scholarly journals Origin of precious opal revisited: Possible quick formation of precious opal

Author(s):  
Hiroki Okudera ◽  
Tetsuyoshi Takeda

Abstract It has been well known that a sedimentary precious opal is composed of closely packed uni-size silica spheres with voids filled by an air or water, and that an interference among reflections from the boundaries of those spheres and filler yields play-of-colour (iridescence). So, occurrence of a play-of-colour means occurrence of natural selection in size of spheres, or suppression of further nucleation after initial outburst of spheres, during its formation process. We had been exploring the possibility if we can regard a Stöber process as an analogue of the formation process of precious opal. The key is the reason why variation in size is rarely found on both precious opal and Stöber colloid. To give a clue, we examined the internal structure of Stöber particles and how those particles were formed at very initial stage of the process. The answers for evenness in shape and size are a quick supersaturation of reactive silica species, consecutive formation of large and loose polymers by fast dehydration, and their quick aggregation as the initial burst of silica spheres in highly diffusive medium. These can be achieved in nature by quick but continuous decrease in temperature on “basic” (high pH) geothermal hot water moving upward through cracks in rocks. Sedimentary precious opal can thus be formed when such naturally occurring colloid is filtered by a permeable bed.

1972 ◽  
Vol 1 (13) ◽  
pp. 97
Author(s):  
H.R. Kivisild ◽  
G.D. Ransford

Ice effects on coastal structures, and more particularly the maximum forces caused by ice action, depend on a number of factors, such as:- (a) The physical properties of the ice encountered. (b) The thickness of ice formations. (c) The size of these formations, and their motion. (d) The shape and size of the structures concerned. Past history of ice accumulations is important too, not only in relation to ice properties (as when new ice and multiyear ice are found together at the one location), but also for instance when structures become frozen in, or when ice debris accumulates on sloping faces or when ice bustles form around piers. The very considerable difficulties in carrying out insitu experimental work, not only on the overall effects of interest to engineers such as ice thrust on fixed structures, but also on ice properties themselves, mean that there are still large gaps in our knowledge of the subject. Finally, the non-isotropic nature of the naturally occurring ice, and the broad spectrum of ice behaviour under loading (brittle,ductile or, when creep predominates, viscous), contribute still further to the complexity of the subject.


Author(s):  
Y. yokota ◽  
H. Hashimoto

The initial stage of the reaction process forming the platinum silicide at Pt/Si (111) interfaces have been investigated by a high resolution electron microscope in both “flat-on” [1] and “cross-sectional” mode.First, platinum of 11 nm thickness was deposited on a Si (111) wafer. For observing the specimen in “flat-on” mode, the top surface and edge of the specimen were covered by paraffin and etched chemically using CP-4 reagent from backside. The specimen for observing in “cross-sectional” mode was prepared as follows. The Si wafer was cut into slips of 3mm width. After stacking 4 to 6 slips together with epoxy resin, the stacks were sliced to a thickness of 0.3-0.4mm by a diamond saw. The slices were mechanically polished to a thickness lower than 0.05mm and then thinned by Ar ion beam.The formation process of platinum silicide (PtSi) was observed in a cross-sectional specimen.


2012 ◽  
Vol 49 (No. 4) ◽  
pp. 159-181 ◽  
Author(s):  
J. Urban

The paper deals with the bionomics and harmfulness of a common cecidogenous aphid Tetraneura ulmi L. (Pemphigidae) which showed outbreak in elms in Moravia in 2002. The majority of examinations was conducted in Ulmus minor in a riparian and accompanying stand of the Svitava river, B&iacute;lovice nad Svitavou near Brno. The aphid was most abundant in U. minor, much less in U. glabra and never occurred in U. laevis. In one leaf, about 2.5 (max. 16) galls were found there (at Čejkovice near Znojmo, as much as 21 galls). Fundatrices hatched from 15 April to 7 May. Through the areal sucking on the abaxial face of leaves, they damaged on average 1.4 cm<sup>2</sup> (about 6%) of the leaf blade, in leaves with 10 and more galls often the whole blade. Within 3&ndash;4 weeks from hatching (from mid-May), fundatrices matured and during 1&ndash;3 weeks they produced on average 35.2 fundatrigeniae. At the beginning of June, galls reached 10.8 mm in length and 6.2 mm in width. Fundatrigeniae developed about 18 days and from 10 to 30 June they formed migrantes alatae. Aphids left 73.3% galls. In 10.4% galls, fundatrices were killed by insect and other predators in the 1<sup>st</sup> instar (in the initial stage of the gall formation). In 7.0% galls, immature fundatrices died in later stages of development due to the effect of a protective activity of plant tissues. The mortality of fundatrigeniae including migrantes alatae was caused to a very small extent only by e.g. Anthocoris confusus Reut., larvae of Syrphidae, caterpillars of Pyralidae and birds. Effects of mortality factors on the shape and size differentiation of galls are documented in the paper. &nbsp;


Author(s):  
Eugene J. Amaral ◽  
Robert C. Rau

Replica and transmission electron microscopy have been used to study the microstructure of precious opal. This mineral is an amorphous silica which is often prized as a gemstone because of its vivid display of iridescent colors when viewed in visible light. For the present study, specimens were examined in fractured, polished, and etched conditions.As shown in the figures, precious opal consists of many tiny silica spheres, of essentially uniform diameter, that have been deposited in an orderly array before silica cementation. Regularly spaced interstitial voids resulting from the ordered packing serve as a three dimensional diffraction grating for visible light, thus giving rise to the characteristic play of colors. The separation of the voids is controlled by sphere diameter, and determines the maximum wavelength of visible light diffracted. Thus specimens consisting of larger spheres diffract higher order colors (longer wavelengths) than specimens consisting of smaller spheres. For example, the specimen shown in Fig. 1 contained spheres of approximately 2700 Å diameter and diffracted all visible colors up through red, while the specimen shown in Fig. 2 contained spheres of approximately 2000 Å diameter and diffracted only blues and greens.


2011 ◽  
Vol 183-185 ◽  
pp. 45-49
Author(s):  
Hong Fang Ji ◽  
Ling Wen Zhang ◽  
Hai Yan Zhang ◽  
Ming Duo Yang ◽  
Jian Li

Laoying Tea, leaves of Litsea coreana L., is conventionally consumed as healthy tea beverage in southern China for hundreds of years. The ethanolic, cold water and hot water extracts were prepared and their antioxidant properties studied. At 160 µg/mL, the cold water extract showed a high reducing power of 1.056. With regard to the scavenging ability on 1,1-diphenyl-2-picrylhydrazyl radicals, extracts were effective in the order: ethanolic > cold water > hot water extracts. EC50values for chelating ability on ferrous ions for ethanolic, cold water and hot water extracts were 10.23, 0.85 and 1.12 mg/mL, respectively. Total phenols were the major naturally occurring antioxidant components found and were in the order: cold water > hot water > ethanolic extracts. Based on EC50values, the various extracts from laoying tea were effective antioxidants.


2002 ◽  
Vol 10 (5) ◽  
pp. 5-7
Author(s):  
Ronald W. Smith

In the beginning there was water-the first stain that delineated structure within a polymeric system. The polymerwas natural rubber (NR) and the system was an air-dried film of natural latex. Grenquist reported in 1929 that a dried film of natural rubber latex soaked in hot water became milky (Figure 1) and, at that stage, the latex particles could be detected by the optical microscope (OM), The contrast mechanism was provided by the absorption of water by the naturally occurring proteinaceous layers present on the congealed NR particle surfaces. There was little demand for polymer staining until the age of electron microscopy.


Author(s):  
Chengcheng Li ◽  
Xiaodong Zhang ◽  
Yuxin Guo ◽  
Farzad Seidi ◽  
Xiaotong Shi ◽  
...  

2009 ◽  
Vol 14 (8) ◽  
pp. 1377-1382 ◽  
Author(s):  
Na Wang ◽  
Wendi Zhang ◽  
Jipeng Xu ◽  
Bin Ma ◽  
Zongzhi Zhang ◽  
...  

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