Wooldridge, Ashley R. Graham, Robin Weber, Allen H. Goldstein, Sebastien Dusanter, Stephen M. Griffith, Philip S. Stevens, Barry L. Lefer, and Ronald C. Cohen Supplementary information contains pages S1 S12 and Figures S1 S8. S1

NO 2 Weekday-Weekend Patterns In Bakersfield, higher NO 2 was observed at night before midnight on weekends. This is driven by higher NO x on Sunday nights and appears to be a consistent feature of the NO x time series. We hypothesize this pattern is due to emissions from the heavy-duty diesel truck fleet, which, having been parked for the weekend, begins the workweek on Sunday evening. In Pasadena, where a large portion of the local NO x is emitted in upwind Los Angeles, integrated weekend daytime (8 am 4 pm LT) NO 2 is lower on weekends, but there is a shift in timing of peak daytime concentrations. This is consistent with previous accounts of diurnal profiles of mobile NO x emissions by day of week. 1 In Figs. S4 S8, we show the weekday-weekend variability in the measured atmospheric conditions, light (photosynthetically active radiation in Bakersfield and solar radiation in Pasadena), relative humidity (RH), and temperature. Each of the five figures resamples the individual environmental parameter datasets to only include those observations when both NO 2 and HONO, for the different analytical techniques, exist. This was done in order to represent the atmospheric conditions of Figs. 1 and S1 S3, as opposed to average atmospheric conditions during the CalNex experiment. Calculating P(HONO) inferred P(HONO) inferred (Eq. 1) was calculated using measurements of HONO, NO, and OH in both cities. Conditions during CalNex were generally sunny but cloudy sky conditions did occur and these data were not removed. The rates, k HONO+OH and k NO+OH, are taken from Sander et al. 2 and j HONO is described below. In Bakersfield, OH was measured by laser-induced fluorescence 3 and S2

NO by a home-built chemiluminescence instrument. 4 In Pasadena, OH was measured by fluorescent assay by gas expansion 5 and NO by a chemiluminescence Thermo 42i-TL detector. (1) P(HONO) inferred = j HONO [HONO] + k HONO+OH [HONO][OH] k NO+OH [NO][OH] In Bakersfield, j HONO was calculated hourly using the TUV calculator (http://cprm.acd.ucar.edu/models/tuv/interactive_tuv) 6 for a clear sky day (7 June ). This j HONO was then used to scale the measured photosynthetically active radiation for the entire CalNex time period at 1-minute time resolution. Inputs to the TUV calculator were as follows: O 3 optical depth equal to 3 Dobson units, as measured by OMI on 7 June (http://www.temis.nl/protocols/o3total.html); 7 measurement altitude equal to.14 km (asl); and surface albedo equal to.8, determined using the MODIS 16 day 5-meter product in band 3 (459 479 nm) for 18 June reprojected at a fine resolution (.1 degree ~ m). In Pasadena, j HONO was measured and these data used. Any missing j HONO (8 days) were filled by computing j HONO hourly using the TUV calculator for clear sky day 5 June, scaling the TUV values by the ratio of j NO2 measured at 1-minute time resolution to the calculated j NO2 for entire study period, and multiplying modeled j HONO by the slope of the correlation of measured versus TUV j HONO for the entire CalNex time period. S3

a) b) 8 NO 2 (ppb) 15 5 HONO (ppt) 6 4 8 12 16 24 4 8 12 16 24 Figure S1. Panel a: Hourly medians of 1-minute LIF NO 2 as a function of time of day on weekdays (black closed circles) and weekends (blue open diamonds) in Bakersfield. Data are only included when HONO SC-AP measurements also exist. Error bars show 1σ variability. Panel b: Hourly medians of corresponding 2-minute HONO on weekdays and weekends, with HONO data only included when NO 2 data also exist. Excluding Saturdays from this data, the longest dataset, had no effect on the observed HONO NO 2 dependence. S4

a) b) 3 15 NO 2 (ppb) 25 15 5 4 8 12 16 24 HONO (ppt) 5 4 8 12 16 24 Figure S2. Panel a: Hourly daily medians of 1-minute CRDS NO 2 on weekdays (black closed circles) and weekends (blue open diamonds) in Pasadena. Data are only included when HONO IBBCEAS measurements also exist and the y-axis is truncated to highlight daytime differences. Error bars show 1σ variability. Panel b: Hourly medians of corresponding -minute HONO on weekdays and weekends. HONO data are only included in the averaging when NO 2 data also exist. S5

NO 2 (ppb) HONO (ppt) 15 5 3 Low 6 12 18 24 6 12 18 24 15 5 3 Mid 6 12 18 24 6 12 18 24 15 5 3 High 6 12 18 24 6 12 18 24 15 5 3 Highest 6 12 18 24 6 12 18 24 Figure S3. Top row, left to right: 9-minute medians of NO 2 measured by LP-DOAS at the low (78 m), middle (121 m), high (255 m), and highest (556 m) light paths on weekdays (black closed circles) and weekends (blue open diamonds) in the Los Angeles area. Error bars are 1σ variability. Bottom row, left to right: 9-minute medians of LP-DOAS HONO at the same heights. The y-axis is truncated to highlight daytime differences S6

light (µmol m 2 s 1 ) 25 15 5 a) b) c) 4 8 12 16 24 relative humitidy (%) 8 6 4 4 8 12 16 24 temperature ( o C) 4 3 4 8 12 16 24 Figure S4. Panel a: Hourly medians of photosynthetically active radiation (µmol m 2 s 1 ) (panel a), relative humidity (%) (panel b), and temperature ( o C) (panel c) on weekdays (black closed circles) and weekends (blue open diamonds) in Bakersfield when AIM-IC HONO observations also exist. S7

light (W m 1 ) 8 a) b) c) 4 8 12 16 24 relative humitidy (%) 8 6 4 4 8 12 16 24 temperature ( o C) 4 3 4 8 12 16 24 Figure S5. Hourly daily medians of solar radiation (W m 2 ) (panel a), relative humidity (%) (panel b), and temperature ( o C) (panel c) on weekdays (black closed circles) and weekends (blue open diamonds) in Pasadena when NI-PT-CIMS HONO observations also exist. S8

light (µmol m 2 s 1 ) 25 15 5 a) b) c) 4 8 12 16 24 relative humitidy (%) 8 6 4 4 8 12 16 24 temperature ( o C) 4 3 4 8 12 16 24 Figure S6. Hourly daily medians of photosynthetically active radiation (µmol m 2 s 1 ) (panel a), relative humidity (%) (panel b), and temperature ( o C) (panel c) on weekdays (black closed circles) and weekends (blue open diamonds) in Bakersfield when SC-AP HONO observations also exist. S9

light (W m 1 ) 8 a) b) c) 4 8 12 16 24 relative humitidy (%) 8 6 4 4 8 12 16 24 temperature ( o C) 4 3 4 8 12 16 24 Figure S7. Hourly daily medians of solar radiation (W m 2 ) (panel a), relative humidity (%) (panel b), and temperature ( o C) (panel c) on weekdays (black closed circles) and weekends (blue open diamonds) in Pasadena when IBBCEAS HONO observations also exist. S

light (W m 1 ) a) b) c) 4 8 4 8 12 16 24 relative humitidy (%) 8 6 4 4 8 12 16 24 temperature ( o C) 3 4 8 12 16 24 Figure S8. Diurnal 9-minute medians of solar radiation at the surface in Pasadena (W m 2 ) (panel a), relative humidity (%) (panel b), and temperature ( o C) (panel c) on weekdays (black closed circles) and weekends (blue open diamonds) in Los Angeles when LP-DOAS HONO observations also exist. S11

References 1. Marr, L. C.; Harley, R. A., Environ. Sci. Technol. 2, 36 (19), 499. 2. Sander, S. P.; Abbatt, J.; Barker, J. R.; Burkholder, J. B.; Friedl, R. R.; Golden, D. M.; Huie, R. E.; Kolb, C. E.; Kurylo, M. J.; Moortgat, G. K.; Orkin, V. L.; Wine, P. H. Chemical Kinetics and Photochemical Data for Use in Atmospheric Studies, Evaluation No. 17; Pasadena: Jet Propulsion Laboratory, 11. 3. Stevens, P. S.; Mather, J. H.; Brune, W. H., J. Geophys. Res.-Atmos. 1994, 99 (D2), 3543. 4. Min, K. E.; Pusede, S. E.; Browne, E. C.; LaFranchi, B. W.; Cohen, R. C., Atmos. Chem. Phys. 14, 14 (11), 5495. 5. Dusanter, S.; Vimal, D.; Stevens, P. S.; Volkamer, R.; Molina, L. T., Atmos. Chem. Phys. 9, 9 (5), 1665. 6. Madronich, S., J. Geophys. Res.-Atmos. 1987, 92 (D8), 974. 7. Veefkind, J. P.; de Haan, J. F.; Brinksma, E. J.; Kroon, M.; Levelt, P. F., IEEE Trans. Geo. Rem. Sens. 6, 44, 1239. S12