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The link between atmospheric radicals and newly formed particles at a spruce forest site in Germany
(2014)
It has been claimed for more than a century that atmospheric new particle formation is primarily influenced by the presence of sulfuric acid. However, the activation process of sulfuric acid related clusters into detectable particles is still an unresolved topic. In this study we focus on the PARADE campaign measurements conducted during August/September 2011 at Mt Kleiner Feldberg in central Germany. During this campaign a set of radicals, organic and inorganic compounds and oxidants and aerosol properties were measured or calculated. We compared a range of organic and inorganic nucleation theories, evaluating their ability to simulate measured particle formation rates at 3 nm in diameter (J3) for a variety of different conditions. Nucleation mechanisms involving only sulfuric acid tentatively captured the observed noon-time daily maximum in J3, but displayed an increasing difference to J3 measurements during the rest of the diurnal cycle. Including large organic radicals, i.e. organic peroxy radicals (RO2) deriving from monoterpenes and their oxidation products, in the nucleation mechanism improved the correlation between observed and simulated J3. This supports a recently proposed empirical relationship for new particle formation that has been used in global models. However, the best match between theory and measurements for the site of interest was found for an activation process based on large organic peroxy radicals and stabilised Criegee intermediates (sCI). This novel laboratory-derived algorithm simulated the daily pattern and intensity of J3 observed in the ambient data. In this algorithm organic derived radicals are involved in activation and growth and link the formation rate of smallest aerosol particles with OH during daytime and NO3 during night-time. Because the RO2 lifetime is controlled by HO2 and NO we conclude that peroxy radicals and NO seem to play an important role for ambient radical chemistry not only with respect to oxidation capacity but also for the activation process of new particle formation. This is supposed to have significant impact of atmospheric radical species on aerosol chemistry and should be taken into account when studying the impact of new particles in climate feedback cycles.
In this survey paper, we present a multiscale post-processing method in exploration. Based on a physically relevant mollifier technique involving the elasto-oscillatory Cauchy–Navier equation, we mathematically describe the extractable information within 3D geological models obtained by migration as is commonly used for geophysical exploration purposes. More explicitly, the developed multiscale approach extracts and visualizes structural features inherently available in signature bands of certain geological formations such as aquifers, salt domes etc. by specifying suitable wavelet bands.
Residual circulation trajectories and transit times into the extratropical lowermost stratosphere
(2010)
Transport into the extratropical lowermost stratosphere (LMS) can be divided into a slow part (time-scale of several months to years) associated with the global-scale stratospheric residual circulation and a fast part (time-scale of days to a few months) associated with (mostly quasi-horizontal) mixing (i.e. two-way irreversible transport, including stratosphere-troposphere exchange). The stratospheric residual circulation can be considered to consist of two branches: a deep branch more strongly associated with planetary waves breaking in the middle to upper stratosphere, and a shallow branch more strongly associated with synoptic-scale waves breaking in the subtropical lower stratosphere. In this study the contribution due to the stratospheric residual circulation alone to transport into the LMS is quantified using residual circulation trajectories, i.e. trajectories driven by the (time-dependent) residual mean meridional and vertical velocities. This contribution represents the advective part of the overall transport into the LMS and can be viewed as providing a background onto which the effect of mixing has to be added. Residual mean velocities are obtained from a comprehensive chemistry-climate model as well as from reanalysis data. Transit times of air traveling from the tropical tropopause to the LMS along the residual circulation streamfunction are evaluated and compared to recent mean age of air estimates. A clear time-scale separation with much smaller transit times into the mid-latitudinal LMS than into polar LMS is found that is indicative of a clear separation of the shallow from the deep branch of the residual circulation. This separation between the shallow and the deep circulation branch is further manifested in a clear distinction in the aspect ratio of the vertical to meridional extent of the trajectories as well as the integrated mass flux along the residual circulation trajectories. The residual transit time distribution reproduces qualitatively the observed seasonal cycle of youngest air in the extratropical LMS in fall and oldest air in spring.
Residual circulation trajectories and transit times into the extratropical lowermost stratosphere
(2011)
Transport into the extratropical lowermost stratosphere (LMS) can be divided into a slow part (time-scale of several months to years) associated with the global-scale stratospheric residual circulation and a fast part (time-scale of days to a few months) associated with (mostly quasi-horizontal) mixing (i.e. two-way irreversible transport, including extratropical stratosphere-troposphere exchange). The stratospheric residual circulation may be considered to consist of two branches: a deep branch more strongly associated with planetary waves breaking in the middle to upper stratosphere, and a shallow branch associated with synoptic and planetary scale waves breaking in the subtropical lower stratosphere. In this study the contribution due to the stratospheric residual circulation alone to transport into the LMS is quantified using residual circulation trajectories, i.e. trajectories driven by the (time-dependent) residual mean meridional and vertical velocities. This contribution represents the advective part of the overall transport into the LMS and can be viewed as providing a background onto which the effect of mixing has to be added. Residual mean velocities are obtained from a comprehensive chemistry-climate model as well as from reanalysis data. Transit times of air traveling from the tropical tropopause to the LMS along the residual circulation streamfunction are evaluated and compared to recent mean age of air estimates. A time-scale separation with much smaller transit times into the mid-latitudinal LMS than into polar LMS is found that is indicative of a separation of the shallow from the deep branch of the residual circulation. This separation between the shallow and the deep circulation branch is further manifested in a distinction in the aspect ratio of the vertical to meridional extent of the trajectories, the integrated mass flux along the residual circulation trajectories, as well as the stratospheric entry latitude of the trajectories. The residual transit time distribution reproduces qualitatively the observed seasonal cycle of youngest air in the extratropical LMS in fall and oldest air in spring.
Der Cornbrash (sandige Fazies des Bathonien) setzt sich im zentralen Teil des Niedersächsischen Beckens aus insgesamt 5 Teilschüttungen zusammen. Zwei Sandschüttungen erfolgten im Unter-Bathonien (Obere Württembergica-Sandsteine); im Ober-Bathonien können insgesamt drei Sandschüttungen ausgehalten werden (Aspidoides-Sandsteine). Während der Einschüttung der Württembergica-Sandsteine sowie der unteren Abteilung des Aspidoides-Sandsteins bildete der Bereich etwa östlich der Linie Steinhuder Meer-Minden eine stabile Plattform, auf der sich von Osten nach Westen Deltas vorbauten (obere Abteilung des Oberen Württembergica-Sandsteins) bzw. hochenergetische Sandplaten zur Ablagerung kamen (untere Abteilung des Oberen Württembergica-Sandsteins sowie des Aspidoides-Sandsteins). Westlich dieser Plattform kam es im Bereich des Wesertroges dagegen zu einem phasenweisen Absinken des Untergrundes. Dementsprechend wechselhaft ist hier die Sedimentation: tonige Schelfablagerungen, deckenförmige Sande eines flach-tiefen Subtidals, hochenergetische Sandplatenbildungen sowie tonige, Bryozoen- und Onkoiden-führende Tone eines geschützten Litorals bilden im höheren Dogger insgesamt 3 regressive Sedimentationszyklen ab. Den insgesamt N-S verlaufenden Beckenkonturen entsprechend war im offenen Schelfbereich (Weser-Wiehengebirge) während des Bathonien ein zum Beckenrand parallel vertautendescnach Norden gerichtetes - Meeresströmungssystem ausgebildet. In Beckenrandbereichen (Süntel) erzeugte dagegen die auflaufende Gezeitenwelle ein senkrecht zum Beckenrand orientiertes, E-W gerichtetes Strömungsmuster. Im höheren Ober-Bathonien erfolgte eine tiefgreifende Umgestaltung der südlichen Beckenteile. Verstärkte Hebungsvorgänge im Bereich der Westfälisch-Lippischen Schwelle führten zu Sandeinschüttungen aus südlichen Richtungen, gleichzeitig verloren die östlichen Liefergebiete an Bedeutung. Sandschüttungen aus Norden, die vermutlich während des gesamten Bathonien erfolgten, haben den Südrand des Niedersächsischen Beckens zu keiner Zeit erreicht.
We have sampled atmospheric ice nuclei (IN) and aerosol in Germany and in Israel during spring 2010. IN were analyzed by the static vapor diffusion chamber FRIDGE, as well as by electron microscopy. During the Eyjafjallajökull volcanic eruption of April 2010 we have measured the highest ice nucleus number concentrations (>600 l−1) in our record of 2 yr of daily IN measurements in central Germany. Even in Israel, located about 5000 km away from Iceland, IN were as high as otherwise only during desert dust storms. The fraction of aerosol activated as ice nuclei at −18 °C and 119% rhice and the corresponding area density of ice-active sites per aerosol surface were considerably higher than what we observed during an intense outbreak of Saharan dust over Europe in May 2008.
Pure volcanic ash accounts for at least 53–68% of the 239 individual ice nucleating particles that we collected in aerosol samples from the event and analyzed by electron microscopy. Volcanic ash samples that had been collected close to the eruption site were aerosolized in the laboratory and measured by FRIDGE. Our analysis confirms the relatively poor ice nucleating efficiency (at −18 °C and 119% ice-saturation) of such "fresh" volcanic ash, as it had recently been found by other workers. We find that both the fraction of the aerosol that is active as ice nuclei as well as the density of ice-active sites on the aerosol surface are three orders of magnitude larger in the samples collected from ambient air during the volcanic peaks than in the aerosolized samples from the ash collected close to the eruption site. From this we conclude that the ice-nucleating properties of volcanic ash may be altered substantially by aging and processing during long-range transport in the atmosphere, and that global volcanism deserves further attention as a potential source of atmospheric ice nuclei.
Explosive volcanism affects weather and climate. Primary volcanic ash particles which act as ice nuclei (IN) can modify the phase and properties of cold tropospheric clouds. During the Eyjafjallajökull volcanic eruption we have measured the highest ice nucleus number concentrations (>600 L) in our record of 2 years of daily IN measurements in central Germany. Even in Israel, located about 5000 km away from Iceland, IN were as high as otherwise only during desert dust storms. These measurements are the only ones available on the properties of IN in the Eyjafjallajökull plume. The measured high concentrations and high activation temperature (−8 °C) point to an important impact of volcanic ash on microphysical and radiative properties of clouds through enhanced glaciation.
In Memoriam: Kurt Kimpel †
(1950)
In vorliegender Untersuchung wurde der Rißlöß zwischen der 1. und 2. fossilen Parabraunerde anhand schwächerer Bodenbildungen und eingeschalteter Abtragungsphasen zu gliedern versucht. Im jüngeren Riß herrschte starke Lößsedimentation vor, wobei es in mindestens 6 kaltfeuchten Abschnitten zur Ausbildung schwacher periglazialer Naßböden kam. Die Naßbodenserie wurde als Bruchköbeler Böden (B) bezeichnet. Im jüngsten Rißlöß ist wenige dm unter dem Eemboden als tephrochronologischer Leithorizont der Krifteler Tuff (vgl. SEMMEL 1968) eingeschaltet. Den mittleren Profilbereich im Rißlöß zeichnen feuchtere Klimaabschnitte mit starken Verschwemmungsphasen aus, die in den meisten Profilen zu erheblichen Diskordanzen geführt haben. An der Basis der wenigen kompletten Rißlöß-Profile treten vorwiegend in Hessen über der zumeist gekappten 2. fossilen Parabraunerde maximal zwei Schwarzerden auf, die von SEMMEL (1968) als Weilbacher Humuszonen bezeichnet werden. Unmittelbar über diesen Schwarzerden folgt die Ostheimer Zone, eine Fließerde aus aufgearbeitetem Solumaterial der liegenden Böden. Insgesamt zeigt die aus den Rißböden rekonstruierte Klimaabfolge — neben geringfügigen Abweichungen — überraschende Parallelen zur paläopedologisch-klimatischen Gliederung der Würmkaltzeit.