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Quasi-steady State Off-cut Recycle Strategy in Binary

Quasi-steady State Off-cut Recycle Strategy in Binary Batch Distillation

Quasi-steady state temperature distribution and calculated temperature

Quasi-steady-state

Quasi-steady-state tunnelling recombination profile for Vk centres in KCl calculated at 180 K .

Quasi-steady-state tunnelling recombination profile for Vt centres in KC1 calculated at 180 K .

Quasi-surface molecule interaction between two doubly occupied orbitals, resulting in a bonding interaction due to electron backdonation from the antibonding fragment orbital to the Fermi level.

Quasi-surface molecule limit solutions of fj B as calculated according to Eq..

Quasi-symmetrical bimolecular reactions with dissociative mechanisms and termolecular intermediates

Quasi-three-dimensional, point projection image of ferritin on tungsten at 30 K before applying a critical desorption field of ferritin. The image is a digital composite of seven images taken at different field strengths, thus at different depths of the covered methane layer.

Quasi-two-dimensional Turing patterns in the CDIMA reaction. Feed concentrations

Quasi-viscosity of selenium glass in the transformation interval ioo tieans

Quasibinary cross-sections in the ternary system Sn—Te—I . Thr -phase equilibria

Quasibinary phase diagram of Sr6Ta20n -Sr6Ta20n-H20, F 20 0.02 atm ,

Quasiclassical and full Cl energy curves for H2 using the 6-3IG basis set.

Quasiclassical cross-sections for the reaction D -I- H2 .

Quasiclassical cross-sections for the reaction D H2 .

Quasicombined cycle t-S diagram on pure C02, bcde opa topping Rankine-like part, oe fh e h ilmo bottoming brayton-like part

Quasicrystal built by the mterpenetration principle. Top

Quasicrystalline particles in Al93Fe3Cr2Ti2 melt-spun ribbon, dark field image

Quasicrystalline structures observed in BCP SA.

Quasicrystals

Quasielastic broadening of the neutron scattering peak observed in the paraelectric phase for the copolymer 60 40. The points represented the experimental results with their statistical error bar. The solid line is the Lorentzian function obtained after the deconvolution process described in the text

Quasielastic components observed in nonadecanelurea at room temperature in tandem with Fabry-Perot interferometers. The central intensity is due to the longitudinal Brillouin doublets. The

Quasielastic neutron scattering intensities at wavevectors offset to varying degrees from the ordering vector



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