UDC 539.26 Using the method of full-profile analysis of X-ray patterns obtained from polycrystals, the structure of carbon nanomaterials manufactured in the presence of a variety of catalysts is investigated. The unit cell period and phase concentration are specified. The formation of nanotubes with an interlayer spacing of 3.44 Å is established in the specimens under study.Keywords: carbon, nanomaterials, X-ray structure analysis.The purpose of this work is to investigate the structural features of carbon nanowebs based on the analysis of the distribution curves of X-ray scattering intensity.The X-ray radiographic investigations were performed with computer-aided DRON-3M and DRON-6 diffractometers using Fe-and CuK α -radiation. The X-ray patterns obtained were analyzed using a PdWin software package [1] and a PDR code for full-profile analysis of X-ray patterns from the crystals [2].The specimens were prepared by the electrospark-ignited combustion of a graphite electrode in the presence of a number of catalysts.During preparation of all specimens except for the first one, the anode consisted of four approximately identical graphite rods 8-9 cm in height. Their cross-section was square, with the side being 2.5 mm. The rods were assembled crosswise into a quadruple electrode that served as a master cathode. Before assembly into the master electrode, the carbon rods were processed in a water solution of iodine. The rods were separated by four thin plates of a respective catalyst placed in between the rods. The system geometry was selected in a way to use four different metals as catalysts. When preparing Specimen 1, the electrode had a sandwich structure, and no processing of the rods with iodine was performed. The helium pressure in the chamber for all of the tests was 600 Torr. Table 1 presented below lists the specimen number, the catalyst type, and special conditions of the specimen preparation.The X-ray patterns from Specimens 1-3 ( Fig. 1) contain five Bragg reflections in the vicinity of the scattering angles 2θ Cu > 40°. For the values 2θ Cu < 30°, there is a diffusion background, whose angular dependences are different. The most intensive low-angle scattering (2θ Cu = 2 to10°) is found in the X-ray pattern from Specimen 2, and the most pronounced diffusion peak (2θ Cu ∼ 17°) -in the X-ray pattern from Specimen 3. Against the background of this diffusion peak there is a narrow asymmetric peak towards the values of 2θ Cu ∼ 26.5°. The position of this peak is somewhat displaced from that corresponding to (002) graphite reflection (2θ Cu = 26.63°).The Bragg reflections observed in the X-ray patterns of all the three specimens ( Fig. 1) for the values of 2θ Cu > 40° correspond, both in their position and intensity, to the X-ray pattern from the material with an fcc-lattice. It is well known that solid solutions of chromium in nickel (nichrome) maintain their fcc-lattice till a chromium concentration of 15-20 wt.% [3]. According to the JCPDS data files, the lattice period of Ni is equal to a Ni = 3.5238 Å,