Národní úložiště šedé literatury Nalezeno 4 záznamů.  Hledání trvalo 0.01 vteřin. 
Metodika č. 25/01/UTAM19 k nízkonákladovému krytí chránícího zakopané technologické infrastrukturní objekty před účinky kumulativních náloží
Šperl, Martin ; Gajdoš, Lubomír ; Wolf, Benjamin
Metodika popisuje specifický postup krytí zakopaných infrastrukturních prvků. Účelem tohoto postupu je ochrana zakopaných technologií před dynamickým ohrožením z povrchu. Jedná se zejména o položené výbušniny a kumulativní nálože. Hlavní postupy byly vloženy do plynárenského normativního předpisu TPG 70204 - Změna 2.
Metodika měření poklesu rychlosti letících projektilů při průniku různými hmotami pomocí digitálního optomechanického zařízení
Šperl, Martin ; Gajdoš, Lubomír ; Wolf, Benjamin
Metodika popisuje postupy, použitá zařízení a software potřebná k měření průběhu poklesu rychlosti letících projektilů skrz různé sypké i pevné hmoty. Výhoda a unikátnost této metodiky spočívá v schopnosti měření útlumových charakteristik různých materiálů při impaktu projektilem o vysoké rychlosti. Metodika je založena na systému tenkých desek s optickým vláknem, které fungují při průletu střely jako světelné časové brány s definovanou vzájemnou roztečí.
Fracture toughness testing for improving the safety of gas pipeline
Gajdoš, Lubomír ; Šperl, Martin
For standard fracture mechanical tests flat specimens (principally CT or SENB) are required. This brings problems for investigating fracture mechanical properties of thin-walled pipes because it is necessary to straighten the pipe bands [1]. However, this operation causes internal stresses to be induced not only in the semi-product subjected to straightening but also in finished specimens. A question therefore arises to what extent are then the magnitudes of the fracture toughness determined representative for the actual cylindrical wall. To solve this problem fracture mechanics tests were carried out on flat (straightened) CT specimens as well as on curved CT specimens with the natural curvature. The R – curves as well as the resulting parameters of the fracture toughness, obtained for both types of CT specimens, were compared and it was concluded that the fracture toughness of the pipe material determined on straightened CT specimens was practically the same as that obtained on curved CT specimens.
Changes in dislocation substructure of S235JR steel during fatigue loading
Jandová, D. ; Gajdoš, Lubomír ; Šperl, Martin ; Kaiser, J.
Changes in dislocation substructure were studied in normalized and annealed S235JR steel in relation to the number of symmetrical reversed stress cycles with the amplitude σa = 242 MPa and corresponding mean life Nf = 17,950 cycles. The microstructure of the steel consisted of ferrite with a small amount of pearlite. The substructure was observed in as received condition and after application of various relative numbers of cycles n/Nf, these being 0.25, 0.50 and 0.75. An irregular dislocation net occurred in the virgin specimen, however, during cyclic loading the dislocations started to accumulate gradually in slip bands and to form a cell substructure in grains of favourable crystallographic orientations. Total dislocation density, dislocation density in slip bands and inter-band distance were measured using transmission electron microscopy (TEM). The total dislocation density was found to slightly decrease and the density in slip bands to increase with increasing number of cycles. The results concerning the dislocation density were compared with changes in the microplastic limit (MPL) which were determined by the measurement of the inductance of the “specimen - coil” system. They consisted in a rapid initial decrease at the first stage of the fatigue process and in a gradual increase during the major part of the life. These changes can be interpreted on the basis of changes in dislocation density as was verified independently by X-ray diffraction and nanoindentation tests. On the basis of the measurement of dislocation density by TEM it appears that changes in MPL can be connected with the dislocation density in slip bands rather than with the total dislocation density.

Chcete být upozorněni, pokud se objeví nové záznamy odpovídající tomuto dotazu?
Přihlásit se k odběru RSS.