103 research outputs found
An improved transmitter system to accurately measure wet-bulb temperature of air
A cost-effective measurement of wet-bulb temperature of air has great benefits to fulfill a growing demand of industry,
cultivation agriculture, and medication. Applying an appropriate algorithm to wet-bulb temperature of air measurement
can effectively improve the accuracy and speed of its measurement. The study aims to research how an improved transmitter system along with the latent heat–based iteration algorithm is used to precisely measure wet-bulb temperature of
air. The work consists of (1) simulation of the iteration algorithm and (2) validation via experimental protocol. The simulation results through latent heat–based iteration algorithm were in good agreement (R2
5 0.99) with the reference. The
performance of the improved wet-bulb temperature of air transmitter system was tested by a latent heat–based iteration algorithm experimental setup. The experimental results demonstrate that the improved wet-bulb temperature of
air in a good consistency with commercial wet-bulb temperature of air in a range of temperature (15C–34C) and relative humidity (28.8%–76.2%). The Bland–Altman plot also shows that the mean value and the standard deviation of the
differences between these two systems are 0.14C and 0.29C, respectively, which indicates that the improved wet-bulb
temperature of air has a good agreement as well. Compared with the commercial wet-bulb temperature of air transmitter system, an advanced processor (STM32F103C8T6) and real-time operating system was applied in the improved wetbulb temperature of air transmitter system. The experimental results show that its measurement accuracy is closer to
the previous study. This study provides an alternative and cost-effective solution to accurately and real-time measure
wet-bulb temperature of ai
Noncentrosymmetric Inorganic Open-Framework Chalcohalides with Strong Middle IR SHG and Red Emission: Ba<sub>3</sub>AGa<sub>5</sub>Se<sub>10</sub>Cl<sub>2</sub> (A = Cs, Rb, K)
Novel SHG effective inorganic open-framework chalcohalides,
Ba<sub>3</sub>AGa<sub>5</sub>Se<sub>10</sub>Cl<sub>2</sub> (A = Cs,
Rb and
K), have been synthesized by high temperature solid state reactions.
These compounds crystallize in the tetragonal space group <i>I</i>4̅ (No.82) with <i>a</i> = <i>b</i> = 8.7348(6) – 8.6341(7) Å, <i>c</i> = 15.697(3)
– 15.644(2) Å, <i>V</i> = 1197.6(3) –
1166.2(2) Ã…<sup>3</sup> on going from Cs to K. The polar framework
of <sup>3</sup><sub>∞</sub>[Ga<sub>5</sub>Se<sub>10</sub>]<sup>5–</sup> is constructed by nonpolar GaSe<sub>4</sub><sup>5– </sup>tetrahedron (T1) and polar supertetrahedral cluster Ga<sub>4</sub>Se<sub>10</sub><sup>8–</sup> (T2) in a zinc-blende topological
structure with Ba/A cations and Cl anions residing in the tunnels.
Remarkably, Ba<sub>3</sub>CsGa<sub>5</sub>Se<sub>10</sub>Cl<sub>2</sub> exhibits the strongest intensity at 2.05 μm (about 100 times
that of the benchmark AgGaS<sub>2</sub> in the particle size of 30–46
μm) among chalcogenides, halides, and chalcohalides. Furthermore,
these compounds are also the first open-framework compounds with red
photoluminescent emissions. The Vienna ab initio theoretical studies
analyze electronic structures and linear and nonlinear optical properties
PbMnIn<sub>2</sub>S<sub>5</sub>: Synthesis, Structure, and Properties
The first manganese member in a Pb–M–In–Q
system, PbMnIn<sub>2</sub>S<sub>5</sub>, has been discovered by a
high-temperature solid-state reaction. It adopts a Sr<sub>2</sub>Tl<sub>2</sub>O<sub>5</sub> structure type in orthorhombic space group <i>Cmcm</i> (No. 63) with <i>a</i> = 3.896(2) Ã…, <i>b</i> = 12.731(7) Ã…, <i>c</i> = 15.770(9) Ã…,
and <i>Z</i> = 1. The structure consists of corrugated layers
made by (In1/Mn1)ÂS<sub>6</sub> octahedra that are further interconnected
by chains of edge-sharing (In2/Mn2)ÂS<sub>6</sub> octahedra into a
three-dimensional framework; Pb<sup>2+</sup> cations are coordinated
in PbS<sub>8</sub> bicapped triangular prisms that are face-shared
along the <i>a</i> direction. The crystallographically distinguished
octahedrally coordinated 8<i>f</i> and 4<i>b</i> sites are disordered by Mn and In atoms. Such a structure allows
antiferromagnetic interactions between the high-spin Mn<sup>2+</sup> anions. The optical band gap is measured to be about 1.45 eV
Noncentrosymmetric Inorganic Open-Framework Chalcohalides with Strong Middle IR SHG and Red Emission: Ba<sub>3</sub>AGa<sub>5</sub>Se<sub>10</sub>Cl<sub>2</sub> (A = Cs, Rb, K)
Novel SHG effective inorganic open-framework chalcohalides,
Ba<sub>3</sub>AGa<sub>5</sub>Se<sub>10</sub>Cl<sub>2</sub> (A = Cs,
Rb and
K), have been synthesized by high temperature solid state reactions.
These compounds crystallize in the tetragonal space group <i>I</i>4̅ (No.82) with <i>a</i> = <i>b</i> = 8.7348(6) – 8.6341(7) Å, <i>c</i> = 15.697(3)
– 15.644(2) Å, <i>V</i> = 1197.6(3) –
1166.2(2) Ã…<sup>3</sup> on going from Cs to K. The polar framework
of <sup>3</sup><sub>∞</sub>[Ga<sub>5</sub>Se<sub>10</sub>]<sup>5–</sup> is constructed by nonpolar GaSe<sub>4</sub><sup>5– </sup>tetrahedron (T1) and polar supertetrahedral cluster Ga<sub>4</sub>Se<sub>10</sub><sup>8–</sup> (T2) in a zinc-blende topological
structure with Ba/A cations and Cl anions residing in the tunnels.
Remarkably, Ba<sub>3</sub>CsGa<sub>5</sub>Se<sub>10</sub>Cl<sub>2</sub> exhibits the strongest intensity at 2.05 μm (about 100 times
that of the benchmark AgGaS<sub>2</sub> in the particle size of 30–46
μm) among chalcogenides, halides, and chalcohalides. Furthermore,
these compounds are also the first open-framework compounds with red
photoluminescent emissions. The Vienna ab initio theoretical studies
analyze electronic structures and linear and nonlinear optical properties
Noncentrosymmetric Inorganic Open-Framework Chalcohalides with Strong Middle IR SHG and Red Emission: Ba<sub>3</sub>AGa<sub>5</sub>Se<sub>10</sub>Cl<sub>2</sub> (A = Cs, Rb, K)
Novel SHG effective inorganic open-framework chalcohalides,
Ba<sub>3</sub>AGa<sub>5</sub>Se<sub>10</sub>Cl<sub>2</sub> (A = Cs,
Rb and
K), have been synthesized by high temperature solid state reactions.
These compounds crystallize in the tetragonal space group <i>I</i>4̅ (No.82) with <i>a</i> = <i>b</i> = 8.7348(6) – 8.6341(7) Å, <i>c</i> = 15.697(3)
– 15.644(2) Å, <i>V</i> = 1197.6(3) –
1166.2(2) Ã…<sup>3</sup> on going from Cs to K. The polar framework
of <sup>3</sup><sub>∞</sub>[Ga<sub>5</sub>Se<sub>10</sub>]<sup>5–</sup> is constructed by nonpolar GaSe<sub>4</sub><sup>5– </sup>tetrahedron (T1) and polar supertetrahedral cluster Ga<sub>4</sub>Se<sub>10</sub><sup>8–</sup> (T2) in a zinc-blende topological
structure with Ba/A cations and Cl anions residing in the tunnels.
Remarkably, Ba<sub>3</sub>CsGa<sub>5</sub>Se<sub>10</sub>Cl<sub>2</sub> exhibits the strongest intensity at 2.05 μm (about 100 times
that of the benchmark AgGaS<sub>2</sub> in the particle size of 30–46
μm) among chalcogenides, halides, and chalcohalides. Furthermore,
these compounds are also the first open-framework compounds with red
photoluminescent emissions. The Vienna ab initio theoretical studies
analyze electronic structures and linear and nonlinear optical properties
Average changes in root dry weight at silking of maize from China (a, high planting density; b, water stress; c, N deficiency) and US Corn Belt (d, high planting density; e, water stress; f, N deficiency) in response to various stresses.
<p>The data derived from individual experiments from China and US Corn Belt were used. The values above columns indicate the reduction (%) under stresses compared with the optimum conditions. The solid line and square within the box represents the median and mean values of all data, the top and bottom edges of the box represent 75 and 25 percentiles and the top and bottom bars represent 95 and 5 percentiles of all data, respectively.</p
Comparisons of root dry weight at silking (silking RDW) between four dominant Chinese maize varieties and US pioneer variety.
<p>The solid line and square within the box represents the median and mean values of all data, the top and bottom edges of the box represent 75 and 25 percentiles and the top and bottom bars represent 95 and 5 percentiles of all data, respectively.</p
Root dry weight and root/shoot ratio at silking and maturity in unpaired data derived from field experiments using maize varieties in China and western countries.
<p>The solid line and square within the box represents the median and mean values of all data, the top and bottom edges of the box represent 75 and 25 percentiles and the top and bottom bars represent 95 and 5 percentiles of all data, respectively.</p
Root dry weight (RDW) and root/shoot ratio (R/S) at silking (76 DAS in 2011 and 82 DAS in 2012), and grain yield, total N uptake and N-use efficiency (NUE) at physiological maturity (148 DAS in 2011 and 153 DAS in 2012) of maize varieties from China (ZD 958 and XY 335) and US (P32D79).
<p>Field trials were performed at the Shangzhuang Experimental Station of the China Agricultural University, Beijing in 2011 and 2012.</p><p>Values in the column in each year followed by different letters had significant difference between varieties (<i>P</i>< 0.05).</p><p>Root dry weight (RDW) and root/shoot ratio (R/S) at silking (76 DAS in 2011 and 82 DAS in 2012), and grain yield, total N uptake and N-use efficiency (NUE) at physiological maturity (148 DAS in 2011 and 153 DAS in 2012) of maize varieties from China (ZD 958 and XY 335) and US (P32D79).</p
Correlation between the maize root/shoot ratio and nitrogen use efficiency (NUE) at silking.
<p>Only data published with root/shoot ratio at silking, grain yield at maturity and total N fertilizer were used in this analysis. Open circles indicate the results from Chinese farmlands and closed circles indicate data from western countries.</p
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