Reducing hazard vulnerability through local government engagement and action

The concept of a natural hazard is a human construct. It is the interaction with human communities and settlements that defines a natural phenomenon as a natural hazard. Thus the end point of hazard mitigation and hazard vulnerability assessment must involve an attempt to reduce, or mitigate, the impact of the natural hazard on human communities. The responsibility to mitigate hazard impact falls primarily upon governments and closely connected non-government and private institutional agencies. In particular, it is most often local government that takes the responsibility for safeguarding its own communities, infrastructure and people. Hazard vulnerability of specific local communities is best assessed by the local government or council, which then faces the responsibility to translate that assessment into community education and infrastructural safeguards for hazard mitigation. This paper illustrates the process of local government engagement in hazard mitigation in Australia, through the Natural Disaster Risk Management Studies, as a first step towards natural disaster reduction.     

Detection of free vertical convection and double-diffusion in groundwater monitoring wells with geophysical borehole measurements

Two algorithms for in-situ detection and identification of vertical free convective and double-diffusive flows in groundwater monitoring wells or boreholes are proposed. With one algorithm the causes (driving forces) and with the other one the effects (convection or double-diffusion) of vertical transport processes can be detected based on geophysical borehole measurements in the water column. Five density-driven flow processes are identified: thermal, solutal, and thermosolutal convection leading to an equalization, as well as saltfingers and diffusive layering leading to an intensification of a vertical density gradient. The occurrence of density-driven transport processes could be proven in many groundwater monitoring wells and boreholes; especially shallow sections of boreholes or groundwater monitoring wells are affected dramatically by such vertical flows. Deep sections are also impaired as the critical threshold for the onset of a density-driven flow is considerably low. In monitoring wells or boreholes, several sections with different types of density-driven vertical flows may exist at the same time. Results from experimental investigations in a medium-scale testing facility with high aspect ratio (height/radius = 19) and from numerical modeling of a water column agree well with paramters of in-situ detected convection cells.     

Field Measurement of Suction, Water Content, and Water Permeability

This paper presents a review of techniques for field measurement of suction, water content, and water hydraulic conductivity (permeability). Main problems in the use of field tensiometers are addressed and hints on how to improve tensiometer performance are given. Advantages and limitations of instruments for indirect measurement of suction including electrical conductivity sensors, thermal conductivity sensors, dielectric permittivity sensors, filter paper, and psychrometer are discussed. Techniques for water content measurement based on dielectric methods are then presented. These include time and amplitude domain reflectometry and capacitance. Finally, a brief overview of methods for measurement of water permeability in the field is presented.     

Discussion of the Möller radiation chart

Summary M?ller's assumptions for the carbon dioxide-water vapor overlap region, which lead to the construction of his radiation chart, are reinvestigated in the light of modern theory. A new radiation chart, taking into account the carbon dioxide-water vapor overlap, is constructed using water vapor and carbon dioxide absorption data as furnished byM?ller andElsasser respectively. The results of the radiative fluxes computed from the new chart are compared with equivalent results using the original M?ller and the revised Elsasser radiation diagrams, as well as with measurements.

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Zusammenfassung Die Berechtigung derM?llerschen Annahme zur getrennten Behandlung von Kohlens?ure- und Wasserdampfabsorption zwecks Konstruktion eines atmosph?rischen Strahlungsdiagrammes wird im Lichte der modernen Theorie diskutiert. Ein neues Strahlungspapier wird vorgelegt, das die gleichzeitige Anwesenheit von Kohlens?ure und Wasserdampf im gleichen Spektralbereich berücksichtigt. Dieses beruht auf Wasserdampf- und Kohlens?uredaten, die vonM?ller undElsasser vorgegeben wurden. Nach dem neuen Strahlungsdiagramm berechnete Werte werden mit Me?werten und theoretischen Werten verglichen, die mit dem ursprünglichen M?llerschen und mit dem verbesserten Elsasserschen Strahlungspapier ermittelt wurden.

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Résumé Au vu des théories modernes, on discute l'hypothèse formulée parM?ller et sa justification, hypothèse selon laquelle il est nécessaire de traiter séparément l'absorption du dioxyde de carbone et celle de la vapeur d'eau lors de l'établissement d'un diagramme du rayonnement atmosphérique. On propose alors un nouvel abaque qui tient compte de la présence simultanée du dioxyde de carbone et de la vapeur d'eau dans la même région spectrale. Cet abaque s'appuie sur les valeurs données parM?ller et parElsasser, valeurs valables pour ces deux gaz. On compare le résultat de calculs effectués avec ce nouvel abaque à des mesures et à des valeurs théoriques ces dernières étant basées tant sur les travaux originaux deM?ller que sur l'abaque amélioré deElsasser.

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With 4 Figures     

A calculation of the large scale three dimensional distribution of diabatic heating in the atmosphere

Summary The large scale three-dimensional diabatic heating in the atmosphere is computed at 12 isentropic surfaces for a particular twelve hour time period. Using a method due toErtel, the continuity equation is combined with the equations of motion to give an explicit relation between diabatic heating and changes in potential vorticity and stability along isentropic surface trajectories. The results are barely of useful accuracy and reliability and this only under favorable conditions. The distribution of diabatic heating is qualitatively reasonable in the regions near the tropopause, close to the ground, above a cloud or moist layer, and within an area of general condensation. Errors and approximations make the computed values completely unreliable in areas of large anticyclonic vorticity or large baroclinity. Comparison of magnitudes with those computed from rainfall observations and with those measured directly at the earth's surface shows agreement in sign and within a factor of three in the areas of best data. The results emphasize that there are regions and periods where diabatic heating in the free atmosphere may be important in controlling atmospheric behavior. Sample calculations in one of these regions using values of diabatic heating computed by this study illustrate that this process is of comparable importance with the adiabatic process in determining vertical velocity.

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Zusammenfassung Die großräumige nichtadiabatische Erwärmung der Atmosphäre in 12 isentropen Flächen während eines 12stündigen Zeitabschnittes wird berechnet. Unter Verwendung einer Methode vonErtel liefert eine Kombination der Kontinuitätsgleichung mit den Bewegungsgleichungen eine explizite Beziehung zwischen der nichtadiabatischen Erwärmung, der potentiellen Vorticity und der Stabilität entlang der isentropen Trajektorien. Das Resultat ist von beschränkter Genauigkeit — und auch dies nur unter günstigen Bedingungen. Qualitativ brauchbare Verteilungen der nichtadiabatischen Erwärmung erhält man nahe der Tropopause, in Bodennähe, über einer Schicht von Wolken oder feuchter Luft und innerhalb der Zonen mit verbreiteter Kondensation. In Gebieten mit großer antizyklonaler Vorticity oder großer Baroklinität werden die berechneten Werte infolge von Meß- und Approximationsfehlern völlig ungenau. In den Gebieten mit optimalen Voraussetzungen stimmen die berechneten Werte mit den aus Niederschlagsmessungen abgeleiteten oder am Boden direkt beobachteten im Vorzeichen und innerhalb eines Faktors von 3 überein. Die Ergebnisse der vorliegenden Untersuchung weisen erneut darauf hin, daß in manchen Gebieten bzw. Zeitabschnitten das Verhalten der freien Atmosphäre durch nichtadiabatische Erwärmung wesentlich beeinflußt sein kann. Stichprobenweise Berechnungen für eines dieser Gebiete zeigen, daß die theoretisch ermittelte nichtadiabatische Erwärmung für die resultierende Vertikalgeschwindigkeit der Luft quantitativ von ähnlicher Bedeutung ist wie der adiabatische Prozeß.

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Résumé L'auteur a calculé le réchauffement non adiabatique, à grande échelle, de l'atmosphère à 12 niveaux isentropes pendant un intervalle de 12 heures. Une méthode établie parErtel combine l'équation de continuité et les équations de mouvement et aboutit à une relation explicite entre le réchauffement non adiabatique, la vorticity potentielle et la stabilité le long de trajectoires isentropes. Le résultat n'a qu'une exactitude approchée, et cela dans des conditions favorables seulement. On obtient une répartition utilisable du réchauffement non adiabatique au voisinage de la tropopause, du sol, au-dessus d'une couche de nuages ou d'air humide, ainsi qu'à l'intérieur des zones à forte condensation. Dans les régions à grande vorticity anticyclonique et à grande baroclinité, les valeurs calculées deviennent tout à fait inexactes par suite d'une approximation insuffisante et d'erreurs de mesure. Dans les régions à conditions favorables par contre, les valeurs calculées correspondent à celles que l'on peut tirer de la mesure des précipitations ou de celles que l'on mesure au sol, cela au signe et à un facteur 3 près. Le résultat de cette étude montre à nouveau que dans certaines régions ou certains laps de temps l'état de l'atmosphère peut être notablement conditionné par un réchauffement non adiabatique. Des épreuves faites pour l'une de ces régions montrent que le réchauffement non adiabatique obtenu par calcul est quantitativement aussi important pour la vitesse verticale résultante de l'air que le processus adiabatique.

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With 7 Figures     

The volcano-magnetic effect

Summary A geometrically simple volcano is considered, havig a spherical magma chamber of 2.5 km radius centred at 10 km depth. The Curie point isotherm is assumed to be a plane at 20 km depth, except for the spherical volume which is also non-magnetic. The stress pattern in the vicinity of the spherical chamber, due to regional stress of sufficient intensity to cause an eruptions, is used to calculate the change in magnetization which results from the piezomagnetic effect through the volume of solid rock. The consequent magnetic field anomaly at the surface is then obtaied by numerical integration of the dipole law of force over the stressed volume. For rocks of the type found on the volcanic island of St. Vincent (West Indies), this model gives a maximum local volcano-magnet c effect of about 7 gammas.     

Modification of an acoustic pinger to transmit temperature data

An acoustic pinger can be modified to transmit two pings per second with the delay time between pings controlled by the temperature of an external thermistor. The precision of the temperature measurements is on the order of 0.1°C. This modification does not interfere with the normal depth indicating function of the pinger and is an inexpensive means of obtaining water temperature data.