550 Geowissenschaften
Refine
Year of publication
Document Type
- Article (907)
- Doctoral Thesis (194)
- Contribution to a Periodical (32)
- Book (26)
- Working Paper (22)
- Part of Periodical (21)
- Conference Proceeding (18)
- Part of a Book (9)
- Diploma Thesis (8)
- diplomthesis (7)
- Other (5)
- Report (5)
- Master's Thesis (4)
- Review (4)
- Periodical (3)
- Bachelor Thesis (2)
- Habilitation (2)
- Preprint (2)
Language
Keywords
- climate change (11)
- Climate change (8)
- Klima (8)
- Klimaänderung (7)
- Modellierung (7)
- COSMO-CLM (6)
- Klimawandel (6)
- Palaeoclimate (6)
- precipitation (6)
- Atmospheric chemistry (5)
Institute
- Geowissenschaften (778)
- Geowissenschaften / Geographie (148)
- Biodiversität und Klima Forschungszentrum (BiK-F) (62)
- Geographie (61)
- Senckenbergische Naturforschende Gesellschaft (57)
- Präsidium (44)
- Extern (28)
- Biowissenschaften (22)
- Institut für Ökologie, Evolution und Diversität (10)
- Physik (8)
Am 7. September 1981 wurde der Raum Bellersen von einem heftigen Unwetter mit Gewitter und sintflutartigen Regenfällen heimgesucht. Das Unwetter richtete einen nicht unbeträchtlichen Schaden im Dorf und in der Feldmark an. Es bot aber auch Gelegenheit, den Einfluß solcher relativ seltener und daher episodisch zu bezeichnenden extremen Niederschlagsereignisse auf die Formung der Erdoberfläche zu erkennen. An dieser Stelle soll an einem Einzelbeispiel gezeigt werden, wie sich die Oberflächenformen im Talgrund von Trockentälern weiterentwickeln können. Genaue quantitative Angaben über den gefallenen Niederschlag lassen sich leider nicht machen, da für das angesprochene Einzugsgebiet keine Messungen vorliegen.
An eclogite barometer has profound importance in the study of upper mantle processes and potential application to diamond prospecting. Studies on the partitioning of Li between clinopyroxene (cpx) and garnet (grt) in natural samples have shown that this particular element is very sensitive to changes in pressure and could be calibrated as the barometer demanded for bimineralic eclogites. Experiments were performed from 4 to 13 GPa and 1100 to 1400°C in the CMAS (CaO, MgO, Al2O3, SiO2) system with Li added as Li3PO4 to quantify this pressure dependence into a barometer expressed in the following equation: P= (0.00255*T-lnKd)/0.2351 where P is in GPa, T is in °C and Kd is defined as the partition coefficient of Li (in ppm) between clinopyroxene and garnet. The experimental pressures are reproduced to ± 0.38 GPa (1σ) by this equation. This barometer is strictly applicable only to CMAS. Experiments at 1300°C, 8-12 GPa showed that Henry’s Law is fulfilled for Li partitioning between cpx and grt in the concentration range of approximately 0.01 – 1 wt% Li. Direct application of the equation to experiments in natural systems performed at 1300°C from 4 GPa to 13 GPa consistently overestimates pressures by approximately 2 GPa. Our previous experiments in the system CaO-MgO-Al2O3-SiO2 + Li3PO4 showed that the partitioning of Li between garnet and clinopyroxene is pressure dependent in eclogitic bulk compositions. This supports experimentally the hypothesis of Seitz et al. (2003), based on the analysis of Li in eclogitic xenoliths and inclusions in diamond, that the partitioning of this particular element between clinopyroxene and garnet is very sensitive to changes in pressure and could be calibrated as a barometer for bimineralic eclogites. In order to calibrate this pressure dependence into a barometer, experiments were performed in natural systems using starting materials sourced from a well preserved eclogitic xenolith from the Roberts Victor kimberlite pipe (South Africa) to extrapolate our findings in CMAS to natural systems. Sixteen multianvil experiments were performed from 4-13 GPa and 1100-1500°C. Our findings reinforced the general trend we observed in the CMAS system, that KdLi cpx-grt for Li decreases with increasing P, and that at P ≥ 12 GPa, garnet is able to incorporate more Li than clinopyroxene. Multiple linear regression was applied to our experimental results to create the barometer: P = (0.000963*T – ln KdLi cpx-grt + 1.581) / 0.252 Where P is pressure in GPa, T is temperature in °C and KdLi cpx-grt is defined as the partitioning coefficient of Li obtained by dividing the concentration of Li in cpx by the concentration of Li in garnet. This barometer reproduces the experimental conditions to ± 0.2 GPa. It is applicable to eclogitic xenoliths, to garnet pyroxenites and to peridotitic and eclogitic inclusions in diamond. Application of the barometer to diamond bearing xenoliths results in pressures in the diamond stability field. Clinopyroxene is easily corrupted in xenoliths and also preferentially takes in Li during short lived metasomatic processes. Care must be taken therefore to analyse primary, unaltered clinopyroxene. Our preliminary application to natural samples shows that the barometer can be applied beyond the experimental range to pressures down to 3 GPa. Seventeen eclogitic xenoliths were chosen from a sample set of greater than 200 for their fresh microscopic and macroscopic appearance and were analyzed for Li content in coexisting garnet (grt) and clinopyroxene (cpx). These samples can be subdivided into two groups on the basis of Mg in cpx (cpfu: cations per formula unit, based on 6 oxygens): Group 1 with Mg > 0.75, and Group 2 with Mg < 0.75. Group 1 xenoliths show lower Li contents in both grt and cpx compared to Group 2. The Li barom ter calibrated in Hanrahan et al. (2009b)/Chapter 3 was applied to these samples as well as available literature data to obtain pressures of provenance - Group 2 xenoliths often provide pressures that appear unrealistic for eclogitic xenoliths. In light of observed crystal chemical relations in the natural samples, a new fitting procedure was applied to the experimental data presented in Chapter 3. This new fit appears to be more realistic than the previous fit, although a strong relationship with Mg# remains present, suggesting that Li-barometry is, at present, only applicable to Mg-rich eclogites. Inclusions in diamond, with the exception of eclogitic inclusions of coexisting majorite and cpx, often yield pressures that are inconsistent with the pressures required for diamond formation. Although an interesting observation when comparing all of the data is that inclusions in diamond have significantly higher average Li concentrations compared to xenoliths, which suggests that Li is highly present in the fluids from which diamonds form in the mantle, an observation which was previously made for the deep mantle as a result of high Li in ferropericlase inclusions in diamond (Seitz et al. 2003).
During a 4-week run in October–November 2006, a pilot experiment was performed at the CERN Proton Synchrotron in preparation for the Cosmics Leaving OUtdoor Droplets (CLOUD) experiment, whose aim is to study the possible influence of cosmic rays on clouds. The purpose of the pilot experiment was firstly to carry out exploratory measurements of the effect of ionising particle radiation on aerosol formation from trace H2SO4 vapour and secondly to provide technical input for the CLOUD design. A total of 44 nucleation bursts were produced and recorded, with formation rates of particles above the 3 nm detection threshold of between 0.1 and 100 cm -3 s -1, and growth rates between 2 and 37 nm h -1. The corresponding H2O concentrations were typically around 106 cm -3 or less. The experimentally-measured formation rates and htwosofour concentrations are comparable to those found in the atmosphere, supporting the idea that sulphuric acid is involved in the nucleation of atmospheric aerosols. However, sulphuric acid alone is not able to explain the observed rapid growth rates, which suggests the presence of additional trace vapours in the aerosol chamber, whose identity is unknown. By analysing the charged fraction, a few of the aerosol bursts appear to have a contribution from ion-induced nucleation and ion-ion recombination to form neutral clusters. Some indications were also found for the accelerator beam timing and intensity to influence the aerosol particle formation rate at the highest experimental SO2 concentrations of 6 ppb, although none was found at lower concentrations. Overall, the exploratory measurements provide suggestive evidence for ion-induced nucleation or ion-ion recombination as sources of aerosol particles. However in order to quantify the conditions under which ion processes become significant, improvements are needed in controlling the experimental variables and in the reproducibility of the experiments. Finally, concerning technical aspects, the most important lessons for the CLOUD design include the stringent requirement of internal cleanliness of the aerosol chamber, as well as maintenance of extremely stable temperatures (variations below 0.1 °C)
In order to quantitatively analyse the chemical and dynamical evolution of the polar vortex it has proven extremely useful to work with coordinate systems that follow the vortex flow. We propose here a two-dimensional quasi-Lagrangian coordinate system {X i, delta X i}, based on the mixing ratio of a long-lived stratospheric trace gas i, and its systematic use with i = N2O, in order to describe the structure of a well-developed Antarctic polar vortex. In the coordinate system {X i, delta X i} the mixing ratio X i is the vertical coordinate and delta X i = X i(theta) - X i vort(theta) is the meridional coordinate (X i vort(theta) being a vertical reference profile in the vortex core). The quasi-Lagrangian coordinates {X i, delta X i} persist for much longer time than standard isentropic coordinates, potential temperature theta and equivalent latitude Phi e, do not require explicit reference to geographic space, and can be derived directly from high-resolution in situ measurements. They are therefore well-suited for studying the evolution of the Antarctic polar vortex throughout the polar winter with respect to the relevant chemical and microphysical processes. By using the introduced coordinate system {X N2O, delta X N2O} we analyze the well-developed Antarctic vortex investigated during the APE-GAIA (Airborne Polar Experiment – Geophysica Aircraft in Antarctica – 1999) campaign (Carli et al., 2000). A criterion, which uses the local in-situ measurements of X i=X i(theta) and attributes the inner vortex edge to a rapid change (delta-step) in the meridional profile of the mixing ratio X i, is developed to determine the (Antarctic) inner vortex edge. In turn, we suggest that the outer vortex edge of a well-developed Antarctic vortex can be attributed to the position of a local minimum of the X H2O gradient in the polar vortex area. For a well-developed Antarctic vortex, the delta X N2O-parametrization of tracer-tracer relationships allows to distinguish the tracer inter-relationships in the vortex core, vortex boundary region and surf zone and to examine their meridional variation throughout these regions. This is illustrated by analyzing the tracer-tracer relationships X i : X N2O obtained from the in-situ data of the APE-GAIA campaign for i = CFC-11, CFC-12, H-1211 and SF6. A number of solitary anomalous points in the CFC-11 : N2O correlation, observed in the Antarctic vortex core, are interpreted in terms of small-scale cross-isentropic dispersion.
Östlich des Rwenzori Gebirges im Westen Ugandas wurden magnetotellurische Messungen durchgeführt. An 23 Stationen wurden Übertragungsfunktionen und Phasen Tensor Elemente zwischen den gemessenen magnetischen- und tellurischen Feldern im Periodenbereich von 10s bis 10000s geschätzt. Die Übertragungsfunktionen deuten eine komplexe drei dimensionale Leitfähigkeitsstruktur innerhalb der Kruste an, insbesondere in der Verbindungszone zwischen dem Rwenzori Gebirge und der östlichen Riftschulter. In dieser Arbeit wird eine alternative Darstellung der Phasen Tensor Ellipsen als Balken eingeführt. Für Perioden größer 100s zeigen die maximalen Phasen der Phasen Tensor Balken aller Stationen einheitlich in SSW-NNE und die Phasen Tensor Invarianten f min und f max weisen eine Differenz von mindestens 20° auf. Dieses auffällige Verhalten und die kleinen vertikalen magnetischen Feldr im gleich Periodenbereich kann mit einer anisotropen Leitfähigkeit in einer Tiefenbereich zwischen 30-50km mit der gut leitenden Richtung senkrecht zur Riftachse erklärt werden. Die Anisotropie könnte ihren Ursprung in orientierten Olivien Kristallen im oberen Mantel haben, wobei die Orientierungsrichtung mit der Delamination der Unterkruste unter den Rwenzoris zusammen hängen kann. Eine gut leitende Zone süd-östlich der Rwenzoris wurde in 15km Tiefe gefunden, die mit einer seismischen low velocity zone übereinstimmt und partielle Schmelzen innerhalb der Kruste andeutet. An allen Stationen steigt die minimale Phase bei der Periode 200s über 45° und zeigt einen Anstieg der elektrischen Leitfähigkeit unterhalb der Lithosphäre an.
Die Magnesitlagerstätte Beli Kamen, die so nachdem Berge im Dorfe Strezovce, unweit von Novo Brdo, benannt wurde, war der Gegenstand unserer Untersuchungen fünf volle Jahre hindurch - von Juni 1956 bis Juli 1961. In der ersten Phase dieses Zeitabschnittes war es unsere Aufgabe, alle Untersuchungsarbeiten in diesem bisher ungenügend bearbeiteten Objekte, von dem seitens unserer Wirtschaft und unserer Forscher viel erwartet wurde - anzusetzen und durchzuführen. Die Ergebnisse dieser Arbeiten wurden in unserem Elaborat (1959), mit einer ausführlichen Dokumentation über die allgemeine Charakteristik und praktischen Wert der untersuchten Magnesitmasse dargestellt. In der zweiten Phase - in Zusammenhang mit der Planung und Finansieurng wissenschaftlicher Arbeiten seitens des Rates für wissenschaftliche Arbeit, V. R. Serbien, und seitens des Geologischen Forschungsinstitutes, V. R. Serbien, wurden die Untersuchungen über die Frage des Auftretens des Magnesit in der Lagerstätte Beli Kamen fortgesetzt, wobei das Untersuchungsgebiet bedeutend erweitert und eingehender erfasst wurde. Unumgänglich nötige nachträgliche Begehungen und neue Untersuchungen wurden von der Tatsache diktiert, dass eine wissenschaftliche Bearbeitung solcher Lagerstätten, insbesondere deren Entstehung, bedeutend zahlreichere Angaben forderte, als es alle durchgeführten, von praktischen Standpunkt aus ansomsten zufriedenstellende und umfangreiche Untersuchungsarbeiten boten. So musste in der zweiten Phase, von 1958 bis 1961 mehrmals das Terrain begangen werden und dabei stiessen wir auf neue Probleme, allmählich das Untersuchungsgebiet immer mehr erweiternd. Ausserdem war es nötig, gleichzeitig die umfangreiche Probensammlung, die nicht nur Magnesit, sondern auch verschiedenartiges taubes Material enthielt, laboratorisch zu bearbeiten. Die Ergebnisse dieser vervollständigten, vor allem wissenschfatlichen Behandlung der Magnesitlagerstätte Beli Kamen und deren Nebengesteine, sowie natürlich auch jene aus dem erwähnten Elaborat (1959), werden nun in dieser Studie dargestellt. Wir sind der Ansicht, dass viele Einzelheiten dieser Studie, die wie vorliegend geordnet ist und in den Hauptzügen ausreichend bearbeitet ist, von besonderem InLeresse für die Fachwelt sein wird, um so mehr, da sich dieselbe tatsächlich auf eine ganz besonderes, in der Welt seltenes Magnesitvorkommen handelt. Von den insgesamt gewonnen Ergebnissen der wissenschaftlichen Bearbeitung der Lagerstätte Beli Kamen wollen wir nur die allgemeinsten und ausgeprägtesten hervorheben.
Active chlorine species play a dominant role in the catalytic destruction of stratospheric ozone in the polar vortices during the late winter and early spring seasons. Recently, the correct understanding of the ClO dimer cycle was challenged by the release of new laboratory absorption cross sections (Pope et al., 2007) yielding significant model underestimates of observed ClO and ozone loss (von Hobe et al., 2007). Under this aspect, nocturnal Arctic stratospheric limb emission measurements carried out by the balloon version of the Michelson Interferometer for Passive Atmospheric Sounding (MIPAS-B) from Kiruna (Sweden) on 11 January 2001 and 20/21 March 2003 have been reanalyzed with regard to the chlorine reservoir species ClONO2 and the active species, ClO and ClOOCl (Cl2O2). New laboratory measurements of IR absorption cross sections of ClOOCl for various temperatures and pressures allowed for the first time the retrieval of ClOOCl mixing ratios from remote sensing measurements. High values of active chlorine (ClOx) of roughly 2.3 ppbv at 20 km were observed by MIPAS-B in the cold mid-winter Arctic vortex on 11 January 2001. While nighttime ClOOCl shows enhanced values of nearly 1.1 ppbv at 20 km, ClONO2 mixing ratios are less than 0.1 ppbv at this altitude. In contrast, high ClONO2 mixing ratios of nearly 2.4 ppbv at 20 km have been observed in the late winter Arctic vortex on 20 March 2003. No significant ClOx amounts are detectable on this date since most of the active chlorine has already recovered to its main reservoir species ClONO2. The observed values of ClOx and ClONO2 are in line with the established polar chlorine chemistry. The thermal equilibrium constants between the dimer formation and its dissociation, as derived from the balloon measurements, are on the lower side of reported data and in good agreement with values recommended by von Hobe et al. (2007). Calculations with the ECHAM/MESSy Atmospheric Chemistry model (EMAC) using established kinetics show similar chlorine activation and deactivation, compared to the measurements in January 2001 and March 2003, respectively.
Atmospheric observation-based global SF6 emissions - comparison of top-down and bottom-up estimates
(2009)
Emissions of sulphur hexafluoride (SF6), one of the strongest greenhouse gases on a per molecule basis, are targeted to be collectively reduced under the Kyoto Protocol. Because of its long atmospheric lifetime (≈3000 years), the accumulation of SF6 in the atmosphere is a direct measure of its global emissions. Examination of our extended data set of globally distributed high-precision SF6 observations shows an increase in SF6 abundance from near zero in the 1970s to a global mean of 6.7 ppt by the end of 2008. In-depth evaluation of our long-term data records shows that the global source of SF6 decreased after 1995, most likely due to SF6 emission reductions in industrialised countries, but increased again after 1998. By subtracting those emissions reported by Annex I countries to the United Nations Framework Convention of Climatic Change (UNFCCC) from our observation-inferred SF6 source leaves a surprisingly large gap of more than 70–80% of non-reported SF6 emissions in the last decade.
Emissions of sulphur hexafluoride (SF6), one of the strongest greenhouse gases on a per molecule basis, are targeted to be collectively reduced under the Kyoto Protocol. Because of its long atmospheric lifetime (estimated as 800 to 3200 years), the accumulation of SF6 in the atmosphere is a direct measure of its global emissions. Examination of our extended data set of globally distributed high-precision SF6 observations shows an increase in SF6 abundance from near zero in the 1970s to a global mean of 6.7 ppt by the end of 2008. In-depth evaluation of our long-term data records shows that the global source of SF6 decreased after 1995, most likely due to SF6 emission reductions in industrialised countries, but increased again after 1998. By subtracting those emissions reported by Annex I countries to the United Nations Framework Convention of Climatic Change (UNFCCC) from our observation-inferred SF6 source leaves a surprisingly large gap of more than 70–80% of non-reported SF6 emissions in the last decade. This suggests a strong under-estimation of emissions in Annex I countries and underlines the urgent need for independent atmospheric verification of greenhouse gases emissions accounting.
Samples of freshly fallen snow were collected at the high alpine research station Jungfraujoch, Switzerland, during the Cloud and Aerosol Characterization Experiments (CLACE) 5 in February and March 2006. Sampling was carried out on the Sphinx platform. Headspace-solid-phase-dynamic extraction (HS-SPDE) combined with gas chromatography/mass spectrometry (GC/MS) was used to quantify C6–C10 n-aldehydes in the snow samples. The most abundant n-aldehyde was n-hexanal (median concentration 1.324 micro g L -1) followed by n-nonanal, n-decanal, n-octanal and n-heptanal (median concentrations 1.239, 0.863, 0.460, and 0.304 micro g L -1, respectively). A wide range of concentrations was found among individual snow samples, even for samples taken at the same time. Higher median concentrations of all n-aldehydes were observed when air masses reached Jungfraujoch from the north-northwest in comparison to air masses arriving from the southeast-southwest. Results suggest that the n-aldehydes detected most likely are of direct and indirect biogenic origin, and that they entered the snow through the particle phase.
Both, gas and particle scavenging contribute to the transport of organic compounds by ice crystals in the troposphere. To simulate these processes an experimental setup was developed to form airborne ice crystals under atmospheric conditions. Experiments were performed in a wall independent reactor (WIR) installed in a walk-in cold chamber maintained constantly at -20°C. Aerosol particles were added to the carrier gas of ambient air by an aerosol generator to allow heterogeneous ice formation. Temperature variations and hydrodynamic conditions of the WIR were investigated to determine the conditions for ice crystal formation and crystal growth by vapour deposition. In detail, the dependence of temperature variations from flow rate and temperature of the physical wall as well as temperature variations with an increasing reactor depth were studied. The conditions to provide a stable aerosol concentration in the carrier gas flow were also studied. The temperature distribution inside the reactor was strongly dependent on flow rate and physical wall temperature. At an inlet temperature of -20°C, a flow rate of 30 L•min exp -1 and a physical wall temperature of +5°C turned out to provide ideal conditions for ice formation. At these conditions a sharp and stable laminar down draft "jet stream" of cold air in the centre of the reactor was produced. Temperatures measured at the chamber outlet were kept well below the freezing point in the whole reactor depth of 1.0 m. Thus, melting did not affect ice formation and crystal growth. The maximum residence time for airborne ice crystals was calculated to at 40 s. Ice crystal growth rates increased also with increasing reactor depth. The maximum ice crystal growth rate was calculated at 2.82 mg• exp -1. Further, the removal efficiency of the cleaning device for aerosol particles was 99.8% after 10 min. A reliable particle supply was attained after a preliminary lead time of 15 min. Thus, the minimum lead time was determined at 25 min. Several test runs revealed that the WIR is suitable to perform experiments with airborne ice crystals.
Within the present study the occurrence and fate of the organophosphorus flame retardants and plasticizers tris(2-chloroethyl) phosphate (TCEP), tris(2-chloro-1-methylethyl) phosphate (TCPP), tris(1,3-dichloro-2-propyl) phosphate (TDCP), tris(2-butoxyethyl) phosphate (TBEP), tri-iso-butyl phosphate (TiBP), and tri-n-butyl phosphate (TnBP) in precipitation, lake water, surface runoff and groundwater from urban and remote areas in Germany was investigated between June 2007 and October 2009. 255 samples of precipitation, 210 samples of lentic surface water and 72 samples of groundwater were analyzed for the six organophosphates (OPs) by solid phase extraction followed by gas chromatography-mass spectrometry. The research focused on aspects concerning (1) the atmospheric washout of OPs by precipitation, (2) the temporal variation of OP concentrations in precipitation and in lentic surface waters as well as (3) the pollution of groundwater by OPs. The results of the study emphasize the importance of precipitation as an all-season entry-pathway for OPs in the aquatic environment, particularly in densely populated urban environments with high traffic volume and abundant usage of flame-protected products. No seasonal trends were observed for all analytes in precipitation at the urban sampling site. TCPP dominated in all precipitation and storm water holding tank (SWHT) water samples with maximum levels exceeding 1 µg/L. An accumulation of OPs deposited in SWHTs was observed with concentrations often exceeding those observed in wet precipitation. Median concentrations of TCPP (880 ng/L), TDCP (13 ng/L), and TBEP (77 ng/L) at the urban SWHT were more than twice as high as those measured at the urban precipitation sampling site (403 ng/L, 5 ng/L, 21 ng/L) located close to the SWHT. OP levels in more remote lakes were often below or close to the limits of quantitation (LOQ). Nevertheless, TCPP was the substance with the highest median concentration in rural volcanic lakes (7–18 ng/L) indicating an atmospheric transport of the compound. At urban lakes the median OP concentrations were in the range of 23–61 ng/L (TCEP), 85–126 ng/L (TCPP), <LOQ–53 ng/L (TBEP), 8–10 ng/L (TiBP), and 17–32 ng/L (TnBP). In laboratory experiments, TBEP, TiBP, and TnBP were photochemically degraded in spiked lake water samples upon exposure to sunlight. In the SWHT a seasonal trend with decreasing concentrations in summer/autumn was evident for TiBP and TnBP but not for the chlorinated OPs. The decreasing concentrations can be explained by in-lake photodegradation. Results have also shown that the occurrence of OPs in groundwater is depending on the anthropogenic impact during groundwater recharge/natural replenishment. Infiltration of precipitation was found to be no important entry-pathway for OPs into aquifers at rural sites. Highest OP concentrations (>0.1 µg/L) were determined in groundwater polluted by percolating leachate from contaminated sites or groundwater recharged via bank filtration of OP-loaded recipients. Concentrations of TCEP, TCPP, TiBP and TnBP in groundwater decreased rapidly (89–97%) during bank filtration with increasing distance from the recipient due to adsorption processes and/or biotransformation. Although TCEP and TCPP are stable within the aquifer, they are not suitable as conservative organic tracers in groundwater.
Nucleation experiments starting from the reaction of OH radicals with SO2 have been performed in the IfT-LFT flow tube under atmospheric conditions at 293±0.5 K for a relative humidity of 13–61%. The presence of different additives (H2, CO, 1,3,5-trimethylbenzene) for adjusting the OH radical concentration and resulting OH levels in the range (4–300) ×105 molecule cm -3 did not influence the nucleation process itself. The number of detected particles as well as the threshold H2SO4 concentration needed for nucleation was found to be strongly dependent on the counting efficiency of the used counting devices. High-sensitivity particle counters allowed the measurement of freshly nucleated particles with diameters down to about 1.5 nm. A parameterization of the experimental data was developed using power law equations for H2SO4 and H2O vapour. The exponent for H2SO4 from different measurement series was in the range of 1.7–2.1 being in good agreement with those arising from analysis of nucleation events in the atmosphere. For increasing relative humidity, an increase of the particle number was observed. The exponent for H2O vapour was found to be 3.1 representing an upper limit. Addition of 1.2×1011 molecule cm -3 or 1.2×1012 molecule cm -3 of NH3 (range of atmospheric NH3 peak concentrations) revealed that NH3 has a measureable, promoting effect on the nucleation rate under these conditions. The promoting effect was found to be more pronounced for relatively dry conditions, i.e. a rise of the particle number by 1–2 orders of magnitude at RH = 13% and only by a factor of 2–5 at RH = 47% (NH3 addition: 1.2×1012 molecule cm -3). Using the amine tert-butylamine instead of NH3, the enhancing impact of the base for nucleation and particle growth appears to be stronger. Tert-butylamine addition of about 1010 molecule cm -3 at RH = 13% enhances particle formation by about two orders of magnitude, while for NH3 only a small or negligible effect on nucleation in this range of concentration appeared. This suggests that amines can strongly influence atmospheric H2SO4-H2O nucleation and are probably promising candidates for explaining existing discrepancies between theory and observations.
We report the first measurements of 1,1,1,2,3,3,3-heptafluoropropane (HFC-227ea), a substitute for ozone depleting compounds, in remote regions of the atmosphere and present evidence for its rapid growth. Observed mixing ratios ranged from below 0.01 ppt in deep firn air to 0.59 ppt in the northern mid-latitudinal upper troposphere. Firn air samples collected in Greenland were used to reconstruct a history of atmospheric abundance. Year-on-year increases were deduced, with acceleration in the growth rate from 0.026 ppt per year in 2000 to 0.057 ppt per year in 2007. Upper tropospheric air samples provide evidence for a continuing growth until late 2009. Fur- thermore we calculated a stratospheric lifetime of 370 years from measurements of air samples collected on board high altitude aircraft and balloons. Emission estimates were determined from the reconstructed atmospheric trend and suggest that current "bottom-up" estimates of global emissions for 2005 are too high by more than a factor of three.
We report the first measurements of 1,1,1,2,3,3,3-heptafluoropropane (HFC-227ea), a substitute for ozone depleting compounds, in air samples originating from remote regions of the atmosphere and present evidence for its accelerating growth. Observed mixing ratios ranged from below 0.01 ppt in deep firn air to 0.59 ppt in the current northern mid-latitudinal upper troposphere. Firn air samples collected in Greenland were used to reconstruct a history of atmospheric abundance. Year-on-year increases were deduced, with acceleration in the growth rate from 0.029 ppt per year in 2000 to 0.056 ppt per year in 2007. Upper tropospheric air samples provide evidence for a continuing growth until late 2009. Furthermore we calculated a stratospheric lifetime of 370 years from measurements of air samples collected on board high altitude aircraft and balloons. Emission estimates were determined from the reconstructed atmospheric trend and suggest that current "bottom-up" estimates of global emissions for 2005 are too high by a factor of three.
A comprehensive evaluation of seasonal backward trajectories initialized in the northern hemisphere lowermost stratosphere (LMS) has been performed to investigate the factors that determine the temporal and spatial structure of troposphere-to-stratosphere-transport (TST) and it’s impact on the LMS. In particular we explain the fundamental role of the transit time since last TST (tTST) for the chemical composition of the LMS. According to our results the structure of the LMS can be characterized by a layer with tTST<40 days forming a narrow band around the local tropopause. This layer extends about 30K above the local dynamical tropopause, corresponding to the extratropical tropopause transition layer (ExTL) as identified by CO. The LMS beyond this layer shows a relatively well defined separation as marked by an aprupt transition to longer tTST indicating less frequent mixing and a smaller fraction of tropospheric air. Thus the LMS constitutes a region of two well defined regimes of tropospheric influence. These can be characterized mainly by different transport times from the troposphere and different fractions of tropospheric air. Carbon monoxide (CO) mirrors this structure of tTST due to it’s finite lifetime on the order of three months. Water vapour isopleths, on the other hand, do not uniquely indicate TST and are independent of tTST, but are determined by the Lagrangian Cold Point (LCP) of air parcels. Most of the backward trajectories from the LMS experienced their LCP in the tropics and sub-tropics, and TST often occurs 20 days after trajectories have encountered their LCP. Therefore, ExTL properties deduced from CO and H2O provide totally different informations on transport and particular TST for the LMS.
Two different single particle mass spectrometers were operated in parallel at the Swiss High Alpine Research Station Jungfraujoch (JFJ, 3580 m a.s.l.) during the Cloud and Aerosol Characterization Experiment (CLACE 6) in February and March 2007. During mixed phase cloud events ice crystals from 5–20 micro m were separated from larger ice aggregates, non-activated, interstitial aerosol particles and supercooled droplets using an Ice-Counterflow Virtual Impactor (Ice-CVI). During one cloud period supercooled droplets were additionally sampled and analyzed by changing the Ice-CVI setup. The small ice particles and droplets were evaporated by injection into dry air inside the Ice-CVI. The resulting ice and droplet residues (IR and DR) were analyzed for size and composition by the two single particle mass spectrometers: a custom-built Single Particle Laser-Ablation Time-of-Flight Mass Spectrometer (SPLAT) and a commercial Aerosol Time-of-Flight Mass Spectrometer (ATOFMS, TSI Model 3800). During CLACE 6 the SPLAT instrument characterized 355 individual IR that produced a mass spectrum for at least one polarity and the ATOFMS measured 152 IR. The mass spectra were binned in classes, based on the combination of dominating substances, such as mineral dust, sulfate, potassium and elemental carbon or organic material. The derived chemical information from the ice residues is compared to the JFJ ambient aerosol that was sampled while the measurement station was out of clouds (several thousand particles analyzed by SPLAT and ATOFMS) and to the composition of the residues of supercooled cloud droplets (SPLAT: 162 cloud droplet residues analyzed, ATOFMS: 1094). The measurements showed that mineral dust was strongly enhanced in the ice particle residues. Close to all of the SPLAT spectra from ice residues did contain signatures from mineral compounds, albeit connected with varying amounts of soluble compounds. Similarly, close to all of the ATOFMS IR spectra show a mineral or metallic component. Pure sulfate and nitrate containing particles were depleted in the ice residues. Sulfate and nitrate was found to dominate the droplet residues (~90% of the particles). The results from the two different single particle mass spectrometers were generally in agreement. Differences in the results originate from several causes, such as the different wavelength of the desorption and ionisation lasers and different size-dependent particle detection efficiencies.