Measurement report: Photochemical production and loss rates of formaldehyde and ozone across Europe

Abstract

Various atmospheric sources and sinks regulate the abundance of tropospheric formaldehyde (HCHO), which is an important trace gas impacting the ${\mathrm{HO}}_{\mathit{\text{x}}}$ ($\equiv$ ${\mathrm{HO}}_{\mathrm{2}}$ $+$ OH) budget and the concentration of ozone (${\mathrm{O}}_{\mathrm{3}}$). In this study, we present the formation and destruction terms of ambient HCHO and ${\mathrm{O}}_{\mathrm{3}}$ calculated from in situ observations of various atmospheric trace gases measured at three different sites across Europe during summertime. These include a coastal site in Cyprus, in the scope of the Cyprus Photochemistry Experiment (CYPHEX) in 2014, a mountain site in southern Germany, as part of the Hohenpeißenberg Photochemistry Experiment (HOPE) in 2012, and a forested site in Finland, where measurements were performed during the Hyytiälä United Measurements of Photochemistry and Particles (HUMPPA) campaign in 2010. We show that, at all three sites, formaldehyde production from the OH oxidation of methane (${\mathrm{CH}}_{\mathrm{4}}$), acetaldehyde (${\mathrm{CH}}_{\mathrm{3}}\mathrm{CHO}$), isoprene (${\mathrm{C}}_{\mathrm{5}}{\mathrm{H}}_{\mathrm{8}}$) and methanol (${\mathrm{CH}}_{\mathrm{3}}\mathrm{OH}$) can almost completely balance the observed loss via photolysis, OH oxidation and dry deposition. Ozone chemistry is clearly controlled by nitrogen oxides (${\mathrm{NO}}_x$ $\equiv$ NO $+$ ${\mathrm{NO}}_{\mathrm{2}}$) that include${\mathrm{O}}_{\mathrm{3}}$ production from ${\mathrm{NO}}_{\mathrm{2}}$ photolysis and ${\mathrm{O}}_{\mathrm{3}}$ loss via the reaction with NO. Finally, we use the HCHO budget calculations to determine whether net ozone production is limited by the availability of VOCs (volatile organic compounds; VOC-limited regime) or ${\mathrm{NO}}_x$ (${\mathrm{NO}}_x$-limited regime). At the mountain site in Germany, ${\mathrm{O}}_{\mathrm{3}}$ production is VOC limited, whereas it is${\mathrm{NO}}_x$ limited at the coastal site in Cyprus. The forested site in Finland is in the transition regime.

1 Introduction

Formaldehyde (HCHO) is an important atmospheric trace gas which provides insight into various photochemical processes taking place in the Earth's atmosphere. It has both anthropogenic sources, such as industrial and vehicle emissions, and natural sources including, for example, biomass burning or volatile organic compound (VOC) precursors, with natural sources dominating in remote locations . The majority of these HCHO sources is secondary, and due to its short lifetime, the atmospheric transport of HCHO from primary (direct) emissions (e.g., biomass burning or industry) to remote locations can be mostly neglected . Loss processes of HCHO include deposition, reaction with OH and photolysis yielding mainly ${\mathrm{HO}}_{\mathrm{2}}$, CO and ${\mathrm{H}}_{\mathrm{2}}$ . HCHO production paths are more diverse and include oxidation processes of almost any VOC, including acetone (${\mathrm{CH}}_{\mathrm{3}}{\mathrm{COCH}}_{\mathrm{3}}$), methane (${\mathrm{CH}}_{\mathrm{4}}$), acetaldehyde (${\mathrm{CH}}_{\mathrm{3}}\mathrm{CHO}$), methanol (${\mathrm{CH}}_{\mathrm{3}}\mathrm{OH}$), isoprene (${\mathrm{C}}_{\mathrm{5}}{\mathrm{H}}_{\mathrm{8}}$), methyl hydroperoxide (${\mathrm{CH}}_{\mathrm{3}}\mathrm{OOH}$), ethene (${\mathrm{C}}_{\mathrm{2}}{\mathrm{H}}_{\mathrm{4}}$) (these selected species are included in this study due to the availability of measurement data) and many more, the majority of which are initiated by the OH radical during the day . Net production processes of formaldehyde, therefore, influence the ${\mathrm{HO}}_{\mathit{\text{x}}}$ (${\mathrm{HO}}_{\mathit{\text{x}}}$ $\equiv$ OH $+$ ${\mathrm{HO}}_{\mathrm{2}}$) budget, which, in turn, controls the atmospheric oxidizing capacity . This includes the regulation of the atmospheric ozone (${\mathrm{O}}_{\mathrm{3}}$) abundance, a trace gas with adverse health effects for humans, animals and plants, leading to cardiovascular and respiratory diseases and the decrease in life expectancy . It is, therefore, important to understand the processes influencing and contributing to HCHO and ${\mathrm{O}}_{\mathrm{3}}$ formation and loss processes in the Earth's atmosphere (see also Figs.  and  for an overview of the reactions considered in this study).

Previous studies have investigated the processes contributing to HCHO production from secondary sources. identified isoprene, methane and methanol to be the main HCHO precursors over the United States of America, contributing over 80 % in the GEOS-CHEM model (Goddard Earth Observing System global 3-D model of tropospheric chemistry). evaluated HCHO concentrations in the tropical western Pacific and found methane and acetaldehyde to be the main precursors of HCHO, based on box model simulations. identified methane to be the main precursor of HCHO in remote regions, based on model simulations and measurements during the INTEX-B campaign (Intercontinental Transport Experiment – Phase B) in 2006. investigated the HCHO budget at a forest in Pellston, Michigan (USA), based on observations in the scope of PROPHET (Program for Research on Oxidants: Photochemistry, Emission and Transport) in 1998. They identified isoprene to be the main HCHO precursor, contributing around 80 %. investigated the relationship between OH reactivity and HCHO production rates during the shipborne campaign AQABA (Air Quality and Climate Change in the Arabian Basin) around the Arabian Peninsula in 2017, which they found to be highest in polluted areas, suggesting a high diversity of HCHO precursors. studied OH reactivities and HCHO concentrations in the Po Valley, based on zeppelin measurements during the research campaign PEGASOS (Pan-European Gas-AeroSOls Climate Interaction Study) in 2012 in comparison with model simulations, and attributed the discrepancies to possible primary HCHO emissions from agriculture.

Tropospheric ozone chemistry is dependent on the ${\mathrm{O}}_{\mathrm{3}}$ precursors ${\mathrm{NO}}_x$ (${\mathrm{NO}}_x$ $\equiv$ NO $+$ ${\mathrm{NO}}_{\mathrm{2}}$) and volatile organic compounds (VOCs). Depending on the ambient concentrations of ${\mathrm{NO}}_x$ and VOCs, net ozone formation can either be ${\mathrm{NO}}_x$ or VOC limited. A ${\mathrm{NO}}_x$ limitation is usually dominant for low ${\mathrm{NO}}_x$ concentrations in which increasing ${\mathrm{NO}}_x$ leads to an increase in ${\mathrm{O}}_{\mathrm{3}}$ formation. For high ${\mathrm{NO}}_x$ concentrations, ozone formation is usually VOC limited, and an increase in ambient ${\mathrm{NO}}_x$ reduces ${\mathrm{O}}_{\mathrm{3}}$ formation through loss of ${\mathrm{HO}}_{\mathit{\text{x}}}$ as OH is converted to HN${\mathrm{O}}_{\mathrm{3}}$ . Consequently, changes in ambient ${\mathrm{NO}}_x$ concentrations can either increase or decrease ${\mathrm{O}}_{\mathrm{3}}$ or – at a transition between both regimes – have only a weak net effect on the ${\mathrm{O}}_{\mathrm{3}}$ production. In urban environments, the chemical regime can be characterized using the weekend effect, which describes the ozone response to decreasing ${\mathrm{NO}}_x$ emissions at weekends, as reported by , , , and many more . Another measure for identifying the prevailing chemical regime is the ratio of HCHO and ${\mathrm{NO}}_{\mathrm{2}}$, which has been determined via satellite measurements in various studies . initially suggested a threshold of 0.28 for the ratio $\mathrm{HCHO}/{\mathrm{NO}}_y$ (${\mathrm{NO}}_y$ is here the sum of ${\mathrm{NO}}_x$, HN${\mathrm{O}}_{\mathrm{3}}$, peroxyacetyl nitrates and alkyl nitrates), below which the chemistry is VOC limited, based on model simulations for Lake Michigan and the northeastern corridor (USA). investigated the ratio of the $\mathrm{HCHO}/{\mathrm{NO}}_{\mathrm{2}}$ column based on satellite observations and found a threshold of 1. This is in agreement with findings from , who suggested a threshold of 1 for a VOC-limited regime, a threshold of 2 for a ${\mathrm{NO}}_x$-limited regime and a transition in between both using remote sensing. present in situ measurements of HCHO and ${\mathrm{NO}}_{\mathrm{2}}$ to determine the dominant regime and point out that exact thresholds are geographically variable due to locally different atmospheric composition and ambient conditions, such as VOC variety or humidity.

In this study, we evaluate the formaldehyde and ozone budget during the field experiment CYPHEX (Cyprus Photochemistry Experiment), which took place in July 2014 at a coastal site in Cyprus (Ineia), based on in situ trace gas observations of NO, ${\mathrm{NO}}_{\mathrm{2}}$, ${\mathrm{O}}_{\mathrm{3}}$, OH, ${\mathrm{HO}}_{\mathrm{2}}$, ${\mathrm{CH}}_{\mathrm{4}}$, ${\mathrm{CH}}_{\mathrm{3}}\mathrm{OH}$ (methanol), ${\mathrm{C}}_{\mathrm{5}}{\mathrm{H}}_{\mathrm{8}}$ (isoprene), ${\mathrm{CH}}_{\mathrm{3}}\mathrm{CHO}$ (acetaldehyde), ${\mathrm{CH}}_{\mathrm{3}}{\mathrm{COCH}}_{\mathrm{3}}$ (acetone), ${\mathrm{CH}}_{\mathrm{3}}\mathrm{OOH}$ (methyl hydroperoxide), ${\mathrm{C}}_{\mathrm{2}}{\mathrm{H}}_{\mathrm{4}}$ (ethene), ${\mathrm{CH}}_{\mathrm{3}}{\mathrm{SCH}}_{\mathrm{3}}$ (DMS) and HCHO . We compare the results with two other field campaigns in central and northern Europe, namely the Hohenpeißenberg Photochemistry Experiment (HOPE 2012; ) at a mountain site in Germany and the Hyytiälä United Measurements of Photochemistry and Particles (HUMPPA 2010; ) at a boreal forest site in Finland. Only a few studies have evaluated the HCHO budget mainly through model simulations. To our knowledge, there is only one study, by , that has previously presented HCHO budget calculations from in situ trace gas observations in the USA in 1998. We are first to present HCHO budget calculations from in situ measurements across Europe and show that, in all three locations, HCHO production can be predominantly accounted for by the oxidation of methane, methanol, acetaldehyde and isoprene.

2 Observations and methods

2.1 HCHO chemistry calculations

Figure  shows an overview of the main production and loss processes for formaldehyde which we consider in this study and for which measurements were obtained during the field campaign CYPHEX (see Sect.  for further details). The relationships we derive in this study are based on boundary layer conditions, and we, therefore, assume no relevant intrusion from higher altitudes. Acetone and methane can form methyl radicals (CH${}_{\mathrm{3}}$) through oxidation by OH or photolysis, which are subsequently oxidized to methyl peroxy radicals (${\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}$) by molecular oxygen (${\mathrm{O}}_{\mathrm{2}}$). Another pathway yielding ${\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}$ is the OH oxidation of acetaldehyde which forms ${\mathrm{CH}}_{\mathrm{3}}\mathrm{C}\left(\mathrm{O}\right)$ in the first step and which can then be oxidized to ${\mathrm{CH}}_{\mathrm{3}}\mathrm{C}\left(\mathrm{O}\right){\mathrm{O}}_{\mathrm{2}}$ when ${\mathrm{O}}_{\mathrm{2}}$ is present. ${\mathrm{CH}}_{\mathrm{3}}\mathrm{C}\left(\mathrm{O}\right){\mathrm{O}}_{\mathrm{2}}$ yields ${\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}$ through a reaction with nitric oxide (NO) or the hydroperoxyl radical (${\mathrm{HO}}_{\mathrm{2}}$) via ${\mathrm{CH}}_{\mathrm{3}}{\mathrm{CO}}_{\mathrm{2}}$. The ${\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}$ yield from the reaction of ${\mathrm{CH}}_{\mathrm{3}}\mathrm{C}\left(\mathrm{O}\right){\mathrm{O}}_{\mathrm{2}}$ with ${\mathrm{HO}}_{\mathrm{2}}$ is approximately 50 % ($k_{\mathrm{c}}$). Other reaction pathways result in the formation of ${\mathrm{CH}}_{\mathrm{3}}\mathrm{C}\left(\mathrm{O}\right)$OH ($k_{\mathrm{a}}$) and ${\mathrm{CH}}_{\mathrm{3}}\mathrm{C}\left(\mathrm{O}\right)$OOH $k_{\mathrm{b}}$;. We calculate the overall fraction ${\mathit{\alpha }}_{{\mathrm{CH}}_{\mathrm{3}}\mathrm{CHO}}$ of acetaldehyde oxidation that results in ${\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}$ formation via Eq. ().

1$$\begin{array}{rl}& {\mathit{\alpha }}_{{\mathrm{CH}}_{\mathrm{3}}\mathrm{CHO}}=\\ & {\displaystyle \frac{k_{{\mathrm{CH}}_{\mathrm{3}}\mathrm{C}\left(\mathrm{O}\right){\mathrm{O}}_{\mathrm{2}}+\mathrm{NO}}\times \left[\mathrm{NO}\right]+k_{\mathrm{c}}\times \left[{\mathrm{HO}}_{\mathrm{2}}\right]}{k_{{\mathrm{CH}}_{\mathrm{3}}\mathrm{C}\left(\mathrm{O}\right){\mathrm{O}}_{\mathrm{2}}+\mathrm{NO}}\times \left[\mathrm{NO}\right]+k_{\mathrm{a}}\times \left[{\mathrm{HO}}_{\mathrm{2}}\right]+k_{\mathrm{b}}\times \left[{\mathrm{HO}}_{\mathrm{2}}\right]+k_{\mathrm{c}}\times \left[{\mathrm{HO}}_{\mathrm{2}}\right]}}.\end{array}$$ Additionally, methyl hydroperoxide (${\mathrm{CH}}_{\mathrm{3}}\mathrm{OOH}$) forms ${\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}$ via OH oxidation 60 %; or reacts directly to HCHO via photolysis or OH-initiated oxidation, 40 %;. ${\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}$ can then either react with ${\mathrm{HO}}_{\mathrm{2}}$ to form ${\mathrm{CH}}_{\mathrm{3}}\mathrm{OOH}$ or yield HCHO through a reaction with NO or OH via ${\mathrm{CH}}_{\mathrm{3}}\mathrm{O}$ . The importance of the ${\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}$ loss via OH in remote locations has recently been shown in several studies, and the reaction primarily yields HCHO . For simplification, we assume this yield to be 100 %, which slightly increases the uncertainty of the calculation but is negligible given the small fraction of ${\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}$ that reacts with OH ($<$ 10 % for CYPHEX). In our study, we use the rate constant $k_{{\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}+\mathrm{OH}}$ recommended by the . Table S1 in the Supplement gives an overview of all rate constants used in this study, most of which were taken from . The fraction of ${\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}$ that forms HCHO (${\mathit{\alpha }}_{{\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}}$) is dependent on the ambient concentrations of ${\mathrm{HO}}_{\mathrm{2}}$, NO and OH and can be calculated via Eq. (). ${\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}$ loss via self-reaction is negligibly small and, therefore, not included. The reaction with ${\mathrm{NO}}_{\mathrm{2}}$ forming ${\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}$${\mathrm{NO}}_{\mathrm{2}}$ can also be excluded due to its thermal instability in the boundary layer. 2$$\begin{array}{rl}& {\mathit{\alpha }}_{{\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}}=\\ & {\displaystyle \frac{k_{{\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}+\mathrm{NO}}\times \left[\mathrm{NO}\right]+k_{{\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}+\mathrm{OH}}\times \left[\mathrm{OH}\right]}{k_{{\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}+\mathrm{NO}}\times \left[\mathrm{NO}\right]+k_{{\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}+\mathrm{OH}}\times \left[\mathrm{OH}\right]+k_{{\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}+{\mathrm{HO}}_{\mathrm{2}}}\times \left[{\mathrm{HO}}_{\mathrm{2}}\right]}}.\end{array}$$

Figure 1

Overview of the chemical and photolytic reactions which lead to HCHO production and loss, considering the trace gases measured during the CYPHEX field experiment. The black and bold font identifies the species which contribute mainly ($\sim$80 %) to HCHO formation according to the findings in this study. For a better overview, we have omitted intermediate steps with a 100 % yield which are, instead, described in the main text.

[Figure omitted. See PDF]

Isoprene oxidation results in the formation of HCHO through the intermediate products methyl vinyl ketone and methacrolein, as described by . The HCHO yield from isoprene (${\mathit{\alpha }}_{\text{Isoprene}}$) is dependent on the ambient NO concentration and varies between around 30 % for low ${\mathrm{NO}}_x$ and 60 % for high ${\mathrm{NO}}_x$ ${\mathrm{RO}}_{\mathrm{2}}$ reacts primarily with NO;. We calculate the HCHO yield via Eq. () and estimate [${\mathrm{HO}}_{\mathrm{2}}$] $\approx$ [${\mathrm{RO}}_{\mathrm{2}}$], as suggested by . This assumption is justified when looking at ${\mathrm{O}}_{\mathrm{3}}$ production ($P\left({\mathrm{O}}_{\mathrm{3}}\right)$) terms. $P\left({\mathrm{O}}_{\mathrm{3}}\right)$ can either be calculated via the photolytic reaction of ${\mathrm{NO}}_{\mathrm{2}}$, as presented in Sect. , or via the reaction of ${\mathrm{HO}}_{\mathrm{2}}$ or ${\mathrm{RO}}_{\mathrm{2}}$ with NO. We equate the two terms, using the rate constant of the reaction of NO and ${\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}$ as estimate for the reaction of NO and ${\mathrm{RO}}_{\mathrm{2}}$, and calculate ${\mathrm{RO}}_{\mathrm{2}}$. We show the diurnal profiles of ${\mathrm{HO}}_{\mathrm{2}}$ and calculate ${\mathrm{RO}}_{\mathrm{2}}$ in Fig. S1a in the Supplement. Conversely, we calculate $P\left({\mathrm{O}}_{\mathrm{3}}\right)$ for both cases, equating ${\mathrm{RO}}_{\mathrm{2}}$ to ${\mathrm{HO}}_{\mathrm{2}}$, which show close agreement, and can be seen in Fig. S1b. This is also confirmed by findings from (presented in Fig. 9), based on model simulations of ${\mathrm{HO}}_{\mathrm{2}}$ and ${\mathrm{RO}}_{\mathrm{2}}$ during HUMPPA. The yield can vary between 34 % (in the absence of NO) and 57 % (when NO chemistry dominates the fate of the ${\mathrm{RO}}_{\mathrm{2}}$ formed), according to Eq. (), which was originally determined experimentally by . We discuss the effects of the threshold values in Sect. . ${\mathrm{C}}_{\mathrm{5}}{\mathrm{H}}_{\mathrm{8}}\left(\mathrm{OH}\right){\mathrm{O}}_{\mathrm{2}}$ is the peroxy radical resulting from isoprene oxidation and has six relevant isomers which can undergo multiple reactions yielding HCHO and many other products . Additionally, the formation of HCHO from isoprene does not occur instantaneously (as, for example, from methane or other VOC), but is likely time dependent. However, the consideration of this time-dependent formation and the detailed evaluation of the reactions paths from each peroxy radical isomer is beyond the scope of this study, and we, therefore, adapt the methodology presented by to estimate the HCHO production from isoprene. 3$${\mathit{\alpha }}_{\text{Isoprene}}=\mathrm{0.34}+\mathrm{0.23}\times \left({\displaystyle \frac{k_{{\mathrm{C}}_{\mathrm{5}}{\mathrm{H}}_{\mathrm{8}}\left(\mathrm{OH}\right){\mathrm{O}}_{\mathrm{2}}+\mathrm{NO}}\times \left[\mathrm{NO}\right]}{\begin{array}{c}{k}_{{\mathrm{C}}_{\mathrm{5}}{\mathrm{H}}_{\mathrm{8}}\left(\mathrm{OH}\right){\mathrm{O}}_{\mathrm{2}}+\mathrm{NO}}\times \left[\mathrm{NO}\right]\\ +k_{{\mathrm{C}}_{\mathrm{5}}{\mathrm{H}}_{\mathrm{8}}\left(\mathrm{OH}\right){\mathrm{O}}_{\mathrm{2}}+{\mathrm{HO}}_{\mathrm{2}}}\times \left[{\mathrm{HO}}_{\mathrm{2}}\right]\\ +k_{{\mathrm{C}}_{\mathrm{5}}{\mathrm{H}}_{\mathrm{8}}\left(\mathrm{OH}\right){\mathrm{O}}_{\mathrm{2}}+{\mathrm{RO}}_{\mathrm{2}}}\times \left[{\mathrm{RO}}_{\mathrm{2}}\right]\end{array}}}\right).$$

Methanol reacts with OH yielding HCHO via ${\mathrm{CH}}_{\mathrm{2}}\mathrm{OH}$ and ${\mathrm{CH}}_{\mathrm{3}}\mathrm{O}$ and following oxidation by ${\mathrm{O}}_{\mathrm{2}}$ . Ethene is a precursor to HCHO through OH oxidation or ozonolysis . A potential source of HCHO in marine environments is dimethyl sulfide (DMS) via OH oxidation . Terpenes, such as limonene or $\mathit{\alpha }$-/$\mathit{\beta }$-pinene emitted from plants, can additionally be HCHO sources, as described by .

Reactions ()–() present the chemical loss processes of HCHO through OH oxidation and two different photolysis pathways. In addition, HCHO dry deposition – the uptake of HCHO by the Earth's surface – plays a role in HCHO loss, particularly during the night . While HCHO loss can also occur via wet deposition, as, for example, described by , or via liquid-phase reactions in cloud droplets, as shown by , this study investigates summertime campaigns without significant precipitation. $$\begin{array}{}\text{R1}& {\displaystyle }& {\displaystyle }\mathrm{HCHO}+\mathrm{OH}+{\mathrm{O}}_{\mathrm{2}}\to \mathrm{CO}+{\mathrm{HO}}_{\mathrm{2}}+{\mathrm{H}}_{\mathrm{2}}\mathrm{O}\text{R2}& {\displaystyle }& {\displaystyle }\mathrm{HCHO}+h\mathit{\nu }\to \mathrm{CO}+{\mathrm{H}}_{\mathrm{2}}\text{R3}& {\displaystyle }& {\displaystyle }\mathrm{HCHO}+h\mathit{\nu }+\mathrm{2}{\mathrm{O}}_{\mathrm{2}}\to \mathrm{CO}+\mathrm{2}{\mathrm{HO}}_{\mathrm{2}}.\end{array}$$

We will show in the scope of this work that reactions of methane, acetaldehyde, methanol and isoprene with OH almost completely account for HCHO production in the environments considered in this paper across Europe. We have highlighted these pathways in Fig.  in a black and bold font. Equations () and () show the calculation of the basic production $P(\mathrm{HCHO}{)}_{\text{basic}}$ (compared to the reactions shown in Fig. ) and the loss $L\left(\mathrm{HCHO}\right)$ terms. The $k$ values represent the rate coefficients, $j\left(\mathrm{HCHO}\right)$ is the summed photolysis frequency for Reactions () and (), $v_{\mathrm{d}}$ describes the dry deposition velocity in centimeters per second ($\mathrm{cm}{\mathrm{s}}^{-\mathrm{1}}$) and BLH is the boundary layer height in centimeters. 4$$\begin{array}{rl}& P(\mathrm{HCHO}{)}_{\text{basic}}\\ & =P_{{\mathrm{CH}}_{\mathrm{4}}+\mathrm{OH}}+P_{{\mathrm{CH}}_{\mathrm{3}}\mathrm{CHO}+\mathrm{OH}}+P_{{\mathrm{CH}}_{\mathrm{3}}\mathrm{OH}+\mathrm{OH}}+P_{{\mathrm{C}}_{\mathrm{5}}{\mathrm{H}}_{\mathrm{8}}+\mathrm{OH}}\\ & =\left[\mathrm{OH}\right]\times \left(\right[{\mathrm{CH}}_{\mathrm{4}}]\times k_{{\mathrm{CH}}_{\mathrm{4}}+\mathrm{OH}}\times {\mathit{\alpha }}_{{\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}}+[{\mathrm{CH}}_{\mathrm{3}}\mathrm{CHO}]\\ & \times k_{{\mathrm{CH}}_{\mathrm{3}}\mathrm{CHO}+\mathrm{OH}}\times {\mathit{\alpha }}_{{\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}}\times {\mathit{\alpha }}_{{\mathrm{CH}}_{\mathrm{3}}\mathrm{CHO}}+\left[{\mathrm{CH}}_{\mathrm{3}}\mathrm{OH}\right]\\ & \times k_{{\mathrm{CH}}_{\mathrm{3}}\mathrm{OH}+\mathrm{OH}}+\left[{\mathrm{C}}_{\mathrm{5}}{\mathrm{H}}_{\mathrm{8}}\right]\times k_{{\mathrm{C}}_{\mathrm{5}}{\mathrm{H}}_{\mathrm{8}}+\mathrm{OH}}\times {\mathit{\alpha }}_{\text{Isoprene}}).\end{array}$$

5$$\begin{array}{rl}L\left(\mathrm{HCHO}\right)=& L_{\mathrm{HCHO}+\mathrm{OH}}+L_{\mathrm{HCHO}+h\mathit{\nu }}+L_{\text{deposition}}\\ =& \left[\mathrm{HCHO}\right]\times \left(\right[\mathrm{OH}]\times k_{\mathrm{HCHO}+\mathrm{OH}}\\ & +j\left(\mathrm{HCHO}\right)+{\displaystyle \frac{v_{\mathrm{d}}\left(\mathrm{HCHO}\right)}{\text{BLH}}}).\end{array}$$

Changes in the HCHO concentration are represented by Eq. (), which include the production and loss from Eqs. ()–(), a transport term $T\left(\mathrm{HCHO}\right)$, such as advection or entrainment (can be positive or negative), and a term for primary emissions . 6$$\begin{array}{rl}{\displaystyle \frac{\mathrm{d}\left[\mathrm{HCHO}\right]}{\mathrm{d}t}}=& P(\mathrm{HCHO}{)}_{\text{basic}}-L(\mathrm{HCHO})\\ & +T\left(\mathrm{HCHO}\right)+P_{\text{emission}}.\end{array}$$

2.2

${\mathrm{O}}_{\mathrm{3}}$ chemistry calculations

Figure  presents the main processes contributing to ${\mathrm{O}}_{\mathrm{3}}$ formation and loss. The only significant chemical source of tropospheric ${\mathrm{O}}_{\mathrm{3}}$ is the photolysis of nitrogen dioxide (${\mathrm{NO}}_{\mathrm{2}}$), which is converted to NO and $\mathrm{O}{(}^{\mathrm{3}}\mathrm{P})$ under the influence of sunlight. The reaction of $\mathrm{O}{(}^{\mathrm{3}}\mathrm{P})$ with molecular oxygen (${\mathrm{O}}_{\mathrm{2}}$) subsequently yields ${\mathrm{O}}_{\mathrm{3}}$ . ${\mathrm{NO}}_{\mathrm{2}}$, in turn, is generated from the oxidation of NO by ozone or peroxy radicals ${\mathrm{HO}}_{\mathrm{2}}$ and ${\mathrm{RO}}_{\mathrm{2}}$;.

Figure 2

Overview of the chemical and photolytic reactions which lead to ${\mathrm{O}}_{\mathrm{3}}$ production and loss.

[Figure omitted. See PDF]

Ozone loss processes include the reaction with NO forming ${\mathrm{NO}}_{\mathrm{2}}$, conversion with OH or ${\mathrm{HO}}_{\mathrm{2}}$ to ${\mathrm{HO}}_{\mathrm{2}}$ and OH, respectively, deposition processes and photolysis. ${\mathrm{O}}_{\mathrm{3}}$ photolysis yields $\mathrm{O}{(}^{\mathrm{1}}\mathrm{D})$, which is deactivated to $\mathrm{O}{(}^{\mathrm{3}}\mathrm{P})$ (and then ${\mathrm{O}}_{\mathrm{3}}$) via collision with nitrogen (${\mathrm{N}}_{\mathrm{2}}$) and oxygen (${\mathrm{O}}_{\mathrm{2}}$). ${\mathrm{O}}_{\mathrm{3}}$ loss occurs when $\mathrm{O}{(}^{\mathrm{1}}\mathrm{D})$ reacts with water to form OH. The fraction of this reaction is presented by ${\mathit{\alpha }}_{{\mathrm{O}}^{\mathrm{1}}\mathrm{D}}$ as shown in Eq. () . The reaction of ${\mathrm{O}}_{\mathrm{3}}$ and ${\mathrm{NO}}_{\mathrm{2}}$ to form ${\mathrm{NO}}_{\mathrm{3}}$ could potentially yield a net loss of ${\mathrm{O}}_{\mathrm{3}}$ when being photolyzed back to ${\mathrm{NO}}_x$. However, only around 10 % of the ${\mathrm{NO}}_{\mathrm{3}}$ photolysis leads to NO formation which results in a ${\mathrm{O}}_{\mathrm{3}}$ net loss;. Additionally, the reaction is likely negligible during the day, as ${\mathrm{O}}_{\mathrm{3}}$ reacts much more rapidly with NO. 7$$\begin{array}{rl}& {\mathit{\alpha }}_{{\mathrm{O}}^{\mathrm{1}}\mathrm{D}}\\ & ={\displaystyle \frac{k_{{\mathrm{O}}^{\mathrm{1}}\mathrm{D}+{\mathrm{H}}_{\mathrm{2}}\mathrm{O}}\times \left[{\mathrm{H}}_{\mathrm{2}}\mathrm{O}\right]}{k_{{\mathrm{O}}^{\mathrm{1}}\mathrm{D}+{\mathrm{N}}_{\mathrm{2}}}\times \left[{\mathrm{N}}_{\mathrm{2}}\right]+k_{{\mathrm{O}}^{\mathrm{1}}\mathrm{D}+{\mathrm{O}}_{\mathrm{2}}}\times \left[{\mathrm{O}}_{\mathrm{2}}\right]+k_{{\mathrm{O}}^{\mathrm{1}}\mathrm{D}+{\mathrm{H}}_{\mathrm{2}}\mathrm{O}}\times \left[{\mathrm{H}}_{\mathrm{2}}\mathrm{O}\right]}}.\end{array}$$

Equations () and () present the calculations for ${\mathrm{O}}_{\mathrm{3}}$ production and loss. $$\begin{array}{}\text{8}& {\displaystyle }P\left({\mathrm{O}}_{\mathrm{3}}\right)=P_{{\mathrm{NO}}_{\mathrm{2}}+h\mathit{\nu }}=\left[{\mathrm{NO}}_{\mathrm{2}}\right]\times j\left({\mathrm{NO}}_{\mathrm{2}}\right)\text{9}& {\displaystyle }\begin{array}{rl}L\left({\mathrm{O}}_{\mathrm{3}}\right)=& L_{{\mathrm{O}}_{\mathrm{3}}+\mathrm{NO}}+L_{{\mathrm{O}}_{\mathrm{3}}+\mathrm{OH}}+L_{{\mathrm{O}}_{\mathrm{3}}+{\mathrm{HO}}_{\mathrm{2}}}\\ & +L_{{\mathrm{O}}_{\mathrm{3}}+h\mathit{\nu }}+L_{\text{deposition}}\\ =& \left[{\mathrm{O}}_{\mathrm{3}}\right]\times \left(\right[\mathrm{NO}]\times k_{{\mathrm{O}}_{\mathrm{3}}+\mathrm{NO}}+[\mathrm{OH}]\times k_{{\mathrm{O}}_{\mathrm{3}}+\mathrm{OH}}\\ & +\left[{\mathrm{HO}}_{\mathrm{2}}\right]\times k_{{\mathrm{O}}_{\mathrm{3}}+{\mathrm{HO}}_{\mathrm{2}}}+j\left({\mathrm{O}}^{\mathrm{1}}\mathrm{D}\right)\times {\mathit{\alpha }}_{{\mathrm{O}}^{\mathrm{1}}\mathrm{D}}+{\displaystyle \frac{v_{\mathrm{d}}\left({\mathrm{O}}_{\mathrm{3}}\right)}{\text{BLH}}}).\end{array}\end{array}$$

As for HCHO, net changes in ${\mathrm{O}}_{\mathrm{3}}$ are represented by production, loss and a transport term (either positive or negative), as shown in Eq. (). 10$${\displaystyle \frac{\mathrm{d}\left[{\mathrm{O}}_{\mathrm{3}}\right]}{\mathrm{d}t}}=P\left({\mathrm{O}}_{\mathrm{3}}\right)-L\left({\mathrm{O}}_{\mathrm{3}}\right)+T\left({\mathrm{O}}_{\mathrm{3}}\right).$$

2.3 Field experiments

We have analyzed trace gases and further measurement parameters with regard to the HCHO and ${\mathrm{O}}_{\mathrm{3}}$ budget at three different measurement sites across Europe, which are located in Cyprus (CYPHEX campaign, 2014), southern Germany (HOPE campaign, 2012) and Finland (HUMPPA campaign, 2010). Their geographic locations are shown in Fig. . We provide details on each campaign in the following sections. Please note that all times are in UTC (coordinated universal time). The time difference between 12:00 UTC and mean local noon is UTC$+$128 min for Cyprus, UTC$+$ 44 min for Germany and UTC$+$96 min for Finland .

Figure 3

Geographic locations of the measurement sites included in this analysis. CYPHEX – 34.96${}^{\circ }$ N, 32.38${}^{\circ }$ E, 650 $\mathrm{m}\mathrm{a}.\mathrm{s}.\mathrm{l}.$ (above sea level) and UTC$+$128 min (mean local time); HOPE – 47.80${}^{\circ }$ N, 11.01${}^{\circ }$ E, 980 $\mathrm{m}\mathrm{a}.\mathrm{s}.\mathrm{l}.$ and UTC$+$44 min; HUMPPA – 61.85${}^{\circ }$ N, 24.28${}^{\circ }$ E, 181 $\mathrm{m}\mathrm{a}.\mathrm{s}.\mathrm{l}.$ and UTC$+$96 min.

[Figure omitted. See PDF]

2.3.1 CYPHEX campaign in 2014

The Cyprus Photochemistry Experiment (CYPHEX) took place in Ineia, Cyprus, in July and August 2014. The measurement site was situated on a hilltop 650 $\mathrm{m}\mathrm{a}.\mathrm{s}.\mathrm{l}.$ (34.96${}^{\circ }$ N, 32.38${}^{\circ }$ E) in a remote location, with low population in the surrounding areas. The distance to the coastline of the Mediterranean Sea is approximately 10 km in the north and in the west. A detailed description of the measurement site can be found in , and . In this study, we consider the campaign days for which the trace gas measurements were available simultaneously, which is the time period 22–31 July 2014. NO and ${\mathrm{NO}}_{\mathrm{2}}$ were measured via photolytic chemiluminescence (detector from ECO PHYSICS AG CLD 790 SR, Dürnten, Switzerland, and photolytic converter from Droplet Measurement Technologies, Boulder, CO, USA) with a total uncertainty of 20 % and 30 % and a detection limit of 5 and 20 pptv (parts per trillion by volume), respectively . ${\mathrm{O}}_{\mathrm{3}}$ was measured via UV photometry (model 49 ${\mathrm{O}}_{\mathrm{3}}$ analyzer, Thermo Environmental Instruments, USA) with a detection limit of 2 ppbv (parts per billion by volume) and a total uncertainty of 5 %. OH and ${\mathrm{HO}}_{\mathrm{2}}$ were measured via laser-induced fluorescence spectroscopy with the custom-built HORUS (HydrOxyl Radical measurement Unit based on fluorescence Spectroscopy) instrument accuracy of 28.5 % and 36 % and a detection limit of 1 $\times$ 10${}^{\mathrm{6}}$ $\mathrm{molec}.{\mathrm{cm}}^{-\mathrm{3}}$ and 0.8 pptv, respectively;. HCHO was measured via the Hantzsch method with a commercial instrument (Aero-Laser GmbH, model AL 4021, Garmisch-Partenkirchen, Germany) with a detection limit of 38 pptv and a total uncertainty of 16 % . ${\mathrm{C}}_{\mathrm{2}}{\mathrm{H}}_{\mathrm{4}}$ and ${\mathrm{CH}}_{\mathrm{4}}$ were determined via gas chromatography flame ionization detection (GC 5000 VOC, AMA Instruments GmbH, Ulm, Germany). ${\mathrm{CH}}_{\mathrm{4}}$ measurements had a detection limit of 20 ppbv and a total uncertainty of 2 %, and ${\mathrm{C}}_{\mathrm{2}}{\mathrm{H}}_{\mathrm{4}}$ measurements had a detection limit of 1–8 pptv and a total uncertainty of 10 % . Isoprene was measured via gas chromatography mass spectrometry (MSD 5973, Agilent Technologies, Inc., Böblingen, Germany) with a detection limit of 1 pptv and a total uncertainty of 14.5 % . Oxygenated VOC (OVOC) was measured via proton transfer reaction time-of-flight mass spectrometry PTR-TOF-MS; Ionicon Analytik GmbH, Innsbruck, Austria; ${\mathrm{CH}}_{\mathrm{3}}\mathrm{OH}$ – 242 pptv limit of detection (LOD) and 37 % total uncertainty (TU); ${\mathrm{CH}}_{\mathrm{3}}{\mathrm{COCH}}_{\mathrm{3}}$ – 97 $\mathrm{pptv}$ LOD and 10 % TU; ${\mathrm{CH}}_{\mathrm{3}}\mathrm{CHO}$ – 85 pptv LOD and 22 % TU; DMS – 18 pptv LOD and 12 % TU; the TU is 4 %–7 % higher for a relative humidity below 25 %;. ${\mathrm{CH}}_{\mathrm{3}}\mathrm{OOH}$ was measured via high-performance liquid chromatography with a detection limit of 25 pptv and a total uncertainty of 9 %. Photolysis frequencies were determined with a single monochromator spectral radiometer (Meteorologie Consult GmbH, Königstein, Germany) with a total uncertainty of around 10 %. The photolysis frequencies for acetaldehyde $j\left({\mathrm{CH}}_{\mathrm{3}}\mathrm{CHO}\right)$ and formaldehyde $j\left(\mathrm{HCHO}\right)$ were determined via parameterizations based on $j\left({\mathrm{NO}}_{\mathrm{2}}\right)$ and $j\left({\mathrm{O}}^{\mathrm{1}}\mathrm{D}\right)$, according to Eq. (S1) in the Supplement, with the coefficients presented in Table S2. The latter were derived from least squares fits to photolysis frequencies from a large set of spectroradiometer measurements at Jülich, Germany , under all weather conditions and were originally derived for the HUMPPA campaign. In this work, more recent quantum yields for the HCHO photolysis as recommended by were used with an estimated uncertainty of 20 %. An example for the performance of the parameterization is shown in Fig. S2. An overview of all measured trace gases, including the measurement uncertainty and the time resolution of the data used in this study, can be found in Table S3. For the point-by-point calculations, the data were interpolated to the OH time stamp with a 4 min time resolution. All stated detection limits refer to the time resolution shown in Table S3.

2.3.2 HOPE campaign in 2012

The Hohenpeißenberg Photochemistry Experiment (HOPE) took place from June to September 2012 in Hohenpeißenberg, Germany at the Global Atmospheric Watch meteorological observatory (47.80${}^{\circ }$ N, 11.01${}^{\circ }$ E). The measurement location was situated on a hilltop, 980 $\mathrm{m}\mathrm{a}.\mathrm{s}.\mathrm{l}.$, in a remote and vegetated area. More details on the campaign and the site location can be found in . ${\mathrm{O}}_{\mathrm{3}}$, HCHO, OH and ${\mathrm{HO}}_{\mathrm{2}}$ were measured with the same methods as described for the CYPHEX campaign in Sect. . NO and ${\mathrm{NO}}_{\mathrm{2}}$ were measured via (photolysis) chemiluminescence by the German Weather Service, with an estimated uncertainty of 10 %. ${\mathrm{CH}}_{\mathrm{4}}$ was measured via GC-FID (gas chromatography–flame ionization detector). Isoprene and OVOC were determined via a custom-built GC (Agilent Technologies, Inc.) FID/MS (mass spectrometry) system . $j\left({\mathrm{NO}}_{\mathrm{2}}\right)$ and $j\left({\mathrm{O}}^{\mathrm{1}}\mathrm{D}\right)$ were measured with filter radiometers (Meteorologie Consult GmbH, Königstein, Germany) with an uncertainty of 10 % . $j\left(\mathrm{HCHO}\right)$ was determined via parameterization (Sect. ). BLH (boundary layer height) measurements were not performed and instead adopted from , which are 1500 m for daytime ($j\left({\mathrm{NO}}_{\mathrm{2}}\right)$ $>$ 10${}^{-\mathrm{3}}$ ${\mathrm{s}}^{-\mathrm{1}}$) and 200 m for nighttime ($j\left({\mathrm{NO}}_{\mathrm{2}}\right)$ $<$ 10${}^{-\mathrm{3}}$ ${\mathrm{s}}^{-\mathrm{1}}$). These values were derived from BLH measurements at other locations during summertime, including the CYPHEX and the HUMPPA measurement site, and at a site in central Germany situated at a comparable altitude. We assume that this estimate increases the uncertainty from 20 % (BLH measurements) to 30 %. We determined the deposition velocity $v_{\mathrm{d}}$ from the HCHO nighttime loss, as previously performed by , for ${\mathrm{H}}_{\mathrm{2}}{\mathrm{O}}_{\mathrm{2}}$. The loss rate coefficient $k_{\mathrm{d}}$ was determined from the [HCHO] decrease from 21:00–01:30 UTC divided by the average HCHO concentration $[\mathrm{HCHO}{]}_{\text{av}}$ during this time interval. Multiplication with the nighttime BLH (200 m) then yielded the deposition velocity according to Eq. (). The HCHO loss via deposition during nighttime is independent of the BLH (see Eqs.  and ).

11$$v_{\mathrm{d}}={\displaystyle \frac{k_{\mathrm{d},\text{night}}\times {\text{BLH}}_{\text{night}}}{x}}={\displaystyle \frac{{\displaystyle \frac{\mathrm{d}\left[\mathrm{HCHO}\right]}{\mathrm{d}t}}}{[\mathrm{HCHO}{]}_{\text{av}}\times x}}\times {\text{BLH}}_{\text{night}}.$$ Please note that $v_{\mathrm{d}}$ derived this way represents a lower limit of the nighttime loss rate, as HCHO could be formed from ${\mathrm{NO}}_{\mathrm{3}}$ and ${\mathrm{O}}_{\mathrm{3}}$ chemistry (for example, from ozone and isoprene) at night . The factor $x$ considers the inconsistent mixing of the boundary layer at night, for which $x$ was 2, assuming a linear gradient between the top and the bottom of the boundary layer. During the day, $x$ equaled 1 . As we determined the loss rate from the nighttime decrease in HCHO, the daytime deposition velocity was twice the nighttime deposition velocity according to Eq. (), which gives $v_{\mathrm{d}}\left(\text{day}\right)$ = 0.94 $\mathrm{cm}{\mathrm{s}}^{-\mathrm{1}}$ and $v_{\mathrm{d}}\left(\text{night}\right)$ = 0.47 $\mathrm{cm}{\mathrm{s}}^{-\mathrm{1}}$. Literature values for daytime deposition velocities range between 0.36 and 1.5 $\mathrm{cm}{\mathrm{s}}^{-\mathrm{1}}$ and for nighttime between 0.18 and 0.65 $\mathrm{cm}{\mathrm{s}}^{-\mathrm{1}}$ . We, therefore, consider our calculation to yield reasonable estimates.

Figure 4

The determination of the deposition velocity is based on the HCHO nighttime loss, which is here exemplarily shown for 1 night during the campaign HOPE (2012) in Hohenpeißenberg, southern Germany.

[Figure omitted. See PDF]

We have performed this calculation for 9 nights. Figure  exemplarily shows the nighttime loss of HCHO for 1 night during the HOPE campaign. Red data points represent the HCHO mixing ratios, the black color highlights the data points which we included in our analysis (nighttime HCHO loss) and the cyan line is the linear fit of these data points. An overview of the nights thus analyzed can be found in Fig. S3b. The uncertainty of each calculation results from the single uncertainties of $\frac{\mathrm{d}\left[\mathrm{HCHO}\right]}{\mathrm{d}t}$, $[\mathrm{HCHO}{]}_{\text{av}}$ and the nighttime BLH. The uncertainty of $\frac{\mathrm{d}\left[\mathrm{HCHO}\right]}{\mathrm{d}t}$ is composed of the HCHO measurement uncertainty (16 %) and the uncertainty of the fit (30 % upper limit) with the latter dominating. The uncertainty of $[\mathrm{HCHO}{]}_{\text{av}}$ is based on the HCHO measurement uncertainty and the HCHO averaging (20 % upper limit). Again, the uncertainty of the averaging prevails over the measurement uncertainty. The uncertainty of the BLH is 30 %. Gaussian error propagation gives an overall uncertainty of $\sqrt{\mathrm{30}{\mathit{\%}}^{\mathrm{2}}+\mathrm{30}{\mathit{\%}}^{\mathrm{2}}+\mathrm{20}{\mathit{\%}}^{\mathrm{2}}}=\mathrm{47}\mathit{\%}$ from the calculation. Besides the uncertainty resulting from the calculation, an additional uncertainty arises from the atmospheric variability which describes ambient, instrumentally independent variations in the considered trace gases and parameters caused by, for example, atmospheric turbulence. The uncertainty from the atmospheric variability represented by the 1$\mathit{\sigma }$ standard deviation of the mean over the considered 9 nights is 54 %, which exceeds the uncertainty from the calculation. We, therefore, estimate the uncertainty of $v_{\mathrm{d}}$ to be 54 %. Please note that, in our uncertainty analysis, we consider the arising statistical errors but not the systematic errors which are not quantifiable but could potentially increase the overall uncertainty. An overview of all uncertainties and the time resolution of the measured trace gases can be found in Table S3. Absolute ${\mathrm{H}}_{\mathrm{2}}\mathrm{O}$ concentrations were estimated from the measured relative humidity via the Magnus formula over water. Please note that some trace gases were not available simultaneously or only for a short overlap. We, therefore, present the averaged diurnal profiles.

2.3.3 HUMPPA campaign in 2010

The Hyytiälä United Measurements of Photochemistry and Particles (HUMPPA) campaign took place in July and August 2010 at SMEAR II (Station for Measuring Ecosystem–Atmosphere Relation) in Hyytiälä, Finland (61.85${}^{\circ }$ N, 24.28${}^{\circ }$ E, 181 $\mathrm{m}\mathrm{a}.\mathrm{s}.\mathrm{l}.$). The site is located in a remote area in a boreal forest. A detailed description of the campaign can be found in . The measurement methods for ${\mathrm{NO}}_x$, ${\mathrm{O}}_{\mathrm{3}}$, HCHO and ${\mathrm{CH}}_{\mathrm{4}}$ were the same as those presented for the CYPHEX campaign. ${\mathrm{CH}}_{\mathrm{3}}\mathrm{OH}$ was measured via a cold trap PTR-MS with a detection limit of around 50 pptv (integration time of 5 min). Acetaldehyde was measured via PTR-MS with a detection limit of 50 pptv integration time of 6 min;. Isoprene was measured via GC (GC 6890A, Agilent Technologies, Inc.) coupled to a mass selective detector (MSD 5973 inert, Agilent Technologies, Inc.) with an uncertainty of around 15 %. Highly constrained box model simulations, which were in fair agreement with experimental data, were available for OH and ${\mathrm{HO}}_{\mathrm{2}}$, as described by , with an uncertainty in the order of 30 %–40 %. $j\left({\mathrm{NO}}_{\mathrm{2}}\right)$ and $j\left({\mathrm{O}}^{\mathrm{1}}\mathrm{D}\right)$ were measured with filter radiometers (Meteorologie Consult GmbH, Königstein, Germany) with an uncertainty of around 10 %; $j\left(\mathrm{HCHO}\right)$ was determined via parameterization (analogous to CYPHEX and HOPE). ${\mathrm{H}}_{\mathrm{2}}\mathrm{O}$ was measured with an infrared light absorption analyzer (URAS 4 H2O, Hartmann & Braun AG, Frankfurt am Main, Germany). The BLH was measured by radio soundings, as presented by , ranging from 200 m during nighttime (here $j\left({\mathrm{NO}}_{\mathrm{2}}\right)$ $<$ 10${}^{-\mathrm{3}}$ ${\mathrm{s}}^{-\mathrm{1}}$) to 1500 m during daytime here $j\left({\mathrm{NO}}_{\mathrm{2}}\right)$ $<$ 10${}^{-\mathrm{3}}$ ${\mathrm{s}}^{-\mathrm{1}}$;. The deposition velocity was determined analogously to the HOPE campaign, based on the nighttime HCHO loss on the basis of 14 nights, and was 0.85 $\mathrm{cm}{\mathrm{s}}^{-\mathrm{1}}$ during the day and 0.43 $\mathrm{cm}{\mathrm{s}}^{-\mathrm{1}}$ during the night. The uncertainty of the calculation results from the single uncertainties of $\frac{\mathrm{d}\left[\mathrm{HCHO}\right]}{\mathrm{d}t}$ (16 %), $[\mathrm{HCHO}{]}_{\text{av}}$ (33 %) and the nighttime BLH (20 %). Gaussian error propagation gives an overall uncertainty of 42 % from the calculation. The atmospheric variability equals 54 %. We, therefore, estimate the total uncertainty of the deposition velocity to be 54 %. An overview of all considered nights and the respective HCHO loss is presented in Fig. S3c. The deposition velocity of ozone was adopted from for the time period during calendar weeks 25–34 of the year and a relative humidity below 70 %, which is 0.491 $\mathrm{cm}{\mathrm{s}}^{-\mathrm{1}}$ for daytime and 0.069 $\mathrm{cm}{\mathrm{s}}^{-\mathrm{1}}$ for nighttime. A modeling study by presents the average values in the same order of magnitude ($\sim$ 0.2–0.3 $\mathrm{cm}{\mathrm{s}}^{-\mathrm{1}}$ for July and August). Again, uncertainties and time resolution are shown in Table S3. Similar to the HOPE campaign, some trace gases were not available simultaneously, and we, therefore, present the averaged diurnal profiles.

3 Results and discussion

3.1 Net HCHO production during CYPHEX in 2014

HCHO concentrations during the CYPHEX campaign ranged between 0.3 and 1.9 $\mathrm{ppbv}$ (1.1 $\pm$ 0.4 ppbv on average), with a maximum in the diel cycle during morning hours (04:00 UTC) and a minimum in the afternoon (15:00 UTC). Please note the mean local time difference stated in Sect.  and Fig. . The temporal development of HCHO concentrations during the campaign and the respective $j\left({\mathrm{NO}}_{\mathrm{2}}\right)$ values (to illustrate the daily cycle) are shown in Fig. S3a. Figure S4a presents the diurnal average of HCHO, including its rate of change $\frac{\mathrm{d}\left[\mathrm{HCHO}\right]}{\mathrm{d}t}$. The uncertainty is dominated by the atmospheric variability which is on average 27 % for daytime HCHO.

Figure 5

Temporal development of (a) HCHO production terms, (b) HCHO loss terms and (c) net HCHO from 22 July to 31 July 2014 during the CYPHEX research campaign in Cyprus. The ${\mathrm{NO}}_{\mathrm{2}}$ photolysis frequency $j\left({\mathrm{NO}}_{\mathrm{2}}\right)$ is shown in panel (d) as an illustration of the diurnal cycle. All times are in UTC.

[Figure omitted. See PDF]

Figure  shows the time series of the HCHO production terms (Fig. a), the HCHO loss terms (Fig. b) and the net HCHO production (Fig. c) during the CYPHEX research campaign in Cyprus in July 2014. We calculated the HCHO production terms for all measured gas-phase precursors shown in Fig. . The individual production terms are shown in Fig. S5. The total measurement uncertainties were determined via Gaussian error propagation and were 28 % for HCHO production (31 % for only considering the OH oxidation of methane, methanol, isoprene and acetaldehyde) and 26 % for HCHO loss. Table S4 provides an overview of all calculated uncertainties. We present two example step-by-step calculations via Gaussian error propagation in Eqs. (S2)–(S8). All other calculations were made accordingly. We have neglected the uncertainties for the HCHO yield from isoprene, ${\mathit{\alpha }}_{{\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}}$ and ${\mathit{\alpha }}_{{\mathrm{CH}}_{\mathrm{3}}\mathrm{CHO}}$ and instead present a sensitivity study for these parameters later in this section. Dark green colors show the overall HCHO production as the sum of all single production terms. All production terms show a diurnal cycle which follows the course of the photolysis frequency $j\left({\mathrm{NO}}_{\mathrm{2}}\right)$, which we show in Fig. d. Photolysis reactions do not take place after sunset, and oxidation reactions are dependent on the abundance of OH radicals, which is low during nighttime. Therefore, HCHO production approaches zero during nighttime. Due to data gaps, a full diurnal profile was only available for 23, 28 and 30 July, where the overall HCHO production reached maxima between 0.6 and 0.8 $\mathrm{ppbv}{\mathrm{h}}^{-\mathrm{1}}$. The reactions of methane, methanol, isoprene and acetaldehyde with OH dominated the HCHO production processes. This is additionally illustrated in Fig. , which presents the daily average share (including day- and nighttime values) of each production term based on a balance to the overall loss rate. HCHO production was, therefore, dominated by the reaction of methane and OH (almost a third), followed by the oxidation of acetaldehyde contributing around 15 % and the OH oxidations of isoprene and methanol, both contributing around 14 %. These four species together represented 75 % of the overall HCHO production required to balance the sinks. The production through the OH oxidation of methyl hydroperoxide and dimethyl sulfide and through the reaction of isoprene and ozone contributed by around 1 %–2 % each. The remaining species each yielded less than 1 % of the overall HCHO. Less than 20 % was unaccounted for (the rest in Fig. ). This part also includes HCHO production from terpenes via oxidation through OH or ${\mathrm{O}}_{\mathrm{3}}$. The yields from these reactions vary greatly in the literature. Considering the yields from OH oxidation, suggested by , from laboratory investigations, limonene, $\mathit{\beta }$- and $\mathit{\alpha }$-pinene would account for 3 %, 2 % and 1 % of the overall HCHO production, respectively. The isoprene yield is limited to a value between 34 % and 57 %. The lower limit would give a HCHO production from isoprene of 11 %, and the upper limit would yield 19 %. The value for ${\mathit{\alpha }}_{{\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}}$ can theoretically be between 0 % and 100 % but is likely situated at the upper end due to the availability of NO. As an example, a 20 % decrease in ${\mathit{\alpha }}_{{\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}}$ would give a HCHO production from ${\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}$ of 38 % (compared to 47 % for the calculated ${\mathit{\alpha }}_{{\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}}$). A 20 % increase would yield 57 % on average and decrease the rest to less than 10 %. For ${\mathit{\alpha }}_{{\mathrm{CH}}_{\mathrm{3}}\mathrm{CHO}}$, a 20 % decrease and increase would give a HCHO yield from acetaldehyde of 12 % and 18 %, respectively, assuming a constant ${\mathit{\alpha }}_{{\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}}$. Please note that the uncertainty of the absolute values used to create this pie chart is dominated by the atmospheric and diurnal variability in the single terms and is of the order of 100 %.

Figure 6

Chemical production terms of HCHO during CYPHEX, including daily averages of all data.

[Figure omitted. See PDF]

HCHO loss was determined from the reaction with OH and photolysis. Red colors in Fig. b show the overall calculated HCHO loss. Similar to the HCHO production, HCHO loss via OH and photolysis only plays a role during the daytime. At night, dry deposition is the only HCHO loss mechanism, and the deposition velocity $v_{\mathrm{d}}$ can be determined from the nighttime decrease in ambient HCHO concentrations, as shown by . However, we often observed increasing HCHO concentrations during nighttime, particularly before sunrise. The reason for this nighttime HCHO increase is not yet fully understood. The role of the deposition processes at elevated altitudes is not yet fully understood but is likely influenced by flows along mountain slopes and horizontal advection on hilltops. For hilltops, incoming air through advection likely originated from areas without deposition too high above the ground;. Please note that the effect of deposition processes could also be counteracted by a nighttime HCHO source, such as terpene oxidation by ozone or advection. The determined value for the deposition can, therefore, be seen as being a lower estimate . As we do not observe the net loss of HCHO at night during the CYPHEX campaign, we estimate the dry deposition to be negligible. Figure c shows the overall HCHO production and loss rates, as well as the difference between both, which we refer to as net HCHO production, in black. Production and loss showed a good balance with values of $\pm$ 0.2 $\mathrm{ppbv}{\mathrm{h}}^{-\mathrm{1}}$. On most days, HCHO loss prevailed over HCHO production, based on measured precursors.

Figure 7

Diurnal profiles of (a) HCHO production $P\left(\mathrm{HCHO}\right)$, (b) HCHO loss $L\left(\mathrm{HCHO}\right)$ and (c) HCHO net terms during the CYPHEX campaign in 2014. Solid lines show the hourly averaged HCHO production and loss terms, based on the point-by-point calculation of simultaneous parameter measurements. The uncertainty from the atmospheric variability is represented by the 1$\mathit{\sigma }$ error shades. For the dashed lines, all measurement parameters were averaged first, followed by the calculation of hourly HCHO production and loss terms. The uncertainty is based on the atmospheric variability of all parameters and is exemplarily shown by the error bar for one point for each production and loss term. The gray dashed line represents the diurnal solar elevation angle at the measurement site, as determined by help of the .

[Figure omitted. See PDF]

In order to better account for diurnal changes, we investigated the daily cycle of HCHO production and loss rates based on hourly averages over all measurement days. Figure  shows the diurnal profiles of the main HCHO production terms (Fig. a) as determined above, the HCHO loss terms (Fig. b) and net HCHO production (Fig. c). The solid lines represent the hourly averages of the point-by-point calculation of the production and loss terms. The uncertainty is composed of the measurement uncertainty and the atmospheric variability, where the latter is demonstrated by the 1$\mathit{\sigma }$ error shades. For HCHO production, the measurement uncertainty was 31 %, and the daytime atmospheric variability was 40 % (61 % for day and night). For HCHO loss, the uncertainties were 26 % and 34 % (57 %), respectively. In both cases, the overall uncertainty was dominated by the atmospheric variability. The dashed lines show the hourly production and loss terms calculated from the hourly averaged trace gas concentrations. The uncertainty from the atmospheric variability was 22 % (34 %) for HCHO production and 25 % (52 %) for HCHO loss and is exemplarily indicated by an error bar for one point for each production and loss term in Fig. . Both methods have advantages and disadvantages. The point-by-point calculation allows for a simultaneous consideration of all measurement parameters. Potential atmospheric changes or incidents such as wind, precipitation or rare primary emission events are reflected by all parameters as they are monitored at the same time. On the other hand, this method reduces the number of data points used as only one single missing species prevents the calculation of the overall term. In order to increase the number of results, we have interpolated the values for the isoprene yield (data coverage 81 %), ${\mathit{\alpha }}_{{\mathrm{CH}}_{\mathrm{3}}\mathrm{CHO}}$ and ${\mathit{\alpha }}_{{\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}}$ (data coverage 64 %). Calculating production and loss terms from the hourly averaged trace gas concentrations allows for the inclusion of all measured parameters but could potentially increase the uncertainty of the estimate, depending on the duration and overlap of the single measurements. However, in this case, the data were limited to 1 week in July with mainly simultaneous measurements of all parameters, and we, therefore, do not expect large uncertainties. The similarity of the results, as shown in Fig. , indicates that both methods provide reasonable results.

For HCHO production, the daily maxima of around 0.4–0.45 $\mathrm{ppbv}{\mathrm{h}}^{-\mathrm{1}}$ were reached between 09:00 and 10:00 UTC, which was coincident with the maximum of the photolysis frequency $j\left({\mathrm{NO}}_{\mathrm{2}}\right)$. HCHO production from methane dominated the overall production term, with a maximum of close to 0.2 $\mathrm{ppbv}{\mathrm{h}}^{-\mathrm{1}}$, followed by acetaldehyde, isoprene and methanol. HCHO loss peaked around 09:00 UTC, with a value of 0.5 $\mathrm{ppbv}{\mathrm{h}}^{-\mathrm{1}}$, with around 55 % contribution from photolysis and 45 % from OH oxidation. Figure c shows that the calculated production term for HCHO can almost completely balance the loss, which, assuming that the major loss processes are well constrained, leads to the conclusion that HCHO production can be approximated by OH oxidation of methane, acetaldehyde, isoprene and methanol. This is in line with the HCHO rate of change presented in Fig. S4a which oscillated around zero. Therefore, transport processes and primary emissions during CYPHEX can likely be excluded.

3.2

Net ${\mathrm{O}}_{\mathrm{3}}$ production during CYPHEX in 2014

Ozone varied between 46 and 104 ppbv during the CYPHEX campaign (70 $\pm$ 13 ppbv on average), with a diel maximum at 04:00 UTC and a minimum at 15:00 UTC. The time series of ${\mathrm{O}}_{\mathrm{3}}$ concentrations is presented in Fig. S6a. The diel mean, including the rate of change $\mathrm{d}{\mathrm{O}}_{\mathrm{3}}/\mathrm{d}t$, can be found in Fig. S7a. The uncertainty is dominated by the atmospheric variability, which is on average 16 % (1$\mathit{\sigma }$) for ${\mathrm{O}}_{\mathrm{3}}$.

Figure 8

Diurnal profiles of (a) ozone production $P\left({\mathrm{O}}_{\mathrm{3}}\right)$, (b) ozone loss $L\left({\mathrm{O}}_{\mathrm{3}}\right)$ and (c) ozone net terms during the CYPHEX campaign in 2014. Solid lines show the hourly averaged ${\mathrm{O}}_{\mathrm{3}}$ production and loss terms, based on the point-by-point calculation of simultaneous parameter measurements. The uncertainty from the atmospheric variability is represented by the 1$\mathit{\sigma }$ error shades. For the dashed lines, all measurement parameters were averaged first, followed by the calculation of hourly ${\mathrm{O}}_{\mathrm{3}}$ production and loss terms. The uncertainty is mostly dominated by the atmospheric variability in all parameters and is exemplarily shown by the error bar for one point for each production and loss term. Please find the temporal development of production and loss terms throughout the campaign in Fig. S8.

[Figure omitted. See PDF]

Figure  shows the diurnal cycle of the production and loss rates for ozone, analogous to Fig. . Solid lines show the hourly averaged point-by-point calculations of the ${\mathrm{O}}_{\mathrm{3}}$ production and loss terms. The 1$\mathit{\sigma }$ error shades present the atmospheric variability, which was 59 % for ${\mathrm{O}}_{\mathrm{3}}$ production and 37 % for ${\mathrm{O}}_{\mathrm{3}}$ daytime loss (44 % for day and night). The measurement uncertainties were 32 % and 16 %, respectively, and the overall uncertainty was, therefore, dominated by the atmospheric variability. Dashed lines show the ${\mathrm{O}}_{\mathrm{3}}$ production and loss terms based on the hourly averaged measurement parameters. The uncertainty resulting from the averaging of the individual parameters is exemplarily shown by the error bar for one point and is similar to the atmospheric variability obtained by the point-by-point method (57 % for $P\left({\mathrm{O}}_{\mathrm{3}}\right)$ and 35 % (49 %) for $L\left({\mathrm{O}}_{\mathrm{3}}\right)$). Figure a shows ${\mathrm{O}}_{\mathrm{3}}$ production represented by the photolysis of ${\mathrm{NO}}_{\mathrm{2}}$. Figure b shows the ${\mathrm{O}}_{\mathrm{3}}$ loss terms. ${\mathrm{O}}_{\mathrm{3}}$ loss through reaction with NO was dominant, followed by photolysis. The loss via OH and ${\mathrm{HO}}_{\mathrm{2}}$ was negligibly small. ${\mathrm{O}}_{\mathrm{3}}$ net production during the CYPHEX campaign was, therefore, clearly dominated by nitrogen oxides chemistry. Figure c shows the net ${\mathrm{O}}_{\mathrm{3}}$ production. ${\mathrm{O}}_{\mathrm{3}}$ production and loss were similar throughout the day, with peak values of 4–7 $\mathrm{ppbv}{\mathrm{h}}^{-\mathrm{1}}$ between 05:00 and 10:00 UTC. Net ${\mathrm{O}}_{\mathrm{3}}$ production was between $-$1 and 1 $\mathrm{ppbv}{\mathrm{h}}^{-\mathrm{1}}$. Please note that we have excluded the ${\mathrm{NO}}_{\mathrm{2}}$ data from 24 July between 13:15 and 16:15 UTC due to a singular high-concentration event. The large spike in ${\mathrm{NO}}_{\mathrm{2}}$ (${\mathrm{O}}_{\mathrm{3}}$ titration of NO) is likely the result of sampling air impacted by the exhaust from a diesel generator which provided on-site power and was located about 200 m from the containers housing the instruments. We show ${\mathrm{O}}_{\mathrm{3}}$ net production, including all ${\mathrm{NO}}_{\mathrm{2}}$ data points, in Fig. S9a. ${\mathrm{O}}_{\mathrm{3}}$ production is directly proportional to the ${\mathrm{NO}}_{\mathrm{2}}$ concentration, according to Eq. (), which explains the large afternoon production peak. We show the diel profile of ${\mathrm{NO}}_{\mathrm{2}}$ concentrations with and without the afternoon peak in Fig. S9b. Production and loss terms for ${\mathrm{O}}_{\mathrm{3}}$ were balanced, and the ${\mathrm{O}}_{\mathrm{3}}$ rate of change oscillated around zero (Fig. S7a), suggesting that the diel variability was likely not impacted by transport processes.

Figure 9

Diurnal profiles of HCHO production $P\left(\mathrm{HCHO}\right)$ and loss $L\left(\mathrm{HCHO}\right)$ terms during the HOPE campaign 2012 (top row) and the HUMPPA campaign 2010 (bottom row). (a) $P\left(\mathrm{HCHO}\right)$, (b) $L\left(\mathrm{HCHO}\right)$, (c) net HCHO), (d) $P\left(\mathrm{HCHO}\right)$, (e) $L\left(\mathrm{HCHO}\right)$ and (f) net($\mathrm{HCHO}$).

[Figure omitted. See PDF]

3.3 Comparison with HOPE (2012) and HUMPPA (2010)

3.3.1 Net HCHO production

We have shown, in Sect.  and , that the hourly averaging of measurement parameters and subsequent calculation of production and loss terms yielded reliable results during the CYPHEX campaign. For HUMPPA and HOPE, we have pursued this approach regarding the calculations of HCHO and ${\mathrm{O}}_{\mathrm{3}}$ production and loss terms, as the simultaneous data availability for all measurement parameters was too low for a point-by-point analysis.

HCHO mixing ratios during the HOPE campaign varied between 0.1 and 3.2 ppbv (1.1 $\pm$ 0.5 ppbv on average), with a maximum in the diel cycle at 15:00 UTC and a minimum at 06:00 UTC. The average mixing ratio was similar to the average mixing ratio during the CYPHEX campaign, but the variability was higher, which is likely due to the longer time period of available data which was about 4 weeks for HOPE (compared to a bit more than 1 week for CYPHEX), including, e.g., larger temperature variations. HCHO mixing ratios in Hyytiälä during the HUMPPA campaign ranged between 0.03 and 5.7 $\mathrm{ppbv}$, with an average of 0.4 $\pm$ 0.5 ppbv. The variability is high because of biomass burning events in Russia which were detected at the site in Finland on 26–30 July and 9 August, as described by . The large HCHO peaks detected on these days can also be seen in Fig. S3c. Figure S4b and c present the diurnal cycles for HCHO, including the rate of change $\frac{\mathrm{d}\left[\mathrm{HCHO}\right]}{\mathrm{d}t}$ during HOPE and HUMPPA. The uncertainty is dominated by the atmospheric variability represented by the 1$\mathit{\sigma }$ standard deviation, which is, on average, 44 % for HCHO for HOPE and 106 % for HUMPPA.

Figure  shows the HCHO production and loss rates for the two campaigns. For all cases, the uncertainty was dominated by the atmospheric variability (1$\mathit{\sigma }$), which was 42 % for daytime HCHO production and 40 % for daytime HCHO loss in Hohenpeißenberg and 38 % and 77 % in Hyytiälä, respectively. The measurement uncertainty was around 30 % to 40 %. We present the atmospheric variability with the error bars in Fig. . For better clarity, we only show one error bar for each term. An overview of all calculated uncertainties can be found in Table S4. HCHO production during HOPE is shown in Fig. a. The maximum production rate of 0.48 $\mathrm{ppbv}{\mathrm{h}}^{-\mathrm{1}}$ was reached between 11:00 and 12:00 UTC, and a comparison to $j\left({\mathrm{NO}}_{\mathrm{2}}\right)$ shows good agreement with local noon. The production of HCHO was dominated by the oxidation of acetaldehyde, which contributed to the peak production by around 50 %, followed by methane, isoprene and methanol. We show a pie chart representing the contribution of the single HCHO production terms during HOPE in Fig. S10a. HCHO loss is shown in Fig. b. The maximum loss rate of HCHO was 0.46 $\mathrm{ppbv}{\mathrm{h}}^{-\mathrm{1}}$. During the day, HCHO loss was dominated by photolysis and oxidation, while, at nighttime, deposition was the main loss path for formaldehyde in Hohenpeißenberg. Figure c shows HCHO net production during HOPE. The calculated production of HCHO slightly prevailed over its loss. At 11:00 UTC, HCHO loss was $>$ 95 % of HCHO production. Overall absolute loss and production terms were very similar compared to the results obtained for the site in Cyprus. The main difference is the composition of the HCHO production, which was dominated by the oxidation of acetaldehyde in Hohenpeißenberg and by the oxidation of methane in Cyprus. HCHO production and loss during the HUMPPA campaign are shown in Fig. d–f. HCHO production reached a peak value of 0.15 $\mathrm{ppbv}{\mathrm{h}}^{-\mathrm{1}}$ at 12:00 UTC. Methane and acetaldehyde contributed to the overall production by approximately equal parts, followed by isoprene and methanol. Figure S10b shows the share of the individual HCHO production terms during HUMPPA. showed that the contribution from terpene oxidation to HCHO production was small (1 %–2 % each), which is in line with our findings for the CYPHEX campaign. HCHO loss was dominated by photolysis during the day and by dry deposition at night. Figure f shows that HCHO production and loss were in good agreement throughout the day ($\sim$ 90 %), apart from the morning hours 06:00–07:00 UTC when HCHO production prevailed over its loss by around 2 to 3 times, indicating a missing loss term, most likely due to dilution with HCHO-poor air during the rise of the planetary boundary layer in the early morning hours (accompanied by a peak in the HCHO rate of change as shown in Fig. S4b). Overall production and loss terms for HCHO were around 3 times smaller compared to the values obtained for the sites in Germany and Cyprus. We also observed smaller concentrations of ${\mathrm{CH}}_{\mathrm{4}}$, OH radicals and HCHO. It is notable that HCHO production was slightly higher than the loss for both the HUMPPA and the HOPE campaign. This is also reflected by peaks in the rate of change (0.1–0.2 $\mathrm{ppbv}{\mathrm{h}}^{-\mathrm{1}}$) in the morning/midday hours (Fig. S4b and c) and could indicate a transport effect from areas with lower HCHO concentration, e.g., entrainment, according to Eq. (). For HUMPPA, this idea is supported when excluding the data impacted by biomass burning, which we show in Fig. S11a. It can be seen that HCHO production prevailed over its loss, suggesting a missing loss term. The difference was highest in the morning hours, with approximately 0.1 $\mathrm{ppbv}{\mathrm{h}}^{-\mathrm{1}}$, and decreased throughout the day indicating, e.g., a vertical dilution from higher, HCHO-poor altitudes. For comparison, Fig. S11b shows the HCHO production and loss terms when only considering data impacted by biomass burning. Due to high HCHO mixing ratios, the loss terms were substantially higher compared to its production. In periods influenced by biomass burning, the highest HCHO yield was from acetaldehyde (averaged diel mixing ratios of 1.1 ppbv compared to 0.6 ppbv without biomass burning); when excluding biomass burning, the yield from methane was slightly higher.

Figure 10

Diurnal profiles of ${\mathrm{O}}_{\mathrm{3}}$ production $P\left({\mathrm{O}}_{\mathrm{3}}\right)$ and loss $L\left({\mathrm{O}}_{\mathrm{3}}\right)$ terms during the HOPE campaign 2012 (top row) and the HUMPPA campaign 2010 (bottom row). (a) $P\left({\mathrm{O}}_{\mathrm{3}}\right)$, (b) $L\left({\mathrm{O}}_{\mathrm{3}}\right)$, (c) net ${\mathrm{O}}_{\mathrm{3}}$, (d) $P\left({\mathrm{O}}_{\mathrm{3}}\right)$, (e) $L\left({\mathrm{O}}_{\mathrm{3}}\right)$ and (f) net(${\mathrm{O}}_{\mathrm{3}}$).

[Figure omitted. See PDF]

3.3.2

Net ${\mathrm{O}}_{\mathrm{3}}$ production

Ozone concentrations in Hohenpeißenberg were, on average, 44 $\pm$ 11 ppbv, with a minimum of 5 ppbv and a maximum of 97 ppbv. The campaign-averaged diel profile displayed a peak of 48 ppbv at 16:00 UTC and a minimum of 39 ppbv at 07:00 UTC. In Hyytiälä, ozone concentrations were between 20 and 76 ppbv and 42 $\pm$ 11 ppbv on average. A diel peak of 49 ppbv was reached between 15:00 and 16:00 UTC and a minimum of 34 ppbv at 05:00 UTC. The temporal development of ozone concentrations during the campaigns and the diurnal averages can be found in Figs. S6 and S7. The uncertainty is dominated by the atmospheric variability (1$\mathit{\sigma }$) which is, on average, 24 % for ${\mathrm{O}}_{\mathrm{3}}$ for HOPE and 23 % for HUMPPA.

Figure  shows the ozone production and loss terms for the research campaigns HOPE and HUMPPA. The overall uncertainty was again dominated by the atmospheric variability (1$\mathit{\sigma }$), which was 58 % for the daytime ${\mathrm{O}}_{\mathrm{3}}$ production and 90 % for the daytime ${\mathrm{O}}_{\mathrm{3}}$ loss in Hohenpeißenberg and 44 % and 51 %, respectively, in Hyytiälä. In comparison, the measurement uncertainty regarding overall production and loss was between 10 % and 15 %. A detailed overview of the uncertainties can be found in Table S4. We adopted the dry deposition velocity for ozone in Hyytiälä from . No literature values for the ozone dry deposition in Hohenpeißenberg were available. Therefore, we applied the same values as for the HUMPPA campaign, which increased the uncertainty of the analysis. However, the fraction of ozone dry deposition of the overall loss was small. For the applied deposition velocity, dry deposition contributed by around 4 % during the daytime. For a change in $v_{\mathrm{d}}$ of $\pm$ 100 %, the fraction varied between 2 % and 7 %. We, therefore, assume a maximum additional uncertainty of 5 % resulting from this estimate. Ozone production in Hohenpeißenberg reached peak values of 38 $\mathrm{ppbv}{\mathrm{h}}^{-\mathrm{1}}$. In contrast, ozone loss showed a maximum of only 21 $\mathrm{ppbv}{\mathrm{h}}^{-\mathrm{1}}$, most of which was due to the reaction with NO. In Hyytiälä, ozone production was 6.7 $\mathrm{ppbv}{\mathrm{h}}^{-\mathrm{1}}$ at its diurnal maximum, while ozone loss reached 5.1 $\mathrm{ppbv}{\mathrm{h}}^{-\mathrm{1}}$ and was mainly composed of the loss via NO, followed by dry deposition. The differences between production and loss terms could again indicate a transport effect, according to Eq. (), as described for HCHO. The rate of change for ${\mathrm{O}}_{\mathrm{3}}$ showed peak values (2–3 $\mathrm{ppbv}{\mathrm{h}}^{-\mathrm{1}}$) during the morning/midday hours, which was not observed for the CYPHEX campaign (Fig. S7). ${\mathrm{O}}_{\mathrm{3}}$ production and loss terms during HUMPPA and CYPHEX were similar, while the values were significantly higher during HOPE. ${\mathrm{O}}_{\mathrm{3}}$ production in Hohenpeißenberg was almost 1 order of magnitude higher compared to the other sites, which was likely due to the higher ambient ${\mathrm{NO}}_x$ concentrations. The net ${\mathrm{O}}_{\mathrm{3}}$ production (the difference between ${\mathrm{O}}_{\mathrm{3}}$ production and loss) at each site could give a hint regarding the dominant chemical ozone regime. For HOPE, net ${\mathrm{O}}_{\mathrm{3}}$ production was significantly above zero, with diurnal maximum values of around 20 $\mathrm{ppb}{\mathrm{h}}^{-\mathrm{1}}$ at 10:00 UTC, which could indicate a VOC limitation. In contrast, net ${\mathrm{O}}_{\mathrm{3}}$ production was close to zero for CYPHEX, and the ozone regime was more likely ${\mathrm{NO}}_x$ limited. We will discuss the dominant chemical ozone regime in detail in the following section.

Figure 11

Determination of the dominant chemical regime via (a) the $\mathrm{HCHO}/{\mathrm{NO}}_{\mathrm{2}}$ ratio (colored areas indicate the dominant chemical regime, according to , which are blue ($\mathrm{HCHO}/{\mathrm{NO}}_{\mathrm{2}}$ $>$ 2) for a ${\mathrm{NO}}_x$ limitation, green ($\mathrm{HCHO}/{\mathrm{NO}}_{\mathrm{2}}$ $<$ 1) for a VOC limitation and yellow (1 $<$ $\mathrm{HCHO}/{\mathrm{NO}}_{\mathrm{2}}$ $<$ 2) for the transition), (b) the fraction of methyl peroxy radicals forming HCHO and (c) the HCHO yield from isoprene.

[Figure omitted. See PDF]

3.4 Chemical regime

Various methods exist to determine the prevailing chemical ozone regime (i.e., the net efficiency of production or loss), one of which is the ratio of formaldehyde and nitrogen dioxide. We have calculated the diel $\mathrm{HCHO}/{\mathrm{NO}}_{\mathrm{2}}$ ratios for all three measurement sites, which is shown in Fig. a. The $\mathrm{HCHO}/{\mathrm{NO}}_{\mathrm{2}}$ ratio was highest in Cyprus with 8.0 $\pm$ 2.4, followed by 1.4 $\pm$ 0.7 in Hyytiälä and 0.7 $\pm$ 0.2 in Hohenpeißenberg. According to findings by and these values indicate a dominant ${\mathrm{NO}}_x$-limited regime during CYPHEX and a dominant VOC-limited regime during HOPE. The regime during HUMPPA was likely transitioning between both limitations. We show two additional approaches for determining the present chemical regime in Fig. . In Fig. b, we present the daytime averages of ${\mathit{\alpha }}_{{\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}}$ versus the NO concentration. All campaigns show a linear correlation. Daytime average NO concentrations during CYPHEX ranged from 1 to 45 pptv, accompanied by an increase in ${\mathit{\alpha }}_{{\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}}$ from around 55 % to 75 %, giving a slope of 5.54 ${\mathrm{ppbv}}^{-\mathrm{1}}$. The slope for the increase in ${\mathit{\alpha }}_{{\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}}$ with NO is approximately half for the HUMPPA campaign, with a value of 2.52 ${\mathrm{ppbv}}^{-\mathrm{1}}$. The NO concentration ranged from 22 to 76 pptv, along with an increase in ${\mathit{\alpha }}_{{\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}}$ from 73 % to 87 %. Finally, for the HOPE campaign, NO concentrations and its range were highest with values between 60 and 350 pptv. At the same time, ${\mathit{\alpha }}_{{\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}}$ showed the smallest increase by only 3 percentage points. The resulting slope was the smallest, with a value of 0.11 ${\mathrm{ppbv}}^{-\mathrm{1}}$. ${\mathit{\alpha }}_{{\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}}$ indicates the share of ${\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}$ that forms HCHO, predominantly through the reaction with NO. The competing reaction is the conversion with ${\mathrm{HO}}_{\mathrm{2}}$ to ${\mathrm{CH}}_{\mathrm{3}}\mathrm{OOH}$. A high value for ${\mathit{\alpha }}_{{\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}}$, which is not (or only a little) responsive to a changing NO concentration, indicates a VOC limited regime, while in a ${\mathrm{NO}}_x$-limited regime, small changes in ambient NO have a large effect on the HCHO formation from ${\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}$. Analogously, we show the HCHO yield from isoprene, according to Eq. (), versus NO concentrations in Fig. c, which we suggest as an indicator for the present chemical regime too. For the CYPHEX campaign, the isoprene yield was most responsive to ambient NO concentrations with a slope of 1.61 ${\mathrm{ppbv}}^{-\mathrm{1}}$, indicating a ${\mathrm{NO}}_x$ limitation. In contrast, the isoprene yield during the HOPE campaign was almost non-responsive to changing NO, indicating a VOC limitation (slope of 0.05 ${\mathrm{ppbv}}^{-\mathrm{1}}$). Although specialized instrumentation is still necessary to measure NO, OH and ${\mathrm{HO}}_{\mathrm{2}}$, these methods to determine the dominant chemical regime only require the knowledge of a small number of trace gas concentrations and the ambient temperature.

4 Conclusions

In this study, we have analyzed the photochemical processes contributing to formaldehyde and ozone production and loss across Europe based on in situ trace gas observations during three different stationary field campaigns in Cyprus (CYPHEX in 2014), Germany (HOPE in 2012) and Finland (HUMPPA in 2010). Very consistently across all sites, we found that formaldehyde loss can be predominantly accounted for by the production via the OH oxidation of methane, acetaldehyde, isoprene and methanol. Formaldehyde loss is represented by photolysis, OH oxidation and, to a small extent, by dry deposition. Ozone chemistry is mainly controlled by nitrogen oxides. The production can be described by ${\mathrm{NO}}_{\mathrm{2}}$ photolysis, and the loss is mainly a function of NO reduction and, to a smaller extent, of photolysis and dry deposition. We found a good agreement between ${\mathrm{O}}_{\mathrm{3}}$ production and loss in Cyprus and Finland, while the production was approximately double its loss in southern Germany. Finally, we have presented several different approaches for determining the prevalent chemical regime, which included the $\mathrm{HCHO}/{\mathrm{NO}}_{\mathrm{2}}$ ratio, and the fraction of ${\mathrm{CH}}_{\mathrm{3}}{\mathrm{O}}_{\mathrm{2}}$ forming HCHO, and the HCHO yield from isoprene in its dependence on the ambient NO concentration. We identify a VOC-limited regime during the HOPE campaign in Germany and a ${\mathrm{NO}}_x$-limited regime during the CYPHEX campaign in Cyprus, whereas chemistry during the HUMPPA campaign in Finland was likely at a transitional point.

While ongoing research on HCHO photochemical processes has continuously widened the contributors to possible production paths and the complexity of calculations and models, we show that the consideration of only four precursor VOCs is capable of almost completely representing the HCHO production term at various sites across Europe. We encourage extending the HCHO budget calculations based on in situ trace gas observations to more sites worldwide as a simple, but effective, tool to monitor photochemical processes and air quality, including the dominant chemical regime.

Data availability

All data generated and analyzed for this study are available from KEEPER (; https://keeper.mpdl.mpg.de/, last access: 6 December 2021) upon request to the authors.

The supplement related to this article is available online at: https://doi.org/10.5194/acp-21-18413-2021-supplement.

Author contributions

HF had the idea. CMN and HF designed the study. CMN analyzed the data and wrote the paper. JS, JNC and BB provided J values. CPD provided trace gas measurements for HOPE. JNC provided OH and ${\mathrm{HO}}_{\mathrm{2}}$ model data for HUMPPA. JW provided VOC data. HH, CE, AN, KT, MM, CM and LT provided OH and ${\mathrm{HO}}_{\mathrm{2}}$ data for CYPHEX and HOPE. HCHO data were measured and provided by AR and RA. SH provided ${\mathrm{CH}}_{\mathrm{3}}\mathrm{OOH}$ data. ${\mathrm{NO}}_x$ and ${\mathrm{O}}_{\mathrm{3}}$ data were obtained from HF. JL significantly contributed to planning the research campaigns.

Competing interests

The contact author has declared that neither they nor their co-authors have any competing interests.

Disclaimer

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Acknowledgements

We acknowledge all researchers and supporting personnel who participated in the CYPHEX campaign in 2014, the HOPE campaign in 2012 and the HUMPPA campaign in 2010. We would like to thank Pekka Rantala (University of Helsinki), for providing the ${\mathrm{CH}}_{\mathrm{3}}\mathrm{CHO}$ data for HUMPPA. This work was supported by the Max Planck Graduate Center with the Johannes Gutenberg-Universität Mainz (MPGC).

Financial support

The article processing charges for this open-access publication were covered by the Max Planck Society.

Review statement

This paper was edited by John Liggio and reviewed by two anonymous referees.