42 research outputs found
Theoretical Study of Mechanism and Dynamics on Reaction of (CH<sub>3</sub>)<sub>2</sub>NH with CH<sub>3</sub>
The
mechanism and dynamics for the bimolecular reaction of (CH<sub>3</sub>)<sub>2</sub>NH with CH<sub>3</sub> have been investigated
based on the G3//MP2/6-311GĀ(<i>d</i>,<i>p</i>)
level of theory. Our calculations show that when the two reactants
approach each other, three prereaction complexes, RC1, RC2, and RC3,
can be formed through van der Waals force or hydrogen bonding. From
RC1, RC2, and RC3, six routes have been established. Among the six
routes, the two routes (R1 and R2) from van der Waals prereaction
complex RC1 are the main routes for the title reaction. R1 and R2
are hydrogen abstractions routes associated with H<sub>N</sub> and
H<sub>CĪ±</sub> atoms in DMA, respectively. The calculated energy
barriers for R1 and R2 are 12.3 and 13.7 kcal/mol, respectively. Both
the potential energy surfaces of R1 and R2 locate a āreactant-likeā
transition state, as well as van der Waals complexes before and after
the transition state. The slight preference of R1 over R2 might be
related to the higher similarity between the structures of RC1 and
the transition state for R1 (TS1), namely, the structure of TS1 is
more āreactant-likeā. The rate constants of the two
favorable H abstraction reaction routes, R1 and R2, are evaluated
over a wide temperature range of 200ā3000 K by the variational
transition state theory (VTST) methods, which can be expressed as <i>k</i><sub>R1</sub> = 5.30 Ć 10<sup>ā13</sup>(<i>T</i>/1000)<sup>3.0</sup> expĀ(ā2883/<i>T</i>) cm<sup>3</sup> molecule<sup>ā1</sup> s<sup>ā1</sup> and <i>k</i><sub>R2</sub> = 8.34 Ć 10<sup>ā13</sup>(<i>T</i>/1000)<sup>4.5</sup> expĀ(ā3100/<i>T</i>) cm<sup>3</sup> molecule<sup>ā1</sup> s<sup>ā1</sup>, respectively. The predicted rate constant of the H<sub>N</sub> abstraction
(route R1) is in good agreement with the available experimental data
On the Potential of Using the Al<sub>7</sub> Superatom as an Excess Electron Acceptor To Construct Materials with Excellent Nonlinear Optical Properties
With the aid of density
functional theory (DFT) calculations, we found that, when alkali metal
approaches the Al<sub>7</sub> superatom, its outermost s-value electron
can be trapped by Al<sub>7</sub> to give the superatom compound MAl<sub>7</sub> (M = Li, Na, K) with an excess electron. Different analyses
including natural bond orbital (NBO), electron localization function
(ELF), and energy decomposition analysis (EDA) show that the resulting
MāAl bond is strong and has a polar covalent character. The
optimizations of self-assemblies (MAl<sub>7</sub>)<sub><i>n</i></sub> (<i>n</i> = 2, 3) have been performed to explore
the stability of MAl<sub>7</sub> in the solid state. The results reveal
that only NaAl<sub>7</sub> can keep its structural integrity as a
building block upon self-assembling, while serious aggregations between
Al<sub>7</sub> clusters occur in the dimers and trimers of LiAl<sub>7</sub> and KAl<sub>7</sub>, despite the fact that the LiāAl<sub>7</sub> and KāAl<sub>7</sub> bond energies are comparable
to that of NaāAl<sub>7</sub>. BornāOppenheimer molecular
dynamics (BOMD) simulations for (NaAl<sub>7</sub>)<sub><i>n</i></sub> (<i>n</i> = 2, 3) indicate that these species are
stable toward fragmentation at 300 K. The Ī²<sub>0</sub> values
of (NaAl<sub>7</sub>)<sub><i>n</i></sub> (<i>n</i> = 1, 2, and 3) predicted at the CAM-B3LYP/6-311+GĀ(3df) level of
theory are in the range of 1.6 Ć 10<sup>4</sup>a.u. to 7.5 Ć
10<sup>4</sup> a.u.. This theoretical study implies that NaAl<sub>7</sub> is a promising candidate for nolinear optical (NLO) materials.
We provide theoretical evidence for the possibility of using the Al<sub>7</sub> superatom as an excess electron acceptor to construct materials
with excellent NLO properties. Further experimental research is invited
Empirical Mass and Kinetic Models for the Flash Evaporation of NaClāWater Solution
This paper attempts to provide empirical
mass and kinetic models for the flash evaporation of sodium chloride
(NaCl) aqueous solution based on experimental phenomena. The models
have nine parameters and six affecting factors including initial temperature,
operation pressure, NaCl mass fraction, solution depth, evaporator
diameter and time. On the basis of a large number of flash evaporation
experimental data from various literatures, the mass model parameters
were optimized and validated. After optimization of the model parameters
with 283 sets of literature experimental data, the average relative
error between the model values and the experimental data is about
5.7%. And a statistical method proved the mass model is well posed.
The verification with other 215 sets of literature experimental data
showed the mass model is in good agreement with flash evaporation
phenomena, and the average relative error between the model values
and the experimental data is about 8.3%. Then, the kinetic model of
flash evaporation was obtained according to the empirical mass model.
Finally, the analysis of these models indicated that the increase
of initial temperature or evaporator diameter and the decrease of
operating pressure are in favor of evaporation. Although the increase
of solution depth can improve the evaporated mass, the corresponding
evaporation efficiency will be slightly reduced. And the increase
of salt content is having a detrimental effect on the evaporation
of NaClāwater solution. In addition, the influence of salt
content on evaporation at higher operating pressure is more obvious
than that at lower operating pressure. The above results show that
these models proposed in our work have high accuracy, wide practicability,
and good rationality
The Quest for MetalāMetal Quadruple and Quintuple Bonds in Metal Carbonyl Derivatives: Nb<sub>2</sub>(CO)<sub>9</sub> and Nb<sub>2</sub>(CO)<sub>8</sub>
The synthesis by Power and co-workers of the first metalāmetal
quintuple bond (<i>Science</i> <b>2005</b>, <i>310</i>, 844) is a landmark in inorganic chemistry. The 18-electron
rule suggests that Nb<sub>2</sub>(CO)<sub>9</sub> and Nb<sub>2</sub>(CO)<sub>8</sub> are candidates for binary metal carbonyls containing
metalāmetal quadruple and quintuple bonds, respectively. Density
functional theory (MPW1PW91 and BP86) indeed predicts structures having
very short NbāNb distances of ā¼2.5 Ć
for Nb<sub>2</sub>(CO)<sub>9</sub> and ā¼2.4 Ć
for Nb<sub>2</sub>(CO)<sub>8</sub> as well as relatively large NbāNb Wiberg
bond indices supporting these high formal NbāNb bond orders.
However, analysis of the frontier molecular orbitals of these unbridged
structures suggests formal Nbī¼Nb triple bonds and 16-electron
metal configurations. This contrasts with an analysis of the frontier
orbitals in a model chromiumĀ(I) alkyl linear CH<sub>3</sub>CrCrCH<sub>3</sub>, which confirms the generally accepted presence of chromiumāchromium
quintuple bonds in such molecules. The presence of Nbī¼Nb triple
bonds rather than quadruple or quintuple bonds in the Nb<sub>2</sub>(CO)<sub><i>n</i></sub> (<i>n</i> = 9, 8) structures
frees up dĀ(<i>xy</i>) and dĀ(<i>x</i><sup>2</sup>ā<i>y</i><sup>2</sup>) orbitals for dĻāpĻ*
back-bonding to the carbonyl groups. The lowest energy Nb<sub>2</sub>(CO)<sub><i>n</i></sub> structures (<i>n</i> =
9, 8) are not these unbridged structures but structures having bridging
carbonyl groups of various types and formal NbāNb orders no
higher than three. Thus, the two lowest energy Nb<sub>2</sub>(CO)<sub>9</sub> structures have Nbī¼Nb triple bond distances of ā¼2.8
Ć
and three semibridging carbonyl groups, leading to a 16-electron
configuration rather than an 18-electron configuration for one of
the niobium atoms. The lowest energy structure of the highly unsaturated
Nb<sub>2</sub>(CO)<sub>8</sub> is unusual since it has a formal <i>single</i> NbāNb bond of length ā¼3.1 Ć
and
two four-electron donor Ī·<sup>2</sup>-Ī¼-CO groups, thereby
giving each niobium atom only a 16-electron configuration
Construction of the Tetrahedral Trifluorophosphine Platinum Cluster Pt<sub>4</sub>(PF<sub>3</sub>)<sub>8</sub> from Smaller Building Blocks
The experimentally known but structurally
uncharacterized Pt<sub>4</sub>(PF<sub>3</sub>)<sub>8</sub> is predicted
to have an <i>S</i><sub>4</sub> structure with a central
distorted Pt<sub>4</sub> tetrahedron having four short Ptī»Pt
distances, two long PtāPt distances, and all terminal PF<sub>3</sub> groups. The structures of the lower nuclearity species PtĀ(PF<sub>3</sub>)<sub><i>n</i></sub> (<i>n</i> = 4, 3,
2), Pt<sub>2</sub>(PF<sub>3</sub>)<sub><i>n</i></sub> (<i>n</i> = 7, 6, 5, 4), and Pt<sub>3</sub>(PF<sub>3</sub>)<sub>6</sub> were investigated by density functional theory to assess
their possible roles as intermediates in the formation of Pt<sub>4</sub>(PF<sub>3</sub>)<sub>8</sub> by the pyrolysis of PtĀ(PF<sub>3</sub>)<sub>4</sub>. The expected tetrahedral, trigonal planar, and linear
structures are found for PtĀ(PF<sub>3</sub>)<sub>4</sub>, PtĀ(PF<sub>3</sub>)<sub>3</sub>, and PtĀ(PF<sub>3</sub>)<sub>2</sub>, respectively.
However, the dicoordinate PtĀ(PF<sub>3</sub>)<sub>2</sub> structure
is bent from the ideal 180Ā° linear structure to approximately
160Ā°. Most of the low-energy binuclear Pt<sub>2</sub>(PF<sub>3</sub>)<sub><i>n</i></sub> (<i>n</i> = 7, 6,
5) structures can be derived from the mononuclear PtĀ(PF<sub>3</sub>)<sub><i>n</i></sub> (<i>n</i> = 4, 3, 2) structures
by replacing one of the PF<sub>3</sub> groups by a PtĀ(PF<sub>3</sub>)<sub>4</sub> or PtĀ(PF<sub>3</sub>)<sub>3</sub> ligand. In some of
these binuclear structures one of the PF<sub>3</sub> groups on the
PtĀ(PF<sub>3</sub>)<sub><i>n</i></sub> ligand becomes a bridging
group. The low-energy binuclear structures also include symmetrical
[PtĀ(PF<sub>3</sub>)<sub><i>n</i></sub>]<sub>2</sub> dimers
(<i>n</i> = 2, 3) of the coordinately unsaturated PtĀ(PF<sub>3</sub>)<sub><i>n</i></sub> (<i>n</i> = 3, 2).
The four low-energy structures for the trinuclear Pt<sub>3</sub>(PF<sub>3</sub>)<sub>6</sub> include two structures with central equilateral
Pt<sub>3</sub> triangles and two structures with isosceles Pt<sub>3</sub> triangles and various arrangements of terminal and bridging
PF<sub>3</sub> groups. Among these four structures the lowest-energy
Pt<sub>3</sub>(PF<sub>3</sub>)<sub>6</sub> structure has an unprecedented
four-electron donor Ī·<sup>2</sup>-Ī¼<sub>3</sub>-PF<sub>3</sub> group bridging the central Pt<sub>3</sub> triangle through
three PtāP bonds and one PtāF bond. Thermochemical studies
on the aggregation of these Pt-PF<sub>3</sub> complexes suggest the
tetramerization of PtĀ(PF<sub>3</sub>)<sub>2</sub> to Pt<sub>4</sub>(PF<sub>3</sub>)<sub>8</sub> to be highly exothermic regardless of
the mechanistic details
DataSheet5_Role and mechanism of NCAPD3 in promoting malignant behaviors in gastric cancer.ZIP
Background:Gastric cancer (GC) is one of the major malignancies threatening human lives and health. Non-SMC condensin II complex subunit D3 (NCAPD3) plays a crucial role in the occurrence of many diseases. However, its role in GC remains unexplored.Materials and Methods:The Cancer Genome Atlas (TCGA) database, clinical samples, and cell lines were used to analyze NCAPD3 expression in GC. NCAPD3 was overexpressed and inhibited by lentiviral vectors and the CRISPR/Cas9 system, respectively. The biological functions of NCAPD3 were investigated in vitro and in vivo. Gene microarray, Gene set enrichment analysis (GSEA) and ingenuity pathway analysis (IPA) were performed to establish the potential mechanisms.Results:NCAPD3 was highly expressed in GC and was associated with a poor prognosis. NCAPD3 upregulation significantly promoted the malignant biological behaviors of gastric cancer cell, while NCAPD3 inhibition exerted a opposite effect. NCAPD3 loss can directly inhibit CCND1 and ESR1 expression to downregulate the expression of downstream targets CDK6 and IRS1 and inhibit the proliferation of gastric cancer cells. Moreover, NCAPD3 loss activates IRF7 and DDIT3 to regulate apoptosis in gastric cancer cells.Conclusion:Our study revealed that NCAPD3 silencing attenuates malignant phenotypes of GC and that it is a potential target for GC treatment.</p
Cyclization of Thiocarbonyl Groups in Binuclear Homoleptic Nickel Thiocarbonyls To Give Ligands Derived from Sulfur Analogues of Croconic and Rhodizonic Acids
The
sulfur analogue of the well-known NiĀ(CO)<sub>4</sub>, namely, NiĀ(CS)<sub>4</sub>, has been observed spectroscopically in low temperature matrices
but is not known as a stable species under ambient conditions. Theoretical
studies show that NiĀ(CS)<sub>4</sub> with monomeric CS ligands and
tetrahedrally coordinated nickel is disfavored by ā¼17 kcal/mol
relative to unusual isomeric NiĀ(C<sub>2</sub>S<sub>2</sub>)<sub>2</sub> structures. In the latter structures the CS ligands couple pairwise
through CāC bond formation to give dimeric Sī»Cī»Cī»S
ligands, which bond preferentially to the nickel atom through their
Cī»S bonds rather than their Cī»C bonds. Coupling of CS
ligands in the lowest energy binuclear Ni<sub>2</sub>(CS)<sub><i>n</i></sub> (<i>n</i> = 7, 6, 5) structures results
in cyclization to give remarkable C<sub><i>n</i></sub>S<sub><i>n</i></sub> (<i>n</i> = 5, 6) ligands containing
five- and six-membered carbocyclic rings. Such ligands, which are
the sulfur analogues of the well-known croconate (<i>n</i> = 5) and rhodizonate (<i>n</i> = 6) oxocarbon ligands,
function as bidentate ligands to the central Ni<sub>2</sub> unit.
Higher energy Ni<sub>2</sub>(CS)<sub><i>n</i></sub> (<i>n</i> = 7, 6, 5) structures contain dimeric C<sub>2</sub>S<sub>2</sub> ligands, which can bridge the central Ni<sub>2</sub> unit.
Dimeric C<sub>2</sub>S<sub>2</sub> ligands rather than tetrathiosquare
C<sub>4</sub>S<sub>4</sub> ligands are found in the lowest energy
Ni<sub>2</sub>(CS)<sub>4</sub> structures
DataSheet7_Role and mechanism of NCAPD3 in promoting malignant behaviors in gastric cancer.ZIP
Background:Gastric cancer (GC) is one of the major malignancies threatening human lives and health. Non-SMC condensin II complex subunit D3 (NCAPD3) plays a crucial role in the occurrence of many diseases. However, its role in GC remains unexplored.Materials and Methods:The Cancer Genome Atlas (TCGA) database, clinical samples, and cell lines were used to analyze NCAPD3 expression in GC. NCAPD3 was overexpressed and inhibited by lentiviral vectors and the CRISPR/Cas9 system, respectively. The biological functions of NCAPD3 were investigated in vitro and in vivo. Gene microarray, Gene set enrichment analysis (GSEA) and ingenuity pathway analysis (IPA) were performed to establish the potential mechanisms.Results:NCAPD3 was highly expressed in GC and was associated with a poor prognosis. NCAPD3 upregulation significantly promoted the malignant biological behaviors of gastric cancer cell, while NCAPD3 inhibition exerted a opposite effect. NCAPD3 loss can directly inhibit CCND1 and ESR1 expression to downregulate the expression of downstream targets CDK6 and IRS1 and inhibit the proliferation of gastric cancer cells. Moreover, NCAPD3 loss activates IRF7 and DDIT3 to regulate apoptosis in gastric cancer cells.Conclusion:Our study revealed that NCAPD3 silencing attenuates malignant phenotypes of GC and that it is a potential target for GC treatment.</p
DataSheet4_Role and mechanism of NCAPD3 in promoting malignant behaviors in gastric cancer.ZIP
Background:Gastric cancer (GC) is one of the major malignancies threatening human lives and health. Non-SMC condensin II complex subunit D3 (NCAPD3) plays a crucial role in the occurrence of many diseases. However, its role in GC remains unexplored.Materials and Methods:The Cancer Genome Atlas (TCGA) database, clinical samples, and cell lines were used to analyze NCAPD3 expression in GC. NCAPD3 was overexpressed and inhibited by lentiviral vectors and the CRISPR/Cas9 system, respectively. The biological functions of NCAPD3 were investigated in vitro and in vivo. Gene microarray, Gene set enrichment analysis (GSEA) and ingenuity pathway analysis (IPA) were performed to establish the potential mechanisms.Results:NCAPD3 was highly expressed in GC and was associated with a poor prognosis. NCAPD3 upregulation significantly promoted the malignant biological behaviors of gastric cancer cell, while NCAPD3 inhibition exerted a opposite effect. NCAPD3 loss can directly inhibit CCND1 and ESR1 expression to downregulate the expression of downstream targets CDK6 and IRS1 and inhibit the proliferation of gastric cancer cells. Moreover, NCAPD3 loss activates IRF7 and DDIT3 to regulate apoptosis in gastric cancer cells.Conclusion:Our study revealed that NCAPD3 silencing attenuates malignant phenotypes of GC and that it is a potential target for GC treatment.</p
DataSheet13_Role and mechanism of NCAPD3 in promoting malignant behaviors in gastric cancer.xlsx
Background:Gastric cancer (GC) is one of the major malignancies threatening human lives and health. Non-SMC condensin II complex subunit D3 (NCAPD3) plays a crucial role in the occurrence of many diseases. However, its role in GC remains unexplored.Materials and Methods:The Cancer Genome Atlas (TCGA) database, clinical samples, and cell lines were used to analyze NCAPD3 expression in GC. NCAPD3 was overexpressed and inhibited by lentiviral vectors and the CRISPR/Cas9 system, respectively. The biological functions of NCAPD3 were investigated in vitro and in vivo. Gene microarray, Gene set enrichment analysis (GSEA) and ingenuity pathway analysis (IPA) were performed to establish the potential mechanisms.Results:NCAPD3 was highly expressed in GC and was associated with a poor prognosis. NCAPD3 upregulation significantly promoted the malignant biological behaviors of gastric cancer cell, while NCAPD3 inhibition exerted a opposite effect. NCAPD3 loss can directly inhibit CCND1 and ESR1 expression to downregulate the expression of downstream targets CDK6 and IRS1 and inhibit the proliferation of gastric cancer cells. Moreover, NCAPD3 loss activates IRF7 and DDIT3 to regulate apoptosis in gastric cancer cells.Conclusion:Our study revealed that NCAPD3 silencing attenuates malignant phenotypes of GC and that it is a potential target for GC treatment.</p