calculated intensity
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2019 ◽  
Vol 4 (1) ◽  
pp. 258-268
Author(s):  
M.O. Lebedev ◽  

The paper examines the construction of a railway tunnel in limestone rock with different degrees of fracture density. As a result of field observations at the test sites, the stress intensity values for framing and lining were obtained. The results of the field observations were compared with the calculated intensity values obtained through an implementation of various methods, as well as with the actual engineering geological construction conditions.


2017 ◽  
Vol 12 (1) ◽  
pp. 57-64
Author(s):  
Peter Kapalo ◽  
Orest Voznyak

Abstract Doing the replacement of old wooden windows in a new plastic windows, in the old buildings, we get the great reducing of the building heat loss. Simpler maintenance and attendance of window is the next advantage. New windows are characterized by better tightness. The aim of the article is determination due to the performed experimental measurements, how much more are reduce the uncontrolled ventilation that is caused of the infiltration windows. In the article there is presented the experimental measurement of indoor air quality in the room in two phases. In the first phase there is the room installed by 55 year old wood window. In the second phase there is the same room installed by new plastic window. Due to the experimental measurement of indoor air quality it is calculated intensity of ventilation - infiltration. These results of ventilation intensity are reciprocally compared.


2006 ◽  
Vol 510-511 ◽  
pp. 118-121
Author(s):  
Titipun Thongtem ◽  
Somchai Thongtem

Li1-xNi1+xO2 powder was prepared by using tartaric acid as a complexing agent. A 1 : 1 : 2 mole ratio of Li : Ni : tartaric acid was used to form carboxylate precursors which were calcined at 650–800 oC for 14–48 h. TGA of the precursors showed that formation of Li1-xNi1+xO2 initiates at 600 oC and above. By using XRD, Li1-xNi1+xO2 with 650–800 oC calcination was detected. Calculated intensity ratios of I(003)/I(104) and I(006+102)/I(101) showed that the best condition is at 750 oC for 34 h. The crystallite size was estimated using the Scherrer equation. AAS and titration techniques showed that Ni3+/(Ni3+ + Ni2+) and mean oxidation state of nickel are 66.50 wt% and 2.67 respectively. EDX showed that the powder was comprised by Ni and O. The faceted particles are shown by SEM. TEM and electron diffraction showed the results that are in accordance with the above.


2003 ◽  
Vol 797 ◽  
Author(s):  
Victor Coello ◽  
Thomas Søndergaard ◽  
Sergey I. Bozhevolnyi

ABSTRACTWe model the operation of a micro-optical interferometer for surface plasmon polaritons (SPPs) that comprises an SPP beam-splitter formed by equivalent scatterers lined up and equally spaced. The numerical calculations are carried out by using a vector dipolar model for multiple SPP scattering. The SPP beam-splitter is simulated for different angles of the incident SPP beam, radii of the particles, and inter-particle distances in order to find a suitable configuration for realization of a 3dB SPP beam-splitter. The results obtained are in good agreement with experimental data available in the literature. The feasibility of fabricating an interferometer is thereby corroborated and the calculated intensity maps are found rather similar to those experimentally reported.


1994 ◽  
Vol 376 ◽  
Author(s):  
Uwe Glatzel ◽  
Andreas MÜller

ABSTRACTNeutron scattering experiments have been carried out with undeformed and creep deformed samples of the superalloy CMSX-4. From the measured constrained misfit data, obtained from different reflecting planes with respect to the external load axis, two strain tensors for horizontal and vertical matrix plates can be extracted.A careful data analysis is necessary since the technical manufactured single crystals show a mosaic spreading of 0.5° and the wavelength spreading of the incident neutron beam, Δλ/λ is about 410-3 This is in the same range as the unknown constrained misfit quantities δc. A method has been developed which allows a calculated intensity distribution to be fitted to the measured one.


1991 ◽  
Vol 95 (8) ◽  
pp. 5556-5564 ◽  
Author(s):  
Henrik G. Kjaergaard ◽  
John D. Goddard ◽  
Bryan R. Henry

1989 ◽  
Vol 43 (5) ◽  
pp. 845-850 ◽  
Author(s):  
Riaz Waris ◽  
Kenneth W. Street ◽  
William E. Acree ◽  
John C. Fetzer

Fluorescence properties of benzo[e]pyrene, benzo[a)pyrene, dibenzo[a,ejpyrene (naphtho[1,2,3,4def]chrysene), 1-chloropyrene, tribenzo[de, kl,rst]pentaphene, dinaphtho[2,1,8,7defg,2′,1,8′,7'ijkl]pentaphene, benz [rst]anthra[9,1,2cde]pentaphene, and dibenzo[fg,ij]phenanthro[2,1,10,9,8,7pqrstuv]pentaphene dissolved in solvents of varying polarity are reported. Measurements indicate that emission intensities of benzo[e)pyrene (BePy) and dibenzophenanthropentaphene (DBPP) depend on solvent polarity. Two new polarity scales are defined, BePy = I/IV and DBPP = I/II, on the basis of the ratio of the fluorescence intensities of select vibronic bands. For fluorescence spectra for the remaining six compounds studied, either the spectra were not clearly resolvable or the calculated intensity ratios remained nearly constant, irrespective of solvent polarity.


1989 ◽  
Vol 4 (1) ◽  
pp. 24-25 ◽  
Author(s):  
G.A. Costa ◽  
M. Ferretti ◽  
M.L. Fornasini ◽  
E.A. Franceschi ◽  
G.L. Olcese

AbstractSince the discovery of the superconductivity in Ba2YCu3 O7-x, the system Ba-Y-Cu-O has generated vast interest. The presence and the properties of the intermediate phases were examined, and the existence of the BaY2O4 phase was confirmed.We have determined the crystal structure of this material from powder data; it is orthorhombic, Pnma (no 62) with a = 10.394(3) Å, b = 3.450(1) Å, c = 12.113(4) Å, isotypic with SrY2O4 (CaFe2O4-type). The observed and calculated intensity values are reported together with the powder diffraction data, obtained both by Guinier and diffractometer methods.


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