305 research outputs found
Influence of water vapour on the height distribution of positive ions, effective recombination coefficient and ionisation balance in the quiet lower ionosphere
Mesospheric water vapour concentration effects on the ion composition and
electron density in the lower ionosphere under quiet geophysical conditions
were examined. Water vapour is an important compound in the mesosphere and
the lower thermosphere that affects ion composition due to hydrogen radical
production and consequently modifies the electron number density. Recent
lower-ionosphere investigations have primarily concentrated on the
geomagnetic disturbance periods. Meanwhile, studies on the electron density
under quiet conditions are quite rare. The goal of this study is to
contribute to a better understanding of the ionospheric parameter responses
to water vapour variability in the quiet lower ionosphere. By applying a
numerical D region ion chemistry model, we evaluated efficiencies for the
channels forming hydrated cluster ions from the NO<sup>+</sup> and O<sub>2</sub><sup>+</sup>
primary ions (i.e. NO<sup>+</sup>.H<sub>2</sub>O and O<sub>2</sub><sup>+</sup>.H<sub>2</sub>O,
respectively), and the channel forming H<sup>+</sup>(H<sub>2</sub>O)<sub><i>n</i></sub> proton
hydrates from water clusters at different altitudes using profiles with low
and high water vapour concentrations. Profiles for positive ions, effective
recombination coefficients and electrons were modelled for three particular
cases using electron density measurements obtained during rocket campaigns.
It was found that the water vapour concentration variations in the mesosphere
affect the position of both the Cl<sub>2</sub><sup>+</sup> proton hydrate layer upper
border, comprising the NO<sup>+</sup>(H<sub>2</sub>O)<sub><i>n</i></sub> and
O<sub>2</sub><sup>+</sup>(H<sub>2</sub>O)<sub><i>n</i></sub> hydrated cluster ions, and the
Cl<sub>1</sub><sup>+</sup> hydrate cluster layer lower border, comprising the
H<sup>+</sup>(H<sub>2</sub>O)<sub><i>n</i></sub> pure proton hydrates, as well as the numerical
cluster densities. The water variations caused large changes in the effective
recombination coefficient and electron density between altitudes of 75 and
87 km. However, the effective recombination coefficient, α<sub>eff</sub>, and electron number density did not respond even to large
water vapour concentration variations occurring at other altitudes in the
mesosphere. We determined the water vapour concentration upper limit at
altitudes between 75 and 87 km, beyond which the water vapour concentration
ceases to influence the numerical densities of Cl<sub>2</sub><sup>+</sup> and Cl<sub>1</sub><sup>+</sup>,
the effective recombination coefficient and the electron number density
in the summer ionosphere. This water vapour concentration limit corresponds
to values found in the H<sub>2</sub>O-1 profile that was observed in the summer
mesosphere by the Upper Atmosphere Research Satellite (UARS). The electron density modelled using the
H<sub>2</sub>O-1 profile agreed well with the electron density measured in the
summer ionosphere when the measured profiles did not have sharp gradients.
For sharp gradients in electron and positive ion number densities, a water
profile that can reproduce the characteristic behaviour of the ionospheric
parameters should have an inhomogeneous height distribution of water vapour
A case study of gravity waves in noctilucent clouds
We present a case study of a noctilucent cloud (NLC) display appearing on 10-11 August 2000 over Northern Sweden. Clear wave structures were visible in the clouds and time-lapse photography was used to derive the parameters characterising the gravity waves which could account for the observed NLC modulation. Using two nearby atmospheric radars, the Esrange MST Radar data and Andoya MF radar, we have identified gravity waves propagating upward from the upper stratosphere to NLC altitudes. The wave parameters derived from the radar measurements support the suggestion that gravity waves are responsible for the observed complex wave dynamics in the NLC
Inertia gravity waves in the upper troposphere during the MaCWAVE winter campaign – Part I: Observations with collocated radars
During the {MaCWAVE} campaign, combined rocket, radiosonde and ground-based measurements have been performed at the Norwegian Andøya Rocket Range (ARR) near Andenes and the Swedish Rocket Range (ESRANGE) near Kiruna in January 2003 to study gravity waves in the vicinity of the Scandinavian mountain ridge. The investigations presented here are mainly based on the evaluation of continuous radar measurements with the ALWIN VHF radar in the upper troposphere/ lower stratosphere at Andenes (69.3° N, 16.0° E) and the ESRAD VHF radar near Kiruna (67.9° N, 21.9° E). Both radars are separated by about 260 km. Based on wavelet transformations of both data sets, the strongest activity of inertia gravity waves in the upper troposphere has been detected during the first period from 24–26 January 2003 with dominant vertical wavelengths of about 4–5 km as well as with dominant observed periods of about 13–14 h for the altitude range between 5 and 8 km under the additional influence of mountain waves. The results show the appearance of dominating inertia gravity waves with characteristic horizontal wavelengths of ~200 km moving in the opposite direction than the mean background wind. The results show the appearance of dominating inertia gravity waves with intrinsic periods in the order of ~5 h and with horizontal wavelengths of 200 km, moving in the opposite direction than the mean background wind. From the derived downward energy propagation it is supposed, that these waves are likely generated by a jet streak in the upper troposphere. The parameters of the jet-induced gravity waves have been estimated at both sites separately. The identified gravity waves are coherent at both locations and show higher amplitudes on the east-side of the Scandinavian mountain ridge, as expected by the influence of mountains
Inertia gravity waves in the upper troposphere during the MaCWAVE winter campaign ? Part II: Radar investigations and modelling studies
International audienceWe present an experimental and modelling study of a strong gravity wave event in the upper troposphere/lower stratosphere near the Scandinavian mountain ridge. Continuous VHF radar measurements during the MaCWAVE rocket and ground-based measurement campaign were performed at the Norwegian Andoya Rocket Range (ARR) near Andenes (69.3° N, 16° E) in January 2003. Detailed gravity wave investigations based on PSU/NCAR Fifth-Generation Mesoscale Model (MM5) data have been used for comparison with experimentally obtained results. The model data show the presence of a mountain wave and of an inertia gravity wave generated by a jet streak near the tropopause region. Temporal and spatial dependencies of jet induced inertia gravity waves with dominant observed periods of about 13 h and vertical wavelengths of ~4.5?5 km are investigated with wavelet transform applied on radar measurements and model data. The jet induced wave packet is observed to move upstream and downward in the upper troposphere. The model data agree with the experimentally obtained results fairly well. Possible reasons for the observed differences, e.g. in the time of maximum of the wave activity, are discussed. Finally, the vertical fluxes of horizontal momentum are estimated with different methods and provide similar amplitudes. We found indications that the derived positive vertical flux of the horizontal momentum corresponds to the obtained parameters of the jet-induced inertia gravity wave, but only at the periods and heights of the strongest wave activity
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Inertia gravity waves in the upper troposphere during the MaCWAVE winter campaign - Part I: Observations with collocated radars
During the {MaCWAVE} campaign, combined rocket, radiosonde and ground-based measurements have been performed at the Norwegian Andøya Rocket Range (ARR) near Andenes and the Swedish Rocket Range (ESRANGE) near Kiruna in January 2003 to study gravity waves in the vicinity of the Scandinavian mountain ridge. The investigations presented here are mainly based on the evaluation of continuous radar measurements with the ALWIN VHF radar in the upper troposphere/ lower stratosphere at Andenes (69.3° N, 16.0° E) and the ESRAD VHF radar near Kiruna (67.9° N, 21.9° E). Both radars are separated by about 260 km. Based on wavelet transformations of both data sets, the strongest activity of inertia gravity waves in the upper troposphere has been detected during the first period from 24–26 January 2003 with dominant vertical wavelengths of about 4–5 km as well as with dominant observed periods of about 13–14 h for the altitude range between 5 and 8 km under the additional influence of mountain waves. The results show the appearance of dominating inertia gravity waves with characteristic horizontal wavelengths of ~200 km moving in the opposite direction than the mean background wind. The results show the appearance of dominating inertia gravity waves with intrinsic periods in the order of ~5 h and with horizontal wavelengths of 200 km, moving in the opposite direction than the mean background wind. From the derived downward energy propagation it is supposed, that these waves are likely generated by a jet streak in the upper troposphere. The parameters of the jet-induced gravity waves have been estimated at both sites separately. The identified gravity waves are coherent at both locations and show higher amplitudes on the east-side of the Scandinavian mountain ridge, as expected by the influence of mountains
Reduced Population Control of an Insect Pest in Managed Willow Monocultures
BACKGROUND: There is a general belief that insect outbreak risk is higher in plant monocultures than in natural and more diverse habitats, although empirical studies investigating this relationship are lacking. In this study, using density data collected over seven years at 40 study sites, we compare the temporal population variability of the leaf beetle Phratora vulgatissima between willow plantations and natural willow habitats. METHODOLOGY/PRINCIPAL FINDINGS: The study was conducted in 1999-2005. The density of adult P. vulgatissima was estimated in the spring every year by a knock-down sampling technique. We used two measures of population variability, CV and PV, to compare temporal variations in leaf beetle density between plantation and natural habitat. Relationships between density and variability were also analyzed to discern potential underlying processes behind stability in the two systems. The results showed that the leaf beetle P. vulgatissima had a greater temporal population variability and outbreak risk in willow plantations than in natural willow habitats. We hypothesize that the greater population stability observed in the natural habitat was due to two separate processes operating at different levels of beetle density. First, stable low population equilibrium can be achieved by the relatively high density of generalist predators observed in natural stands. Second, stable equilibrium can also be imposed at higher beetle density due to competition, which occurs through depletion of resources (plant foliage) in the natural habitat. In willow plantations, competition is reduced mainly because plants grow close enough for beetle larvae to move to another plant when foliage is consumed. CONCLUSION/SIGNIFICANCE: To our knowledge, this is the first empirical study confirming that insect pest outbreak risk is higher in monocultures. The study suggests that comparative studies of insect population dynamics in different habitats may improve our ability to predict insect pest outbreaks and could facilitate the development of sustainable pest control in managed systems
Inertia gravity waves in the upper troposphere during the MaCWAVE winter campaign – Part II: Radar investigations and modelling studies
Electron density profiles in the quiet lower ionosphere based on the results of modeling and experimental data
D-region electron density and effective recombination coefficients during twilight – experimental data and modelling during solar proton events
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