9 research outputs found
Unique Pore Selectivity for Cs<sup>+</sup> and Exceptionally High NH<sub>4</sub><sup>+</sup> Exchange Capacity of the Chalcogenide Material K<sub>6</sub>Sn[Zn<sub>4</sub>Sn<sub>4</sub>S<sub>17</sub>]
Highly selective ion-exchange properties and -exchange capacities of the open framework
chalcogenide material K6Sn[Zn4Sn4S17] (1) with Cs+ and NH4+ are reported. Because the structure of this
framework is known in great detail, these studies are a rare example where structure/property relationships
can be directly drawn. 1 possesses three types of micropore cavities. The largest pore of 1 presents an
exact fit for Cs+ and exhibits high selectivity for this ion, as demonstrated by competitive ion-exchange
experiments. The next largest pore has a greater capacity (up to four cations) and is well suited for NH4+
ions. This leads to a high ammonium-exchange capacity for 1 of 3.06 mequiv/gr, which is close to the
NH4+-exchange capacities of natural zeolites. The single-crystal structures of ammonium-exchanged
products at various stages reveal an unusual mechanism for the exchange process of 1 which involves
diffusion of ammonium cations from the large cavity to the small ones of the framework. Thermal analysis
of one of these ammonium-exchanged products, in combination with mass spectroscopy, showed the
decomposition of NH4+ cations to NH3 and H2S with the parallel transformation of the exchanged product
to a mixture of crystalline phases. Since K6Sn[Zn4Sn4S17] can be grown in suitably large crystals (much
larger than most zeolites), it defines an excellent model system in which ion-exchange processes and
products can be characterized and studied in detail in various reaction stages
Unique Pore Selectivity for Cs<sup>+</sup> and Exceptionally High NH<sub>4</sub><sup>+</sup> Exchange Capacity of the Chalcogenide Material K<sub>6</sub>Sn[Zn<sub>4</sub>Sn<sub>4</sub>S<sub>17</sub>]
Highly selective ion-exchange properties and -exchange capacities of the open framework
chalcogenide material K6Sn[Zn4Sn4S17] (1) with Cs+ and NH4+ are reported. Because the structure of this
framework is known in great detail, these studies are a rare example where structure/property relationships
can be directly drawn. 1 possesses three types of micropore cavities. The largest pore of 1 presents an
exact fit for Cs+ and exhibits high selectivity for this ion, as demonstrated by competitive ion-exchange
experiments. The next largest pore has a greater capacity (up to four cations) and is well suited for NH4+
ions. This leads to a high ammonium-exchange capacity for 1 of 3.06 mequiv/gr, which is close to the
NH4+-exchange capacities of natural zeolites. The single-crystal structures of ammonium-exchanged
products at various stages reveal an unusual mechanism for the exchange process of 1 which involves
diffusion of ammonium cations from the large cavity to the small ones of the framework. Thermal analysis
of one of these ammonium-exchanged products, in combination with mass spectroscopy, showed the
decomposition of NH4+ cations to NH3 and H2S with the parallel transformation of the exchanged product
to a mixture of crystalline phases. Since K6Sn[Zn4Sn4S17] can be grown in suitably large crystals (much
larger than most zeolites), it defines an excellent model system in which ion-exchange processes and
products can be characterized and studied in detail in various reaction stages
Unique Pore Selectivity for Cs<sup>+</sup> and Exceptionally High NH<sub>4</sub><sup>+</sup> Exchange Capacity of the Chalcogenide Material K<sub>6</sub>Sn[Zn<sub>4</sub>Sn<sub>4</sub>S<sub>17</sub>]
Highly selective ion-exchange properties and -exchange capacities of the open framework
chalcogenide material K6Sn[Zn4Sn4S17] (1) with Cs+ and NH4+ are reported. Because the structure of this
framework is known in great detail, these studies are a rare example where structure/property relationships
can be directly drawn. 1 possesses three types of micropore cavities. The largest pore of 1 presents an
exact fit for Cs+ and exhibits high selectivity for this ion, as demonstrated by competitive ion-exchange
experiments. The next largest pore has a greater capacity (up to four cations) and is well suited for NH4+
ions. This leads to a high ammonium-exchange capacity for 1 of 3.06 mequiv/gr, which is close to the
NH4+-exchange capacities of natural zeolites. The single-crystal structures of ammonium-exchanged
products at various stages reveal an unusual mechanism for the exchange process of 1 which involves
diffusion of ammonium cations from the large cavity to the small ones of the framework. Thermal analysis
of one of these ammonium-exchanged products, in combination with mass spectroscopy, showed the
decomposition of NH4+ cations to NH3 and H2S with the parallel transformation of the exchanged product
to a mixture of crystalline phases. Since K6Sn[Zn4Sn4S17] can be grown in suitably large crystals (much
larger than most zeolites), it defines an excellent model system in which ion-exchange processes and
products can be characterized and studied in detail in various reaction stages
Unique Pore Selectivity for Cs<sup>+</sup> and Exceptionally High NH<sub>4</sub><sup>+</sup> Exchange Capacity of the Chalcogenide Material K<sub>6</sub>Sn[Zn<sub>4</sub>Sn<sub>4</sub>S<sub>17</sub>]
Highly selective ion-exchange properties and -exchange capacities of the open framework
chalcogenide material K6Sn[Zn4Sn4S17] (1) with Cs+ and NH4+ are reported. Because the structure of this
framework is known in great detail, these studies are a rare example where structure/property relationships
can be directly drawn. 1 possesses three types of micropore cavities. The largest pore of 1 presents an
exact fit for Cs+ and exhibits high selectivity for this ion, as demonstrated by competitive ion-exchange
experiments. The next largest pore has a greater capacity (up to four cations) and is well suited for NH4+
ions. This leads to a high ammonium-exchange capacity for 1 of 3.06 mequiv/gr, which is close to the
NH4+-exchange capacities of natural zeolites. The single-crystal structures of ammonium-exchanged
products at various stages reveal an unusual mechanism for the exchange process of 1 which involves
diffusion of ammonium cations from the large cavity to the small ones of the framework. Thermal analysis
of one of these ammonium-exchanged products, in combination with mass spectroscopy, showed the
decomposition of NH4+ cations to NH3 and H2S with the parallel transformation of the exchanged product
to a mixture of crystalline phases. Since K6Sn[Zn4Sn4S17] can be grown in suitably large crystals (much
larger than most zeolites), it defines an excellent model system in which ion-exchange processes and
products can be characterized and studied in detail in various reaction stages
Unique Pore Selectivity for Cs<sup>+</sup> and Exceptionally High NH<sub>4</sub><sup>+</sup> Exchange Capacity of the Chalcogenide Material K<sub>6</sub>Sn[Zn<sub>4</sub>Sn<sub>4</sub>S<sub>17</sub>]
Highly selective ion-exchange properties and -exchange capacities of the open framework
chalcogenide material K6Sn[Zn4Sn4S17] (1) with Cs+ and NH4+ are reported. Because the structure of this
framework is known in great detail, these studies are a rare example where structure/property relationships
can be directly drawn. 1 possesses three types of micropore cavities. The largest pore of 1 presents an
exact fit for Cs+ and exhibits high selectivity for this ion, as demonstrated by competitive ion-exchange
experiments. The next largest pore has a greater capacity (up to four cations) and is well suited for NH4+
ions. This leads to a high ammonium-exchange capacity for 1 of 3.06 mequiv/gr, which is close to the
NH4+-exchange capacities of natural zeolites. The single-crystal structures of ammonium-exchanged
products at various stages reveal an unusual mechanism for the exchange process of 1 which involves
diffusion of ammonium cations from the large cavity to the small ones of the framework. Thermal analysis
of one of these ammonium-exchanged products, in combination with mass spectroscopy, showed the
decomposition of NH4+ cations to NH3 and H2S with the parallel transformation of the exchanged product
to a mixture of crystalline phases. Since K6Sn[Zn4Sn4S17] can be grown in suitably large crystals (much
larger than most zeolites), it defines an excellent model system in which ion-exchange processes and
products can be characterized and studied in detail in various reaction stages
Factors Controlling the Enhanced Mechanical and Thermal Properties of Nanodiamond-Reinforced Cross-Linked High Density Polyethylene
A systematic
investigation of the factors influencing the notable
enhancement of the mechanical and thermal properties of nanodiamonds
(NDs)-reinforced cross-linked high density polyethylene (PEX) is presented
in this work. The effects of crystal structure and molecular conformation
as well as filler dispersion and adhesion with the matrix were found
to govern the mechanical properties of the final composites. A considerable
increase in the strength, toughness, and elastic modulus of the materials
was found for the composites with filler content below 1 wt %. For
higher NDs concentrations, the properties degraded. When filler concentration
does not exceed 1 wt %, enhanced adhesion with the matrix is achieved,
allowing a more successful load transfer between the filler and the
matrix, thus enabling an effective reinforcement of the composites.
The higher degree of crystallinity along with larger crystal size
are also positively influencing the mechanical properties of PEX.
Higher filler concentrations, on the other hand, lead to the formation
of larger aggregates, which lead to lower adhesion with the matrix,
while they also constitute stress concentrators and therefore reduce
the positive reinforcement of the matrix. The thermal conductivity
of the composites was also found to be significantly increased for
low-filler concentrations. This enhancement was less significant for
higher NDs concentrations. It is concluded that this reinforcement
is due to the heat capacity increase that NDs incorporation causes
in PEX. Additionally, a thermal stability enhancement was found for
the composite with minimum filler content
Amino-Functionalized Multiwalled Carbon Nanotubes Lead to Successful Ring-Opening Polymerization of Poly(ε-caprolactone): Enhanced Interfacial Bonding and Optimized Mechanical Properties
In this work, the synthesis, structural
characteristics, interfacial bonding, and mechanical properties of
poly(ε-caprolactone) (PCL) nanocomposites with small amounts
(0.5, 1.0, and 2.5 wt %) of amino-functionalized multiwalled carbon
nanotubes (<i>f</i>-MWCNTs) prepared by ring-opening polymerization
(ROP) are reported. This method allows the creation of a covalent-bonding
zone on the surface of nanotubes, which leads to efficient debundling
and therefore satisfactory dispersion and effective load transfer
in the nanocomposites. The high covalent grafting extent combined
with the higher crystallinity provide the basis for a significant
enhancement of the mechanical properties, which was detected in the
composites with up to 1 wt % <i>f</i>-MWCNTs. Increasing
filler concentration encourages intrinsic aggregation forces, which
allow only minor grafting efficiency and poorer dispersion and hence
inferior mechanical performance. <i>f</i>-MWCNTs also cause
a significant improvement on the polymerization reaction of PCL. Indeed,
the in situ polymerization kinetics studies reveal a significant decrease
in the reaction temperature, by a factor of 30–40 °C,
combined with accelerated the reaction kinetics during initiation
and propagation and a drastically reduced effective activation energy
Multistates and Polyamorphism in Phase-Change K<sub>2</sub>Sb<sub>8</sub>Se<sub>13</sub>
The
phase-change (PC) materials in the majority of optical data
storage media in use today exhibit a fast, reversible crystal →
amorphous phase transition that allows them to be switched between
on (1) and off (0) binary states. Solid-state inorganic materials
with this property are relatively common, but those exhibiting an
amorphous → amorphous transition called <i>polyamorphism</i> are exceptionally rare. K<sub>2</sub>Sb<sub>8</sub>Se<sub>13</sub> (KSS) reported here is the first example of a material that has
both amorphous → amorphous polyamorphic transition and amorphous
→ crystal transition at easily accessible temperatures (227
and 263 °C, respectively). The transitions are associated with
the atomic coordinative preferences of the atoms, and all three states
of K<sub>2</sub>Sb<sub>8</sub>Se<sub>13</sub> are stable in air at
25 °C and 1 atm. All three states of K<sub>2</sub>Sb<sub>8</sub>Se<sub>13</sub> exhibit distinct optical bandgaps, <i>E</i><sub>g</sub> = 1.25, 1.0, and 0.74 eV, for the amorphous-II, amorphous-I,
and crystalline versions, respectively. The room-temperature electrical
conductivity increases by more than 2 orders of magnitude from amorphous-I
to -II and by another 2 orders of magnitude from amorphous-II to the
crystalline state. This extraordinary behavior suggests that a new
class of materials exist which could provide multistate level systems
to enable higher-order computing logic circuits, reconfigurable logic
devices, and optical switches
Multistates and Polyamorphism in Phase-Change K<sub>2</sub>Sb<sub>8</sub>Se<sub>13</sub>
The
phase-change (PC) materials in the majority of optical data
storage media in use today exhibit a fast, reversible crystal →
amorphous phase transition that allows them to be switched between
on (1) and off (0) binary states. Solid-state inorganic materials
with this property are relatively common, but those exhibiting an
amorphous → amorphous transition called <i>polyamorphism</i> are exceptionally rare. K<sub>2</sub>Sb<sub>8</sub>Se<sub>13</sub> (KSS) reported here is the first example of a material that has
both amorphous → amorphous polyamorphic transition and amorphous
→ crystal transition at easily accessible temperatures (227
and 263 °C, respectively). The transitions are associated with
the atomic coordinative preferences of the atoms, and all three states
of K<sub>2</sub>Sb<sub>8</sub>Se<sub>13</sub> are stable in air at
25 °C and 1 atm. All three states of K<sub>2</sub>Sb<sub>8</sub>Se<sub>13</sub> exhibit distinct optical bandgaps, <i>E</i><sub>g</sub> = 1.25, 1.0, and 0.74 eV, for the amorphous-II, amorphous-I,
and crystalline versions, respectively. The room-temperature electrical
conductivity increases by more than 2 orders of magnitude from amorphous-I
to -II and by another 2 orders of magnitude from amorphous-II to the
crystalline state. This extraordinary behavior suggests that a new
class of materials exist which could provide multistate level systems
to enable higher-order computing logic circuits, reconfigurable logic
devices, and optical switches
