3 research outputs found
Residence Time Distribution in an Asymmetrical Twin-Screw Extruder
Residence time distribution (RTD) is an important parameter
for
characterizing axial conveying and mixing in a twin-screw extruder
(TSE). This work studies the RTD and flow patterns in an asymmetrical
TSE (ATSE) using a transparent barrel for visualization. The RTD of
an aqueous solution of sodium carboxymethyl cellulose is measured
by using red fine sand particles as tracers, collecting them by a
moving thin film at the die exit, and counting them for further statistical
calculation. The effects of the screw configuration, screw speed,
and feed rate are considered. When the geometrical dimensions and
operating parameters are identical, the mean residence time t̅ in the ATSE is larger than those in a classical
(symmetrical) TSE. This is a signature of backflow occurring in the
intermeshing regions through the radial gaps between the low flight
and the inner wall of the barrel. It is confirmed by particle image
velocimetry. Moreover, a response surface model is developed to quantify
the effects of the screw configuration and operating parameters on t̅
One-Pot Synthesis of Arylketones from Aromatic Acids via Palladium-Catalyzed Suzuki Coupling
A palladium-catalyzed
one-pot procedure for the synthesis of aryl
ketones has been developed. Triazine esters when coupled with aryl
boronic acids provided aryl ketones in moderate to excellent yields
(up to 95%) in the presence of 1 mol % Pd(PPh<sub>3</sub>)<sub>2</sub>Cl<sub>2</sub> for 30 min
Coherent Random Lasing in Colloidal Quantum Dot-Doped Polymer-Dispersed Liquid Crystal with Low Threshold and High Stability
High-concentration
(2–10 wt %) ZnCdSeS/ZnS alloyed quantum
dot-doped polymer-dispersed liquid crystals
(QD-PDLCs)
were prepared via ultraviolet (UV) curing. The QD-PDLC morphology
and resonance characteristics of a coherent random laser were investigated.
The doping concentration of the liquid crystal and quantum dots was
varied to investigate its effect on the lasing threshold, line width,
and stability with respect to the density and grain size of the liquid
crystal droplets inside the PDLC structure. Furthermore, the QD-PDLC
laser performance was influenced by the pump position and area because
of spatial localization of the random resonators. Moreover, the QD-PDLC
showed good long-term stability; after 15 days of laser excitation
(3 h/day), the laser output was maintained at 92% of the original
emission intensity. The random laser threshold was as low as 50 μJ/cm2 with the optimized preparation process, which suggested strong
potential for applications in polymer random fiber lasers, sensors,
and displays
