On the theoretical understanding of nanocrystalline soft magnetic materials

Nanocrystalline structures offer a new opportunity for tailoring soft magnetic materials. The most prominent examples are devitrified glassy FeCuNbSiB alloys, which exhibit a homogeneous ultrafine grain structure of bcc FeSi, with grain sizes of typically 10 to 15 nm and random texture. Due to the small grain size, the local magnetocrystalline anisotropy is randomly averaged out by exchange interactions so that there is only a small anisotropy net effect on the magnetization process. Moreover, the structural phases present lead to low or vanishing saturation magnetostriction. Both the suppressed magnetocrystalline anisotropy and the low magnetostriction provide the basis for the superior soft magnetic properties comparable to those of Permalloys or near-zero magnetostrictive Co-base amorphous alloys, but at a higher saturation induction.     

A Printable Optical Time‐Temperature Integrator Based on Shape Memory in a Chiral Nematic Polymer Network

An optical and irreversible temperature sensor (e.g., a time‐temperature integrator) is reported based on a mechanically embossed chiral‐nematic polymer network. The polymer consists of a chemical and a physical (hydrogen‐bonded) network and has a reflection band in the visible wavelength range. The sensors are produced by mechanical embossing at elevated temperatures. A relative large compressive deformation (up to 10%) is obtained inducing a shift to shorter wavelength of the reflection band (>30 nm). After embossing, a temperature sensor is obtained that exhibits an irreversible optical response. A permanent color shift to longer wavelengths (red) is observed upon heating of the polymer material to temperatures above the glass transition temperature. It is illustrated that the observed permanent color shift is related to shape memory in the polymer material. The films can be printed on a foil, thus showing that these sensors are potentially interesting as time‐temperature integrators for applications in food and pharmaceutical products.     

Effects of type IV phosphodiesterase inhibition on cardiac function in the presence and absence of catecholamines

Variations in the density of the fat-free mass (DFFM) across ethnic groups is a critical factor that invalidates the use of body fat equations. It has also been suggested that resistance trained athletes may have higher body densities (BDs) than untrained subjects. Thus, the validity of using anthropometric (ANT) equations, which have mainly been derived on white nonathletic groups, has been questioned for athletic white and black men. This study compared BD and percent body fat (%BF) between 34 white (20 +/- 1 yr, 184 +/- 11 cm, 84 +/- 12 kg, 25 +/- 3 BMI) and 30 black (20 +/- 1 yr, 182 +/- 9 cm, 84 +/- 12 kg, 25 +/- 2 BMI) male collegiate athletes and determined the accuracy of 5 ANT equations in estimating %BF. Subjects were underwater weighed (UWW), and skinfold measurements were obtained from the chest, mid-axillary, abdomen, suprailiac, subscapula, triceps, and thigh. BD was obtained from UWW and estimated from the five skinfold equations. From UWW, significant (P < or = 0.05) differences were found for BD (1.075 +/- 0.007 vs 1.0817 +/- 0.009), but not for %BF (10.49 +/- 2.8 vs 11.59 +/- 3.4) for white and black subjects, respectively. Differences were noted for subcutaneous skinfold sites (abdominal (vertical), suprailiac, and thigh), sum of three and seven skinfolds, and proportion of subscapular subcutaneous fat. One out of five and five out of five ANT equations (Siri conversions) yielded significantly lower estimates compared with UWW %BF for the white and black athletes, respectively. Use of the Schutte equation for the black athletes resulted in overpredictions of %BF for five out of five equations. In addition, the Schutte equation offered slightly greater accuracy than did the Siri equation for estimating %BF in black athletes. These data confirm earlier concerns that ANT equations derived on general populations may not be as accurate for athletic populations and also suggest that correction equations are necessary for converting BD into %BF for populations differing with respect to race or training status.     

Getreide, Getreideerzeugnisse u. dgl.

Ohne Zusammenfassung     

Grain size dependence of coercivity and permeability innanocrystalline ferromagnets

Amorphous ribbons of composition Fe_74.5-xCu_xNb₃Si_13.5B₉ (x=0, 1 at.%) have been annealed between about 500°C and 900°C. This produced a series of crystallized samples with grain sizes between about 10 nm and 300 nm and with coercivities H _c and initial permeabilities μ_i varying over several orders of magnitude. The best soft magnetic properties (H _c≈0.01 A/cm and μ_i≈80×10³ ) were observed for the smallest grain sized of about 10 nm. With increasing grain size D, coercivity steeply increases following a D⁶-power law (up to D≈50 nm). H_c then runs through a maximum of H_c≈30 A/cm and decreases again for grain sizes above 150 nm according to the well-known 1/D law for polycrystalline magnets. The initial permeability was found to vary in a similar manner, essentially being inversely proportional to coercivity. The variation of the soft magnetic properties with the average grain size is discussed and compared with the predictions of the random anisotropy model and other theories for the magnetization reversal     

Role of adenosine in noradrenergic neurotransmission during hemorrhagic hypotension

Glucagon-like peptide-1-(7-36) amide (GLP-1) and glucose-dependent insulinotropic peptide (GIP) are known incretin hormones, released from enteroendocrine cells in response to food, that enhance insulin secretion, but only in the presence of elevated blood glucose. We used a rat insulinoma cell line, RIN 1046-38, to study the mechanisms underlying the interaction of incretins and glucose. We measured insulin secretion using RIA and the reverse hemolytic plaque assay. GLP-1 stimulates insulin secretion, with a half-maximal concentration of 34 pM. GLP-1 is approximately 2 orders of magnitude more potent than GIP. GLP-1 and GIP have additive effects at submaximal concentrations, but probably not at maximal concentrations, suggesting a common signal transduction pathway. The glucose requirement for GLP-1 action can be replaced by cell membrane depolarization (20 mM KCl in the extracellular medium), suggesting that a rise of intracellular Ca2+ may be an early step required for GLP-1 action. GLP-1 stimulates insulin secretion by significantly increasing the maximum rate of insulin secretion from 10.3 +/- 2.25 to 25.2 +/- 2.94 ng insulin/mg protein.h. GLP-1 acts by recruiting 1.5-fold more cells to secrete insulin as well as enhancing insulin secretion by individual cells. Combinations of stimuli, such as glucose, cell membrane depolarization, and GLP-1, can recruit 90% of RIN 1046-38 cells to secrete insulin.     

Experimental study and simulations on two different avalanche modes in trench power MOSFETs

The avalanche behaviour of a new trench power MOSFET was investigated with the help of measurements and electro-thermal device simulation techniques. Two different destruction regimes were identified experimentally: energy-related destruction and current-related destruction. Possible simulation approaches to account for the different effects were proposed. The corresponding results agreed well with measurements. Furthermore, the simulations qualitatively predicted the experimental results' dependence of avalanche behaviour on design parameters.     

Contact Angle Analysis During the Electro‐oxidation of Self‐Assembled Monolayers Formed by n‐Octadecyltrichlorosilane

The electrochemical oxidation process of self‐assembled monolayers formed by n‐octadecyltrichlorosilane (OTS) molecules on silicon wafers has been studied in a droplet of water by means of in situ water contact angle measurements. The application of different bias voltages between the substrate and a counter electrode placed into the droplet resulted in changes of the chemical nature of the monolayer, which yielded a significant alteration of the surfaces properties. Due to the changes of the wetting properties of the monolayer during the electro‐oxidation process a change in the contact angles of the water droplet is concomitantly observed. This allows the in situ monitoring of the electro‐oxidation process for large modified areas of several millimeters in diameter. The chosen approach represents an easy way to screen the major parameters that influence the oxidation process. Afterwards, the oxidized regions are characterized by Fourier‐transform infrared (FT‐IR) spectroscopy, X‐ray photoelectron spectroscopy (XPS) measurements, and atomic force microscopy (AFM) investigations to obtain more information about the electro‐oxidation process. The observations are correlated to experimental results obtained for oxidations performed on a smaller dimension range in the water meniscus of a conductive, biased AFM tip. A good correlation of the results in the different dimension ranges could be found.