21 research outputs found
Hypokinesia in adolescents
Title: Hypokinesia in adolescents Objectives: The main target is, to find out how frequent and extensive the hypokinesis appears in terms of the exploratory subject. We mainly search for the relationship of high school adolescents to the physical activities, how often it's being practicised and in which kind of environment. Methods: In order to prove my thesis, we decided to use a long version of international standardized IPAQ questionnaire translated to the czech language. The exploratory sample consisted of 46 high school adolescent students. The results were afterwards analysed according to the basic statistic principles. Subsequently we compared the quantity of physical activity between boys and girls during seven days of the research. Results: The results of research apparently meet the criteria of the sufficient count of teenager activities. In the average the sample was evaluated as moderately active individuals in both gender types. Despite the negative public image in terms of quantity of youth physical activities, the actual rate meets general requirements. Boys reached the rate of 1333,8 MET- min/week, girls reached the count of 2013,9 MET-min/week. Keywords: adolescence, physical activity, lack of exercise, lifestyl
Synthesis and Characterization of Nickel(II) Phosphonate Complexes Utilizing Pyridonates and Carboxylates as Co-ligands
The synthesis and structures of five new nickel complexes containing phosphonate ligands are reported. The compounds utilize pivalic acid (HPiv) and 6-chloro-2-pyridonate (Hchp) as co-ligands with the resulting complexes being of formulas [Ni<sub>10</sub>(chp)<sub>4</sub>(Hchp)<sub>4.5</sub>(O<sub>3</sub>P<sup>t</sup>Bu)<sub>3</sub>(Piv)<sub>5</sub>(HPiv)<sub>2</sub>(OH)<sub>6</sub>(H<sub>2</sub>O)<sub>4.5</sub>](HNEt<sub>3</sub>)·0.5MeCN·2.5H<sub>2</sub>O <b>1</b>, [Ni<sub>12</sub>(chp)<sub>12</sub>(Hchp)<sub>2</sub>(PhPO<sub>3</sub>)<sub>2</sub><sub></sub>(Piv)<sub>5</sub>(HPiv)<sub>2</sub>(OH)<sub>2</sub>(H<sub>2</sub>O)<sub>6</sub>](F)·4.5MeCN·2H<sub>2</sub>O <b>2</b>, [Ni<sub>10</sub>(chp)<sub>6</sub>(O<sub>3</sub>PCH<sub>2</sub>Ph)<sub>2</sub>(Piv)<sub>8</sub>(F)<sub>2</sub>(MeCN)<sub>4</sub>] <b>3</b>, [Ni<sub>10</sub>(chp)<sub>6</sub>(O<sub>3</sub>PMe)<sub>2</sub>(Piv)<sub>8</sub>(F)<sub>2</sub> (MeCN)<sub>4</sub>]·5MeCN·2H<sub>2</sub>O <b>4</b>, and [Ni<sub>10</sub>(chp)<sub>6</sub>(O<sub>3</sub>PCH<sub>2</sub>Nap)<sub>2</sub>(Piv)<sub>8</sub>(F)<sub>2</sub>(MeCN)<sub>2</sub>(H<sub>2</sub>O)<sub>2</sub>] <b>5</b>. The metallic core of compounds <b>1</b> and <b>2</b> display tetra- and hexa-capped trigonal prismatic arrangements, while the metallic and phosphorus core of <b>3</b>, <b>4</b>, and <b>5</b> display three face-sharing octahedra. Variable temperature direct current (dc) magnetic susceptibility measurements reveal dominant antiferromagnetic exchange interactions within each cluster, with diamagnetic spin ground states found
Synthesis and Characterization of Nickel(II) Phosphonate Complexes Utilizing Pyridonates and Carboxylates as Co-ligands
The synthesis and structures of five new nickel complexes containing phosphonate ligands are reported. The compounds utilize pivalic acid (HPiv) and 6-chloro-2-pyridonate (Hchp) as co-ligands with the resulting complexes being of formulas [Ni<sub>10</sub>(chp)<sub>4</sub>(Hchp)<sub>4.5</sub>(O<sub>3</sub>P<sup>t</sup>Bu)<sub>3</sub>(Piv)<sub>5</sub>(HPiv)<sub>2</sub>(OH)<sub>6</sub>(H<sub>2</sub>O)<sub>4.5</sub>](HNEt<sub>3</sub>)·0.5MeCN·2.5H<sub>2</sub>O <b>1</b>, [Ni<sub>12</sub>(chp)<sub>12</sub>(Hchp)<sub>2</sub>(PhPO<sub>3</sub>)<sub>2</sub><sub></sub>(Piv)<sub>5</sub>(HPiv)<sub>2</sub>(OH)<sub>2</sub>(H<sub>2</sub>O)<sub>6</sub>](F)·4.5MeCN·2H<sub>2</sub>O <b>2</b>, [Ni<sub>10</sub>(chp)<sub>6</sub>(O<sub>3</sub>PCH<sub>2</sub>Ph)<sub>2</sub>(Piv)<sub>8</sub>(F)<sub>2</sub>(MeCN)<sub>4</sub>] <b>3</b>, [Ni<sub>10</sub>(chp)<sub>6</sub>(O<sub>3</sub>PMe)<sub>2</sub>(Piv)<sub>8</sub>(F)<sub>2</sub> (MeCN)<sub>4</sub>]·5MeCN·2H<sub>2</sub>O <b>4</b>, and [Ni<sub>10</sub>(chp)<sub>6</sub>(O<sub>3</sub>PCH<sub>2</sub>Nap)<sub>2</sub>(Piv)<sub>8</sub>(F)<sub>2</sub>(MeCN)<sub>2</sub>(H<sub>2</sub>O)<sub>2</sub>] <b>5</b>. The metallic core of compounds <b>1</b> and <b>2</b> display tetra- and hexa-capped trigonal prismatic arrangements, while the metallic and phosphorus core of <b>3</b>, <b>4</b>, and <b>5</b> display three face-sharing octahedra. Variable temperature direct current (dc) magnetic susceptibility measurements reveal dominant antiferromagnetic exchange interactions within each cluster, with diamagnetic spin ground states found
Single-Molecule Magnetism in Tetrametallic Terbium and Dysprosium Thiolate Cages
Metalation of ethanethiol by [{(Me<sub>3</sub>Si)<sub>2</sub>N}<sub>3</sub>Ln(μ-Cl)Li(thf)<sub>3</sub>] (Ln = Gd,
Tb, Dy) in thf
produces the thiolate-bridged tetralanthanide compounds [Li(thf)<sub>4</sub>][Ln<sub>4</sub>{N(SiMe<sub>3</sub>)<sub>2</sub>}<sub>4</sub>(μ-SEt)<sub>8</sub>(μ<sub>4</sub>-SEt)], where Ln = Gd
is [Li(thf)<sub>4</sub>][<b>1</b>], Ln = Tb is [Li(thf)<sub>4</sub>][<b>2</b>], and Ln = Dy is [Li(thf)<sub>4</sub>][<b>3</b>]. Crystallographic studies reveal that the monoanions <b>1</b>–<b>3</b> are essentially isostructural, consisting
of tetrametallic Ln<sub>4</sub> units in which the lanthanides are
bridged by μ-ethanethiolate ligands and the individual lanthanide
centers occupy distorted six-coordinate {LnNS<sub>5</sub>} coordination
environments. The magnetic susceptibility properties of all three
compounds were measured in a static (dc) field of 1000 G: the data
for the gadolinium anion <b>1</b> were reproduced by a model
that suggests weak antiferromagnetic and ferromagnetic exchange, with
coupling constants of <i>J</i> = −0.09 and +0.04
cm<sup>–1</sup> (−2<i>J</i> formalism). Magnetic
susceptibility measurements in a dynamic (ac) field at various frequencies
on [Li(thf)<sub>4</sub>][<b>2</b>] and [Li(thf)<sub>4</sub>][<b>3</b>], in zero dc field, reveal properties characteristic of
a single-molecule magnet (SMM). Analysis of the out-of-phase magnetic
susceptibility for <b>2</b> in zero applied field yielded a
small anisotropy barrier of <i>U</i><sub>eff</sub> = 4.6
cm<sup>–1</sup>, and a similar analysis on <b>3</b> produced <i>U</i><sub>eff</sub> = 46 cm<sup>–1</sup>. Compounds [Li(thf)<sub>4</sub>][<b>2</b>] and [Li(thf)<sub>4</sub>][<b>3</b>] are rare examples of sulfur-ligated SMMs
Single-Molecule Magnetism in Tetrametallic Terbium and Dysprosium Thiolate Cages
Metalation of ethanethiol by [{(Me<sub>3</sub>Si)<sub>2</sub>N}<sub>3</sub>Ln(μ-Cl)Li(thf)<sub>3</sub>] (Ln = Gd,
Tb, Dy) in thf
produces the thiolate-bridged tetralanthanide compounds [Li(thf)<sub>4</sub>][Ln<sub>4</sub>{N(SiMe<sub>3</sub>)<sub>2</sub>}<sub>4</sub>(μ-SEt)<sub>8</sub>(μ<sub>4</sub>-SEt)], where Ln = Gd
is [Li(thf)<sub>4</sub>][<b>1</b>], Ln = Tb is [Li(thf)<sub>4</sub>][<b>2</b>], and Ln = Dy is [Li(thf)<sub>4</sub>][<b>3</b>]. Crystallographic studies reveal that the monoanions <b>1</b>–<b>3</b> are essentially isostructural, consisting
of tetrametallic Ln<sub>4</sub> units in which the lanthanides are
bridged by μ-ethanethiolate ligands and the individual lanthanide
centers occupy distorted six-coordinate {LnNS<sub>5</sub>} coordination
environments. The magnetic susceptibility properties of all three
compounds were measured in a static (dc) field of 1000 G: the data
for the gadolinium anion <b>1</b> were reproduced by a model
that suggests weak antiferromagnetic and ferromagnetic exchange, with
coupling constants of <i>J</i> = −0.09 and +0.04
cm<sup>–1</sup> (−2<i>J</i> formalism). Magnetic
susceptibility measurements in a dynamic (ac) field at various frequencies
on [Li(thf)<sub>4</sub>][<b>2</b>] and [Li(thf)<sub>4</sub>][<b>3</b>], in zero dc field, reveal properties characteristic of
a single-molecule magnet (SMM). Analysis of the out-of-phase magnetic
susceptibility for <b>2</b> in zero applied field yielded a
small anisotropy barrier of <i>U</i><sub>eff</sub> = 4.6
cm<sup>–1</sup>, and a similar analysis on <b>3</b> produced <i>U</i><sub>eff</sub> = 46 cm<sup>–1</sup>. Compounds [Li(thf)<sub>4</sub>][<b>2</b>] and [Li(thf)<sub>4</sub>][<b>3</b>] are rare examples of sulfur-ligated SMMs
Synthesis, Structure, and Paramagnetism of Manganese(II) Iminophosphate Complexes
The coordination chemistry of the bidentate bis(imino)bis(amino)phosphate
ligands [Me<sub>3</sub>SiNP{NR}{N(H)R}<sub>2</sub>]<sup>−</sup>, where R = <i>n</i>-propyl is [L<sup>1</sup>H<sub>2</sub>]<sup>−</sup>, R = cyclohexyl is [L<sup>2</sup>H<sub>2</sub>]<sup>−</sup>, and R = <i>tert</i>-butyl is [L<sup>3</sup>H<sub>2</sub>]<sup>−</sup>, with manganese(II), is
described. The bis(imino)bis(amino)phosphate-manganese(II) complexes
[(η<sup>5</sup>-Cp)Mn(μ-L<sup>1</sup>H<sub>2</sub>)]<sub>2</sub> (<b>1</b>), [Mn(L<sup>2</sup>H<sub>2</sub>)<sub>2</sub>]·THF (<b>2</b>·THF), and [(η<sup>5</sup>-Cp)Mn(L<sup>3</sup>H<sub>2</sub>)] (<b>3</b>) were synthesized by monodeprotonation
of the respective pro-ligands by manganocene, Cp<sub>2</sub>Mn. The
molecular structures of <b>1</b>–<b>3</b> reveal
that the steric demands of the ligand N-substituents play a dominant
role in determining the aggregation state and overall composition
of the manganese(II) complexes. The coordination geometries of the
Mn(II) centers are six-coordinate pseudotetrahedral in <b>1</b>, four-coordinate distorted tetrahedral in <b>2</b>, and five-coordinate
in <b>3</b>, resulting in formal valence electron counts of
17, 13, and 15, respectively. EPR studies of <b>1</b>–<b>3</b> at Q-band reveal high-spin manganese(II) (<i>S</i> = <sup>5</sup>/<sub>2</sub>) in each case. In the EPR spectrum of <b>1</b>, no evidence of intramolecular magnetic exchange was found.
The relative magnitudes of the axial zero-field splitting parameter, <i>D</i>, in <b>2</b> and <b>3</b> are consistent with
the symmetry of the manganese environment, which are <i>D</i><sub>2<i>d</i></sub> in <b>2</b> and <i>C</i><sub>2<i>v</i></sub> in <b>3</b>
Wells–Dawson Cages as Molecular Refrigerants
Five clusters with the general formula
[Ni<sub>6</sub>Gd<sub>6</sub>(μ<sub>3</sub>-OH)<sub>2</sub>(μ<sub>2</sub>-OAc)<sub>2</sub>(O<sub>3</sub>PR)<sub>6</sub>(O<sub>2</sub>C<sup><i>t</i></sup>Bu)<sub>16</sub>], where R = methyl
(<b>1</b>), phenyl
(<b>2</b>), <i>n</i>-hexyl (<b>3</b>), benzyl
(<b>4</b>), <i>n</i>-octyl (<b>5</b>), have
been prepared. All of the clusters have a {Ni<sub>6</sub>Gd<sub>6</sub>P<sub>6</sub>} core that can be related to the Wells–Dawson
ion. We have also prepared analogues where the gadolinium is replaced
with diamagnetic yttrium: [Ni<sub>6</sub>Y<sub>6</sub>(μ<sub>3</sub>-OH)<sub>2</sub>(μ<sub>2</sub>-OAc)<sub>2</sub>(O<sub>3</sub>PR)<sub>6</sub>(O<sub>2</sub>C<sup><i>t</i></sup>Bu)<sub>16</sub>] (R = methyl (<b>6</b>), <i>n</i>-hexyl (<b>7</b>), benzyl (<b>8</b>), <i>n</i>-octyl (<b>9</b>)), allowing the magnetic exchange within the
{Ni<sub>3</sub>} units to be analyzed by modeling as the sum of two
noninteracting isosceles triangles. The variation in the magnetic
entropy changes for magnetization (−Δ<i>S</i><sub>M</sub>) among compounds <b>1</b>–<b>5</b> could be attributed not only to the molecular weight of the compounds
but also to intramolecular magnetic interactions
Systematic Study of a Family of Butterfly-Like {M<sub>2</sub>Ln<sub>2</sub>} Molecular Magnets (M = Mg<sup>II</sup>, Mn<sup>III</sup>, Co<sup>II</sup>, Ni<sup>II</sup>, and Cu<sup>II</sup>; Ln = Y<sup>III</sup>, Gd<sup>III</sup>, Tb<sup>III</sup>, Dy<sup>III</sup>, Ho<sup>III</sup>, and Er<sup>III</sup>)
A family
of 3d–4f [M<sup>II</sup><sub>2</sub>Ln<sup>III</sup><sub>2</sub>(μ<sub>3</sub>-OH)<sub>2</sub>(O<sub>2</sub>C<sup><i>t</i></sup>Bu)<sub>10</sub>]<sup>2–</sup> “butterflies”
(where M<sup>II</sup> = Mg, Co, Ni, and Cu; Ln<sup>III</sup> = Y,
Gd, Tb, Dy, Ho, and Er) and [Mn<sup>III</sup><sub>2</sub>Ln<sup>III</sup><sub>2</sub>(μ<sub>3</sub>-O)<sub>2</sub>(O<sub>2</sub>C<sup><i>t</i></sup>Bu)<sub>10</sub>]<sup>2–</sup> molecules
(where Ln<sup>III</sup> = Y, Gd, Tb, Dy, Ho, and Er) has been synthesized
and characterized through single-crystal X-ray diffraction, SQUID
magnetometry, and ab initio calculations. All dysprosium- and some
erbium-containing tetramers showed frequency-dependent maxima in the
out-of-phase component of the susceptibility associated with slow
relaxation of magnetization, and hence, they are single-molecule magnets
(SMMs). AC susceptibility measurements have shown that the SMM behavior
is entirely intrinsic to the Dy and Er sites and the magnitude of
the energy barrier is influenced by the interactions between the 4f
and the 3d metal. A trend is observed between the strength of the
3d-4f exchange interaction between and the maximum observed in the χ″<sub>M</sub>(<i>T</i>)
Wells–Dawson Cages as Molecular Refrigerants
Five clusters with the general formula
[Ni<sub>6</sub>Gd<sub>6</sub>(μ<sub>3</sub>-OH)<sub>2</sub>(μ<sub>2</sub>-OAc)<sub>2</sub>(O<sub>3</sub>PR)<sub>6</sub>(O<sub>2</sub>C<sup><i>t</i></sup>Bu)<sub>16</sub>], where R = methyl
(<b>1</b>), phenyl
(<b>2</b>), <i>n</i>-hexyl (<b>3</b>), benzyl
(<b>4</b>), <i>n</i>-octyl (<b>5</b>), have
been prepared. All of the clusters have a {Ni<sub>6</sub>Gd<sub>6</sub>P<sub>6</sub>} core that can be related to the Wells–Dawson
ion. We have also prepared analogues where the gadolinium is replaced
with diamagnetic yttrium: [Ni<sub>6</sub>Y<sub>6</sub>(μ<sub>3</sub>-OH)<sub>2</sub>(μ<sub>2</sub>-OAc)<sub>2</sub>(O<sub>3</sub>PR)<sub>6</sub>(O<sub>2</sub>C<sup><i>t</i></sup>Bu)<sub>16</sub>] (R = methyl (<b>6</b>), <i>n</i>-hexyl (<b>7</b>), benzyl (<b>8</b>), <i>n</i>-octyl (<b>9</b>)), allowing the magnetic exchange within the
{Ni<sub>3</sub>} units to be analyzed by modeling as the sum of two
noninteracting isosceles triangles. The variation in the magnetic
entropy changes for magnetization (−Δ<i>S</i><sub>M</sub>) among compounds <b>1</b>–<b>5</b> could be attributed not only to the molecular weight of the compounds
but also to intramolecular magnetic interactions
Wells–Dawson Cages as Molecular Refrigerants
Five clusters with the general formula
[Ni<sub>6</sub>Gd<sub>6</sub>(μ<sub>3</sub>-OH)<sub>2</sub>(μ<sub>2</sub>-OAc)<sub>2</sub>(O<sub>3</sub>PR)<sub>6</sub>(O<sub>2</sub>C<sup><i>t</i></sup>Bu)<sub>16</sub>], where R = methyl
(<b>1</b>), phenyl
(<b>2</b>), <i>n</i>-hexyl (<b>3</b>), benzyl
(<b>4</b>), <i>n</i>-octyl (<b>5</b>), have
been prepared. All of the clusters have a {Ni<sub>6</sub>Gd<sub>6</sub>P<sub>6</sub>} core that can be related to the Wells–Dawson
ion. We have also prepared analogues where the gadolinium is replaced
with diamagnetic yttrium: [Ni<sub>6</sub>Y<sub>6</sub>(μ<sub>3</sub>-OH)<sub>2</sub>(μ<sub>2</sub>-OAc)<sub>2</sub>(O<sub>3</sub>PR)<sub>6</sub>(O<sub>2</sub>C<sup><i>t</i></sup>Bu)<sub>16</sub>] (R = methyl (<b>6</b>), <i>n</i>-hexyl (<b>7</b>), benzyl (<b>8</b>), <i>n</i>-octyl (<b>9</b>)), allowing the magnetic exchange within the
{Ni<sub>3</sub>} units to be analyzed by modeling as the sum of two
noninteracting isosceles triangles. The variation in the magnetic
entropy changes for magnetization (−Δ<i>S</i><sub>M</sub>) among compounds <b>1</b>–<b>5</b> could be attributed not only to the molecular weight of the compounds
but also to intramolecular magnetic interactions