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Journal articles on the topic 'Secondary diffusion'

Author: Grafiati

Published: 2 June 2025

Last updated: 31 July 2025

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1

Gundersen, Knut, and Frode Svartdal. "Diffusion of treatment interventions: exploration of ‘secondary’ treatment diffusion." Psychology, Crime & Law 16, no. 3 (2010): 233–49. http://dx.doi.org/10.1080/10683160802612924.

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2

Cook, J. D., and R. E. Showalter. "Microstructure Diffusion Models with Secondary Flux." Journal of Mathematical Analysis and Applications 189, no. 3 (1995): 731–56. http://dx.doi.org/10.1006/jmaa.1995.1048.

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3

Sabioni, Antônio Claret Soares, Anne Marie Huntz, F. Silva, and François Jomard. "Study of Fe Diffusion in Cr₂O₃ by Secondary Ion Mass Spectrometry." Defect and Diffusion Forum 237-240 (April 2005): 940–45. http://dx.doi.org/10.4028/www.scientific.net/ddf.237-240.940.

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Chromia protective layers are used to prevent corrosion by oxidation of many alloys, such as the stainless steels, for instance. To check if chromia is a barrier to the outward diffusion of iron in these alloys, iron diffusion in chromia was studied in both polycrystals and oxide films formed by oxidation of Ni-30Cr alloy in the temperature range 700-1100°C at an oxygen pressure equal to 10-4 atm. An iron film of about 70 nm thick was deposited on the chromia surface, and after the diffusing treatment, the iron depth profiles were established by secondary ion mass spectrometry (SIMS). Using a

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4

Mesarovic, Sinisa Dj. "Lattice continuum and diffusional creep." Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences 472, no. 2188 (2016): 20160039. http://dx.doi.org/10.1098/rspa.2016.0039.

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Diffusional creep is characterized by growth/disappearance of lattice planes at the crystal boundaries that serve as sources/sinks of vacancies, and by diffusion of vacancies. The lattice continuum theory developed here represents a natural and intuitive framework for the analysis of diffusion in crystals and lattice growth/loss at the boundaries. The formulation includes the definition of the Lagrangian reference configuration for the newly created lattice, the transport theorem and the definition of the creep rate tensor for a polycrystal as a piecewise uniform, discontinuous field. The valu

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5

LOH, S. W., D. H. ZHANG, C. Y. LI, R. LIU, and A. T. S. WEE. "STUDY OF COPPER DIFFUSION INTO TANTALUM AND TANTALUM DIFFUSION INTO COPPER." International Journal of Modern Physics B 16, no. 01n02 (2002): 100–107. http://dx.doi.org/10.1142/s0217979202009512.

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We have carried out direct diffusion measurements of Cu into Ta and Ta into Cu. Thin films of 50nm thickness of Cu were grown onto a thick Ta layer of 1 μm by Ionized Metal Plasma. Samples were annealed in a rapid thermal system from temperatures ranging from 400°C to 800°C for periods of 60s and 180s. The diffusion profile was performed using Secondary ion mass spectroscopy. The Cu diffusion coefficients in Ta can be described by 3.0246 × 10-15 exp(-0.1747eV/kT) at 60s and 2.7532 × 10-15 exp(-0.1737eV/kT) at 180s. The Ta diffusion coefficients in Cu can be described by 2.7532 × 10-15 exp(-0.1

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6

Caccavale, F., F. Segato, I. Mansour, J. M. Almeida, and A. P. Leite. "Secondary ion mass spectrometry study of erbium diffusion in lithium niobate crystals." Journal of Materials Research 13, no. 6 (1998): 1672–78. http://dx.doi.org/10.1557/jmr.1998.0231.

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A systematic investigation of erbium diffusion in lithium niobate (LiNbO3) crystal as a function of crystal cut-direction, diffusion process parameters (temperature and time), and initial film thickness is reported. Depth concentration profiles of erbium are obtained by secondary ion mass spectrometry (SIMS). Combining experimental data with diffusion theory, the relevant diffusion parameters are derived. Diffusion from an infinite source of erbium ions is studied to evaluate the solid solubility lower limit of Er in LiNbO3. A thin film diffusion regime, with complete depletion of ion source,

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Schmitz, Anke, and Steven F. Perry. "Bimodal breathing in jumping spiders: morphometric partitioning of the lungs and tracheae in Salticus scenicus (Arachnida, Araneae, Salticidae)." Journal of Experimental Biology 204, no. 24 (2001): 4321–34. http://dx.doi.org/10.1242/jeb.204.24.4321.

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SUMMARY In jumping spiders, both the book lungs and the tracheal system are well-developed. The tracheal system consists of four thick primary tracheae that branch into small secondary tracheae, some of them ending in the opisthosoma and others entering the prosoma. We used stereological morphometric methods to investigate the morphological diffusing capacity of the lungs and of the walls of the secondary tracheae (‘lateral diffusing capacity’) of two groups of Salticus scenicus with mean body masses of 2.69 mg (group A) and 5.28 mg (group B). The thickness of the gas-exchange epithelium of th

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8

De Souza, Roger A., and Manfred Martin. "Probing Diffusion Kinetics with Secondary Ion Mass Spectrometry." MRS Bulletin 34, no. 12 (2009): 907–14. http://dx.doi.org/10.1557/mrs2009.212.

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AbstractSecondary ion mass spectrometry (SIMS) is a powerful analytical technique for determining elemental and isotopic distributions in solids. One of its main attractions to researchers in the field of solid-state ionics is its ability to distinguish between isotopes of the same chemical element as a function of position in a solid. With enriched stable isotopes as diffusion sources, this allows self-diffusion kinetics in solids to be studied. In this article, taking oxygen isotope diffusion in oxides as our main example, we present the standard experimental method, and, subsequently, we di

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9

Elaiw, A. M., and A. S. Alofi. "Global Dynamics of Secondary DENV Infection with Diffusion." Journal of Mathematics 2021 (June 28, 2021): 1–17. http://dx.doi.org/10.1155/2021/5585175.

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During the past eras, many mathematicians have paid their attentions to model the dynamics of dengue virus (DENV) infection but without taking into account the mobility of the cells and DENV particles. In this study, we develop and investigate a partial differential equations (PDEs) model that describes the dynamics of secondary DENV infection taking into account the spatial mobility of DENV particles and cells. The model includes five nonlinear PDEs describing the interaction among the target cells, DENV-infected cells, DENV particles, heterologous antibodies, and homologous antibodies. In th

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10

Rudraiah, N., M. Venkatachalappa, and Sujit Kumar Khan. "Atmospheric diffusion model of secondary pollutants with settling." International Journal of Environmental Studies 52, no. 1-4 (1997): 243–67. http://dx.doi.org/10.1080/00207239708711105.

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11

Mashelkar, R. A., and C. V. Venkatasubramanian. "Influence of secondary flow on diffusion with reaction." AIChE Journal 31, no. 3 (1985): 440–49. http://dx.doi.org/10.1002/aic.690310311.

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12

Kappl, Rolf, and Annika Reinert. "Secondary cosmic positrons in an inhomogeneous diffusion model." Physics of the Dark Universe 16 (June 2017): 71–80. http://dx.doi.org/10.1016/j.dark.2017.04.007.

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13

Dybkov, Vasil I. "Interfacial Interaction and Diffusion in Binary Systems." Defect and Diffusion Forum 263 (March 2007): 75–80. http://dx.doi.org/10.4028/www.scientific.net/ddf.263.75.

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A physico-chemical consideration of the interfacial interaction and diffusion resulting in the formation of chemical compound layers at the interface of initial substances A and B is presented. The layer-growth kinetics is shown to be much more complicated than it follows from conventional diffusional views neglecting interfacial reactions. In the majority of multiphase binary systems, layer occurrence appears to be sequential rather than simultaneous. Under conditions of diffusion control, the number of simultaneously growing compound layers at the A–B interface cannot exceed two. Multiple la

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14

Zhang, Bin, Peng Liu, Yi Wu, et al. "Experimental Study on Grouting Diffusion Law of Tunnel Secondary Lining Cracks Based on Different Slurry Viscosities." Applied Sciences 15, no. 4 (2025): 1955. https://doi.org/10.3390/app15041955.

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To investigate the diffusion law of ultrafine cement slurry (UCS) with different water–cement ratios in tunnel second lining cracks during grouting, the grouting of ultrafine cement slurry with different water–cement ratios was carried out by experimental and theoretical analysis methods in this study. Through the collection and data analysis grouting experiment of the diffusion time history, the diffusion morphological characteristics based on different slurry viscosities were obtained, which were divided into three grouting diffusion patterns: circular diffusion zone, excessive diffusion zon

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15

Linnarsson, Margareta K., and Anders Hallén. "Diffusion of Alkali Metals in SiC." Materials Science Forum 778-780 (February 2014): 297–300. http://dx.doi.org/10.4028/www.scientific.net/msf.778-780.297.

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Diffusion of lithium, sodium and potassium in SiC has been studied by secondary ion mass spectrometry. The alkali metal diffusion sources have been introduced by ion implantation. Subsequent anneals have been carried out in vacuum or in Ar atmosphere in the temperature range 700 °C - 1500 °C for 5 min to 16 h. The bombardment-induced defects in the vicinity of the ion implanted profile are readily decorated by the implanted . In the bulk, the diffusing alkali metals are most likely trapped and detrapped at boron and/or other defects during diffusion. The diffusivity of the studied alkali metal

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16

Norris, G., and R. G. Dominy. "Diffusion rate influences on inter-turbine diffusers." Proceedings of the Institution of Mechanical Engineers, Part A: Journal of Power and Energy 211, no. 3 (1997): 235–42. http://dx.doi.org/10.1243/0957650971537141.

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Inter-turbine diffusers are becoming of increasing importance to the aero gas turbine designer to diffuse the flow between the HP (high-pressure) or IP (intermediate-pressure) turbine and the LP (low-pressure) turbine. Diffusing the flow upstream of the LP turbine and raising the mean passage radius increases stage efficiency. These inter-turbine diffusers, which have high curvature, S-shaped geometry and low-energy wakes created by the upstream turbine, together give rise to secondary flows, making the flow fully three-dimensional. Using both experimental measurements and CFD (computational f

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17

Hollingshead, Joshua M., Makayla L. L. Ianuzzi, Alexandra C. Risha, Jeffrey D. Moore, and Grant A. Risha. "Influence of Annular Flow Area and a 30-Degree Impingement Angle on Methane/Oxygen Diffusion Flame Stability." Methane 4, no. 3 (2025): 16. https://doi.org/10.3390/methane4030016.

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This work examined the effects of secondary annular flow area on flame stability in an experimental diffusion flame burner. The burner was composed of a horizontally mounted, rectangular chamber that utilized a retractable spark plug for ignition and an inverse coaxial injector. The primary and secondary gaseous reactants were oxygen and methane, respectively. Three injectors were assessed to have a fixed primary flow area and secondary flow impingement angle of 30 degrees with the primary flow and distinct secondary annular flow areas. Resultant flames and flame standoff distances were record

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18

Ye, Qing, Ellis Shipley Robinson, Xiang Ding, Penglin Ye, Ryan C. Sullivan, and Neil M. Donahue. "Mixing of secondary organic aerosols versus relative humidity." Proceedings of the National Academy of Sciences 113, no. 45 (2016): 12649–54. http://dx.doi.org/10.1073/pnas.1604536113.

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Atmospheric aerosols exert a substantial influence on climate, ecosystems, visibility, and human health. Although secondary organic aerosols (SOA) dominate fine-particle mass, they comprise myriad compounds with uncertain sources, chemistry, and interactions. SOA formation involves absorption of vapors into particles, either because gas-phase chemistry produces low-volatility or semivolatile products that partition into particles or because more-volatile organics enter particles and react to form lower-volatility products. Thus, SOA formation involves both production of low-volatility compound

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19

Chaus, Alexander S., and F. I. Rudnickii. "Diffusion and Secondary Carbide Precipitation in High-Speed Steels." Defect and Diffusion Forum 297-301 (April 2010): 1071–76. http://dx.doi.org/10.4028/www.scientific.net/ddf.297-301.1071.

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Besides primary carbides, so-called secondary carbides are usually observed in high-speed steel (HSS) microstructure, which precipitate from the oversaturated solid solution upon its cooling. Some of the secondary carbides precipitate from an oversaturated austenite at cooling during solidification or quenching, in both cases, in the form of the relatively big particles in the bulk of a matrix. Considerably finer secondary carbides precipitate in martensitic condition during tempering inducing secondary hardening in HSSs. In general, secondary carbides of both types have obvious effect on the

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20

Sauret, E., and I. Vallet. "Near-Wall Turbulent Pressure Diffusion Modeling and Influence in Three-Dimensional Secondary Flows." Journal of Fluids Engineering 129, no. 5 (2006): 634–42. http://dx.doi.org/10.1115/1.2723811.

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The purpose of this paper is to develop a second-moment closure with a near-wall turbulent pressure diffusion model for three-dimensional complex flows, and to evaluate the influence of the turbulent diffusion term on the prediction of detached and secondary flows. A complete turbulent diffusion model including a near-wall turbulent pressure diffusion closure for the slow part was developed based on the tensorial form of Lumley and included in a re-calibrated wall-normal-free Reynolds-stress model developed by Gerolymos and Vallet. The proposed model was validated against several one-, two, an

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21

Romanchenko, V. "Character of formation of secondary protective structures during operation of parts in friction." Problems of tribology 97, no. 3 (2020): 19–24. http://dx.doi.org/10.31891/2079-1372-2020-97-3-19-24.

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The structure and nature of the formation of secondary protective structures during the operation of parts in an oxidizing environment are considered. It has been established that the stability of film coatings in operation depends on the material of the main part and the development of diffusion processes with the formation of various phases and their interactions. Based on comprehensive studies using the optical-mathematical method for the description of phases and their combinations, the development of diffusion processes during friction, the possibility of predicting the formation of more

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22

Uematsu, Masashi, Marika Gunji, and Kohei M. Itoh. "Oxygen Self-Diffusion in Silicon Dioxide: Effect of the Si/SiO₂ Interface." Defect and Diffusion Forum 258-260 (October 2006): 554–61. http://dx.doi.org/10.4028/www.scientific.net/ddf.258-260.554.

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The effect of the SiO2/Si interface on oxygen self-diffusion in SiO2 during thermal oxidation was investigated using oxygen isotopes. A Si18O2 layer was first grown in 18O2 and then the sample was reoxidized in 16O2 at 900 ~ 1100 °C. The O diffusion in SiO2 during the 16O2 oxidation was investigated by secondary ion mass spectrometry (SIMS) measurements. Near the SiO2/Si interface, a significant broadening of the 18O profile toward the newly grown Si16O2 was observed. This 18O diffusion became slower with oxidation time and hence with increasing distance between 18O diffusion region and the in

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23

Venables, David, and Dennis M. Maher. "Doping-induced contrast in secondary electron images of silicon." Proceedings, annual meeting, Electron Microscopy Society of America 52 (1994): 1024–25. http://dx.doi.org/10.1017/s0424820100172851.

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As device dimensions in integrated circuits continue to decrease to dimensions on the order of 0. 1μm, obtaining two dimensional maps of the dopant distribution becomes increasingly important. In particular, process simulators attempt to predict the extent of both lateral and vertical diffusion of the dopants. However, experimental information on lateral diffusion has been difficult to obtain, although a variety of techniques based on microscopic and electrical data have been attempted. Recently, Perovic et al. showed that direct secondary electron (SE) images of n-i-p-i superlattice structure

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24

María Castellano, José. "Secondary education and broadband diffusion: a qualitative comparative analysis." info 12, no. 6 (2010): 121–38. http://dx.doi.org/10.1108/14636691011086080.

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25

Paulussen, Theo, Gerjo Kok, Herman Schaalma, and Guy S. Parcel. "Diffusion of AIDS Curricula Among Dutch Secondary School Teachers." Health Education Quarterly 22, no. 2 (1995): 227–43. http://dx.doi.org/10.1177/109019819502200210.

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26

Balasubramanian, Vidhya, Girija Jayaraman, and S. R. K. Iyengar. "Influence of secondary flow on diffusion with heterogeneous reaction." Chemical Engineering Journal 92, no. 1-3 (2003): 15–26. http://dx.doi.org/10.1016/s1385-8947(02)00085-2.

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27

Takeda, Sahori, Yuria Saito, and Hideya Yoshitake. "Restricted Diffusion of Lithium Ions in Lithium Secondary Batteries." Journal of Physical Chemistry C 124, no. 47 (2020): 25712–20. http://dx.doi.org/10.1021/acs.jpcc.0c07693.

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28

Czyżewski, Z., and D. C. Joy. "Calculation of secondary electron production using a diffusion matrix." Scanning 13, no. 3 (1991): 227–32. http://dx.doi.org/10.1002/sca.4950130304.

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29

Cosenza, Philippe, and Dean Korošak. "Secondary consolidation of clay as an anomalous diffusion process." International Journal for Numerical and Analytical Methods in Geomechanics 38, no. 12 (2014): 1231–46. http://dx.doi.org/10.1002/nag.2256.

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30

Kavanagh, L., and Charles W. Magee. "Diffusion of Ge in GaAs at SiO2-encapsulated Ge–GaAs interfaces." Canadian Journal of Physics 65, no. 8 (1987): 987–90. http://dx.doi.org/10.1139/p87-157.

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The diffusion of Ge in semi-insulating GaAs was investigated for annealing temperatures in the range 650–800 °C. The samples consisted of electron-beam or metalorganic chemical-vapour deposition deposited Ge–GaAs interfaces encapsulated with SiO2. Ge diffusion profiles, measured with secondary-ion mass spectroscopy (SIMS), had a characteristic plateau and steep slope at the diffusion front, similar to those obtained for Si and Sn diffusion at SiO2-encapsulated GaAs. A saturated-surface concentration of 2 × 1019 atoms∙cm−3 was observed for anneals above 750 °C, likely the solid solubility of Ge

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31

Wisler, D. C., R. C. Bauer, and T. H. Okiishi. "Secondary Flow, Turbulent Diffusion, and Mixing in Axial-Flow Compressors." Journal of Turbomachinery 109, no. 4 (1987): 455–69. http://dx.doi.org/10.1115/1.3262127.

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The relative importance of convection by secondary flows and diffusion by turbulence as mechanisms responsible for mixing in multistage, axial-flow compressors has been investigated by using the ethylene tracer-gas technique and hot-wire anemometry. The tests were conducted at two loading levels in a large, low-speed, four-stage compressor. The experimental results show that considerable cross-passage and spanwise fluid motion can occur and that both secondary flow and turbulent diffusion can play important roles in the mixing process, depending upon location in the compressor and loading leve

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32

Uematsu, Masashi, Kenzo Ibano, and Kohei M. Itoh. "Effect of the SiO₂/Si Interface on Self-Diffusion in SiO₂ Upon Oxidation." Defect and Diffusion Forum 273-276 (February 2008): 685–92. http://dx.doi.org/10.4028/www.scientific.net/ddf.273-276.685.

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The effect of the SiO2/Si interface on Si self-diffusion in SiO2 during thermal oxidation was investigated using silicon isotopes. Samples with natSiO2/28Si heterostructures were oxidized at 1150 ~ 1250 °C and the 30Si diffusion in 28SiO2 during the thermal oxidation was investigated by secondary ion mass spectrometry (SIMS) measurements. Near the SiO2/Si interface, a significant profile broadening of the 30Si isotope from natSiO2 toward the newly grown 28SiO2 was observed. This 30Si self-diffusivity sharply decreases with oxidation time and hence with increasing distance between 30Si diffusio

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33

Chattopadhyay, A.K., B. Kundu, S.K. Nath, and Elias Aifantis. "Transmissibility in Interactive Nanocomposite Diffusion: The Nonlinear Double-Diffusion Model." Frontiers in Applied Mathematics and Statistics 8 (June 3, 2022): 852040. https://doi.org/10.3389/fams.2022.852040.

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Model analogies and exchange of ideas between physics or chemistry with biology or epidemiology have often involved inter-sectoral mapping of techniques. Material mechanics has benefitted hugely from such interpolations from mathematical physics where dislocation patterning of platstically deformed metals and mass transport in nanocomposite materials with high diffusivity paths such as dislocation and grain boundaries, have been traditionally analyzed using the paradigmatic Walgraef-Aifantis (W-A) double-diffusivity (D-D) model. A long standing challenge in these studi

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34

Funazukuri, Toshitaka, Chang Yi Kong, and Seiichiro Kagei. "Correction of the secondary flow effect for binary diffusion coefficients using coated/uncoated diffusion columns." Chemical Engineering Science 59, no. 14 (2004): 3029–36. http://dx.doi.org/10.1016/j.ces.2004.03.033.

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35

Beke, Dezső L., A. Lakatos, G. Erdélyi, et al. "Investigation of Grain Boundary Diffusion in Thin Films by SNMS Technique." Defect and Diffusion Forum 312-315 (April 2011): 1208–15. http://dx.doi.org/10.4028/www.scientific.net/ddf.312-315.1208.

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It was shown more recently in our Laboratory [1,2,3] that having a substrate/diffusant/thin-film/cap-layer structure (the thin film was typically several 10 nm thick, with the same order of magnitude of grain size; the refractory metal cap layer was used just to avoid the oxidation), first the diffusant atoms migrated very fast across the thin film and segregated at the film/cap-layer interface. The accumulated atoms at the film/cap layer interface form a secondary diffusion reservoir and atoms diffuse back to the layer. Later on, the thin film was gradually filled up with the diffusing atoms

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Price, Hannah C., Johan Mattsson, Yue Zhang та ін. "Water diffusion in atmospherically relevant α-pinene secondary organic material". Chemical Science 6, № 8 (2015): 4876–83. http://dx.doi.org/10.1039/c5sc00685f.

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Slavova, Miglena, Elena Mihaylova-Dimitrova, Emiliya Mladenova, Borislav Abrashev, Blagoy Burdin, and Daria Vladikova. "Zeolite based gas-diffusion electrodes for secondary metal air batteries." Journal of Electrochemical Science and Engineering 10, no. 2 (2020): 229–34. http://dx.doi.org/10.5599/jese.763.

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In recent years, secondary metal air batteries have received considerable attention as promising technology for energy storage in combination with renewable energy sources. The oxidation of carbon in conventional gas-diffusion electrodes reduces the life of the secondary metal-air batteries. Replacement of the carbon-based material with zeolite is a possible solution for overcoming this problem which is the aim of this work.Zeolite is a natural or synthetic porous material which provides the necessary gas permeability. The required hydrophobicity of the electrodes is ensured by mixing the zeol

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Watanabe, Ken, Tetsuya Kida, Isao Sakaguchi, Naoki Ohashi, Kengo Shimanoe, and Hajime Haneda. "Effect of Annealing Atmosphere on Oxygen Diffusion through Ba-Fe-Based Perovskite Oxide." Key Engineering Materials 485 (July 2011): 141–44. http://dx.doi.org/10.4028/www.scientific.net/kem.485.141.

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To determine the effect of the annealing atmosphere on oxygen diffusion through Ba0.95La0.05FeO3-d pellets, 18O2 tracer diffusion and high-resolution secondary ion mapping were performed. When annealing in air, the 18O concentration around the surface up to a depth of 40 µm was almost constant. On the other hand, when annealing in vacuum, the 18O concentration obviously decreased. High-resolution secondary ion mapping indicated that the 18O concentration around the grain boundary was reduced. These results suggested that the grain boundary of BLF annealed in vacuum prevents oxygen diffusion.

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39

Zhong, Hua, Bao Ping Sun, and Fang Ying Zhao. "A Preliminary Bioinformatics Analysis of Cation Diffusion Facilitator (CDF) Proteins in Different Plants." Advanced Materials Research 282-283 (July 2011): 453–56. http://dx.doi.org/10.4028/www.scientific.net/amr.282-283.453.

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The amino acid sequence of Cation Diffusion Facilitator from Populus trichocarpa, Thlaspi goesingense, Arabidopsis lyrata subsp. Lyrata, Brassica juncea and Medicago sativa, registered in GenBank, were analyzed and researched by the bioinformatic tools in the several aspects, including hydrophobicity / hydrophilicity properties, post-translational modification, secondary structures prediction and transmembrane domain. The results showed that Cation Diffusion Facilitator is a hydrophobic and transmembrane protein, which exists in endoplasmic reticulum and other secretory pathway. The main motif

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40

Hong, Su-Been, Thai-Thanh Nguyen, Jinhong Jeon, and Hak-Man Kim. "Distributed Operation of Microgrids Considering Secondary Frequency Restoration Based on the Diffusion Algorithm." Energies 13, no. 12 (2020): 3207. http://dx.doi.org/10.3390/en13123207.

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This paper proposes a distributed control of the microgrid (MG) system based on the diffusion algorithm. Unlike the existing decentralized strategy that focuses on the economic operation of the MG system, the proposed strategy performs secondary frequency regulation in addition to the optimization of the MG system. The hierarchical control technique is employed in this study, where the primary layer is responsible for power control and the secondary layer is responsible for the frequency control and economic operation of the MG system. A tested MG system with four distributed generations (DGs)

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Chabriat, Hugues, Nicolas Molko, Sabina Pappata, et al. "Thalamic microstructural alterations secondary to white-matter damage in CADASIL: evidence from diffusion tensor imaging study." Stroke 32, suppl_1 (2001): 342. http://dx.doi.org/10.1161/str.32.suppl_1.342-a.

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P18 Background and Purpose: Variable microstructural changes have been reported within the white-matter in CADASIL. Lacunar infarcts are frequently observed in the subcortical grey matter. However, whether microstructural tissular alterations are also present within the non-infarcted putamen (NIP) or thalamus (NIT), remains unknown. Methods: We used diffusion tensor imaging, a MRI method highly sensitive to the cerebral microstructure, in 20 CADASIL patients and 12 age-matched controls. Both Trace(D) and anisotropy (volume-ratio index) of diffusion were measured within the NIP and NIT. In addi

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42

Larsson, Rolf. "Lateral Mixing in Channels due to Secondary Currents." Hydrology Research 17, no. 4-5 (1986): 391–98. http://dx.doi.org/10.2166/nh.1986.0030.

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Different mechanisms generating secondary currents in channels are presented. It is shown by an order-of-magnitude analysis that secondary currents of magnitude 1% of the downstream velocity are as important for lateral mixing as turbulent diffusion. Results from numerical simulations that support the analysis are presented.

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Devakirubai, Dr MS Jaslyn, and Dr N. Murali. "Role of diffusion tensor imaging and diffusion metrics in primary, secondary brain tumours and tumour mimics." International Journal of Radiology and Diagnostic Imaging 3, no. 4 (2020): 11–15. http://dx.doi.org/10.33545/26644436.2020.v3.i4a.129.

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44

van Rens, Lisette, Joop van der Schee, and Albert Pilot. "Teaching Molecular Diffusion Using an Inquiry Approach. Diffusion Activities in a Secondary School Inquiry-Learning Community." Journal of Chemical Education 86, no. 12 (2009): 1437. http://dx.doi.org/10.1021/ed086p1437.

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Takachi, Masamitsu, Yuya Fukuzumi, and Yutaka Moritomo. "Na+ diffusion kinetics in nanoporous metal-hexacyanoferrates." Dalton Transactions 45, no. 2 (2016): 458–61. http://dx.doi.org/10.1039/c5dt03276h.

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Odom, Arthur Louis. "Secondary & College Biology Students' Misconceptions about Diffusion & Osmosis." American Biology Teacher 57, no. 7 (1995): 409–15. http://dx.doi.org/10.2307/4450030.

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Giorgiutti, F., L. Limat, and J. Wesfreid. "Phase diffusion in the vicinity of an oscillatory secondary bifurcation." Physical Review E 57, no. 3 (1998): 2843–48. http://dx.doi.org/10.1103/physreve.57.2843.

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Whitlow, S. J., and R. P. Wool. "Investigation of diffusion in polystyrene using secondary ion mass spectroscopy." Macromolecules 22, no. 6 (1989): 2648–52. http://dx.doi.org/10.1021/ma00196a019.

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Segalman, Rachel A., Aaron Jacobson, Edward J. Kramer, and Steven R. Lustig. "Polymer Diffusion in Semicrystalline Polymers Using Secondary Ion Mass Spectroscopy." Macromolecules 37, no. 7 (2004): 2613–17. http://dx.doi.org/10.1021/ma035705a.

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Abramson, Evan, Dan Imre, Josef Beránek, Jacqueline Wilson, and Alla Zelenyuk. "Experimental determination of chemical diffusion within secondary organic aerosol particles." Physical Chemistry Chemical Physics 15, no. 8 (2013): 2983. http://dx.doi.org/10.1039/c2cp44013j.

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