Abstract
An ideal polycrystalline material or power is an ensemble of a very large number of randomly oriented crystallites. It is shown the effect that this random orientation has on the diffraction of a specimen assumed to contain only one reciprocal lattice node. The most remarkable difference with the single-crystal case is that now must think of scattering vectors not as lying on discrete nodes of reciprocal lattice vectors, the distances from the single-crystal reciprocal lattice nodes to the origin of reciprocal space.
Giacovazzo, C
[1]
- Bari Univ. (Italy). Dip. Geomineralogico
Citation Formats
Giacovazzo, C.
About some practical aspects of X-ray diffraction : From single crystal to powders.
Italy: N. p.,
1996.
Web.
Giacovazzo, C.
About some practical aspects of X-ray diffraction : From single crystal to powders.
Italy.
Giacovazzo, C.
1996.
"About some practical aspects of X-ray diffraction : From single crystal to powders."
Italy.
@misc{etde_465283,
title = {About some practical aspects of X-ray diffraction : From single crystal to powders}
author = {Giacovazzo, C}
abstractNote = {An ideal polycrystalline material or power is an ensemble of a very large number of randomly oriented crystallites. It is shown the effect that this random orientation has on the diffraction of a specimen assumed to contain only one reciprocal lattice node. The most remarkable difference with the single-crystal case is that now must think of scattering vectors not as lying on discrete nodes of reciprocal lattice vectors, the distances from the single-crystal reciprocal lattice nodes to the origin of reciprocal space.}
place = {Italy}
year = {1996}
month = {Sep}
}
title = {About some practical aspects of X-ray diffraction : From single crystal to powders}
author = {Giacovazzo, C}
abstractNote = {An ideal polycrystalline material or power is an ensemble of a very large number of randomly oriented crystallites. It is shown the effect that this random orientation has on the diffraction of a specimen assumed to contain only one reciprocal lattice node. The most remarkable difference with the single-crystal case is that now must think of scattering vectors not as lying on discrete nodes of reciprocal lattice vectors, the distances from the single-crystal reciprocal lattice nodes to the origin of reciprocal space.}
place = {Italy}
year = {1996}
month = {Sep}
}