Flame flickering frequency on a rotating Bunsen burner

The empirical correlation (St^*2/Ri=0.00028Re^*2/3: St^* is the reduced Strouhal number, Ri the Richardson number, Re^* the reduced Reynolds number) proposed by Kostiuk and Cheng [1995. The coupling of conical wrinkled laminar flames with gravity. Combustion and Flame 103, 27-40] for predicting buoyancy-induced flame flickering frequency, has been experimentally investigated under the swirling flow conditions produced by a rotating Bunsen burner, focusing on how the flame flickering frequency changes with increasing swirl number S. Under low swirling conditions up to S≈0.1, the flame flickering frequency f_t did not change and monotonically increased with increasing the bulk flow velocity from the burner tube U. The trend of the data is similar to those obtained by Durox et al. [1995. Some effects of gravity on the behavior of premixed flames. Combustion and Flame 82, 66-74] and Kostiuk and Cheng (1995) and could be fitted well with the empirical correlation Kostiuk and Cheng (1995). However, under high swirling  conditions (S>1), f_t significantly decreased up to ≈80% of that with non-swirling condition, and became insensitive to U. As a result, the data under S>1 could not be correlated by the empirical equation. From results obtained by laser doppler velocimetry (LDV), this inconsistency is due to flow divergence shown by the change in the velocity distribution between the burner exit and the flame tip with burner rotation. A minimum value of the centerline velocity u_j,min between the burner exit and the flame tip fulfills an important role in controlling the flame flickering frequency. The use of this parameter allows the empirical correlation to be extended to the high swirling case by means of a modified empirical correlation St^*2/Ri=0.00028(Re^*exp(-0.64S^1.78))^2/3.     

磁性稀土材料在VM制冷机中的应用

介绍用液氮作中间冷却剂产生１０Ｋ低温的ＶＭ制冷机。介绍了磁性回热材料的选择以及磁性稀土材料在制冷机中的应用与发展。在回热器中用低温下比热值较大的磁性稀土材料Ｅｒ（Ｎｉ０．７９Ｃｏ０．２１）２部分代替铅丸进行试验，无负荷温度降低，在２０Ｋ时间测得制冷量增加，证明了回热器的效率有所提高。     

Moiré interferometry measurements of neartip deformation in inhomogeneous elasticplastic fracture specimens

Moiré interferometry was used for direct measurements of the crack tip behavior in the homogeneous compact tension (CT) specimens of A533B and HT80 steels, and in electron-beam welded inhomogeneous CT specimens of the two materials. These two materials have considerably different yield stresses, although their elastic properties are the same. Five types of homogeneous and inhomogeneous specimens were used in the experiment. Moiré fringe patterns of the five specimen types were directly compared for elastic, elastic-plastic and unloaded stages. Although the global deformations in terms of the load versus COD relations exhibit little inhomogeneity effects, large inhomogeneity effects were observed in the moiré fringe patterns in the elastic-plastic and unloaded stages. The near-tip deformations were also compared with the corresponding HRR singular fields. In a horizontal weld specimen, due to strong hardening in the weld region, the slope of the displacement field does not shift the characteristic HRR field for the A533B or the HT80 steel for increasing load.     

Dynamic J integral, separated dynamic J integral and component separation method for dynamic interfacial cracks in piezoelectric bimaterials

First, the near-tip stress and electric displacement fields are analytically solved for a dynamically propagating interfacial crack in a piezoelectric bimaterial. Second, from the rate formulation of the energy balance in a piezoelectric material, the path independent dynamic J integral is derived, which has the physical significance of the energy release rate. Using the present near-tip analytical solutions, the relationships between the dynamic J integral and the stress and electric displacement intensity factors are also obtained. It is shown that the path independent dynamic J integral contains the static J integral and the dynamic J integral for elastic materials, and static J integral for piezoelectric materials as special cases. Third, for an interfacial crack in a piezoelectric bimaterial, the path independent separated dynamic J integrals are derived, which have the physical significance of energy flow rates into the propagating interfacial crack tip from the individual material sides or, equivalently, the separated dynamic energy release rates. Fourth, to accurately evaluate mixed-mode stress and electric displacement intensity factors, the component separation method of the dynamic J integral is developed. Finally, the finite element analyses of a static stationary interfacial crack in a piezoelectric bimaterial subject to mechanical, electrical and combined loading are carried out to demonstrate the applicability of the generalized (dynamic) J integral and the separated J integral, and the component separation method.     

Mice with focal pulmonary fibrosis caused by monocrotaline are insensitive to urethane induction of lung tumorigenesis

To establish the characteristics of an optimized pulmonary fibrosis model, male ICR mice were given 4 weekly sc injections of 150 or 0 mg/kg monocrotaline (MCT) and maintained without further treatment for 33 wk (Experiment 1). The final mortality in the MCT group was 64%. Epithelial cells with large bizarre nuclei and an increased incidence of alveolar/bronchiolar hyperplasias were typically observed. In areas of pulmonary fibrosis, the PCNA labeling index (LI) in the alveolar/airway epithelium was significantly elevated. DNA content analysis demonstrated a larger range (4-8C) for the ploidy pattern of alveolar epithelium with large bizarre nuclei than in the normal epithelium (2C). In Experiment 2, the relationship between pulmonary fibrosis development and lung tumorigenesis was investigated. Mice were given 4 weekly sc injections of 150 and 0 mg/kg MCT, followed by a single i.p. injection of 1,000 or 500 mg/kg urethane (UR) on week 7, then maintained without further treatment for an additional 15 wk. UR following MCT-induced inflammatory changes, fibrosis, and epithelia with large bizarre nuclei but no tumorous lesions, in spite of the fact that treatment with UR alone caused a high incidence of pulmonary tumors. Hyperplasias were seen in all groups, but the multiplicity in the combined groups tended to be decreased by the MCT pretreatment. The present study demonstrated that this new protocol is more suitable than previous one for the experimental production of pulmonary fibrosis. Furthermore, the induction of lung tumors by UR was completely depressed in mice with MCT-induced pulmonary fibrosis, suggesting that alveolar epithelial cells are resistant to this lung carcinogen under these conditions.     

Ring test of 304 stainless steel tube oxidized in high temperature steam

The residual mechanical strength and ductility of 304 stainless steel claddings were studied in tests of ring compression, ring tension and hardness. The tests were made after the specimens had been heated in steam and in argon gas to temperatures between 900° C and 1350° C. The effects of crystal grain growth and oxygen absorption in the metal on the residual properties were also studied. The experiments showed that the claddings retained their ductility well at temperatures below 1300° C and when the oxide scale thickness was below 40% of the initial wall thickness. The claddings maintained a constant level of residual strength when heated at temperatures over 1000° C or when the oxide thickness was over five percent. These results were used to support our proposals for limits on stainless steel cladding damage in a LOCA.     

Electrical conductivity and thermoelectric power in irradiated UO2 + x

Two kinds of UO_{2 + x}, the O/U ratios of which were 2.002 and 2.004, respectively, were irradiated to a dose range between 1.14 × 10¹⁴ and 1.90 × 10¹⁸ fissions/cm³, and electrical conductivity changes were measured. A steep decrease in conductivity was observed with increasing dose up to 1 × 10¹⁵ fissions/cm³, a gradual increase followed between 1 × 10¹⁵ and 1 × 10¹⁸ fissions/cm³ and above this dose the conductivity abruptly increased. Thermoelectric power measurements were also carried out for the specimens irradiated in the dose range up to 1.90 × 10¹⁸ fissions/cm³. It might be suggested that p-type conduction contributes to the electrical conductivity in irradiated specimens up to 1.90 × 10¹⁸ fissions/cm³.     

Reconstruction of cartilage tissue using scaffold-free organoid culture technique

We applied the scaffold-free culture method to chondrocytes and attempted to reconstitute articular cartilage grafts. Primary rat costal chondrocytes were immobilized into hollow fibers by centrifugation at a density of 3 x 10(8) cells/cm(3) to induce the formation of cylindrical-shaped multicellular aggregates (organoids) and cultured for one month. The organoids were evaluated by histological and gene expression analyses. Chondrocytes formed cylindrical organoids in hollow fibers (HFs). Histochemical analysis revealed the accumulation of a cartilage extracellular matrix (collagen and proteoglycan) around cells in the lumen of HFs with culture time, forming a low-cellular-density tissue similar to native cartilage by day 28. Furthermore, in contrast to that in traditional monolayer culture, the organoid maintained the gene expression of the cartilage extracellular matrix (type II collagen, aggrecan) for one month of culture. In conclusion, our organoid formation method was effective in producing a cartilage-like tissue. This result suggests that the technique may be applicable to the development of an articular cartilage graft.     

Verification of Iron Loss Calculation Method Using a High‐Precision Iron Loss Analyzer

Because of the improved performance of power devices, the volume of the ac filter inductors used in high‐frequency PWM inverters has been reduced. However, the temperature rise in the filter inductor due to this miniaturization has become more pronounced. Therefore, we have proposed an iron loss calculation method for the ac filter inductor. However, the accuracy of the value calculated via the loss map method cannot be verified, because the iron loss arising during each switching period cannot be measured with conventional power measuring instruments. In order to resolve this problem, we developed an inductor loss analyzer (ILA), which allows precise measurement of the iron loss in the inductor during each switching period. The accuracy of the calculation of iron loss in the filter inductor by the loss map method was verified with the ILA. We found that the value calculated by the loss map method differed slightly from the value measured with the ILA. However, these differences can be reduced if we take into account the accurate flux density calculation and the effect of the duty ratio of PWM pulses on the loss. Finally, we verified that the loss map method can provide accurate iron loss calculations.     

Iron Loss Calculation of AC Filter Inductor for Three‐Phase PWM Inverters

In recent years, remarkable advancement of new power semiconductor devices, such as SiC and GaN, enables the increase of switching frequency of power converters, and hence the volume of passive components, such as ac filters and transformers, can be reduced. However, temperature rise caused by the inductor loss is increasing, and hence iron loss evaluation of the inductor is one of the most important issues to realize high power density converters. Conventionally, an improved generalized Steinmetz equation (iGSE) has proposed in order to calculate the iron loss under a pulse voltage magnetizing condition. However, accurate iron loss calculation of the ac filter inductor used in a PWM inverter cannot be realized. The authors have proposed two methods of iron loss evaluation of ac filter inductors. The first one is a loss map method which can calculate the iron loss without using a real PWM inverter. Another one is an ILA (Inductor Loss Analyzer) which can measure the iron loss in every switching period in a real PWM inverter. In this paper, comparisons of the iron loss between the ILA and the loss map method on both the single‐phase and three‐phase inverters are studied. It is found that iron loss of the ac filter inductor in the three‐phase PWM inverter which is calculated by the loss map method cause a large error on a specific condition. In order to prevent the calculation error, the authors proposed a revised loss map method and proved the effectiveness of the method.