Does porous mean soft? On the elastic behaviour and structural evolution of zeolites under pressure

Author(s):  
G. Diego Gatta

This is a comparative study on lattice compressibility, pressure (

2019 ◽  
Vol 6 (6) ◽  
pp. 1527-1534 ◽  
Author(s):  
Paolo Dolcet ◽  
Kristin Kirchberg ◽  
Alice Antonello ◽  
Christian Suchomski ◽  
Roland Marschall ◽  
...  

ZnFe2O4 was synthesised through three different low-temperature routes to study the effect on the structural evolution of the compounds.


1996 ◽  
Vol 225 (1-2) ◽  
pp. 94-102 ◽  
Author(s):  
E. Bonetti ◽  
L. Del Bianco ◽  
P. Allia ◽  
P. Tiberto ◽  
F. Vinai

2014 ◽  
Vol 78 (2) ◽  
pp. 267-291 ◽  
Author(s):  
G. D. Gatta ◽  
Y. Lee

AbstractThis is a review of the elastic behaviour and pressure (P)-induced structural evolution of zeolites and presents a comparative analysis of the deformation mechanisms of the Si/Al-framework and the rearrangement of the extra-framework species in response to applied pressure. The interaction betweenP-transmitting fluids and zeolites, which can lead to phenomena such as ‘P-induced over-hydration’, is described. The comparative elastic analysis and the high-Pstructural data of zeolites reported so far allow us to make some generalizations: (1) The range of compressibility among this class of openframework silicates is large, with bulk moduli ranging between 15 and 70 GPa; (2) Microporosity does not necessarily imply high compressibility, as several zeolites are less compressible than other nonzeolitic rock-forming minerals; (3) Compressibilities of zeolites do not seem to be directly related to microporosity, at least if we model microporosity with the ‘framework density’; (4) The flexibility observed in zeolites under hydrostatic compression is mainly governed by tilting of rigid tetrahedra around O atoms that behave as hinges within the framework. Pressure-induced tilting commonly leads to continuous rearrangement of the framework without any phase transition. More rarely, tilting induces displacive phase transitions and isothermalP-induced reconstructive phase transitions (i.e. with change in framework topology), have not been reported in this class of materials; (5) Deformation mechanisms in response to applied pressure are generally dictated by the topological configuration of the framework rather than the Si/Al-distribution or the extra-framework content. The channel content governs the compressibility of the cavities, leading to different unit-cell-volume compressibilities in isotypic structures.


2008 ◽  
Vol 10 (2) ◽  
pp. 177-185 ◽  
Author(s):  
Jenny Tellier ◽  
Philippe Boullay ◽  
Dorra Ben Jennet ◽  
Daniele Mercurio

2008 ◽  
Vol 35 (9) ◽  
pp. 521-533 ◽  
Author(s):  
G. Diego Gatta ◽  
Nicola Rotiroti ◽  
Martin Fisch ◽  
Milen Kadiyski ◽  
Thomas Armbruster

2006 ◽  
Vol 70 (3) ◽  
pp. 309-317 ◽  
Author(s):  
G.D. Gatta ◽  
F. Nestola ◽  
J.M. Walter

AbstractThe high-temperature (HT) behaviour of kyanite (Al2SiO5) was investigated by in situ neutron powder diffraction up to 1200°C. Within the investigated T range, no phase transition was observed. The axial and volume thermal expansion coefficient (αj = lj-1(𝜕1j/𝜕T), αv = V-1 (𝜕V/𝜕T)), calculated by weighted linear regression through the data points, are: αa = 5.5(2) x 10-5, αb= 5.9(2) x 10-5, αc = 5.18(8) xl0-5, αv = 7.4(1) x 10-3 “C-1, with αa:αb:αc = 1.06:1.14:1. All three angles of the kyanite lattice show a slight decrease with T, with 𝜕α/𝜕T = -2(2) x 10-5, 𝜕β/𝜕T = -4(1) x 10-5, 𝜕γ/𝜕T = –10(2) x 10-5%C. The magnitudes of the principal Lagrangian unit-strain coefficients (ε1,ε2, ε3) and the orientations of the thermal strain-ellipsoids, between the ambient temperature and each measured T, were calculated. The magnitude and the orientation of all the three unit-strain coefficients are almost maintained constant with T. At T-To = 1177°C , ε^a = 76(2)°, ε^b = 70(2)°, ε^c = 38(3)°, ε2^a = 49(3)°, ε2^b = 66(3)°, ε2^c = 127(4)°, ε3^a = 135(3)°, ε3^b = 31(3)°, ε3^c = 91(2)° with ε1:ε2:ε3 = 1.57:1.29:1. The structural refinements, performed at 23, 600, 650, 700, 750, 800, 900, 950, 1050 and 1200°C allowed the description of the structural evolution and the main T-induced deformation mechanisms, which are mainly represented by the polyhedral distortions of the AlO6 octahedra.


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