The Dexi-SH* model for a multivariate assessment of agro-ecological sustainability of dairy grazing systems

Dexi-SH* is an ex ante multivariate model for assessing the sustainability of dairy cows grazing systems. This model is composed of three sub-models that evaluate the impact of the systems on: (i) biotic resources; (ii) abiotic resources, and (iii) pollution risks. The structuring of the hierarchical tree was inspired by that of the Masc model. The choice of criteria and their aggregation modalities were discussed within a multi-disciplinary group of scientists. For each cluster, a utility function was established in order to determine weighting and priority functions between criteria. The model can take local and regional conditions and standards into account by adjusting criterion categories to the agroecological context, and the specific views of the decision makers by changing the weighting of criteria

Thermal Conductivity of Ordered Mesoporous Nanocrystalline Silicon Thin Films Made from Magnesium Reduction of Polymer-Templated Silica

This paper reports the cross-plane thermal conductivity of ordered mesoporous nanocrystalline silicon thin films between 25 and 315 K. The films were produced by evaporation induced self-assembly of mesoporous silica followed by magnesium reduction. The periodic ordering of pores in mesoporous silicon was characterized by X-ray diffraction and direct SEM imaging. The average crystallite size, porosity, and film thickness were about 13 nm, 25-35%, and 140-340 nm, respectively. The pores were arranged in a face-centered cubic lattice. The cross-plane thermal conductivity of the mesoporous silicon thin films was measured using the 3ω method. It was between 3 and 5 orders of magnitude smaller than that of bulk single crystal silicon in the temperature range considered. The effects of temperature, film thickness, and copolymer template on the thermal conductivity were investigated. A model based on kinetic theory was used to accurately predict the measured thermal conductivity for all temperatures. On the one hand, both the measured thermal conductivity and the model predictions showed a temperature dependence of k proportional to T2 at low temperatures, typical of amorphous and strongly disordered materials. On the other hand, at high temperatures the thermal conductivity of mesoporous silicon films reached a maximum, indicating a crystalline-like behavior. These results will be useful in designing mesoporous silicon with desired thermal conductivity by tuning its morphology for various applications

Thermal conductivity of cubic and hexagonal mesoporous silica thin films

This paper reports the cross-plane thermal conductivity of highly ordered cubic and hexagonal templated mesoporous amorphous silica thin films synthesized by evaporation-induced self-assembly process. Cubic and hexagonal films featured spherical and cylindrical pores and average porosities of 25% and 45%, respectively. The pore diameters ranged from 3 to 18 nm and film thickness from 80 to 540 nm, while the average wall thickness varied from 3 to 12 nm. The thermal conductivity was measured at room temperature using the 3 omega method. The experimental setup and the associated analysis were validated by comparing the thermal conductivity measurements with the data reported in literature for the silicon substrate and for high quality thermal oxide thin films with thicknesses ranging from 100 to 500 nm. The cross-plane thermal conductivity of the synthesized mesoporous silica thin films does not show strong dependence on pore size, wall thickness, or film thickness. This is due to the fact that heat is mainly carried by very localized nonpropagating vibrational modes. The average thermal conductivity for the cubic mesoporous silica films was 0.30 +/- 0.02 W/m K, while it was 0.20 +/- 0.01 W/m K for the hexagonal films. This corresponds to reductions of 79% and 86% from bulk fused silica at room temperature

Thermal Conductivity of Highly-Ordered Mesoporous Titania Thin Films from 30 to 320 K

This paper reports the cross-plane thermal conductivity of highly-ordered amorphous and crystalline templated mesoporous titania thin films measured by the 3ω method from 30 to 320 K. Both sol-gel and nanocrystal-based films were synthesized by evaporation-induced self-assembly, with average porosity of 30% and 35%, respectively. The pore diameter ranged from 14 to 25 nm. The size of crystalline domains in polycrystalline mesoporous films was 12 to 13 nm while the nanocrystals in the nanocrystal-based film were 9 nm in diameter. At high temperatures, the thermal conductivity of amorphous dense and mesoporous films showed similar trends with respect to temperature. This was attributed to the fact that the presence of pores had a purely geometrical effect by reducing the cross-sectional area through which heat can diffuse. By contrast, the thermal conductivity of polycrystalline dense and mesoporous films behave differently with temperature due to phonon scattering by pores and crystalline nanosize domains. In addition, at low temperatures, the presence of pores caused the thermal conductivity of mesoporous films to be less temperature dependent than their dense counterparts. Despite its crystallinity, the thermal conductivity of the nanocrystal-based film was about 40% less than that of the polycrystalline mesoporous films. This was mainly attributed to its larger porosity, smaller crystal size, and strong phonon scattering at the poorly interconnected nanocrystal boundaries. These results suggest various ways to control the thermal conductivity of mesoporous materials for various applications

Specificity of cGMP binding to a purified cGMP-stimulated phosphodiesterase from bovine adrenal tissue.

The binding of [3H]cGMP (guanosine 3',5'-monophosphate) to purified bovine adrenal cGMP-stimulated phosphodiesterase was measured by Millipore filtration on cellulose ester filter. [3H]cGMP-binding activity was enhanced when the assay was terminated in buffer containing 70% of saturated ammonium sulfate to dilute the enzyme and wash the filters. The cGMP-binding activity was co-purified with the phosphodiesterase activity. The binding of [3H]cGMP to purified enzyme was measured in the presence or absence of the phosphodiesterase inhibitor, 1-methyl-3-isobutylxanthine. 1-Methyl-3-isobutylxanthine showed linear competitive inhibition with respect to cGMP as substrate in the phosphodiesterase reaction but stimulated the [3H]cGMP-binding activity in the binding assay. The stimulatory effect appeared not to be the result of preservation from [3H]cGMP hydrolysis; no cGMP phosphodiesterase activity has been measured under the cGMP-binding assay conditions, in the absence or presence of the inhibitor. Half-maximal stimulation by 1-methyl-3-isobutylxanthine occurred in the 5-7 microM concentration range. The specificity of binding of [3H]cGMP was investigated by adding increasing concentration of unlabeled analogs of cAMP (adenosine 3',5'-monophosphate) and cGMP. The binding of [3H]cGMP (50 nM) was displaced by unlabeled cGMP and cAMP with the following potency: 50% displacement was reached at the 0.1 microM cGMP range and only at a fiftyfold higher cAMP concentration. Our data with comparative series of analogs (e.g. 5'-amino-5'-deoxyguanosine 3',5'-monophosphate and 3'-amino-3'-deoxyguanosine 3',5'-monophosphate) showed that the potencies of stimulation of cAMP phosphodiesterase activity parallels displacement curves or [3H]cGMP binding to purified enzyme with no correlation with phosphodiesterase inhibition sequences. Those experiments suggest that the cGMP-binding activity is directly related to the non-catalytic (allosteric) cGMP-binding site.Journal ArticleResearch Support, Non-U.S. Gov'tinfo:eu-repo/semantics/publishe