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31.
In this paper we revisit old swelling data on polymer networks that have not been interpreted theoretically on a closed molecular basis. If the osmotic pressure of the swollen network is compared to the osmotic pressure of the corresponding uncrosslinked solution unsolved problems appear, when the relative osmotic pressure is plotted against the degree of swelling, i.e. the deformation due to swelling. A significant maximum appears which cannot be explained by any of the recently derived elastic models, such as junction constraint or other entanglement models. It is suggested in this paper that the maximum is a consequence of structural heterogeneities of fractal nature. If such fractal heterogeneities are assumed a strong maximum in the relative osmotic pressure can be reproduced. The physical reason is the different thermodynamic behavior of uncrosslinked linear chains and crosslinked self-similar (non-linear) polymers. The conclusion is supported by numerical (Monte Carlo) simulations.  相似文献   
32.
Sommer M  Brazda K  Hantel M 《Physics letters. A》2011,375(37-2):3310-3313
So far fluid mechanical Nambu brackets have mainly been given on an intuitive basis. Alternatively an algorithmic construction of such a bracket for the two-dimensional vorticity equation is presented here. Starting from the Lie-Poisson form and its algebraic properties it is shown how the Nambu representation can be explicitly constructed as the continuum limit from the structure preserving Zeitlin discretization.  相似文献   
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Laser drilling of stainless steel with nanosecond double-pulse   总被引:1,自引:0,他引:1  
Nanosecond double-pulse laser drilling is reported in this paper. The double-pulse herein represents two closely conjoint pulses with 21 ns pulse duration and about 52 ns interpulse separation, which are acquired by temporal pulse shaping. Percussion drilling with such double-pulse is performed in stainless steel samples with different laser fluences, sample's thickness, repetition rates and ambient pressures. The experimental results show that the drilling rates of double-pulse drilling are more than one order of magnitude higher than that of conventional single-pulse drilling in air. Differences in the processing results between single-pulse and double-pulse with various processing parameters are investigated. In addition the ablation mechanisms of the double-pulse drilling are discussed.  相似文献   
35.
Summary If the concentration of elements with Z>22 (Ti) is to be determined in mineral samples and if the concentration of any of these elements is greater than 1%, the sample is diluted by grinding it together with an appropriate amount of quartz powder in an agate mortar mill. The diluted sample is measured in powdered form in a spectro-cup at practically infinite thickness by energy-dispersive X-ray fluorescence; the counting rates are corrected by means of the Compton scattering peak and evaluated by use of calibration curves obtained by measuring standards on the basis of silica gel. The applicability of this method is established by measuring the concentrations of 12 elements with Z>22 in 14 mineral samples of varying composition.We thank the Bundesministerium für Forschung und Technologie for financial support and the Uranerzbergbau GmbH, Bonn, for supplying the mineral samples.  相似文献   
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Ohne Zusammenfassung  相似文献   
37.
Acetate ions are irreversibly oxidized in nonaqueous solutions. The electron transfer reaction is believed to be the rate determining step. Increasing addition of acetic acid which itself is not oxidized shifts the half wave potential towards more positive values. This change is interpreted in terms of the formation of a 1:1 complex between acetate ions and acetic acid. This shift allows to obtain a polarographic wave forDMF in acetic acid-acetate system although the acetate ions on their part give a polarographic wave inDMF.  相似文献   
38.
    
Zusammenfassung Die Emissionsspektrometrie mit Grimmanregungsquelle (GDOS) liefert rationell und einfach zu interpretierende Tiefenprofile. Es können sowohl dünnste Schichten von 2 nm als auch aufgebrachte Metallbeläge bis zu 100 m untersucht werden. Art und Verteilung der Elemente in den Schichten werden innerhalb weniger Minuten nachgewiesen und durch Vergleich mit Standardreferenzmaterialien quantifiziert.Damit stellt die Oberflächenanalytik mittels GDOS ein wichtiges, in vielen Anwendungsfällen unentbehrliches Hilfsmittel bei der Verfahrensentwicklung und Produktcharakterisierung metallischer Werkstoffe dar.
Examples for the characterisation of coated metal surfaces by a GDOS-rapid method
Summary The glow discharge optical spectrometry (GDOS) produces depth profiles in a simple and economical way. Thinnest layers of about 2 nm as well as metal coatings up to 100 m can be analysed. Type and distribution of the elements in coatings are identified and determined within a few minutes by comparing the signals obtained with those of standard reference samples.Hence, the GDOS-surface analysis method proves to be an important and in many cases an undispensable auxiliary means in connection with the improvement of production processes and the characterisation of the metallic products.
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The decay of an excited state by the emission of twoγ-quanta (γ γ-transitions) or two conversion electrons (e e-transitions) or oneγ-quantum and one conversion electron (γ e-transitions) is expected as a second order radiation process. The decay of Ag109m was examined for such events using a special arrangement of two NaJ-scintillation counters in coincidence. The energies of coincident quanta were displayed on the two axes of an “X-Y”-Oscilloscope respectively. For the ratio ofγ γ-transitions to one-quantum transitions an upper limit of\(\frac{{W_{\gamma \gamma } }}{{W_\gamma }} \leqq 1,9 \cdot 10^{ - 5} \) was obtained. Furthermore theγ-spectrum in coincidence withK X-rays was studied. From these measurementse e- andγ e-transition rates can be calculated for the case ofK shell conversion. The results obtained are:
$$\frac{{W_{^e K^e K} }}{{W_\gamma }} = \left( {8,1_{ - 1,7}^{ + 0,6} } \right) \cdot 10^{ - 3} and\frac{{W_{\gamma ^e K} }}{{W_\gamma }}< 1,5 \cdot 10^{ - 3} .$$  相似文献   
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