2001
DOI: 10.1134/1.1417179
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Investigation of the mobility of paraffin molecules in channel urea clathrates by nuclear magnetic resonance relaxation spectroscopy

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Cited by 3 publications
(3 citation statements)
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“…14,18,22 The cylindrical shape of the urea channel accounts for the formation of incommensurate host-guest phases, 80 whose fascinating physical properties continue to attract ever-increasing attention. [81][82][83][84][85][86] However, there is a significant distinction of the channel in the dipeptides studied. Unlike for urea, the center of the channel is displaced from the central axis by up to >1 Å (Table 4).…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…14,18,22 The cylindrical shape of the urea channel accounts for the formation of incommensurate host-guest phases, 80 whose fascinating physical properties continue to attract ever-increasing attention. [81][82][83][84][85][86] However, there is a significant distinction of the channel in the dipeptides studied. Unlike for urea, the center of the channel is displaced from the central axis by up to >1 Å (Table 4).…”
Section: Resultsmentioning
confidence: 99%
“…The channels in all dipeptides studied are very uniform, with the variation of diameter as the channel propagates along c translation being 0.2 Å or less (Table ). Such geometry is very uncommon among inclusion architectures and is reminiscent of the channel in urea. ,, The cylindrical shape of the urea channel accounts for the formation of incommensurate host−guest phases, whose fascinating physical properties continue to attract ever-increasing attention. …”
Section: Resultsmentioning
confidence: 99%
“…The dynamics, structure, and phase transitions of n-hexadecane/urea ( Figure 1) have been studied extensively. 11,28,[30][31][32][33][34][35][36][37][38][39][40][41][42][43][44][45] Although much of the early literature, including the first crystal structure of any UIC, 26 treated this as a commensurate structure with c g = 2c h , it has been known since work by Laves et al 46 and Lenné 24 that the repeat length of the guest along the channel (c g ) is somewhat longer (∼22.6 Å) than that of twice the repeat of the host (22.03 Å). In the mid-1980s, Forst reported a rich sequence of four phases from 380 K to 77 K. 32,33 Above 365 K, a hexagonal structure was reported, whereas between this temperature and ∼150 K, the structure was reported to be approximately trigonal.…”
Section: Introductionmentioning
confidence: 99%