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81.
Alja Westerbeek Jan G.E. van Leeuwen Wiktor Szymański Ben L. Feringa Dick B. Janssen 《Tetrahedron》2012,68(37):7645-7650
Six different bacterial haloalkane dehalogenases were recombinantly produced in Escherichia coli, purified, and used to catalyse the conversion of prochiral short-chain dihaloalkanes and a meso dihaloalkane, yielding enantioenriched haloalcohols. A two-reaction one-enzyme process was established in which the desymmetrisation of a dihaloalkane is followed by kinetic resolution of the chiral haloalcohol that is produced in the first step. In case of 1,3-dibromo-2-methylpropane and 1,3-dibromo-2-phenylpropane, an increase of the enantiomeric excess of the respective haloalcohol was observed in time, leading to ee values of >97%, with analytical yields of 24 and 52%, respectively. The results show that haloalkane dehalogenases can be used for the production of highly enantioenriched haloalcohols and that in some cases product enantiopurity can be improved by allowing a two-step one-enzyme tandem reaction. 相似文献
82.
Władysław Piotrowski Koen Lodefier Slawomir Kubacki Witold Elsner Erik Dick 《Flow, Turbulence and Combustion》2008,81(3):369-394
The present paper evaluates two unsteady transition modelling approaches: the prescribed unsteady intermittency method PUIM,
developed at Cambridge University and the dynamic unsteady intermittency method developed at Ghent University. The methods
are validated against experimental data for the N3-60 steam turbine stator profile for steady and for unsteady inlet flow
conditions. The characteristic features of the test case are moderately high Reynolds number and high inlet turbulence intensity,
which causes bypass transition. The tested models rely both on the intermittency parameter and are unsteady approaches. In
the prescribed method, the time-dependent intermittency distribution is obtained from integral relations. In the dynamic method,
the intermittency distribution follows from time-dependent differential equations. For unsteady computations, self-similar
wake profiles are prescribed at the inlet of the computational domain. Joint validation of the prescribed and the dynamic
unsteady intermittency models against experimental data shows that both methods are able to reproduce the global features
of the periodical evolution of the boundary layer under the influence of a periodically impinging wake. The overall quality
of the dynamic method is better than that of the prescribed method. 相似文献
83.
Rainer Dick 《International Journal of Theoretical Physics》1997,36(9):2005-2012
I examine the potential of a pointlike particle carrying SU (N
c) charge in a gauge theory with a dilaton. The potential depends on boundary conditions imposed on the dilaton: For a dilaton
that vanishes at infinity the resulting potential is a regulatized Coulomb potential of the form (r+r
ϕ)−1, withr
ϕ, inversely proportional to the decay constant of the dilaton. Another natural constraint on the dialaton ϕ is independence
of (1/g
2) exp(ϕ/fϕ) from the gauge couplingg. This requirement yields a confining potential proportional tor. 相似文献
84.
In this paper, we give a formula for computing the number of different planat embeddings of any planar biconnected graph. The enumeration method used in deriving the formula readily gives rise to efficient algorithms for the ranking, unranking and random generation of embeddings of the given graph. We also give linear time algorithms for checking planarity and constructing any particular embedding. 相似文献
85.
86.
E. Dick 《国际流体数值方法杂志》1988,8(3):317-326
The flux-vector splitting method is applied to the convective part of the steady Navier-Stokes equations for incompressible flow. By the use of partial upwind differences in the split first-order part and central differences in the second-order part, a set of discrete equations is obtained which can be solved by vector variants of classical relaxation schemes. It is shown that accurate results can be obtained on one of the GAMM backward-facing step test problems. 相似文献
87.
88.
89.
We study the problem of multivariate integration and the construction of good lattice rules in weighted Korobov spaces with
general weights. These spaces are not necessarily tensor products of spaces of univariate functions. Sufficient conditions
for tractability and strong tractability of multivariate integration in such weighted function spaces are found. These conditions
are also necessary if the weights are such that the reproducing kernel of the weighted Korobov space is pointwise non-negative.
The existence of a lattice rule which achieves the nearly optimal convergence order is proven. A component-by-component (CBC)
algorithm that constructs good lattice rules is presented. The resulting lattice rules achieve tractability or strong tractability
error bounds and achieve nearly optimal convergence order for suitably decaying weights. We also study special weights such
as finite-order and order-dependent weights. For these special weights, the cost of the CBC algorithm is polynomial. Numerical
computations show that the lattice rules constructed by the CBC algorithm give much smaller worst-case errors than the mean
worst-case errors over all quasi-Monte Carlo rules or over all lattice rules, and generally smaller worst-case errors than
the best Korobov lattice rules in dimensions up to hundreds. Numerical results are provided to illustrate the efficiency of
CBC lattice rules and Korobov lattice rules (with suitably chosen weights), in particular for high-dimensional finance problems. 相似文献
90.
Dick Bebelaar 《Chemical physics》1974,3(2):205-216
A nanosecond laser spectrometer consisting of a 3nsec ruby/Nd PTM laser, fast detection system and high brightness analysing source is described. An analysis of the geometry considerations is given for crossed beam and collinear arrangement. The excited-state absorption spectra of naphthalene in 3MP at 85°K and 293°K from 14000 to 30000 cm?1 are given. The results provide a direct method to evaluate the quantum yields for fluorescence φf and intersystem crossing φT. Also the excited-state absorption spectra of anthracene in PMM from 16000 to 26000 cm?1 and in 3MP from 26000 to 36000 cm?1 are reported. 相似文献