288 research outputs found
Thermal Conversion of Guanylurea Dicyanamide into Graphitic Carbon Nitride via Prototype CNx Precursors
Guanylurea dicyanamide, [(H2N)C(-O)NHC(NH2)2][N(CN)2], has been synthesized by ion exchange reaction in aqueous solution and structurally characterized by single-crystal X-ray diffraction (C2/c, a = 2249.0(5) pm, b = 483.9(1) pm, c = 1382.4(3) pm, β = 99.49(3)°, V = 1483.8(5) × 106 pm3, T = 130 K). The thermal behavior of the molecular salt has been studied by thermal analysis, temperature-programmed X-ray powder diffraction, FTIR spectroscopy, and mass spectrometry between room temperature and 823 K. The results were interpreted on a molecular level in terms of a sequence of thermally induced addition, cyclization, and elimination reactions. As a consequence, melamine (2,4,6-triamino-1,3,5-triazine) is formed with concomitant loss of HNCO. Further condensation of melamine yields the prototypic CNx precursor melem (2,6,10-triamino-s-heptazine, C6N7(NH2)3), which alongside varying amounts of directly formed CNxHy material transforms into layered CNxHy phases without significant integration of oxygen into the core framework owing to the evaporation of HNCO. Thus, further evidence can be added to melamine and its condensation product melem acting as “key intermediates” in the synthetic pathway toward graphitic CNxHy materials, whose exact constitution is still a point at issue. Due to the characteristic formation process and hydrogen content a close relationship with the polymer melon is evident. In particular, the thermal transformation of guanylurea dicyanamide clearly demonstrates that the formation of volatile compounds such as HNCO during thermal decomposition may render a large variety of previously not considered molecular compounds suitable CNx precursors despite the presence of oxygen in the starting material
Conventional methods fail to measure cp(omega) of glass-forming liquids
The specific heat is frequency dependent in highly viscous liquids. By
solving the full one-dimensional thermo-viscoelastic problem analytically it is
shown that, because of thermal expansion and the fact that mechanical stresses
relax on the same time scale as the enthalpy relaxes, the plane thermal-wave
method does not measure the isobaric frequency-dependent specific heat
c_p(omega). This method rather measures a "longitudinal" frequency-dependent
specific heat, a quantity defined and detailed here that is in-between
c_p(omega) and c_v(omega). This result means that no wide-frequency
measurements of c_p(omega) on liquids approaching the calorimetric glass
transition exist. We briefly discuss consequences for experiment
Thermal Diffusion and Quench Propagation in YBCO Pancake Coils Wound with ZnO-and Mylar Insulations
The thermal diffusion properties of several different kinds of YBCO
insulations and the quench properties of pancake coils made using these
insulations were studied. Insulations investigated include Nomex, Kapton, and
Mylar, as well as insulations based on ZnO, Zn2GeO4, and ZnO-Cu. Initially,
short stacks of YBCO conductors with interlayer insulation, epoxy, and a
central heater strip were made and later measured for thermal conductivity in
liquid nitrogen. Subsequently, three different pancake coils were made. The
first two were smaller, each using one meter total of YBCO tape present as four
turns around a G-10 former. One of these smaller coils used Mylar insulation
co-wound with the YBCO tape, the other used YBCO tape onto which ZnO based
insulation had been deposited. One larger coil was made which used 12 total
meters of ZnO-insulated tape and had 45 turns. The results for all short sample
and coil thermal conductivities were ~1-3 Wm-1K-1. Finally, quench propagation
velocity measurements were performed on the coils (77 K, self field) by
applying a DC current and then using a heater pulse to initiate a quench.
Normal zone propagation velocity (NZP) values were obtained for the coils both
in the radial direction and in the azimuthal direction. Radial NZP values
(0.05-0.7 mm/s) were two orders of magnitude lower than axial values (~14-17
mm/s). Nevertheless, the quenches were generally seen to propagate radially
within the coils, in the sense that any given layer in the coil is driven
normal by the layer underneath it.Comment: 58 pages, 5 tables, 16 fig
A New Crocodylian from the Late Maastrichtian of Spain: Implications for the Initial Radiation of Crocodyloids
The earliest crocodylians are known primarily from the Late Cretaceous of North America and Europe. The representatives of Gavialoidea and Alligatoroidea are known in the Late Cretaceous of both continents, yet the biogeographic origins of Crocodyloidea are poorly understood. Up to now, only one representative of this clade has been known from the Late Cretaceous, the basal crocodyloid Prodiplocynodon from the Maastrichtian of North America.The fossil studied is a skull collected from sandstones in the lower part of the Tremp Formation, in Chron C30n, dated at -67.6 to 65.5 Ma (late Maastrichtian), in Arén (Huesca, Spain). It is located in a continuous section that contains the K/P boundary, in which the dinosaur faunas closest to the K/P boundary in Europe have been described, including Arenysaurus ardevoli and Blasisaurus canudoi. Phylogenetic analysis places the new taxon, Arenysuchus gascabadiolorum, at the base of Crocodyloidea.The new taxon is the oldest crocodyloid representative in Eurasia. Crocodyloidea had previously only been known from the Palaeogene onwards in this part of Laurasia. Phylogenetically, Arenysuchus gascabadiolorum is situated at the base of the first radiation of crocodyloids that occurred in the late Maastrichtian, shedding light on this part of the cladogram. The presence of basal crocodyloids at the end of the Cretaceous both in North America and Europe provides new evidence of the faunal exchange via the Thulean Land Bridge during the Maastrichtian
Thermal conductivity of high- T c superconductors
This paper reviews existing data on the thermal conductivity of high- T c superconductors. Included are discussions of pristine polycrystalline high- T c ceramics, single crystal specimens, and high- T c materials structurally modified by substitution or by radiation damage. The thermal conductivity of high- T c superconductors is compared with that of conventional superconductors, and dramatic differences are found between the two families. Mechanisms of thermal conductivity applicable to high- T c perovskites are discussed and implications for theories of high- T c superconductivity are noted.Peer Reviewedhttp://deepblue.lib.umich.edu/bitstream/2027.42/45121/1/10948_2004_Article_BF00617463.pd
- …