Bond, weak bond

Nature ◽  
1999 ◽  
Author(s):  
Philip Ball
Keyword(s):  
2007 ◽  
Vol 63 (2) ◽  
pp. 296-302 ◽  
Author(s):  
Mikhail A. Strzhemechny ◽  
Vyacheslav N. Baumer ◽  
Anatoli A. Avdeenko ◽  
Oleg S. Pyshkin ◽  
Roman V. Romashkin ◽  
...  

A combination of single-crystal and powder X-ray diffractometry was used to study the structure of two polymorphs of 4-bromobenzophenone over the temperature range from 100 to 300 K. One of the polymorphs of the title compound was known previously and its structure has been determined at room temperature [Ebbinghaus et al. (1997). Z. Kristallogr. 212, 339–340]. Two crystal growth methods were employed, one of which (a modification of the Bridgman–Stockbarger technique) resulted in single crystals of a previously unknown structure. The basic physical properties of the stable polymorph are: growth method, from 2-propanol solutions or gradient sublimation; space group, monoclinic P21/c; melting point, T m = 355.2 K; X-ray density (at 100 K), Dx = 1.646 g cm−3. The same properties of the metastable polymorph (triclinic P\overline 1 ) are: growth method, modified Bridgman–Stockbarger method; X-ray density (at 100 K), Dx = 1.645 g cm−3; T m = 354 K. Thermograms suggest that the melting of the metastable form is accompanied by at least a partial crystallization presumably into the monoclinic form; the transformation is therefore monotropic. Analysis of short distances in both polymorphs shows that numerous weak hydrogen bonds of the C—H...π type ensure additional stabilization within the respective planes normal to the longest dimension of the molecules. The strong temperature dependence of the lattice constants and of the weak bond distances in the monoclinic form suggest that the weak bond interactions might be responsible for both the large thermal expansion within plane bc and the considerable thermal expansion anisotropy.


2018 ◽  
Author(s):  
M. Sagnard ◽  
L. Berthe ◽  
R. Ecault ◽  
F. Touchard ◽  
M. Boustie ◽  
...  
Keyword(s):  

2019 ◽  
Vol 123 ◽  
pp. 105787 ◽  
Author(s):  
Emmanuel Keita ◽  
Hela Bessaies-Bey ◽  
Wenqiang Zuo ◽  
Patrick Belin ◽  
Nicolas Roussel

2018 ◽  
Vol 6 (5) ◽  
pp. 6711-6717 ◽  
Author(s):  
Guodong Sheng ◽  
Yingying Shao ◽  
Weidong Ye ◽  
Chunyan Sun ◽  
Chuncheng Chen ◽  
...  

2001 ◽  
Vol 79 (11-12) ◽  
pp. 1365-1371 ◽  
Author(s):  
L Bellier-Castella ◽  
M JP Gingras ◽  
P CW Holdsworth ◽  
R Moessner

The classical Heisenberg anti-ferromagnet on the pyrochlore lattice is macroscopically and continuously degenerate and the system remains disordered at all temperatures, even in the presence of weak dilution with nonmagnetic ions. We show that, in contrast, weak-bond disorder lifts the ground-state degeneracy in favour of locally collinear spin configurations. We present a proof that for a single tetrahedron the ground state is perfectly collinear but identify two mechanisms that preclude the establishment of a globally collinear state; one due to frustration and the other due to higher order effects. We thus obtain a rugged energy landscape, which is necessary to account for the glassy phenomena found in real systems such as the pyrochlore Y2Mo2O7 recently reported by Booth et al. (Phys. Rev. B: Condens. Matter Mater. Phys. 62, R755 (2000).) to contain a substantial degree of bond disorder. PACS Nos.: 75.10.Hk, 75.40.Mg, 75.40.Gb


2017 ◽  
Vol 5 (5) ◽  
pp. 887-906 ◽  
Author(s):  
Xiaochu Ding ◽  
Yadong Wang

Here we define hydrogels crosslinked by weak bonds as physical hydrogels.


1985 ◽  
Vol 63 (7) ◽  
pp. 1477-1479 ◽  
Author(s):  
D. J. Millen

Expressions are derived from which stretching force constants for the weak bond in weakly bound dimers may be evaluated directly from observed rotational constants and centrifugal stretching distortion constants.


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