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Das Oberjura-Profil im Erdgasgraben bei Hitzhausen (Westliches Wiehengebirge, Nordwestdeutschland)
(1996)
Im Sommer 1995 war beim Bau einer Erdgasleitung im Wiehengebirge nordöstlich Osnabrück kurzfristig die gesamte Schichtenfolge vom tiefen Oxford bis zur Tithon-Basis aufgeschlossen. Die Gesteinsansprache ermöglichte unter Berücksichtigung der Mikrofauna eine feinstratigraphische Gliederung. Die Sedimente wurden außerdem mit einer Gamma-Sonde nach dem Scintillometer-Prinzip vermessen und daraus eine Gamma-ray-Kurve erstellt.
In Oppenwehe, ca. 2 km östlich der Stemweder Berge, befindet sich zwischen dem Oppenweher Moor im Norden und dem Großen Dieckfluß im Süden eine ca. 3 km lange und 1 km breite Erhebung. Sie überragt das umgebende Flachland um ca. 5-6 m und bildet vermutlich das nordwestliche Ende einer bei Hille westlich von Minden verlaufenden saalezeitlichen Stauchungsstruktur, die sich anscheinend in einer Reihe von Rücken bis nach Oppenwehe fortsetzt. In der seit Herbst 1995 am Ostrand von Oppenwehe bestehenden Abgrabung der Fa. Lindemann, Lemförde, konnten detaillierte Beobachtungen zum inneren Aufbau und damit zum Entstehungsablauf dieser Struktur gewonnen werden. Es liegt hier eine glaziäre Abfolge ("Serie") von Vorschüttsanden, Grundmoräne und Nachschüttbildungen vor, die verfaltet und verschuppt ist. Daraus läßt sich eine zweimalige Überfahrung dieses Raumes durch das saalezeitliche Inlandeis ableiten. Eine wenige Meter südlich der Sandgrube abgeteufte Rammkernbohrung erbrachte darüber hinaus Aufschluß über den tieferen Teil der Schichtenfolge des Quartärs. Sie umfaßt holsteinzeitliche Ablagerungen und endet mit einer elsterzeitlichen Grundmoräne, die unmittelbar auf Tonsteinen der Unterkreide liegt.
Ein neues Bajocium-Profil (Mittlerer Jura) im Osnabrücker Bergland (Niedersachsen) : mit 2 Tabellen
(1990)
In den Jahren 1984-1986 wurde südöstlich von Osnabrück beim Bau der Autobahn (A 33) ein großer Aufschluß im Bajocium und Bathonium geschaffen. Mit Hilfe der horizontiert aufgesammelten Ammoniten konnte das Bajocium im Osnabrücker Bergland entsprechend den Standard-Zonen und -Subzonen der nordwesteuropäischen Faunenprovinz untergliedert werden.
The theoretical basis for the link between the leaf exchange of carbonyl sulfide (COS), carbon dioxide (CO2) and water vapour (H2O) and the assumptions that need to be made in order to use COS as a tracer for canopy net photosynthesis, transpiration and stomatal conductance, are reviewed. The ratios of COS to CO2 and H2O deposition velocities used to this end are shown to vary with the ratio of the internal to ambient CO2 and H2O mole fractions and the relative limitations by boundary layer, stomatal and internal conductance for COS. It is suggested that these deposition velocity ratios exhibit considerable variability, a finding that challenges current parameterizations, which treat these as vegetation-specific constants. COS is shown to represent a better tracer for CO2 than H2O. Using COS as a tracer for stomatal conductance is hampered by our present poor understanding of the leaf internal conductance to COS. Estimating canopy level CO2 and H2O fluxes requires disentangling leaf COS exchange from other ecosystem sources/sinks of COS. We conclude that future priorities for COS research should be to improve the quantitative understanding of the variability in the ratios of COS to CO2 and H2O deposition velocities and the controlling factors, and to develop operational methods for disentangling ecosystem COS exchange into contributions by leaves and other sources/sinks. To this end, integrated studies, which concurrently quantify the ecosystem-scale CO2, H2O and COS exchange and the corresponding component fluxes, are urgently needed.
We investigate the potential of carbonyl sulfide (COS) for being used as a tracer for canopy net photosynthesis, transpiration and stomatal conductance by examining the theoretical basis of the link between leaf COS, carbon dioxide (CO2) and water vapour (H2O) exchange. Our analysis identifies several limitations that need to be overcome to this end, however at present we lack appropriate ecosystem-scale field measurements for assessing their practical significance. It however appears that COS represents a better tracer for CO2 than H2O. Concurrent measurements of ecosystem scale COS, CO2 and H2O exchange are advocated.
Sedimentologie und Verwitterungsbeständigkeit des Wellenkalks
(Unterer Muschelkalk) von Osnabrück
(1993)
Die Sedimentologie und Verwitterungsbeständigkeit des Osnabrücker Weilenkalks (Unterer Muschelkalk) werden an Mauersteinen aus zwei Gebäuden in Osnabrück und an Proben aus dem Steinbruch im Botanischen Garten Osnabrück untersucht. Es lassen sich 6 Mikrofaziestypen (A-F) unterscheiden, die ausführlich beschrieben werden. Ihre Analyse erlaubt detaillierte Aussagen zum Sedimentationsraum und zur Entstehung. Darauf aufbauend werden die in der Schichtenfolge beobachtbaren Sedimentationszyklen auf Meeresspiegeländerungen zurückgeführt. Es lassen sich deutliche Unterschiede in der Verwitterungsbeständigkeit der verschiedenen Mikrofaziestypen erkennen. Am verwitterungsbeständigsten sind die Mikrofaziestypen A und B, durch Sturmfluten entstandene Lagen im unteren und oberen Teil des Oolithbank-Members der Wellenkalk-Formation. Die Mikrofaziestypen A und B sind so verwitterungsbeständig., da sie nicht feingeschichtet sind und freiwillige Wasseraufnahme, Schurecht-Ratio (= freiwillige Wasseraufnahme geteilt durch effektive Porosität) sowie der Gehalt an salzsäureunlöslichem Rückstand relativ gering sind.
Die Wetterstation und die Photovoltaikanlage (Leihgabe der Stadtwerke Osnabrück) auf dem Dach des Museums am Schölerberg wurde von Hänel (1998a) beschrieben. In einem weiteren Artikel sind die Daten der Wetterstation und der Photovoltaikanlage für das Jahr 1997 zusammengefasst (Hänel, 1998b), dort ist auch die Herkunft der Vergleichsdaten beschrieben. In Tabelle 1 sind die Monatswerte für 1998 zusammengestellt.
Von der Gemeinde Hagen a.T.W. wurde am Butterberg ein ehemaliger Steinbruch im Osning-Sandstein durch die Anlage eines Schurfgrabens so erweitert, daß jetzt die Basis des Osning-Sandsteins und etwa 20, m der Schichtenfolge aus seinem Liegenden freigelegt sind. Die Basis des Osning-Sandsteins besteht aus einem dünnen Geröllhorizont, dem Osning-Konglomerat. Das Konglomerat wurde transgressiv auf Schichten der Bückeberg-Folge 1 (tiefster "Wealden") geschüttet. Unter den Gesteinen der Bückeberg-Folge, die mit einer Restmächtigkeit von nur noch etwa 5 m erhalten sind, treten in dem Schurfgraben noch ca. 15 m Ablagerungen des Serpulits auf. Dieser neu geschaffene Aufschluß wird langfristig - als Naturdenkmal geschützt - erhalten bleiben.
Zusammenfassung der Ergebnisse.
1. Eine einheitliche Gliederung der diluvialen Terrassen ist Voraussetzung für die vorliegende Untersuchung.
a) Die Bezeichnung "Mittelterrassen" wurde vermieden, vielmehr ist in Hoch- und Talwegterrasse gegliedert worden. b) Die Höhenbezeichnungen wurden durch Altersbestimmungen ersetzt.
2. Eine gemeinsame Behandlung erforderten die älteren Terrassen des Eis- und Eckbaches.
a) Der Oberlauf des Eckbaches ist tektonisch angelegt. In diesem Engtal wie auch in den südlich folgenden fehlen nicht nur die älteren sondern überhaupt jegliche Terrassen.
b) Die Schotterfluren innerhalb der Marnheimer Bucht stellen Gleithänge dar, an denen der Eisbach nach dem Innern hin heruntergerutscht ist.
c) Schon im Pliozän ist die Scholle der Marnheimer Bucht gegen den Rheintalgraben aufgerichtet.
3. Die Hochterrasse ist nur im nördlichen Gebietsteil ausgebildet, im Süden wird sie durch die Ablagerung der Freinsheimer Tonschichten lokal ersetzt.
4. Die Freinsheimer Tonschichten stellen eine lokale prärißeiszeitliche Auffüllung des rückgesunkenen Mitteldiluvialen Senkungsfeldes dar.
5. Die mittel diluviale Reakkumulation ist eine der bedeutendsten Erscheinungen für die Morphologie des Mainzer Beckens.
a) Infolge der starken Niveaudifferenzen am Rand des Pfälzerwaldes mußte die Aufschüttung gerade hier sehr mächtig sein.
b) Die Schuttkegel sind teils ein Ergebnis dieser Aufschüttung teils ein Ergebnis der flächenhaften Abtragung und mechanischen Zertrümmerung am Gebirgsrand.
c) Morphologische Tatsachen beweisen, daß die südlichen Seitenfliisse des Rheins jünger sind als Pfrimm und Eisbach.
6. Die Ursache für die Entstehung des einzelnen Fluß terrassenrestes im Gebirge (Rotliegendausräumung von Lambrecht-Grevenhausen) ist die Stauung des Speyerbaches unmittelbar vor der Verwerfung Albersweiler-Lindenberg-Bad Dürkheim.
7. Der Niederterrasse kommt im südlichen Teil des Untersuchungsgebietes größere morphologische Bedeutung zu als im nördlichen.
8. Der Südwestteil des Mainzer Beckens kann in einzelne tektonische Senkungsfelder eingeteilt werden, die durch· Verwerfungen begrenzt sind.
a) Erst im Mitteldiluvium sind die Hauptschollen des Rheinhessischen Blockgebirges aus dem allgemeinen Senkungsbereich ausgegliedert worden.
b) Verschiedene morphologische Tatsachen, besonders in der Rheinpfalz, sprechen dafür, daß im Rheintalgraben gegensätzliche Bewegungsrichtungen der sich senkenden Schollen geherrscht haben.
c) Im Mitteldiluvium wirkte noch die alte Bewegungstendenz mit größter Intensität im Innern.
d) Frühestens im Riß-Würm-Interglazial sank alsdann das Mitteldiluviale Senkungsfeld gebirgswärts zurück.
e) Aber auch in gleichen Zeitabschnitten herrschten im Rheintal verschiedene Bewegungsrichtungen, wobei sich Wilsers Ansicht bestätigt, daß das Rheintal in quer gerichtete Unterabschnitte zu gliedern ist, die als Einheiten verschiedensinnige Bewegungen zeigen.
We conducted measurements of the five important short-lived organic bromine species in the marine boundary layer (MBL). Measurements were made in the Northern Hemisphere mid-latitudes (Sylt Island, North Sea) in June 2009 and in the tropical Western Pacific during the TransBrom ship campaign in October 2009. For the one-week time series on Sylt Island, mean mixing ratios of CHBr3, CH2Br2, CHBr2Cl and CH2BrCl were 2.0, 1.1, 0.2, 0.1 ppt, respectively. We found maxima of 5.8 and 1.6 ppt for the two main components CHBr3 and CH2Br2. Along the cruise track in the Western Pacific (between 41° N and 13° S) we measured mean mixing ratios of 0.9, 0.9, 0.2, 0.1 and 0.1 ppt for CHBr3, CH2Br2, CHBrCl2, CHBr2Cl and CH2BrCl. Air samples with coastal influence showed considerably higher mixing ratios than the samples with open ocean origin. Correlation analyses of the two data sets yielded strong linear relationships between the mixing ratios of four of the five species (except for CH2BrCl). Using a combined data set from the two campaigns and a comparison with the results from two former studies, rough estimates of the molar emission ratios between the correlated substances were: 9/1/0.35/0.35 for CHBr3/CH2Br2/CHBrCl2/CHBr2Cl. Additional measurements were made in the tropical tropopause layer (TTL) above Teresina (Brazil, 5° S) in June 2008, using balloon-borne cryogenic whole air sampling technique. Near the level of zero clear-sky net radiative heating (LZRH) at 14.8 km about 2.25 ppt organic bromine was bound to the five short-lived species, making up 13% of total organic bromine (17.82 ppt). CH2Br2 (1.45 ppt) and CHBr3 (0.56 ppt) accounted for 90% of the budget of short-lived compounds in that region. Near the tropopause (at 17.5 km) organic bromine from these substances was reduced to 1.35 ppt, with 1.07 and 0.12 ppt attributed to CH2Br2 and CHBr3, respectively.
We conducted measurements of up to the five important short-lived brominated species in the marine boundary layer (MBL) of the mid-latitudes (List/Sylt, North Sea) in June 2009 and of the tropical Western Pacific during the TransBrom ship campaign in October 2009. For the one-week time series in List mean mixing ratios of 2.0, 1.1, 0.2, 0.1 ppt were analysed for CHBr3, CH2Br2, CHBr2Cl and CH2BrCl, with maxima of 5.8 and 1.6 ppt for the two main components CHBr3 and CH2Br2. Along the cruise track in the Western Pacific (between 41° N and 13° S) mean mixing ratios of 1.0, 0.9, 0.2, 0.1 and 0.1 ppt for CHBr3, CH2Br2, CHBrCl2, CHBr2Cl and CH2BrCl were determined. Air samples with coastal influence showed considerably higher mixing ratios than the samples with open ocean origin. Correlation analyses of the two datasets yielded strong linear relationships between the mixing ratios of four of the five species (except for CH2BrCl). Using a combined dataset from the two campaigns, rough estimates of the molar emission ratios between the correlated substances were derived as follows: 9/1/0.3/0.3 for CHBr3/CH2Br2/CHBrCl2/CHBr2Cl. Additional measurements were made in the tropical tropopause layer (TTL) above Teresina (Brazil, 5.07° S, 42.87° W) in June 2008, using balloon-borne cryogenic whole air sampling technique. Near the level of zero clear-sky net radiative heating (LZRH) at 14.8 km about 2.25 ppt organic bromine was bound to the five short-lived species, making up 13 % of total organic bromine (17.82 ppt). CH2Br2 (1.45 ppt) and CHBr3 (0.56 ppt) accounted for 90 % of the budget of short-lived compounds in that region. Near the tropopause (at 17.5 km) organic bromine from short-lived substances was reduced to 1.35 ppt, with 1.07 ppt and 0.12 ppt attributed to CH2Br2 and CHBr3 respectively.
Balloon-borne stratospheric BrO measurements : comparison with Envisat/SCIAMACHY BrO limb profiles
(2005)
For the first time, results of all four existing stratospheric BrO profiling instruments, are presented and compared with reference to the SLIMCAT 3-dimensional chemical transport model (3-D CTM). Model calculations are used to infer a BrO profile validation set, measured by 3 different balloon sensors, for the new Envisat/SCIAMACHY (ENVIronment SATellite/SCanning Imaging Absorption spectroMeter for Atmospheric CHartographY) satellite instrument. The balloon observations include (a) balloon-borne in situ resonance fluorescence detection of BrO, (b) balloon-borne solar occultation DOAS measurements (Differential Optical Absorption Spectroscopy) of BrO in the UV, and (c) BrO profiling from the solar occultation SAOZ (Systeme d'Analyse par Observation Zenithale) balloon instrument. Since stratospheric BrO is subject to considerable diurnal variation and none of the measurements are performed close enough in time and space for a direct comparison, all balloon observations are considered with reference to outputs from the 3-D CTM. The referencing is performed by forward and backward air mass trajectory calculations to match the balloon with the satellite observations. The diurnal variation of BrO is considered by 1-D photochemical model calculation along the trajectories. The 1-D photochemical model is initialised with output data of the 3-D model with additional constraints on the vertical transport, the total amount and photochemistry of stratospheric bromine as given by the various balloon observations. Total [Bry]=(20.1±2.8)pptv obtained from DOAS BrO observations at mid-latitudes in 2003, serves as an upper limit of the comparison. Most of the balloon observations agree with the photochemical model predictions within their given error estimates. First retrieval exercises of BrO limb profiling from the SCIAMACHY satellite instrument agree to <±50% with the photochemically-corrected balloon observations, and tend to show less agreement below 20 km.
Contribution of sulfuric acid and oxidized organic compounds to particle formation and growth
(2012)
Lack of knowledge about the mechanisms underlying new particle formation and their subsequent growth is one of the main causes for the large uncertainty in estimating the radiative forcing of atmospheric aerosols in global models. We performed chamber experiments designed to study the contributions of sulfuric acid and organic vapors to formation and to the early growth of nucleated particles, respectively. Distinct experiments in the presence of two different organic precursors (1,3,5-trimethylbenzene and α-pinene) showed the ability of these compounds to reproduce the formation rates observed in the low troposphere. These results were obtained measuring the sulfuric acid concentrations with two Chemical Ionization Mass Spectrometers confirming the results of a previous study which modeled the sulfuric acid concentrations in presence of 1,3,5-trimethylbenzene.
New analysis methods were applied to the data collected with a Condensation Particle Counter battery and a Scanning Mobility Particle Sizer, allowing the assessment of the size resolved growth rates of freshly nucleated particles. The effect of organic vapors on particle growth was investigated by means of the growth rate enhancement factor (Γ), defined as the ratio between the measured growth rate in the presence of α-pinene and the kinetically limited growth rate of the sulfuric acid and water system. The observed Γ values indicate that the growth is dominated by organic compounds already at particle diameters of 2 nm. Both the absolute growth rates and Γ showed a strong dependence on particle size supporting the nano-Köhler theory. Moreover, the separation of the contributions from sulfuric acid and organic compounds to particles growth reveals that the organic contribution seems to be enhanced by the sulfuric acid concentration. The size resolved growth analysis finally indicates that both condensation of oxidized organic compounds and reactive uptake contribute to particle growth.
A comprehensive set of stratospheric balloon and aircraft samples was analyzed for the position-dependent isotopic composition of nitrous oxide (N2O). Results for a total of 220 samples from between 1987 and 2003 are presented, nearly tripling the number of mass-spectrometric N2O isotope measurements in the stratosphere published to date. Cryogenic balloon samples were obtained at polar (Kiruna/Sweden, 68° N), mid-latitude (southern France, 44° N) and tropical sites (Hyderabad/India, 18° N). Aircraft samples were collected with a newly-developed whole air sampler on board of the high-altitude aircraft M55 Geophysica during the EUPLEX 2003 campaign. All samples were analyzed by laboratory mass spectrometry for their 18O/16O and position-dependent 15N/14N isotope ratios with very high precision (standard deviation about 0.15 per mil for 18O/16O and average 15N/14N ratios, about 0.5 per mil for 15NNO/14NNO and N15NO/N14NO ratios). For mixing ratios above 200 nmol mol−1, relative isotope enrichments (δ values) and mixing ratios display a compact relationship, which is nearly independent of latitude and season and which can be explained equally well by Rayleigh fractionation or mixing. However, for mixing ratios below 200 nmol mol−1 this compact relationship gives way to meridional, seasonal and interannual variations. A comparison to a previously published mid-latitude balloon profile even shows large zonal variations, justifying the use of three-dimensional models for further data interpretation.
In general, the magnitude of the apparent fractionation constants (apparent isotope effects) increases continuously with altitude and decreases from the equator to the North pole, which can be qualitatively understood by the interplay between the time-scales of N2O photochemistry and transport. Deviations from this behavior occur where polar vortex air mixes with nearly N2O-free upper stratospheric/mesospheric air (e.g., during the boreal winter of 2003 and possibly 1992). Aircraft observations in the polar vortex at mixing ratios below 200 nmol mol−1 deviate from isotope variations expected for both Rayleigh fractionation and end-member mixing, but could be explained by continuous weak mixing between intravortex and extravortex air (Plumb et al., 2000). Finally, correlations between 18O/16O and average 15N/14N isotope ratios or between the position-dependent 15N/14N isotope ratios show that photo-oxidation makes a large contribution to the total N2O sink in the lower stratosphere (up to 100%). Towards higher altitudes, the temperature dependence of these isotope correlations becomes visible in the stratospheric observations.
Surface measurements of aerosol and ice nuclei (IN) at a Central European mountain site during an episode of dust transport from the Sahara are presented. Transport is simulated by the Eulerian regional dust model DREAM. Ice nuclei and mineral dust are significantly correlated. The highest correlation is found between IN concentration and aerosol surface area. The ice nucleating characteristics of the aerosol with respect to temperature and supersaturation are similar during the dust episode than during the course of the year. This suggests that dust is always a dominant constituent of ice nucleating aerosols in Central Europe.
Surface measurements of aerosol and ice nuclei (IN) at a Central European mountain site during an episode of dust transport from the Sahara are presented. Ice nuclei were sampled by electrostatic precipitation on silicon wafers and were analyzed in an isothermal static vapor diffusion chamber. The transport of mineral dust is simulated by the Eulerian regional dust model DREAM. Ice nuclei and mineral dust are significantly correlated, in particular IN number concentration and aerosol surface area. The ice nucleating characteristics of the aerosol as analyzed with respect to temperature and supersaturation are similar during the dust episode than during the course of the year. This suggests that dust may be a main constituent of ice nucleating aerosols in Central Europe.
The isotopic composition of methane in the stratosphere : high-altitude balloon sample measurements
(2011)
The isotopic composition of stratospheric methane has been determined on a large suite of air samples from stratospheric balloon flights covering subtropical to polar latitudes and a time period of 16 yr. 154 samples were analyzed for δ13C and 119 samples for δD, increasing the previously published dataset for balloon borne samples by an order of magnitude, and more than doubling the total available stratospheric data (including aircraft samples) published to date. The samples also cover a large range in mixing ratio from tropospheric values near 1800 ppb down to only 250 ppb, and the strong isotope fractionation processes accordingly increase the isotopic composition up to δ13C = −14‰ and δD = +190‰, the largest enrichments observed for atmospheric CH4 so far. When analyzing and comparing kinetic isotope effects (KIEs) derived from single balloon profiles, it is necessary to take into account the residence time in the stratosphere in combination with the observed mixing ratio and isotope trends in the troposphere, and the range of isotope values covered by the individual profile. The isotopic composition of CH4 in the stratosphere is affected by both chemical and dynamical processes. This severely hampers interpretation of the data in terms of the relative fractions of the three important sink mechanisms (reaction with OH, O(1D) and Cl). It is shown that a formal sink partitioning using the measured data severely underestimates the fraction removed by OH, which is likely due to the insensitivity of the measurements to the kinetic fractionation in the lower stratosphere. Full quantitative interpretation of the CH4 isotope data in terms of the three sink reactions requires a global model.
The isotopic composition of methane in the stratosphere : high-altitude balloon sample measurements
(2011)
The isotopic composition of stratospheric methane has been determined on a large suite of air samples from stratospheric balloon flights covering subtropical to polar latitudes and a time period of 16 yr. 154 samples were analyzed for δC and 119 samples for δD, increasing the previously published dataset for balloon borne samples by an order of magnitude, and more than doubling the total available stratospheric data (including aircraft samples) published to date. The samples also cover a large range in mixing ratio from tropospheric values near 1800 ppb down to only 250 ppb, and the strong isotope fractionation processes accordingly increase the isotopic composition up to δ13C=−14‰ and δD= +190‰, the largest enrichments observed for atmospheric CH4 so far. When analyzing and comparing kinetic isotope effects (KIEs) derived from single balloon profiles, it is necessary to take into account the residence time in the stratosphere in combination with the observed mixing ratio and isotope trends in the troposphere, and the range of isotope values covered by the individual profile. Temporal isotope trends can also be determined in the stratosphere and compare reasonably well with the tropospheric trends. The effects of chemical and dynamical processes on the isotopic composition of CH4 in the stratosphere are discussed in detail. Different ways to interpret the data in terms of the relative fractions of the three important sink mechanisms (reaction with OH, O(1D)) and Cl, respectively), and their limitations, are investigated. The classical approach of using global mean KIE values can be strongly biased when profiles with different minimum mixing ratios are compared. Approaches for more local KIE investigations are suggested. It is shown that any approach for a formal sink partitioning from the measured data severely underestimates the fraction removed by OH, which is likely due to the insensitivity of the measurements to the kinetic fractionation in the lower stratosphere. Attempts can be made to correct for the lower stratospheric sink bias, but full quantitative interpretation of the CH4 isotope data in terms of the three sink reactions requires a global model.
This paper presents an analysis of the recent tropospheric molecular hydrogen (H2) budget with a particular focus on soil uptake and European surface emissions. A variational inversion scheme is combined with observations from the RAMCES and EUROHYDROS atmospheric networks, which include continuous measurements performed between mid-2006 and mid-2009. Net H2 surface flux, then deposition velocity and surface emissions and finally, deposition velocity, biomass burning, anthropogenic and N2 fixation-related emissions were simultaneously inverted in several scenarios. These scenarios have focused on the sensibility of the soil uptake value to different spatio-temporal distributions. The range of variations of these diverse inversion sets generate an estimate of the uncertainty for each term of the H2 budget. The net H2 flux per region (High Northern Hemisphere, Tropics and High Southern Hemisphere) varies between −8 and +8 Tg yr−1. The best inversion in terms of fit to the observations combines updated prior surface emissions and a soil deposition velocity map that is based on bottom-up and top-down estimations. Our estimate of global H2 soil uptake is −59±9 Tg yr−1. Forty per cent of this uptake is located in the High Northern Hemisphere and 55% is located in the Tropics. In terms of surface emissions, seasonality is mainly driven by biomass burning emissions. The inferred European anthropogenic emissions are consistent with independent H2 emissions estimated using a H2/CO mass ratio of 0.034 and CO emissions within the range of their respective uncertainties. Additional constraints, such as isotopic measurements would be needed to infer a more robust partition of H2 sources and sinks.