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70 75 80 85 90 95 100105110115120 Stack temperaturę, Tgg(°C) Fig. 7. Results obtained for the optimi
Fig. 3. Behavior of CO and C02 conceniration in the stack gases as a function of stoichiometric raii
10 L. Starkel Fig. 3. Areas investigated and surveyed in the project MR 1 — 25: 1 — paleogeographic
6 L. Starkel Fig. I. Ideał model of the organization of research in the national project MR 1 — 25 “
92 Fig. 4. The results table for calculated CCT diagram of a Steel of the following Chemical composi
FIG. 6. GT-MHR double-break air ingress axial profiles: maximumfuel temperaturę (topframe) and graph
reactor cavity (Fig. 4, top frame), resulting m the axial distnbution of maximum fuel temperaturę pe
62 TRIBOLOGIA 3-2015 Rys. 4. Wskaźnik zużycia badanych powłok w temperaturze 20°C i 300°C Fig.
148 H. Tanaka et al. Fig. 2. 8-GeV hybrid lattice dynamie aperture with only random conventional err
152 J. Ohnishi et al. Fig. 3. Cross-sectional view of a newly designed sex-tupole magnet. X(cm) Fig.
310 V. Semeels gee dans la masse metallique (fig. 6). Ueponge est heterogene a cause de la variation
Fig. 6 - Back analysis of the "Cannicella" landslide Fig. 5 - Scarp of the "Cannicell
Fig. 8 - Cross-sections of Orvieto Hill (For legenda see Fig.3) To conclude, the most important stab
0-0 Fig. 1 Le clocher penchć de St. Moritz dćformations qui furent enregistrśes pour la premifcre fo
et al. (1980) for the stability analysis of Palazzo della Ragione, a 13t h Century building in Milan
Fig.l Cross-section of Chedi showing the three stages of construction around boreholes and laborator
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Fig. 4 of Venetian foundations, with its short wooden piles, the wooden raft and the masonry socle&n
Fig. 3 - Panoramie view of the Southern side of Orvieto Hill. The following can be noted in the
Fig. 9. — Panachure d’un grain cle genotypu / Bz W.t Ds pr / C bz wx ds pr par action dc dćlćtion dc
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