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Double T-beams

Common Am Supply. In this case, the preheated air is not individually supplied to each burner but is fed into a plenum chamber which is formed oy the furnace side wall and by additional mounted steel plates between two double-T beams. The burners are completely surrounded by the plenum chamber. [Pg.171]

In planning tank farms, legally required measures must be taken against the propagation of fires and explosions. Tank farms are built in a closed concrete basin that is sufficiently large to accommodate the contents of the largest tank. A minimum distance must be maintained between the individual tanks. Tanks for liquids are often mounted on double-T beams so that they can be inspected from below (Figure 2.6-2). [Pg.190]

Double ring structure with connecting beams, similar to Equisetum hyemale, constructed out of welded double T-beams. [Pg.299]

Zehnder, A.T. and Rosakis, A.J. (1990). Dynamic Fracture Initiation and Propagation in 4340 Steel under Impact Loading, International Journal of Fracture, 43, pp. 271-285. Kalthoff, J.F., Beinert, J. and Winkler, S. (1977). Measurements of Dynamic Stress Intensity Factors for Fast Running and Arresting Cracks in Double-Cantilever-Beam Specimens. n Fast Fracture and Crack Arrest, ASTMSTP 627, pp. 161-176, Hahn, G.T. and Kanninen, M.F. (Eds.). American Society for Testing and Materials. [Pg.185]

Hojo M, Aoki T. Thickness effect of double cantilever beam specimen on interlaminar fracture toughness of AS4/PEEK and T800/epoxy laminates. In Stinchcomb WW, Ashbaugh NE, editors. Composite materials fatigue and fracture, vol. 1156. ASTM Special Technical Publication 1993. pp. 281—98. http //dx.doi.org/10.1520/ STP24736S. [Pg.227]

Secondly, the same rubber-toughened epoxy adhesive as was used for the T-peel tests [45] discussed in Section 3.3 has also been studied [51,57] using a LEFM test specimen, i.e. the standard tapered-double cantilever-beam specimen [58]. At the same rate of test and for the same locus of joint failure, a value of Gc of 2750 100 J/m was determined using the LEFM test, compared with a value 2900 400 J/m from the T-peel tests. Thus, here we have completely different test geometries giving the same value of Gc. So, again, a cross-check indicates the robustness of the above analytical approach for modelling the peel test. [Pg.293]

BSI (1993) Peel test for a flexible bonded-to-rigid test specimen assembly. 180 degree peel. Adhesives, BSI BSI (2001) Determination of the mode 1 adhesive fracture energy, ( o of structural adhesives using the double cantilever beam (DCB) and tapered double cantilever beam (TDCB) specimens. BS 7991 BSI (2005) T-Ped test for flexible-to-flexible bonded assemblies. Adhesives, BSI... [Pg.500]

The frill width at half maximum of the autocorrelation signal, 21 fs, corresponds to a pulse width of 13.5 fs if a sech shape for the l(t) fiinction is assumed. The corresponding output spectrum shown in fignre B2.1.3(T)) exhibits a width at half maximum of approximately 700 cm The time-bandwidth product A i A v is close to 0.3. This result implies that the pulse was compressed nearly to the Heisenberg indetenninacy (or Fourier transfonn) limit [53] by the double-passed prism pair placed in the beam path prior to the autocorrelator. [Pg.1975]

Two identical reaction solutions were prepared, one at T,(= 25.000 °C) in the sample compartment of a double-beam spectrophotometer, the other at T2( = 27.170 °C) in the reference beam. A direct recording of AAbs = Absi - Abs2 was made as a function of time while the difference in reaction temperature was maintained to 0.0001 °C. Evaluate kffk and AW1 for the run shown note this calculation is possible with an arbitrary time axis. [Pg.177]

Page, R. H., Shen, Y. R., and Lee, Y. T. (1988), Local Modes of Benzene and Benzene Dimer, Studied by Infrared-Ultraviolet Double Resonance in a Supersonic Beam, J. Chem. Phys. 88, 4621, 5362. [Pg.232]

The crystal structures of all amphibole minerals, including the asbestiform varieties, are most easily understood as variations on a basic structural unit called an I-beam. The term I-beam alludes to the cross-sectional shape of the three-part structure consisting of corner-linked (Si04) and/or (A104) tetrahedra (T) linked together into a double-tetrahedral chain that sandwiches a layer of edge-shared and R Og octahedra (O). R elements, which... [Pg.35]

The monochromatic X-ray was obtained by silicon (111) channel cut double crystal using white X-ray (at Beam Line 4A (PF)). The ion chambers were set at the both side of the photoacoustic cell, in order to compare the sp trum of photoacoustic X-ray absorption spectroscopy (PAXAS) with usual absorption spectrum, simultaneously. The chopper at chopping frequency of 10 Hz was t at the up-stream of these detectors. Copper foil (5 pm thick) was used as a sample. [Pg.152]

Spectra were obtained with a Perkin-Elmer Model 13 spectrophotometer (double beam) modified to scan and record linearly in frequency [9]. A calibrated LiF prism was used with estimated frequency accuracy rh 4 cm"1. The spectral slit- width was about 9 cm "1 at 3600 cm"1 and 6 cm"1 at 3000 cm 1v Transmission accuracy is estimated at 0 5% in the region 30-50% T, where most measurements were made. The zero and 100% transmission values were measured for each spectrum, and a correction was applied for false energy. [Pg.157]

Figure 10.12—Sequence of events necessary to obtain a pseudo-double beam spectrum with a Fourier transform IR spectrometer. The instrument records and stores in its memory two spectra representing the variation of lu (blank) and / (sample) as a function of wavenumber (emission spectra 1 and 2 above). Then, it calculates the conventional spectrum, which is identical to that obtained on a double beam instrument, by calculating the ratio T — /// — f(A) for each wavenumber. Atmospheric absorption (CO2 and H20) is thus eliminated. The figure illustrates the spectrum of a polystyrene film. Figure 10.12—Sequence of events necessary to obtain a pseudo-double beam spectrum with a Fourier transform IR spectrometer. The instrument records and stores in its memory two spectra representing the variation of lu (blank) and / (sample) as a function of wavenumber (emission spectra 1 and 2 above). Then, it calculates the conventional spectrum, which is identical to that obtained on a double beam instrument, by calculating the ratio T — /// — f(A) for each wavenumber. Atmospheric absorption (CO2 and H20) is thus eliminated. The figure illustrates the spectrum of a polystyrene film.

See other pages where Double T-beams is mentioned: [Pg.298]    [Pg.148]    [Pg.298]    [Pg.298]    [Pg.148]    [Pg.298]    [Pg.24]    [Pg.338]    [Pg.154]    [Pg.786]    [Pg.317]    [Pg.800]    [Pg.297]    [Pg.288]    [Pg.800]    [Pg.65]    [Pg.395]    [Pg.683]    [Pg.521]    [Pg.390]    [Pg.100]    [Pg.423]    [Pg.304]    [Pg.404]    [Pg.169]    [Pg.186]    [Pg.38]    [Pg.35]    [Pg.37]    [Pg.39]    [Pg.84]    [Pg.319]    [Pg.438]    [Pg.384]    [Pg.92]    [Pg.353]   
See also in sourсe #XX -- [ Pg.298 ]

See also in sourсe #XX -- [ Pg.298 ]




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