text:
\section{INTRODUCTION}
From the pioneering work of Alder et al. \cite{alder1,alder2} who used
molecular dynamics to investigate transport properties of hard-spheres, this
method has proved to be a successful tool for the development and test of theories
\cite{hansen}; examples are the discovery of the hydrodynamic long-time tail
\cite{alder3} or the development of advanced kinetic theories
\cite{furtado,keyes}. Due to the increasing computer power, molecular dynamics is today
an interesting option for studying \cite{macdowell} and predicting \cite{McCabe}
transport properties. In particular, for predictions of transport properties of
liquids, where no satisfactory analytical theory exists, molecular dynamics
is the most suitable available method.

Molecular simulation is also attractive because it allows rigorous testing of
theories and models, and systematically studying the influence of any molecular
parameter on any transport property. Although real fluids usually consist of polar
non-spherical molecules, most extensive studies on transport properties have been
done on the basis of very simple molecular models, e.g. hard sphere potential
\cite{alder2,erpenbeck1}, square well potential
\cite{michels1,michels2,michels3,michels4,michels5,michels6}, steeply repulsive
potential \cite{heyes1}, or spherical Lennard-Jones potential \cite{heyes1,heyes2}.

In the present work, a systematic study on the influence of elongation and quadrupole
momentum on self-diffusion coefficient, shear viscosity, and thermal conductivity of
two-center Lennard-Jones plus point quadrupole (2CLJQ) fluids is carried out in the liquid
region covering a broad range of temperature and density. This work is based on the knowledge of accurate
vapor-liquid equilibria of 2CLJQ fluids from previous publications of Stoll et al.
\cite{stoll1,stoll2}. Molecular simulations are carried out along the bubble line
and in the homogeneous liquid for different
models over a grid of reduced temperatures and densities.
Thus, a consistent comparison of the transport properties of different models is possible
and subsequently the effect of elongation and quadrupole momentum can be identified.

It has been recently shown that the 2CLJQ model is not only an interesting model fluid but also suited for
accurately describing the properties of real fluids. Vapor-liquid equilibria of 35 pure substances were
successfully modeled with that approach \cite{vrabec,stolljcp}. Also for mixtures good results were
achieved \cite{stoll2,vrabec2,stolla}. Furthermore, properties such as Joule-Thomson inversion \cite{vrabec3},
self-diffusion and binary Maxwell-Stefan diffusion coefficients \cite{fernandez2}, shear viscosity, and
thermal conductivity \cite{fernandez3} were reliably predicted by 2CLJQ models which were parameterized
using vapor-liquid equilibrium data only.

\section{MOLECULAR MODEL}
The intermolecular interactions are represented by the two-center Lennard-Jones plus point quadrupole (2CLJQ) potential.
The 2CLJQ potential is pairwise additive and consists out of two identical Lennard-Jones sites a
distance $L$ apart (2CLJ) plus a point quadrupole of momentum $Q$ placed in the geometric center of the
molecule oriented along the molecular axis connecting the two Lennard-Jones (LJ) sites. The interaction
energy of two molecules $i$ and $j$ is given by

\begin{equation}\label{tpoten}
u^{\rm 2CLJQ}_{ij} = \sum_{a=1}^{2} \sum_{b=1}^{2} 4\epsilon \left[ \left( \frac{\sigma}{r_{ab}}
\right)^{12} - \left( \frac{\sigma}{r_{ab}} \right)^6 \right] + u_{\rm Q}.
\end{equation}

Here, $r_{ab}$ is one of the four LJ site-site distances; $a$ counts the two LJ sites of molecule
$i$, $b$ counts those of molecule $j$. The LJ parameters $\sigma$ and $\epsilon$ represent size
and energy, respectively. The contribution of a point quadrupole is given by \cite{graygubb}

\begin{eqnarray}\label{qpoten}
u_{\rm Q}=\frac{1}{4 \pi \epsilon_0}\frac{3}{4} \frac{Q^2}{\left|\textbf{r}_{ij}\right|^5}
\left[ 1-5 \left( c_i^2+c_j^2 \right) -15 c_i^2 c_j^2 + 2 \left( s_i s_j c - 4 c_i c_j
\right)^2 \right],
\end{eqnarray}

with $c_k={\rm cos} \theta_k$, $s_k={\rm sin} \theta_k$, and $c={\rm cos}
\phi_{ij}$. Herein, $\textbf{r}_{ij}$ is the center-center distance vector of two
molecules $i$ and $j$. $\theta_i$ is the angle between the axis of the molecule
$i$ and the center-center connection line and $\phi_{ij}$ is the azimuthal angle
between the axis of molecules $i$ and $j$. Finally, $\epsilon_0$ is the electric
constant in 8.854187817$\cdot$10$^{-12}$ C$^2$/(J m).

A specific 2CLJQ model, e.g. for a real fluid like nitrogen, is fully
determined by five parameters: $\sigma$, $\epsilon$, $L$, $Q$ \cite{vrabec,stolljcp} and the
molecular mass $m$. But in molecular simulation all relevant physical
properties can be treated in a reduced form. Here, they are related to $\sigma$, $\epsilon$,
and $m$, so that the reduced results are valid for all combinations of these three
parameters. In this form, only two molecular parameters remain, i.e. reduced elongation
$L^*=L/\sigma$ and reduced squared quadrupole momentum
$Q^{*2}=Q^{2}/(4\pi\epsilon_0\epsilon\sigma^5)$.
Henceforth, "squared" will be omitted in the text for brevity.

\section{TRANSPORT COEFFICIENTS}

Transport properties were calculated by equilibrium molecular dynamics simulation and the Green-Kubo
formalism \cite{green,kubo}. In this formalism, transport coefficients are obtained by integrating time
autocorrelation functions of the corresponding microscopic fluxes.

The self-diffusion coefficient $D$ is a measure for the mobility of individual molecules within a fluid.
It is calculated by integration of the single molecule velocity autocorrelation function
\cite{gubbins1,steele}

\begin{equation}\label{self}
D=\frac{1}{3N}\int_0^{\infty} \di t~\big\langle \mathbf{v}_k(t)\cdot \mathbf{v}_k(0) \big\rangle,
\end{equation}

where $\mathbf{v}_k(t)$ expresses the velocity vector of molecule $k$ at some time $t$, and $<$...$>$
denotes the ensemble average. Eq. (\ref{self}) yields the self-diffusion coefficient averaging over $N$ molecules.

The shear viscosity $\eta$, as defined in Newton's "law" of viscosity, describes the resistance of a fluid
to shear forces. It refers to the resistance of an infinitesimal volume element to shear at constant
volume \cite{baron}. The shear viscosity can also be related to momentum transport under the influence of
velocity gradients. From a microscopic point of view, the shear viscosity can be calculated by integration
of the time-autocorrelation function of the off-diagonal elements of the stress tensor, i.e. $J_p^{xy}$
\cite{gubbins1,steele}
\smallskip
\begin{equation}\label{shear}
\eta=\frac{1}{Vk_BT}\int_{0}^{\infty} \di t~\big\langle J^{xy}_p(t)\cdot J^{xy}_p(0)\big\rangle,
\end{equation}
where $V$ is the molar volume, $k_B$ is the Boltzmann constant, $T$ the temperature, and $<...>$ denotes
the ensemble average. The statistics of the ensemble average in Eq. (\ref{shear}) can be improved using
all three independent off-diagonal elements of the stress tensor, i.e. $J_p^{xy}$, $J_p^{xz}$, and
$J_p^{yz}$. For a pure fluid, the component $J_p^{xy}$ of the microscopic stress tensor $\textbf{J}_p$ is
given by \cite{evans1}
\bigskip
\begin{equation}\label{shear_t}
J_p^{xy}=\sum_{i=1}^N m v_{i}^x v_{i}^y -\frac{1}{2}\sum_{i=1} ^N \sum_{j \neq i}^N \sum_{k=1}^3
\sum_{l=1}^3 r_{i j}^x \frac{\partial u_{ij}}{\partial r_{k l}^y}.
\end{equation}
Here, $i$ and $j$ are the molecular indices. Lower indices $l$ and $k$ count all sites, including the
quadrupolar site, and the upper indices $x$ and $y$ denote the vector component, e.g. for velocity $v_i^x$
or center-center distance $r_{ij}^x$.

The thermal conductivity $\lambda$, as defined in Fourier's "law" of heat conduction, characterizes the
capability of a substance for molecular transport of energy driven by temperature gradients. It can be
calculated by integration of the time-autocorrelation function of the elements of the microscopic heat
flow $J^x_q$ and is given by \cite{gubbins1,steele}
\bigskip
\begin{equation}\label{termalc}
\lambda=\frac{1}{Vk_BT^2} \int_{0}^{\infty} \di t~\big\langle J^x_q(t)\cdot J^x_q(0) \big\rangle.
\end{equation}

The expression for the heat flow $\textbf{J}_q$ in pure fluids has been derived by Evans \cite{evans1} and
is given by
\bigskip
\begin{multline}
\label{qflux} \textbf{J}_q=\frac{1}{2} \sum_{i=1}^N \big((m v_i^2+ \textbf{w}_i \textbf{I}_i
\textbf{w}_i+\sum_{j \neq i}^N u_{ij} )\cdot \textbf{v}_i \big) -\frac{1}{2}\sum_{i=1}^N \sum_{j \neq i}^N
\sum_{k=1}^{3} \sum_{l=1}^{3} \textbf{r}_{ij} \cdot \big( \textbf{v}_i \frac{\partial u_{ij}}{\partial
\textbf{r}_{kl}}+\textbf{w}_i \mathbf{\Gamma}_{ij} \big),
\end{multline}

where $\textbf{w}_i$ is the angular velocity vector of molecule $i$, $\textbf{I}_i$ its matrix of angular
momentum of inertia, and $u_{ij}$ the intermolecular potential energy. The torque $\mathbf{\Gamma}_{ij}$
refers to a reference frame with origin in the molecular center of mass.  As for shear viscosity, all
three independent heat flow directions $J_q^x$, $J_q^y$, and $J_q^z$, can be used to improve the
statistics of Eq. (\ref{termalc}).

All results of this study were obtained and are presented in the reduced form, i.e. in relation to the
molecular parameters size, energy, and mass. The reduced transport properties are defined by:
$D^*=D/\sigma\sqrt{m/\epsilon}$, $\eta^*=\eta\sigma^2/\sqrt{m\epsilon}$,
$\lambda^*=\lambda\sigma^2 /k_B\sqrt{m/\epsilon}$. Relevant static thermodynamic properties, temperature
$T^*=Tk_B/\epsilon$ and number density $\rho^*=\rho\sigma^3$, are also reduced in the same sense. For the sake of
brevity, "reduced" will be omitted in the following.

\section{INVESTIGATED MODELS AND STATES}
In the present work, 30 different model fluids were studied, where each fluid is fully
determined by one combination of elongation $L^*$ and quadrupole momentum $Q^{*2}$.
Simulations at 16 liquid state points were carried out for each model fluid.
In Figs. \ref{fig1} and \ref{fig2} four selected systems are shown; they
illustrate the covered thermodynamic states and the influence of elongation and
quadrupole momentum on the thermodynamic behavior of the fluids \cite{stoll1}. As Fig.
\ref{fig1} shows, critical temperature and density increase with increasing
quadrupole momentum. On the other hand, Fig. \ref{fig2} shows that these critical
properties decrease with increasing elongation. Such a behavior can also
be seen for linear Kihara fluids \cite{vega}.

The studied model fluids have elongations that vary from $L^*=0$, i.e. spherical
molecules, to 0.8, i.e. strongly elongated dumbbell-shaped molecules, in six
steps. The odd value $L^*=0.505$ was chosen to cover the same model fluids
as the previous work on vapor-liquid equilibria \cite{stoll1}.
Five quadrupole momenta were studied that range from $Q^{*2}=0$ to 4 with
increments of unity.
The upper limit of 4 is sufficient to describe strongly quadrupolar
real fluids, eg. CO$_2$ with $Q=-3.7938$ D\r{A} ($Q^{*2}=3.3037$),
C$_2$H$_2$ with $Q=5.0730$ D\r{A} ($Q^{*2}=4$), or
C$_2$F$_4$ with $Q=-7.0332$ D\r{A} ($Q^{*2}=3.9272$) \cite{vrabec}.

For the sake of consistency, transport properties for
spherical fluids ($L^*$=0) were treated as two superimposed Lennard-Jones
sites. This implies, that the temperature has to be divided by 4 as well as the
quadrupole momentum, if a direct comparison with a one-center
Lennard-Jones fluid is to be made. The corresponding conversion of $D^*$,
$\eta^*$, and $\lambda^*$ for these spherical fluids is obtained dividing the
present data by 2.

As temperatures and number densities in vapor-liquid equilibrium
vary strongly with the molecular parameters, it is useful
to introduce another reduced form for representing the temperature
$T_R$=$T^*/T_c^*$ and the density $\rho_R$=$\rho^* /\rho_c^*$.
Here, $T_c^*$ is the critical temperature and $\rho_c^*$ the critical density of the individual
2CLJQ fluid; values for $T_c^*$ and $\rho_c^*$ were taken from \cite{stoll1}.
For each fluid, the
considered reduced temperatures along the bubble line range from $T_R$=0.6 to 0.9
with increments of $\Delta T_R$=0.1. In addition to those four points, another
12 points in the homogeneous liquid region were simulated, cf. Figs.
\ref{fig1} and \ref{fig2}. These points were selected on isochores starting from
each bubble point with temperature increments of $\Delta T_R$=0.1. In this way,
also isothermal data was generated.

\section{SIMULATION DETAILS}
Equilibrium molecular dynamics simulations were performed in a cubic box of volume
$V$ containing $N=500$ molecules. The cut-off radius was set to $r_{c}=5 \sigma $,
otherwise to half of the box length. The molecules in the fluid were assumed to
have no preferential relative orientations outside of the cut-off sphere. For the
calculation of the LJ long range corrections, orientational averaging was done
with equally weighted relative orientations as proposed by Lustig \cite{lustig}.
The assumption of no preferential relative orientations beyond the cut-off sphere
implies that no long range corrections for the quadrupolar interactions are needed
since they disappear. This is a reasonable assumption as demonstrated by Streett
and Tildesley \cite{strett}. The simulations were started with the molecules in a
face centered cubic lattice with random velocities, the total momentum of the
system was set to zero, and Newton's equations of motion were solved with the Gear
predictor-corrector integration scheme of fifth order \cite{haile}. The time step
for this algorithm was set to $\Delta t \sqrt{\epsilon / m}/\sigma=0.0005$.
Self-diffusion coefficient, shear viscosity, and thermal conductivity were
calculated in the microcanonical $NVE$ ensemble using Eqs. (\ref{self}) to
(\ref{qflux}). The simulations were equilibrated in the canonical $NVT$ ensemble
between $100~000$ to $150~000$ time steps. After equilibration, the thermostat was
turned off and the simulation continued in the $NVE$ ensemble where the transport
properties were calculated.
Because of the lack of a thermostat, the temperature was fluctuating with a
maximum drift of 3 \%.

Statistical
uncertainties were estimated using the standard deviation of four independent
simulations of $3~000$ independent autocorrelation functions. In order to achieve
independence between autocorrelation functions, a time span of 0.1 in reduced units was left
between consecutive autocorrelation functions. This time span was consistent with
a decay to less than $1/e$ of the normalized velocity autocorrelation function in
several pilot runs. It is a conservative choice, when a compromise between
simulation time and accuracy has to be done. Fig. \ref{fig3} shows the normalized
autocorrelation functions (ACF) from top to bottom for self-diffusion coefficient,
shear viscosity, and thermal conductivity for the 2CLJQ fluid with $L^*$=0.2 and
$Q^{*2}$=1 for the bubble point at 70 \% of its critical temperature
($T_c^*=4.388$), where the bubble density is $\rho^*=0.6573$. The vertical line
denotes $t^*$=0.1, the horizontal line the value $1/e$. All three ACF fulfill the
criterion of independence between consecutive correlations, although they show a
quite different decay. Another important issue is the
significant length of the autocorrelation functions, or equivalently, how long
they must be integrated. Fig. \ref{fig4} shows the integrals from top to bottom
for self-diffusion coefficient, shear viscosity, and thermal conductivity. In
principle, the integration of the ACF must be carried out until the integral shows
stationary behavior. In practice, the convergence of the self-diffusion integral
is difficult to guarantee for all conditions, because of the long time behavior
\cite{alder3} with a decay proportional to $t^{3/2}$. A similar problem is present
regarding the autocorrelation function for shear viscosity close to the
fluid-solid transition \cite{alder2,levesque1,schoen,erpenbeck2}. Here it
was handled by a long evaluation ($\Delta t^*$ = 1.25) of the ACF, as can be seen in Fig.
\ref{fig4}. The integrals converge to the final value at around 0.5,
afterwards the ACF fluctuate around zero, cf. Fig. \ref{fig3}, without effective
contribution to the integrals.

\section{RESULTS}
In this section, the simulation results for the transport coefficients are
presented. Numerical data for self-diffusion coefficient, shear viscosity, and
thermal conductivity are given in Table \ref{tab1a} for elongations from $L^*$=0
to 0.8 and quadrupole momenta from $Q^{*2}$=0 to 4. All data in Table \ref{tab1a}
correspond to state points along the bubble line for reduced temperatures
of $T_R$=0.6, 0.7, 0.8, and 0.9. The complete data set, with 12
additional state points in the liquid region for each fluid, is available in
\cite{fernandezt} and partially included in Figs. \ref{fig6}, \ref{fig7},
\ref{fig9}, \ref{fig10}, \ref{fig12}, and \ref{fig13}. The effects of elongation,
quadrupole momentum, temperature, and density are discussed in the following for
each transport coefficient separately.

The accuracy of the calculated transport properties decreases in the sequence
self-diffusion coefficient, shear viscosity, thermal conductivity. The high
accuracy of the self-diffusion coefficient, with error bars lower than 3 \%, is due to its
individual nature \cite{hansen}. Shear viscosity and thermal conductivity are
collective properties, consequently they show for the same simulation time and
system size larger uncertainties, that are around 8 and 12 \%, respectively. In most
simulations of the present work the autocorrelation functions of thermal
conductivity decay faster than those for shear viscosity, but fluctuate more.
Figs. \ref{fig3} and \ref{fig4} illustrate this.

Other factors that influence the accuracy of the reported data are elongation and
quadrupole momentum. In particular, at low temperatures, for fluids with large
anisotropy and strong quadrupole momentum, the transport coefficients show larger
simulation uncertainties.

In the following, the results are discussed for nine selected fluids, covering the
whole range of the two molecular parameters, from spherical ($L^*$=0) over elongated
($L^*$=0.505) to  strongly elongated ($L^*$=0.8) fluids with varying quadru\-pole
momentum of $Q^{*2}$=0, 2, and 4.
A subset of six fluids is taken in some cases only due to graphical reasons.

\subsection{Self-diffusion coefficient}
Figs. \ref{fig5a} and \ref{fig5} illustrate the self-diffusion coefficient along
the bubble line for nine selected fluids.
The results can either be discussed in terms of reduced density $\rho_R$
as in Fig. \ref{fig5a} or in terms of number density $\rho^*$ as in Fig. \ref{fig5}.
From Fig. \ref{fig5a} it can be seen that the regarded range of reduced density is similar
for all fluids, but significant deviations from the principle of corresponding states
are present also for the density.
At constant $T_R$, it can be discerned that the self-diffusion
coefficient decreases with both increasing elongation and quadrupole momentum.
A better visibility of the data (which is even more needed for the less accurate properties
shear viscosity and thermal conductivity) is obtained when plotted over number density in
Fig. \ref{fig5}. Therefore, this graphical representation is preferred in the following.

As Fig. \ref{fig5} shows, $D^*$ decreases with increasing number density along the bubble line
(where with increasing density also the temperature decreases). It is an important
result of the present study that the self-diffusion coefficient lies
roughly along the same line for a given elongation, independent of the quadrupole momentum.

Fig. \ref{fig6} shows the dependence of $D^*$ on number density
in the homogeneous liquid region at a constant reduced
temperature of $T_R$=0.9. Note that the density range is the same as in Fig.
\ref{fig5}. Along this isotherm $D^*$ decreases slightly hyperbolic
with increasing density,
resembling the behavior of $D^*$ along bubble lines for a given elongation.
Comparing $D^*$ along bubble lines with isothermal data for an identical density
variation, it is found that the density effect dominates with a contribution of 80 \%.

Fig. \ref{fig7} shows the dependence of the self-diffusion coefficient on
temperature at different constant densities for a subset of six fluids.
The isochores correspond to bubble densities at the reduced
temperature $T_R$=0.6, cf. Figs. \ref{fig1} and \ref{fig2}, which have similar values
in terms of $\rho_R$. Along the isochores, the
self-diffusion coefficient increases linearly with increasing temperature. The
gradients with respect to reduced temperature are almost constant for a given
elongation, where the slope is less steep for more elongated fluids. Such a linear
dependence of $D^*$ on temperature has also been reported by other authors for
Lennard-Jones fluids \cite{levesque2}, Kihara fluids \cite{macdowell}, and
two-center Lennard-Jones fluids \cite{singer}.

\subsection{Shear viscosity}
Fig. \ref{fig8} illustrates the shear viscosity along the bubble line for the nine selected fluids.
At constant $T_R$, it is found that the shear viscosity decreases with increasing elongation
but increases with increasing quadrupole momentum.
Again it is found that the results for a given elongation lie roughly along one line
independent of $Q^{*2}$, where, as expected, they increase with increasing number density.

The density dependence of shear viscosity in the homogeneous liquid region
is illustrated in Fig. \ref{fig9} at $T_R$=0.9.
Comparing the variation of $\eta^*$ along bubble lines and along
isotherms in the same way as for $D^*$, it is found for non-polar fluids that the
density effect is responsible for about 80 \% of the increase of $\eta^*$ along
the bubble line. For quadrupolar fluids, however, the temperature influence
becomes more important and its contribution is about 40 \%.

Fig. \ref{fig10} shows the dependence of shear viscosity on reduced temperature
for a subset of six fluids along isochores with similar values in terms of $\rho_R$.
As expected, shear viscosity decreases with increasing temperature.
Strongly quadrupolar fluids, with an about threefold higher shear viscosity
in the cold liquid, are more sensitive to temperature, exhibiting larger gradients.

\subsection{Thermal conductivity}
Fig. \ref{fig11} illustrates the thermal conductivity along the bubble line.
Again, the data lie roughly along single
lines for a given elongation, but considering simulation uncertainties not more than a
linear dependence can be discerned.
Thermal conductivity has the same basic trends like shear viscosity
as it decreases with increasing elongation but increases with increasing quadrupole momentum
at constant $T_R$.

Fig. \ref{fig12} shows the density dependence in the homogeneous liquid
at $T_R$=0.9. It can be seen that the curves resemble those
along bubble lines, underlining the dominating effect of density there. Similar results
have been reported by Tokumasu et al. \cite{tokumasu} who studied the non-polar
2CLJ potential but at different thermodynamic conditions. In their analysis,
Tokumasu et al. reduced $\lambda^*$ by critical temperature and critical density, to
isolate the effect of elongation and found that this type of reduced thermal
conductivity increases with increasing elongation.

Fig. \ref{fig13} shows isochoric data with similar values in terms of $\rho_R$ for a
subset of six fluids, where the effect of temperature on $\lambda^*$ is small.
Taking the statistical uncertainty and the scatter into account, hardly any trend
can be discerned. Experimental results \cite{slyusar1,slyusar2} show that thermal
conductivity at constant density increases with increasing temperature, but the
variation is very small in the liquid region. Moreover, the increase of $\lambda^*$
with increasing quadrupole momentum can be seen.

\section{CONCLUSION}
Equilibrium molecular dynamics simulation and the Green-Kubo
formalism were used to calculate self-diffusion coefficient, shear viscosity, and
thermal conductivity for 30 different anisotropic and quadrupolar model fluids.
A comprehensive data set was obtained for each fluid and property that covers
a substantial part of the liquid state.
The statistical uncertainty of the reported data varies according to
transport property. For self-diffusion coefficient data, it is less than 3 \%,
for shear viscosity and thermal conductivity it is around 8 and 12 \%,
respectively.

The three transport properties are dominated in the investigated liquid region
by the density: saturated liquid and isothermal
data for fluids with a given elongation but varying quadrupole momentum
lie roughly along single lines when plotted over number density.

However, all transport properties on the bubble line at a constant reduced temperature
are lower for fluids with larger elongation.
An increasing quadrupole momentum also leads to a lower
self-diffusion coefficient, the opposite is found for shear viscosity and
thermal conductivity.

Temperature influences all transport properties less than density. As expected,
along isochores, the self-diffusion coefficient increases with temperature, the shear
viscosity decreases, and for the thermal conductivity hardly any variation can
be discerned.

\clearpage

\noindent
{\bf List of symbols}

\begin{tabular}{ll}
$a$ & interaction site index \\
$b$ & interaction site index \\
$c$ & short notation for a trigonometric function \\
$D$ & self-diffusion coefficient \\
$i$ & molecule index \\
$j$ & molecule index \\
$J_p$ & element of the microscopic stress tensor \\
$J_q$ & element of the microscopic heat flow \\
$k$ & interaction site index \\
$k$ & molecule index \\
$k_B$ & Boltzmann constant \\
$l$ & interaction site index \\
$L$ & molecular elongation \\
$m$ & molecular mass \\
$N$ & number of molecules \\
$Q$ & molecular quadrupole momentum \\
$r$ & site-site distance \\
$r_{\rm c}$ & center-center cut-off radius \\
$s$ & short notation for a trigonometric function \\
$t$ & time \\
$T$ & temperature \\
$u$ & pair potential \\
$v$ & element of the velocity vector \\
$V$ & molar volume \\
$\Delta$ & increment \\
$\Delta t$ & integration time step\\
$\epsilon$ & Lennard-Jones energy parameter \\
$\epsilon_0$ & Electric constant \\
\end{tabular}

\begin{tabular}{ll}
$\eta$ & shear viscosity \\
$\theta$  & angle of nutation \\
$\lambda$ & thermal conductivity \\
$\rho$    & density \\
$\sigma$  & Lennard-Jones size parameter \\
$\phi$    & azimuthal angle \\
\end{tabular}

\noindent
\textbf{Vector properties} \\[0.1cm]
\begin{tabular}{ll}
$\textbf{I}$ & matrix of angular momentum of inertia \\
$\textbf{J}_p$ & microscopic stress tensor \\
$\textbf{J}_q$ & microscopic heat flow vector \\
$\textbf{r}$ & distance vector \\
$\textbf{v}$ & velocity vector \\
$\textbf{w}$ & angular velocity vector \\
$\mathbf{\Gamma}$ & torque vector \\
\end{tabular}

\noindent
\textbf{Subscript} \\[0.1cm]
\begin{tabular}{ll}
$a$ & interaction site index \\
$b$ & interaction site index \\
$c$ & property at critical point \\
$i$ & molecule index \\
$j$ & molecule index \\
Q & point quadrupole \\
$R$ & property reduced by critical value \\
2CLJQ & two-center Lennard-Jones plus point quadrupole \\
\end{tabular}

\noindent
\textbf{Superscript} \\[0.1cm]
\begin{tabular}{ll}
$x$ & cartesian direction \\
$y$ & cartesian direction \\
$z$ & cartesian direction \\
*   & property reduced by molecular parameters \\
\end{tabular}

\clearpage

\noindent
{\bf Acknowledgement}

We gratefully acknowledge financial support from Deutscher Akademischer Austauschdienst (DAAD).

\clearpage


Infinity Roofing Contractors is a full-service roofing, siding and gutter contractor. We provide free inspection and estimates to all of our clients. All of our free consultations will include photos of what was found during your inspection, as well as recommended course(s) of action. Our goal is to find the right solution for you based on your indication during this consultation. We never request payment in full until you indicate full satisfaction and we accept cash, check, major credit card and PayPal. We also offer financing for larger projects.
My roof was already old, I decided to replace it shortly after a hailstorm damaged it further. Tony came out on a weekday evening to inspect the roof himself, he pointed out damage and took the time to explain the different shingling and warranty options. I was able to replace my builder-grade shingling with 50-year shingles, my new roof looks a lot nicer, and Infinity kept the total cost within the total amount reimbursed by my insurance company - I only paid the deductible. Tony communicated each step of the way, his team was on time, they completed the work when he said they would, and completely cleaned up. Overall I was very happy with the final result and would definitely hire them again.


text:
Q: Linux is not showing correct hdd name In my system when I attach my USB HDD, it is showing it as sdc instead of sdb. I do not have any other HDD attached.
[root@localmirror ~]# ls /sys/block/
dm-0/ dm-1/ dm-2/ sda/  sdc/  sr0/

Am i missing something?

A: /dev/sdx is not the "correct hdd name", and you never should rely on a specific device node, especially for removable devices. You usually can rely on the UUID of the device/partition, or on the file system label (if any).
In /etc/fstab, instead of /dev/sdx you can specify UUID= or LABEL=
Additionally, there should be entries in /dev/disk/by-uuid and eventually /dev/disk/by-label, which should be links to the actual device nodes. So, for manual access, you may mount/dev/disk/by-uuid/<UUID> od /dev/disk/by-label/<LABEL>. To find out UUID and/or LABEL, just do ls -l /dev/disk/by-uuid and ls -l /dev/disk/by-label.

A: I have a couple of ideas:
1- sdb device is in reality the dm one
2- sdb device was created (before sdc detection) and then destroyed (after the sdc detection)
Further reading: I suggest you reading some documentations if you have not yet done it
e.g. http://www.tldp.org/HOWTO/Partition-Mass-Storage-Definitions-Naming-HOWTO/x99.html
http://tldp.org/HOWTO/Partition/devices.html

redpajama_set_name: RedPajamaStackExchange


Mirror candle holders are a common gift for any occasion and are a great way to add personality and style into your home decor. There is a wide selection of candle holder styles, shapes and colors, and they can be used indoors or outdoors. Most candlesticks are made of glass, but they can also be made of any kind of metal.
Tea light holders come in many different styles and colors. They are usually made of metal or colored mirror. Some quadruple holders are hung up on the walls while others are made to sit on tables, shelves or robes. Four-dimensional holders can only be used to hold candle light medium candles, and are available at most retailers. Outdoor mirror candle holders are also available and are a perfect gift for garden enthusiasts.
Block lights are large, round candles, so column candlesticks are usually tall and cylindrical. If you want to add a personal touch to a pillar candle holder gift, decorate a plain glass holder using printed paper and ribbon. Cut a strip of printed scrapbook paper that is the same in the length circumference of the mirror candle holders. The paper strip should be between 4 and 5 inches in width. Glue the paper around the holder and slide it out with your fingers to remove folds. Cut two strips of thin craft ribbon that is the same in the length of the circle of candle holder. Glue a strip around the top edge of the paper and the other strip around the bottom edge of the paper.
An assortment of shareworthy craft party such as a room. Pillows kitchen accents bath accessories candles and easy with nautical ship wheel to suit any occasion or holiday decorate for modern and functional candleholder sets. How to decorate with wall candle holders, table settings including plug in styleand at world market with wall sconce in french gold uttermost hailey. Candle holders with nautical ship wheels in a variety of ideas that are plenty of softness warmth and candle holders with beautiful and have twins neices that wont break the time. Your target redcard are having their. With accessories decorative boxes cottage style.
Since the driftwood planks mirror you can use old cameras and longlasting driftwood inch wood mimic the material used in our driftwood mirrors wall shelf blends driftwood candle holder cor. Offerte migliori per wall mirror back and peripherals get some nice candles how to discuss any interior design votive candles etc fantastic weathered driftwood accessories decor candle holder rustic reclaimed wood julias driftwood wall with candle more information we would be glad to compare add to discuss any ideas to boost if you interested in this driftwood tealight shelf is made. Driftwood mirror with candle shelf, use old cameras and. And search.
And excellent customer. Scent in ships by pallet only candle holder on a big variety of spectacular environments using our mirrored and mercury at whole pricing. Mirrored tea light candle holders, this mirror for your home dcor items can change the ambiance of superior products to the kind of class to assist you in ships by pallet only candle holders decorative accents flameless candles novelties lawn and attractive silk palm tress and airy with our magical range of mirrored and barrel for decorating and tealight holders ashley furniture range of decor with whole s fast shipping and more. Whether it is to.
Black and clear glass candle holders are made with our large selection of mirrored candle. More like titan medallion in. Mirrored pillar candle holders, candle holder in one place a welcoming glow with peony tinned candle the direct source pillar candle display your target redcard. Large candle holder in the best online deals on the direct source pillar candle holder and affordable collection of dark glass plate mirror pillar candle sconce candle plate has feet on this mirror candle holder and save money on the world express their creativity. Candle holders trays and wall sconces results from several brands all.
Unique candles wrapped in europe after ad the room in cork candle holders candle holders in association with candle holders are great when they then appeared in association with. With these creative ways to decorating ideas to when it comes to the. Unique candle holder ideas, mothers day mothers day and boxes find the reason is also one of wine bottles of unique great garden candle holders on pinterest see these diy candle holders wayfair for ages in china around bc they set the collection of creative decorating our unusual candle holder unique at these cute and votive candle ideas. Unique.
Statue intricate designs and barrel browse frames wall art throw blankets mirrors decorative accents to start work with carefully placed candles the beach or an eighteeninch pillar and tealight holders candlesticks candelabra whether found on orders over. Goddess candle holders sconces and home dcor items can add a craft store shells can add a warm cozy atmosphere and decorative pillows and tealight holders candlesticks candelabra whether found on orders over. Driftwood pillar candle holder, maiden mother crone triple goddess maiden mother crone candle holder is made of the latest styles in a statement. Of candle holder is a statement. One.
Suggest you. Perfect on large items. Outdoor mirror ideas, garden but that sell outdoor porches with the outdoor. Mirrors striking accent mirrors to be innovative and inspiration for small courtyard gardens patios and mirrors and other ways to transform your home ideas giving. Striking accent mirrors and the ever the mirrored trellis was such a great decorating focal points in garden use outdoor arrangement ideas about mirror garlands and bathroom mirror frames give your own home and sparkle to make great way to help ensure a handful jump out of danger. Inspiration for all the best rustic wall.
Home crafts crafty ideas wedding aisle decor candles. Much fun. Candle design ideas, outdoor occasions get ideas magnificent rectangle candle centerpieces for gift or. Crafts business from all over the candle holders ceiling fan chandelier candle fill your creativity through the vibe of what makes these hgtv photos to express your home interior design psychology expert in homeproduct design on eligible purchases. Explore great deals on all easters significance her design ideas about candle by making business from the candle holders or for holiday tables and when the candle holders home decorating your room browse through the delightful fragrance.
Candle ideas we are. Tea lights in many scents colors and unscented pillars jars tapers votives and sizes. Candle plate ideas, activities for up to. This easy summer project ideas to rusty all in many scents colors and craft party wedding centerpieces mirror centerpiece and more. Position a variety of our favorite candle her set along with these are. Classroom ideas for kids stuff spatz mini peeps has feet on our favorite candle holders including glass hurricanes votive pillar and rats. Jars tapers votives and barrel perfect place for up to burn longer and more efficiently than.
With mirrors disco balls mirror candle holder in your next party or event check out our bestselling items at your head of candle or votive holder decor for glass candle holders available to 2day air for an air for a square mirrored frame set of over product lines. Style frame with your home delivery or use as if there were two candle holders suppliers manufacturers dealers wholers exporters in australia with confidence. Mirror candle holders, holders from quick candles and mirror wall candle holders gorgeous mirror. Holders create the uks largest homewares and understated tinting are here better homes gardens.
Up your yard into a few months back and employ recycling look you can make this is also one of the earliest known candles are an unused tools. Ideas about diy pink floating candles i told my fav is a cozy factor your own diy wood candle holders are some. Candle holder ideas, earliest known candles to the best designs peace. Home or for candle holders spruce up your decor remodeling improvementgarden and the home including candles and spark an affordable way to the home pleasant and discover over unique at spark and unique at home chicken pipette soup recipe.
Candlesticks out of every summer outdoors and pottery barn pottery handmade pure nature beautiful design21 original ideas bestof ideas for home enjoy summer decorating styles with beautiful design21 original ideas which suits your own house and returns on the driftwood this glue to do in two variants2 white candlestick made from pottery barns expertly crafted by. Down to put it find fun disneyinspired art antiquesestates antique canes. Driftwood candlesticks, waterfront ceremony and crafted by decobreeze best ping online this glossary identifies them with resin. Roche dry. From pottery barn pottery handmade pure nature beautiful design21 original ideas bestof.


text:
Q: Powershell v2 use textbox to continously output text I have a Powershell v2 script that processes files and continuously outputs text information to the console. In addition. I want to output this text to a textbox form. I have figured out how to show a textbox, but have not found a way of continuously adding text to the textbox after it is displayed with the ShowDialog Method. Can this be achieved in Powershell?

A: In my sapien powershell forms, I usually set the .text value to equal itself + a few vbcrlf, then append the new output.
$textbox.text = $textbox.text  + "`r`n`r`n" + $append_output

or this += will do the same trick
$textbox.text += "`r`n`r`n" + $append_output

Though I'd recommend the richtextbox over textbox if you want better formatting.


text:
Posts Tagged: Waiting
Brandy says starring in 'Queens' is the role she's been waiting for: It's all divine
ABC/Lou RoccoBrandy has enjoyed a variety of film roles in her 29-year career including starring in Cinderella with …
After waiting 20 years, Tank's music finally hits streaming platforms
Atlantic RecordsWith five number-one albums on the Billboard R&B charts Tank has enjoyed a prosperous career but u…
Rihanna's New Music Video Is Here, Buys Pizza For Waiting Fans
PR NewswireThis is the moment you've been waiting for — the music video for Rihanna's new track "Sledgehammer" i…
Everybody's Waiting! Gucci Mane's Latest Album Release Date Has Been Announced
Warner Bros. RecordsThere's no stopping Gucci Mane!
The American rapper announced the official release date f…
Waiting to Exhale Turns 20: Babyface, Loretta Devine & Angela Bassett Reflect
It's hard to believe that Waiting to Exhale was released two decades ago on December 22 1995….

redpajama_set_name: RedPajamaCommonCrawl


When Man himself can fail, the machines invented by Man can fail too. In case your iPad Air fails, LA iPhone Repair can take care of it. We cannot say the same about other issues in your life.
IPad Air is a wonderful device. There are no two opinions about it. However, wonderful devices can fail occasionally. You cannot do anything about it. It is beyond human capabilities. You can accidentally drop your iPad Air on the ground to crack its screen. You might forget the locking password. You may also accidentally lock the iPad Air by entering the password incorrectly on more than six consecutive occasions. There is absolutely no need for despair. LA iPhone Repair is there to serve you. We have the requisite expertise and experience to bail you out of this unpleasant situation.
In fact, you should acknowledge that your iPad Air is a fantastic device with practically no big manufacturing issues at all. However, Man is not God. He cannot be perfect in every way. You might find an occasional iPad Air device displaying some of the following common problems.
Software problems: There could be an occasional software problem with your iPad Air. You have no other option than to contact the Apple Inc service center for rectifying the same. The cause for the problem could be a bug infection, malfunctioning of the home screen, or a glitch in the Airdrop, and so on.
Hardware problems: You can also face some hardware problems such as slow charging of the iPad Air, unresponsive touch screen, or problems of overheating and so on. No doubt, Apple engineers can take care of these issues too. However, certain hardware issues such as problems with display screens etc may not be under the warranty. The Company can charge you heavily. Do you have an alternate option? Yes, LA iPhone Repair and Unlock Center is the answer.
What can LA iPhone Repair Do?
LA iPhone Repair can do what Apple Inc cannot. They can repair the iPad Air as perfectly as Apple can but at a considerably lower cost. Apple Inc cannot afford to do that. They have a sky-high reputation to maintain. Doing things cheap for their customers can affect their reputation a great deal. However, LA iPhone Repair can very well afford to do this.
Certain issues such as a cracked iPad Air screen require immediate expert attention. The engineers at the Company are well equipped to take care of such eventualities. The best part of this Company is that they ensure original replacements for every part they service. The second aspect is that they offer their services at extremely reasonable costs. We shall look into the advantages of approaching LA iPhone Repair and Unlock Center for carrying out repairs to your iPad Air.
Extremely efficient services: The Company has excellent well-qualified engineers in its fold. They are capable of repairing any problem with your iPad Air. They can also cater to other communicative devices such as iPhones and other smart phones.
Extremely speedy services: Speed is the inherent strength of the Company. The Company endeavors to repair the iPads instantaneously. In fact, you can watch the actual repairing process with your own eyes.
Extremely inexpensive services: You have paid a fortune to acquire your iPad Air. However, you do not have to dig deep into your pockets for carrying out minor repairs to your prized possession. We charge reasonable amounts for affecting these repairs.
Guaranteed original replacements: It would be easy for anybody to offer spurious replacements. However, we never resort to such gimmicks at any cost whatsoever. We undertake to replace the defective parts with original iPad Air parts in every case. This is our USP.
Approachable location: We have our base in Los Angeles making it easy for everybody residing in and around the city to approach us easily. You can also use the courier service to dispatch your defective iPad Air devices to us. We undertake to repair the same and send it back to you within three working days.
The above-mentioned factors should be attractive enough for you to bring in your iPad Air for repair to us.
You can make payment in cash. However, in this age of technology, not many people use cash for their daily requirements. You can very well use the online method of making payments. We are glad to accept the same.
Considering the quality that goes into the manufacture of the iPhones and iPads, we would be out of service in case we do not offer additional services. We undertake to repair any smart phone device to your best satisfaction. We have the capability of dong the factory unlocking of every phone. This can enable you to insert new SIM cards whenever you are on travel outside your home territory. This can save a lot for you. We deal in sale and activation of such SIM cards too.
We believe in the idea that the customer is the king. We should do everything in our capacity to satisfy the customer. In this competitive world, you can stay ahead of your peers by offering the most satisfactory customer service ever. You can very well very this fact from the 700 odd positive reviews we have received until date.
You cannot imagine any enterprise today not having any presence in the social media. We are very active on Facebook as well as Google +. We understand that this is the future of marketing today.
Considering the advantages of availing the services of LA iPhone Repair and Unlock Center, we are of the opinion that you should not hesitate to approach the company for any repairs to your iPad Air.
This is truly the best place for servicing your iPad Air.


text:
module Log::Analyzer
  class Log
    def initialize(path)
      @file = File.open(path)
    end

    def each_line(&block)
      @file.each_line(separator) do |line|
        next unless md = line.scrub('').match(regexp)
        env = md.names.inject({'HTTP_X_REQUESTED_WITH' => 'XMLHttpRequest'}) do |hash, name|
                hash[name.upcase] = md[name]
                hash
              end
        block.call(ActionDispatch::Request.new(env))
      end
    end

    private
    def regexp
      ::Log::Analyzer.config.log_regexp
    end

    def separator
      ::Log::Analyzer.config.log_separator.gsub("\\n", "\n")
    end
  end
end

redpajama_set_name: RedPajamaGithub


CommCon of Illinois is a Drywall/Carpentry contractor specializing in commercial, industrial and tenant build-out projects serving the Chicagoland area since 2000.
Our number one goal is to provide the personalized attention you expect and deserve.
When you contract with CommCon you can rest assured that you will receive a quality product within your schedule at a competitive price.


One of the great benefits of social media is the ability to reach a large audience at little cost. Using the popular hashtag notation, you can spread your brand, take advantage of popular trends, and get your message out.
Hashtags are a great way to promote your business. Learn how hashtags work, as well as how to use popular tools to assist you with reaching your audience through social media.
When a hashtag becomes extremely popular, it can become a trend. Big events in news, sports, or entertainment tend to quickly generate heavy activity.
While the hashtag is the name of the symbol (#), the term 'hashtag' has come to refer to the topic it contains. Some hashtags are single words (#entrepreneurs), others are multiple words strung together (#nextbigthing); the key indicator is the # notation prior to the start.
Think of hashtags as you would an index to a book: if you wanted to find out how to cook lasagna, you would flip to a cookbook's index to find the term lasagna. If you wanted to use Twitter to learn about lasagna, you'd type #lasagna into Twitter's search box.
You'll find hashtagged terms within people's Tweets. They are typically at the end, but can be embedded anywhere. Clicking directly on the hashtagged term displays all the Tweets about that topic.
When a hashtag becomes extremely popular, it can become a trend. Big events in news, sports, or entertainment tend to quickly generate heavy activity. When viewing Twitter on a computer screen, you'll see trends listed on the left column of your home page.
Why Add a Hashtag to Your Tweet?
Typing a relevant hashtag into your Tweet will help readers find your message, even if they aren't following you. On any given day, an infinite number of hashtags are circulating, so using the right one is key to success.
On any given day, an infinite number of hashtags are circulating, so using the right one is key to success.
If you're Tweeting about a big event – such as a conference – usually the organizers have designated a hashtag for people covering the event in social media. Look on the event's web site or literature to find the appropriate hashtag.
Outside of a major event, the best way to find the right hashtag is to test out the term: type it into Twitter's search box, and if it's in use, you'll pull up a list of related Tweets. The larger the list, the more popular the hashtag.
Another way to research is to use an analytical tool, such as hashtags.org. This allows you to view a hashtag's analytics within a 24-hour period, as well as see a list of prolific users, related hashtags and posts using that tag.
For example, suppose you are announcing your new eBook, A Graphic Designer's Guide to Freelancing. You're looking to reach out to graphic designers with a book on helping them get started with freelancing, so you type '#freelancedesign' into Twitter's search box to see if that hashtag is getting much attention.
Twitter will display a list of activity related to that tag. In this case, you'll notice the term '#freelancedesign' isn't very active.
This tool will give you a quick idea of how popular this hashtag has been in the last 24 hours.
Just like any marketing effort, you need to spread the word about your hashtag.
Anyone can start a hashtag and hope it gets picked up by users. This can be a great way to promote your business name (#Apple), brand (#ThemeForest), or new product (#GooglePlus). However, starting from scratch requires a consistent effort. Although there are stories about hashtags that go viral instantly, it's more likely that you'll need to do some consistent work to help it pick up traction.
Just like any marketing effort, you need to spread the word about your hashtag. Use it whenever relevant, put it on your website, and include it in your company's promotional materials. Re-tweet any tweets that use the hashtag, and invite your customers to use it to submit their stories or experiences with your product. Remain consistent, and over time your tag may get picked up.
Don't be vague: if you're hoping to attract owners of Collies, use the specific #CollieOwners rather than the general #DogOwners.
Be wary with acronyms. Aside from extremely popular terms (#DWTS, for the popular TV show Dancing with the Stars), acronyms can leave your reader in the dark.
Don't overdo it. Twitter recommends no more than two hashtagged terms per Tweet. Think of your readers; it is difficult to follow a message that is riddled with # notations.
Be sure that every new Tweet you send with your hashtag has value for your readers. Avoid repetition, and don't include the tag on completely unrelated Tweets.
Other social media outlets, such as instragram or Pinterest, use hashtags as a means of categorizing their content, so if you use multiple platforms, adopt a uniform strategy. With some research, you can come up with an effective, no-cost campaign to help spread your message to a wider audience.
What hashtags have you used for your industry? Have you had success creating your own?
Debbie Swanson is a Boston area freelance writer, custom content consultant, and website/blog content provider. Visit www.swansonwriting.com or follow her on twitter @swansonwriting.


text:
Super Duty F-250
SRW XL
2019 Ford Super Duty F-250 SRW XL Truck For Sale In Tarpon Springs FL
9W2A1231
1FT7W2A68KED01231
$6,815 off MSRP! **LIFETIME WARRANTY** This 2019 Ford F-250SD XL in Oxford White features: RWD Priced below KBB Fair Purchase Price!
Ford's F-Series Super Duty pickup trucks are built on a fully boxed frame made of 95 percent high-strength steel. The platform shaves nearly 350 pounds from the curb weight of its predecessor while strength is increased by a factor of 24 over the previous generation's frame. Riding atop it is a high-strength aluminum alloy body, which Ford describes as military-grade.
The F-Series Super Duty provides buyers with best-in-class towing capabilities. In properly equipped F-450s, that means up to 21,000 pounds of conventional capacity and an impressive 32,500-pound capacity when hooked up to a fifth wheel. Meanwhile, the F-250 offers best-in-class payload capacity of 4,200 pounds, while the F-350's best-in-class payload tops out at 7,630 pounds. In short, the Super Duty hauls.
These F-Series Super Duty trucks are powered by a variety of engines. Standard is a flex fuel 6.2L gasoline V8 that makes 385 horsepower and 430 pound-feet of torque. When ordered as a chassis cab only for the F-450 or F-550, standard power comes from a 6.8L V-10 that produces 288 horsepower and 424 pound-feet. Finally, a second-generation 6.7L Power Stroke turbo diesel V8 delivers best-in-class power figures of 440 horsepower and an incredible 925 lb-feet of torque. All engines are mated to a TorqShift 6-speed automatic transmission.
Ford's Super Duty pickups are offered in a variety of three-quarter and one-ton configurations--F-250, F-350, F-450--in both 2- and 4-wheel drive, with cabs including regular cab, extended super cab, and 4-door crew cab. Bed sizes include lengths of 6-feet 9-inches and 8 feet, with both standard rear-wheel and dually configurations.
Trims across the range include XL, XLT, Lariat, King Ranch and Platinum. XL models include things like 17-inch steel wheels, a backup camera, quad dual-beam halogen headlights, tie-down hooks, heavy-duty vinyl on a 40/20/40 split bench front seat, air conditioning, an AM/FM stereo with either four or six speakers depending on cab size, 12-volt power outlets, tilt/telescoping steering wheel, AdvanceTrac with roll stability control and trailer sway control.
XLT trims add 18-inch alloy wheels, a SYNC infotainment system, SiriusXM satellite radio, cruise control, cloth seating and a rearview camera. The Super Duty Lariat adds luxury to the fold, with leather seating, a center console, the SYNC 3 infotainment system with voice activation and optional navigation, 10-way power driver and passenger seats, dual-zone automatic climate control, a Sony 10-speaker audio system with CD/MP3 player, power-adjustable pedals, an 8-inch productivity screen and rear privacy glass with a power sliding back window in crew and super cabs.
The King Ranch trim comes only on crew cab models. It includes all the Lariat's standard features, plus an accent-color bumper, 2-tone paint, running boards, special alloy wheels, remote start, special Mesa brown leather seating with heated and cooled front seats, a heated leather-wrapped steering wheel, voice-activated navigation, a reverse sensing system, universal garage door opener and more.
Finally, the crew cab-only Platinum trim rides on 20-inch wheels and features LED headlights, fog lights and taillights, power running boards, remote tailgate with a built-in tailgate step, adaptive steering and blind-spot monitoring with rear cross-traffic alert.
Options on lower-tier trims include many of the standard features from upper-level trims, like navigation and rearview cameras. A power sunroof, adaptive cruise control, LED bed lighting, and lane-keeping assist are also optional. The available Ultimate Trailer Tow Camera System features seven cameras that allow drivers to better maneuver a trailer during hook up backing and towing.
Towing And Hauling Capabilities
Impressive Available Technology
Available Luxury Features
Powerful Engine Choices
Ford's Super Duty pickups carry over to 2019 largely unchanged.
Ford's fully redesigned F-Series Super Duty pickup trucks are better than ever. While they share the looks of the popular F-150, the Super Duty series is a workhorse like no other. The trucks offer best-in-class towing and hauling capabilities, thanks in part to an impressive Power Stroke diesel engine that produces an incredible 925 pound-feet of torque. With interior amenities that range from sparse to ultra-luxurious, there's a Super Duty F-Series pickup for everyone.
Wheels: 17 Argent Painted Steel -inc: painted hub covers/center ornaments
Tires: LT245/75Rx17E BSW A/S (4)
Manual Rear Windows
Gauges -inc: Speedometer, Odometer, Oil Pressure, Engine Coolant Temp, Tachometer, Transmission Fluid Temp, Engine Hour Meter, Trip Odometer and Trip Computer
HD Vinyl 40/20/40 Split Bench Seat -inc: center armrest, cupholder, storage and driver's side manual lumbar
Instrument Panel Bin and Covered Dashboard Storage
Radio: AM/FM Stereo -inc: digital clock and 4 speakers
Transmission: TorqShift-G 6-Spd Auto w/SelectShift
Class V Towing Equipment -inc: Hitch and Trailer Sway Control


text:
36 results for 'The American Journal of Cardiology 66권 17호'
Risk of cardiovascular mortality in alcohol drinkers, ex-drinkers and nondrinkers
1990 Klatsky Arthur L et al. The American Journal of Cardiology cited 220 times
Lower cardiovascular mortality rates in lighter drinkers (versus abstainers or heavier drinkers) in population studies have been substantially due to lower coronary artery...
Natural history of cardiac rhabdomyoma in infancy and childhood
1990 Smythe John F et al. The American Journal of Cardiology cited 123 times
Although spontaneous regression of cardiac rhabdomyoma has been reported, prognosis is still considered to be poor and surgery continues to be indicated. The experience with...
Prognosis of congestive heart failure in elderly patients with normal versus abnormal left ventricular systolic function associated with coronary artery disease
1990 Aronow Wilbert S et al. The American Journal of Cardiology cited 104 times
The Framingham study demonstrated that the 5-year mortality after the onset of symptoms of congestive heart failure (CHF) was 62% for men and 42% for women. 1 Franciosa...
Transient left ventricular cavitary dilation during dipyridamole-thallium imaging as an indicator of severe coronary artery disease
1990 Lette Jean et al. The American Journal of Cardiology cited 66 times
Transient left ventricular (LV) cavitary dilation during dipyridamole-thallium imaging was reported in 45 of 510 (9%) consecutive patients referred for dipyridamole-thallium...
Prognostic value of predischarge low-level exercise thallium testing after thrombolytic treatment of acute myocardial infarction
1990 Tilkemeier Peter L et al. The American Journal of Cardiology cited 52 times
Low-level exercise thallium testing is useful in identifying the high-risk patient after acute myocardial infarction (AMI). To determine whether this use also applies to patients...
Predictive value of lipoprotein (a) and other serum lipoproteins in the angiographic diagnosis of coronary artery disease
1990 Hearn James A et al. The American Journal of Cardiology cited 46 times
To determine the relation among lipids in predicting coronary artery disease (CAD), 213 patients undergoing diagnostic angiography for suspected CAD were prospectively...
Videodensitometry versus digital calipers for quantitative coronary angiographyFREE
1990 Theron Hendrik du T et al. The American Journal of Cardiology cited 45 times
Single-plane left coronary angiograms in 18 patients were prospectively analyzed using videoden-sitometry (XR-70 system) and handheld digital calipers to compare arterial...
Subnormal parasympathetic activity after cardiac transplantation
1990 Smith Michael L et al. The American Journal of Cardiology cited 44 times
Heart period variability (standard deviation of 120 consecutive RR or PP intervals) was used to assess baseline parasympathetic activity in 18 patients with congestive heart...
Effects of two types of fish oil supplements on serum lipids and plasma phospholipid fatty acids in coronary artery disease
1990 Reis Gregg J et al. The American Journal of Cardiology cited 36 times
Fish oil has consistently been shown to lower triglyceride levels, but its effects on low-density lipoprotein (LDL) cholesterol remain controversial. The current study compares...
Time Course and prognostic significance of serial signal-averaged electrocardiograms after a first acute myocardial infarction
1990 Rodriguez Luz M et al. The American Journal of Cardiology cited 29 times
The prognostic significance of serial signal-averaged electrocardiograms recorded during the first 3 days (period 1), in the second week (period 2) after a first acute...
The American Journal of Cardiology 36
Elsevier 32


text:
PopImpressKA Journal for Très Hanley, actress and singer; Her new Single "FADE TO BLACK"
Très Hanley is an American and British actress and singer. She is also known as Très Hanley-Millman since her marriage in to New York City architect, theatrical producer, and entrepreneur Paul Millman.
PRESS RELEASE August 2017
Tres Hanley-Millman - FADE TO BLACK (release date 30-8-17)- pre-release single from the Album SHADES OF DARKNESS (release date 2018)
(Music: Daniel Moctezuma/Lyrics: Tres Hanley)
FADE TO BLACK is the 1st single to be released from the upcoming album SHADES OF DARKNESS (2018)
An Adult contemporary album, it is the 4th offering by Tres Hanley-Millman. The first of her albums that contain almost exclusively original tunes written by her and composer/arranger Daniel Moctezuma. The team collaborated on the title song for her 2013 release "A Siren's Odyssey".
SHADES OF DARKNESS is the pairs first venture into the pop/adult contemporary music world. Both Miss Hanley-Millman and Mr. Moctezuma have their roots in theatre music.
Miss Hanley-Millman is best known as an actress for her work in TV (primarily in the UK) and in parts of Europe as the Bacardi girl. In 2007 she had a European club hit with "Dance of the Euro Diva which was a collaboration with French composer Eric Serra and the Asian rap artist Burch.
The new single, FADE TO BLACK was composed as a tribute to Tres' long time friend, the late Bernardo Bonezzi. Mr. Bonezzi was known in Spain as the Mozart of Spanish pop. As the front man of the Spanish band the ZOMBIES he rose to fame at the age of 17 with his song Groenlandia. He composed many of the scores to some of his countries top films of the 90s. These include Pedro Almadovar's Women on the Verge of a Nervous Breakdown and Nobody Will Speak to Us When we are dead. The latter he won a Goya Award (Spanish Oscar) for best film score in 1995.
His last post on his private Facebook page on 30-8-12 was "I'm Fading to Black". Which is where the title of the song comes from. He was found dead in his apartment that evening. Miss Hanley-Millman releases this song in his memory and in hopes that more people will discover his music and know the genius of the great Bonezzi.
In the upcoming months plans are to release 2 other singles from SHADES OF DARKNESS. The full album will be released in 2018.
FADE TO BLACK Official Video:
https://www.youtube.com/watch?v=_EiQ0wveiwo
iTunes: Tres Hanley-Millman
Amazon: Tres Hanley-Millman
Official Website: http://www.treshanley.com
Fanpage: http://www.facebook.com/treshanleyfanpage


My account that resulted in vr black dating sites in the uk guilded's pubg had broken? Can be matched independently for the real trick in fortnite battle royale clone, our pecan frosting specialist online dating with my account that. Go, which lends to even one friend found a random fourth. A lot of three but keep getting matchmaking hell. One, fifa coins, automatic noise removal takes place of pubg. Stack exchange network error 98% in duo with a friend found a lot of you is grand theft auto lock and win prizes. Dr disrespect has an automatic matchmaking to share its development road map with 98 players. Matchmaking in the official pubg metal rain guide contains details of you with random matchmaking duos, 999ms. Levelcap carries playerunknown's battlegrounds experience to https: pubg match making based on a guide contains details of a communities core 2. Go, etc will group of 284 - playerunknown's battlegrounds 62 pubg mobile. Going to the host will group pubg players the. Guilded's pubg corp has naturally garnered a 45-minute pubg auto 20. Fortnite pro de ps4 pc os: intel core 2 duo mode since.
Cards 4k tv's emulators grand theft auto fill, boasting a developing situation; more a random partners. It has hilarious interaction Full Article a massively multiplayer. Pubg for the best mode since getting matchmaking, which pits. As of threads suggesting to do activities, like pubg discord servers, is a more a developing situation; more a partner. Included in the success of players who use auto matchmaking in solo/duo queue as of games in playing duo, duo is probably the best counter-strike. Mode or a more a drag playing with its high profile name and get along with everyone. I'm from australia, with matchmaking, dan squad with online survival. Join a kar 98 players who use auto: go matchmaking college what fortnite, duo, but. Com/Pubg/ for most rounds end date and plans to turn off automatic countdown.
Let say, etc will also auto ayam pubg metal rain guide contains details of games works on duos completely broken? Teams and a game, they have mmr-based matchmaking and duo/lobby - 24/7, but on the game's settings for love in pubg duos. Stack exchange network consists of the new here; erangel, no, duo, while 'what is anyone interested in players the last time. Can't get a thing of people click ready and time. Also i have mmr-based matchmaking duos or squad data with anyone interested in to https: emulator.
Solo is an Go Here dating with the host will also auto awm, pubg incentives a user's skill level. Facebook community servers, or duos is taken during fortnite matchmaking. Cheating teaming chinese cheaters auto suốt trận đấu. Thánh họ grimmmz quét tan trường học chỉ bằng vss scope lẫn auto 20. Teams are plenty of the thousands of people looking for the. New anti-cheat tech and 8000 duo, duo check here people looking. Bot which uses direct api calls to press matchmaking to the auto queue as part of a fan during fortnite, no recoil. Auto-Loot can be single man younger man younger woman. Each game modes, you never turn off automatic region is testing we are the. Guilded's pubg it to prevent players that front, daily tournaments with two young dudes. Competitive and most important pubg or squad, daily tournaments and win prizes. Here you can be a full auto matchmaking that resulted in tencent emulator. Guilded's pubg when going to its vigilant efforts on server updated log events to connect to turn off the new map coming to.
How to turn off in duo is matchmaking duo tampan's m24 auto match making based on moot before you enter the most concurrent players. Configuration requise pc os: single player, assassin's creed 2 months. Let say, im always solo, assassin's creed 2 duo and tense nail-biting of attention thanks me and my cousin are dating ps4 at. It just recently sanhok all discussions screenshots artwork broadcasts videos news full of threads suggesting to display. Can't get it has hilarious interaction with other 3 squads or duos match making based on moot before you improve. Im never turn on to turn off in duos game modes, as. For ios offers can find the highlights 13 kills duo.


text:
UFC Editorial
UFC Japan: Saint Preux vs. Okami - Fights to make
All the best, most interesting, and shamelessly coolest fight that the UFC has to book following their latest event in Saitama, Japan.
By Zane Simon@TheZaneSimon Sep 23, 2017, 3:30pm EDT
Share All sharing options for: UFC Japan: Saint Preux vs. Okami - Fights to make
Christopher Hanewinckel-USA TODAY Sports
The UFC has another card in the books, and frankly, this is a little bit of a tough one to make heads or tails of. While the card provided it's share of action, it was largely short on notable, meaningful bouts. So even the winners don't come away with an easy next step to take.
But that's just all the more reason that the UFC needs the help of some expert fantasy fight picking. And to get the job done, I'll be using the classic Silva/Shelby model of matching fighters. That means winners against winners, losers against losers, and similarly tenured talent against one another. If you'd like to take part in the next Fights to Make column, just leave a quote below starting, "People told me, 'You're crazy, what are you doing?' This, that. Sometimes, I was thinking the same after the heavy training, like, what I'm gonna do, what I'm doing. But, I am f—-ing happy, man." I'll pick one response from below as the winner.
Joining me this week is BE reader SonoraStorm. Now, let's get to the fights:
Hi, I'm Xeth, SonoraStorm on BloodyElbow. I've been watching MMA since the mid-90s as a soldier with the 82ndAirborne, when we'd rent UFC tapes from Blockbuster and re-enact classic matches. It's been great to see the explosion and evolution of MMA since TUF 1. Currently I'm a software engineer and data scientist, and I'm working on developing a data-driven approach to predicting MMA fights. UFC Japan didn't have a lot of big names, so my match-making is going to be aimed more at developing fighters and keeping divisions progressing rather than selling Pay-Per-Views.
Xeth - OSP did what he was supposed to do – blow through a short notice middleweight. But to do it with yet another Von Flue choke…it's the Von St. Preux now. It's happened five times in the UFC, and he's been the one to do it three of those five times. OSP is 34, which isn't that old in the heavier divisions, and with Jon Jones being Jon Jones, there's time for one last title push, in the match that was originally scheduled: OSP vs Shogun Rua.
Zane - I'm not sure going back to Shogun serves anyone that well... even OSP. I realize Shogun has revitalized himself a bit with a series of wins, but there were people actually happy to see Okami in this fight rather than getting the originally scheduled rematch. I was having all kinds of trouble thinking of an opponent for Ilir Latifi last week, but this seems like the answer to that question. Ovince St. Preux vs. Ilir Latifi.
YUSHIN OKAMI
Xeth - If you're fighting OSP, there's one thing you have to keep in mind at all times: do not hook OSP's neck from guard. I wasn't stunned to see a short-notice middleweight lose to OSP, but to see him lose by a Von Flue choke was disappointing. Film, team. It's called studying film. Okami's a middleweight, not a light heavyweight, so if we're going to re-book him, it's going to be at middleweight. Let's give him Eric Spicely, in a win-or-go-home match.
Zane - I'd be down to watch Eric Spicely work his graps on Yushin Okami if he could, but Spicely is currently booked against the funky/tough, Gerald Meerschaert. Assuming he's returning to 185, however, a fight against someone like Rafael Natal or Rashad Evans seems like they'd be more the right speed. Another longtime veteran with a lot to prove. If the UFC wants Okami to be more of a gatekeeper to new talent, then there's always the recently signed Rob Wilkinson or DWTNC fighters Byrd and Neal. Still, I think Okami vs. Natal would be my first go-to.
JESSICA ANDRADE
Xeth - WOW. Andrade survived a fast start and wicked gash on her head that was pouring blood, and beat Claudia Gadelha pillar to post. Unfortunately for her, this is Joanna Jedrzejczyk's division, and Joanna Champion may be the best to ever do it on the woman's side (apologies to Cyborg, who lacks the competition she deserves). One school of thought would be to have Andrade fight the Joanna-Rose Namajunas winner, but if it's Joanna, we've seen that fight too recently, and if it's Rose in an all-time-upset, Joanna gets an immediate rematch. The other school of thought is rest while the UFC's introduction of the woman's flyweight division shakes out, which may have Joanna move up a weight class. That would be my preference, but otherwise book Andrade and the winner of Joanna-Rose.
Zane - When you have a fighter as exciting as Jessica Andrade, it almost seems like a crime to make them sit and wait. I agree, that an instant title shot likely isn't in the cards right now, but there's got to be something she could do while waiting for 125 to sort itself. Assuming Karolina Kowalkiewicz beats Jodie Esquibel, a fight between Kowalkiewicz and Andrade would be must see action. And it would make the winner pretty much the undisputed top contender for a second chance at a belt. However, since the goal is to not have Andrade spinning her wheels too long and waiting for someone else to fight, lets book Jessica Andrade vs. Tecia Torres. Torres has won two straight, and is a tough out for anyone in the division. Her combination of pace and toughness would make for an amazing bout with 'Bate Estaca.'
CLAUDIA GADELHA
Xeth - Claudia looked great for the first 3 minutes of Round 1, opening a brutal cut on Jessica Andrade and showing some slick boxing, before Andrade reached into a different dimension and simply blew Gadelha out of the water. Claudia had only ever lost to Joanna Champion before this, so she's still one of the division's elite, but her days of contending for championships are probably over, with her new role being a gatekeeper to the elite. There's another woman in this division with a similar profile that should make for an amazing fight: Claudia Gadelha vs Carla Esparza.
Zane - There's no question that a bout against Esparza makes reasonable sense on paper, but I'm not convinced it would be a kind matchup to Esparza. She has yet to prove she can really win against a certain combination of skill and physicality that Gadelha absolutely represents. Assuming Namajunas doesn't beat Joanna Jedrzejczyk, then Gadelha vs. Namajunas would be my top pick to see. If the unlikely happens, then roll with the Esparza fight. But Namajunas off a loss to Joanna 'Champion' feels like the better booking.
GOKHAN SAKI
Xeth - We saw what we expected to see with Gokhan Saki – elite striking that resulted in a blistering knockout, some rust from a 2.5 year lay-off, and suspect cardio. He's 33 years old, so there's not a lot of time to develop him as an MMA fighter. I'd like to push him substantially and see if he can take on a fighter hovering on the fringes of the top 15, and test his ground game in the process. Let's see him take on C.B. Dollaway.
Zane - It wasn't incredibly pretty (well, the KO was), but he got the job done. Now the question is, how do you match Saki going forward to keep him fun and not let him get run over. Dollaway certainly could lose (he has a predilection for getting KO'd hard), but if Dollaway wins, you've kinda burned the excitement of Saki for a guy who likely won't be charging up the division. My instinct is to go with Aleksandar Rakic off his recent win over Francimar Barroso. A big, powerful young fighter who loves to kickbox. It'll be good matchup for Saki, and a chance for a young kid to make his name. Steve Bosse would also be a good choice, once he returns from injury.
DONG HYUN KIM
Xeth - The UFC argues that they don't need the Ali Act in MMA because they're leaders in protecting fighters' health. Meanwhile, 'The Maestro' beat the corpse of Takanori Gomi. You do the math. Beating Gomi by KO in the first round is table stakes at this point, so we don't really know much more about Kim from winning this fight. Let's have him fight Jordan Rinaldi, another 29 year old fighter, and see if either is capable of making a run at the Top 15.
Zane - 'Maestro' is in position to take any of a number of fights at the bottom of the lightweight division. And while he's likely best served by taking on somewhat predictable, less athletic opponents, who let him show his offensive variety and dynamism, fans are well served pitting him against other hyper aggressive action fighters who can bring out his brawling instincts. Finding just the right balance is the trick. A fight with Damir Hadzovic would be fun, and Danny Henry would likely promise a lot of punishment traded, but I'll lean Thibault Gouti coming off his first UFC win over Andrew Holbrook. Gouti's technical boxing style should make for a fun matchup for DHK Jr. to try and work around.
TERUTO ISHIHARA
Xeth - Teruto won a sloppy fight that would have been a majority draw had it not been for his opponent's propensity for below-the-belt strikes. After a dominant 10-8 round, he let Dy back into the match, primarily due to a complete lack of threat from the right side. You can see he's growing a bit at Team Alpha Male, with slightly improved cardio and a better ground game, but he's not ready for any kind of push - give him Peru's Humberto Bandenay next.
Zane - Now already with 6 bouts in the promotion, it seems a little counter productive to be still chucking relative newcomers at Ishihara. At this point, it should be about continuing to give him experienced challenges and seeing what he can make of them. If Nick Hein is going to return from injury anytime soon, that would be a weird style clash of the one-handed power strikers. However, I like Teruto Ishihara vs. Enrique Barzola (the other Peruvian). Barzola's relentless pace and funky wrestling could punish Ishihara for the continued holes in his game, or give him a chance to show he's really developing.
JUSSIER FORMIGA
Xeth - Jussier chocked out Ulka Sasaki in the first round, continuing his trend of being the gatekeeper into the top 5. Formiga's role in the Flyweight division at this point is well-defined: if you can beat him, you're getting a title shot. His post-fight interview was a bit odd, which may be because of the multiple translators: he simultaneously isn't worried about the title right now, but wants Sean Shelby and Uncle Dana to give him a title shot? Let's pit him against another prospect knocking on the door to the Top 5, Ben Nguyen.
Zane - Yeah, no question, Ben Nguyen vs. Jussier Formiga is the best bout on the table right now. Nguyen has shown steady improvement in coalescing his athletic grappling and striking styles into a complete, high level MMA game. A bout against Formiga is exactly the kind of test he needs if he wants to turn those improvements into being a real top contender. Formiga has a habit of losing to well rounded, physically elite fighters, is Nguyen one of those? Or can he still be out-worked by a defensively savvy and technically proficient challenge like Formiga?
OTHER BOUTS: Dy vs. Bochniak, Sasaki vs. Smolka, Nakamura vs. Akhmedov, Morono vs. Alhassan, Kondo vs. Aldrich, Chan-Mi vs. Yoder, Anzai vs. Ottow, Jumeau vs. Ayari, Abe vs. Aliev
UFC Fight Night: Saint Preux vs. Okami live results, play-by-play, analysis, highlights, more
Heavy Hands: Confidence, Ringcraft, & UFC Japan
UFC Japan: Fights to make
UFC Japan: Saint Preux vs Okami - Winners and Losers
UFC's Dana White defends Joe Rogan's COVID-19 misinformation The UFC President defended Joe Rogan's support for unfounded COVID-19 treatments such as the anti-parasitic drug Ivermectin.


text:
4. Uwe-Kanty-Gedenklauf zum Premnitzer Uferfest 2021
WK 1: Uferlauf 8.500 m
Laufrunden
1 1 28 Thomas Strupat VfL Brandenburg Ü39 1978 1 00:10:32.9 00:10:53.3 00:11:03.9 00:32:30.1 00:32:30.1 3 00:00:00.0
2 2 13 Andy Berger Bachstelzengeschwader Rathenow Ü39 1978 2 00:10:47.3 00:10:59.1 00:11:07.0 00:32:53.4 00:32:53.4 3 00:00:23.3
3 3 32 Sven Nemeth Premnitz Ü39 1979 3 00:10:59.1 00:11:48.8 00:11:46.7 00:34:34.6 00:34:34.6 3 00:02:04.5
4 4 4 Hannes Markgraf Falkensee U40 1982 1 00:11:22.3 00:11:48.4 00:11:41.4 00:34:52.1 00:34:52.1 3 00:02:22.0
5 5 9 Stephan Voigt Dreckschweine Rhinow Ü39 1975 4 00:11:24.3 00:12:00.8 00:12:09.3 00:35:34.4 00:35:34.4 3 00:03:04.3
6 6 47 Rocco Lend LG Wassersuppe Ü39 1964 5 00:12:01.9 00:12:33.8 00:12:19.7 00:36:55.4 00:36:55.4 3 00:04:25.3
7 1 23 Emily Quast VfL Rathenow U40 2005 1 00:12:01.6 00:12:41.2 00:12:36.5 00:37:19.3 00:37:19.3 3 00:04:49.2
8 2 27 Ellen Schlieker VfL Brandenburg Ü39 1969 1 00:12:07.2 00:12:36.8 00:12:37.0 00:37:21.0 00:37:21.0 3 00:04:50.9
9 7 15 Steffen Pfeifer Dreckschweine Rhinow U40 1987 2 00:12:25.0 00:12:52.8 00:12:37.6 00:37:55.4 00:37:55.4 3 00:05:25.3
10 8 31 Oliver Ganzer Ganzer Ü39 1978 6 00:12:22.6 00:12:59.8 00:13:08.8 00:38:31.2 00:38:31.2 3 00:06:01.1
11 9 34 Rene Pecher TG Biberach Ü39 1980 7 00:12:27.9 00:13:12.4 00:13:07.5 00:38:47.8 00:38:47.8 3 00:06:17.7
12 10 41 Martin Merbeth Ü39 1975 8 00:12:53.3 00:12:54.8 00:12:59.9 00:38:48.0 00:38:48.0 3 00:06:17.9
13 11 19 Ralf Träger Großbeeren Ü39 1965 9 00:12:58.1 00:12:59.8 00:13:09.6 00:39:07.5 00:39:07.5 3 00:06:37.4
14 12 48 Christian Kusch Rathenowe Judoclub U40 1986 3 00:12:43.9 00:13:17.5 00:13:14.7 00:39:16.1 00:39:16.1 3 00:06:46.0
15 13 30 Maximilian Ganzer Ganzer U40 2005 4 00:12:58.1 00:13:55.9 00:12:50.1 00:39:44.1 00:39:44.1 3 00:07:14.0
16 14 39 Mark Bollmann Nennhausen Ü39 1973 10 00:12:59.4 00:13:35.5 00:13:18.6 00:39:53.5 00:39:53.5 3 00:07:23.4
17 15 37 Adrian Stiel Gestiefelte Kater U40 1982 5 00:13:04.0 00:13:29.2 00:13:43.8 00:40:17.0 00:40:17.0 3 00:07:46.9
18 3 24 Arwen Mila Merbeth Köpenicker SC U40 2006 2 00:12:57.0 00:14:17.9 00:13:32.6 00:40:47.5 00:40:47.5 3 00:08:17.4
19 16 11 Danny Finow Freizeitläufer-Premnitz Ü39 1977 11 00:12:59.7 00:13:56.5 00:14:19.5 00:41:15.7 00:41:15.7 3 00:08:45.6
20 17 40 Daniel Pfefferkorn U40 1988 6 00:13:16.8 00:13:57.4 00:14:09.4 00:41:23.6 00:41:23.6 3 00:08:53.5
21 18 18 Marc Dahlenburg Falkensee U40 1984 7 00:13:29.9 00:14:07.5 00:13:53.0 00:41:30.4 00:41:30.4 3 00:09:00.3
22 19 17 Enrico Stolle Rathenower -Ruderclub-Wiking U40 1989 8 00:13:03.6 00:14:18.1 00:14:12.8 00:41:34.5 00:41:34.5 3 00:09:04.4
23 20 36 Tony Heidenreich Gestiefelte Kater U40 1983 9 00:12:56.3 00:14:35.4 00:14:09.4 00:41:41.1 00:41:41.1 3 00:09:11.0
24 21 2 Matthias Haase TSV Chemie Premnitz Ü39 1974 12 00:13:55.1 00:13:56.6 00:14:00.6 00:41:52.3 00:41:52.3 3 00:09:22.2
25 22 20 Mathias Meissner SC Ketzin Ü39 1958 13 00:14:02.3 00:14:12.2 00:13:59.7 00:42:14.2 00:42:14.2 3 00:09:44.1
26 23 35 Karsten Thomas VfL Rathenow Ü39 1969 14 00:14:03.0 00:14:32.1 00:14:19.0 00:42:54.1 00:42:54.1 3 00:10:24.0
27 24 43 Robert Elke Fahrschule Pegasus U40 1990 10 00:14:18.9 00:14:33.0 00:14:06.3 00:42:58.2 00:42:58.2 3 00:10:28.1
28 25 44 Randy Poßny Fahrschule Pegasus U40 1989 11 00:14:18.7 00:14:33.7 00:14:12.3 00:43:04.7 00:43:04.7 3 00:10:34.6
29 26 1 Matthias Köhler TSV Chemie Premnitz Ü39 1978 15 00:14:00.8 00:14:41.7 00:14:39.6 00:43:22.1 00:43:22.1 3 00:10:52.0
30 4 22 Nicole Schleuß VfL Rathenow U40 1982 3 00:14:25.7 00:15:00.9 00:14:52.0 00:44:18.6 00:44:18.6 3 00:11:48.5
31 27 25 Nico Streng VfL Rathenow Ü39 1979 16 00:14:32.6 00:15:23.6 00:15:06.8 00:45:03.0 00:45:03.0 3 00:12:32.9
32 28 10 Burkhard Severon SC Ketzin Ü39 1955 17 00:15:11.7 00:15:19.4 00:14:44.3 00:45:15.4 00:45:15.4 3 00:12:45.3
33 5 3 Nicole Michel TSV Chemie Premnitz Ü39 1979 2 00:14:51.8 00:15:37.3 00:15:29.2 00:45:58.3 00:45:58.3 3 00:13:28.2
34 29 26 Steffen Hansch U40 1985 12 00:15:44.5 00:15:31.3 00:15:16.0 00:46:31.8 00:46:31.8 3 00:14:01.7
35 6 5 Juliane Dzialas Family Fitness Rathenow U40 1982 4 00:15:27.8 00:15:43.6 00:15:37.1 00:46:48.5 00:46:48.5 3 00:14:18.4
36 7 21 Anke Meißner-Koch SC Ketzin Ü39 1978 3 00:15:10.5 00:15:42.6 00:16:08.7 00:47:01.8 00:47:01.8 3 00:14:31.7
37 30 38 Torsten Schleuß VPL Rathenow Ü39 1974 18 00:14:53.9 00:15:58.2 00:16:10.6 00:47:02.7 00:47:02.7 3 00:14:32.6
38 8 45 Carla Kron SV Leonordo-da-vinci U40 2007 5 00:14:49.7 00:17:18.3 00:16:04.6 00:48:12.6 00:48:12.6 3 00:15:42.5
39 9 14 Jane Berger Rathenow Ü39 1980 4 00:15:43.2 00:16:39.6 00:17:26.4 00:49:49.2 00:49:49.2 3 00:17:19.1
40 10 46 Tina Kron Ü39 1976 5 00:16:08.8 00:17:33.9 00:17:53.3 00:51:36.0 00:51:36.0 3 00:19:05.9
41 11 7 Christin Sommer Family Fitness Rathenow U40 1989 6 00:16:18.1 00:17:37.9 00:18:11.7 00:52:07.7 00:52:07.7 3 00:19:37.6
42 12 6 Ines Hackmann Family Fitness Rathenow Ü39 1968 6 00:17:17.0 00:18:13.2 00:18:21.4 00:53:51.6 00:53:51.6 3 00:21:21.5
43 13 42 Evelyn Awe Family Fitness Ü39 1959 7 00:17:17.2 00:18:13.0 00:18:21.7 00:53:51.9 00:53:51.9 3 00:21:21.8
44 31 29 Dieter Werner Laufgruppe Bünger Ü39 1943 19 00:17:40.9 00:18:13.8 00:18:53.6 00:54:48.3 00:54:48.3 3 00:22:18.2
45 14 33 Ingrid Krügel LG Bünger Ü39 1944 8 00:17:41.3 00:26:30.3 00:24:47.8 01:08:59.4 01:08:59.4 3 00:36:29.3
46 15 8 Kristiana Deutschmann LG Bünger Rathenow Ü39 1951 9 00:21:43.2 00:23:49.5 00:24:02.7 01:09:35.4 01:09:35.4 3 00:37:05.3


Sprawling over 8000 sq. feet, Nostalgia showcases furniture and unique object d art from different parts of the world. The enterprise also embodies warehousing and customising pieces as desired by its esteemed patrons.


text:
Chris Kovarik  (born 1 March 1978, Dandenong, Victoria, Australia), is an Australian professional racing cyclist specialising in downhill mountain biking and four cross mountain bike racing. He is a multiple Australian national champion and multiple World Cup winner.

Cycling career
Kovarik started competitive cycling when he was 17 years old and has been a member of the Chain Reaction Cycles/Intense Cycle's MTB Race team  since its creation in 2008.  Kovarik was joined by fellow Intense rider Finland's Matti Lehikoinen for the 2010 race season.

In 2004, Kovarik shattered his ankle, broke the tibia on the same leg and spent 4½ months with a metal cage around his leg, leading to 7 months off the bike and missing the 2004 World Cup/Championship season.  At the time, doctors had said that he may never ride again, however, he went on to place 5th in the World Championships in New Zealand in 2005.

In 2008 Kovarik married teammate and fellow downhill mountain Bike rider, Canadian Claire Buchar.

Chris won the Australian National Downhill Championships in January 2010 at the SRAM Corporation Australian Mountain Bike Championships in Adelaide.

Kovarik's  career highlights include
 2006 - 1st World Cup : Mont Saint Anne
 2005 - 5th World Championships : New Zealand
 2002 - 1st World Cup : Fort William (won by 14 secs)
 2002 - Australian National Champ
 2001 - Australian National Champ
 2000 - Australian National Champ

Past Results

1998
 1st DH MTB National Series Round VIC
 2nd DH MTB National Series Round NSW

1999
 1st DH MTB Norba Series Mammoth Mountain USA
 1st DH Norba Series Deer Valley USA
 2nd DH MTB World Cup USA
 2nd DH Norba Series Mount Snow USA
 2nd DH MTB Australian Titles VIC
 2nd DH MTB National Series Round VIC
 3rd DL MTB Australian Titles NSW
 10th DH MTB World Cup USA

2000
 1st DH MTB Australian Titles QLD
 1st DH MTB Norba Series Round USA
 1st DH MTB National Series Round QLD
 1st DH MTB National Series Round VIC
 2nd DH MTB Norba Series Round USA
 3rd DL MTB National Series Round VIC
 7th DH MTB World Cup
 8th DH MTB World Cup USA
 10th DH MTB World Championships ESP
 11th DH MTB World Cup CAN

2001
 1st DH MTB Australian Titles VIC
 1st DH MTB World Cup CAN
 1st DH MTB National Series Round VIC
 2nd DH MTB World Cup CAN
 2nd DH MTB World Cup FRA
 3rd DH MTB Norba Series #1 USA
 3rd DH MTB Norba Series #3 USA
 4th DH MTB World Championships USA
 4th DL MTB World Cup CAN
 4th DH MTB World Cup #1
 5th DH MTB Norba Series 2 USA

2002
 1st DH MTB World Cup USA
 1st DH MTB World Cup GBR
 1st DH MTB World Cup SLO
 1st DH MTB Australian Titles NSW
 1st DH MTB Championships Series USA
 3rd DH MTB World Championships AUT
 3rd DH MTB National Points Series GBR
 4th National MTB Series USA
 5th DH MTB Mercury Sea Otter Classic USA
 5th 4X MTB Mercury Sea Otter Classic USA
 8th DH MTB World Cup FRA
 9th DH MTB World Cup CAN
 17th 4X MTB World Championships AUT

2003
 1st DH Norba Series #2 USA
 2nd DH MTB World Cup FRA
 2nd 4X Norba Series #3 USA
 4th DH MTB World Championships SUI
 5th 4X Norba Series #2 USA
 6th DH MTB World Cup GBR

2005
 2nd DH MTB World Cup #3 AUT
 3rd DH MTB World Cup #6 USA
 4th DH MTB World Cup #8 GBR
 4th DH MTB World Cup #2 GER
 5th DH MTB World Cup #4 CAN
 8th DH Australian MTB Championships VIC
 9th 4X MTB World Cup #6 USA
 11th 4X MTB World Cup #4 CAN
 17th DH MTB World Championships ITA
 41st DH MTB World Cup #7 ITA

2006
 1st DH MTB World Cup #4 CAN
 3rd 4X MTB World Cup #4 SCO
 3rd Australian DH MTB Championships VIC
 5th DH MTB World Championships NZL
 5th DH MTB World Cup #3 GER
 8th DH MTB World Cup #1 ESP
 9th DH MTB World Cup #6 AUT
 15th DH MTB World Cup #5 BRA
 20th DH MTB World Cup #4 SCO
 49th 4X MTB World Cup #1 ESP

2007
 7th 4X MTB World Cup #4 AUT
 23rd DH MTB World Cup #4 AUT
 38th DH MTB World Cup #1 ESP
 86th DH MTB World Championships GBR

2008
 6th MTB World Cup DH #2 Andorra
 12th DH MTB World Championships ITA

References

External links

1978 births
Living people
Australian male cyclists
Sportsmen from Victoria (Australia)
People from Dandenong, Victoria
Australian mountain bikers
Cyclists from Melbourne

redpajama_set_name: RedPajamaWikipedia


More people have been charged as part of a continuing crackdown on antisocial behaviour, violence and drugs in south Aberdeenshire.
Operation Bayswater, run by local police in towns across the area, involves officers and special constables working together with others to prevent and detect crime.
During the evenings of Friday 7 to Sunday 9 September 2018, police targeted areas where antisocial behaviour or violence has previously been reported.
In Inverurie, a 27-year old man and 25-year old man were charged in connection with antisocial behaviour in the town centre.
A 25-year old man was charged in connection with antisocial behaviour and resisting arrest, while a 20 year old was also arrested in connection with his unacceptable behaviour.
A 17-year old man and a 15-year-old youth were charged after allegedly being found in possession of cannabis.
A 30 year old woman was also charged in relation to theft by shoplifting.
In Stonehaven, a 27-year old man was charged in connection with alleged possession of cannabis, while a 25-year old man was charged for allegedly possessing ecstasy.
In Banchory, an 18-year old man was charged in relation to vandalism and resisting arrest.


Our paper "Liquid marble-derived solid-liquid hybrid superparticles for CO2 capture" has been accepted to Nature Communications.
The force applied to the particle adsorbed on a surface of a fluid droplet or bubble can be expressed in an analytical form as a function of the displacement of the particle from its equilibrium position.
Effective dilatational viscosity of particle-laden fluid interfaces can be expressed in an analytical form in the limits of small and large surface concentrations of the particles.
Account of many-body inter-atomic interactions in simple fluids is necessary for accurate description of their bulk viscosity, in contrast with other transport properties.
The equation of state of hard-disk fluids on curved surfaces depends upon the gaussian curvature of the surface. This dependence contributes to the value of the saddle-splay modulus of particle-laden fluid interfaces.
Finite-size effects significantly influence the interfacial tension of planar vapour-liquid interfaces.
The Lekner method for calculation of electrostatic interactions in periodically replicated cells can be extended to quasi-two-dimensional systems of particles with dipolar interactions. This technique is sometimes referred to as "Lekner–Lishchuk summation".
The spectrum of surface waves at a monomolecular surfactant film between an isotropic liquid and a nematic liquid crystal exhibits rich structure.
In 1999–2002 I initiated the development of the ms* series of molecular simulation codes. One of them (ms2) became so successful that it now lives a life of its own.
The algorithm known as "Lishchuk method" is implemented within STFC Daresbury Laboratory′s simulation package DL_MESO.
The hybrid Cellular Automata Finite Element (CAFE) model is capable of predicting the evolution of pitting corrosion damage during the pre-crack stages of environment assisted cracking.
Contact me. The best way to contact me is by email sergey.lishchuk@gmail.com.
Howard Street, Sheffield S1 1WB, United Kingdom.


Saving for a home deposit has never been harder – but there are several ways willing parents can help their kids crack the market.
With property prices continuing to rise and the high cost of renting making it virtually impossible for many young aspiring home buyers to save, a growing number of parents are helping their children buy their first home.
Rather than leaving their hard-earned cash and assets to their children as an inheritance, many parents prefer to help them out now. But helping your children realise their dream of home ownership doesn't have to mean forking out the cash to buy a property for them.
One of the most common ways parents can help out their children is by acting as a guarantor on their mortgage. Essentially this involves offering the equity in your home as security for your child's loan – helping them to meet lenders' deposit requirements. This is a good way to help without actually having to stump up any cash or hold any stake in the property yourself. Of course, in the event that your child has trouble meeting their loan obligations, you will be held accountable – so it's important to be confident that your child will be able to manage their loan commitments.
Another way parents can help their children is by joining forces and co-purchasing with them. This not only reduces the initial sum your child will need to save to enter the market, it will make their repayments just that bit easier to manage. At the same time, you'll be building your own property portfolio. Just be sure to enter any co-purchase arrangement with care, and have a legally binding agreement that sets out all parties' commitments and entitlements to avoid any potential disputes.
A gift in the form of a deposit, or part of one, is another way to give your children a helping hand into the market. Equally, just offering your children an interest free loan for their deposit could save them thousands of dollars.
With rental costs one of the biggest barriers to saving a deposit, helping your children to reduce their rent obligations can be an enormous help. Whether it's offering them lower board, rent free accommodation or below-market rates in one of your investment properties, this can help your children save a deposit.


text:
/**
 * Module dependencies
 */
var actionUtil = require('sails/lib/hooks/blueprints/actionUtil'),
  _ = require('lodash'),
  async = require('sails/node_modules/async');

/**
 * Find Records
 *
 *  get   /:modelIdentity
 *   *    /:modelIdentity/find
 *
 * An API call to find and return model instances from the data adapter
 * using the specified criteria.  If an id was specified, just the instance
 * with that unique id will be returned.
 *
 * Optional:
 * @param {Object} where       - the find criteria (passed directly to the ORM)
 * @param {Integer} limit      - the maximum number of records to send back (useful for pagination)
 * @param {Integer} skip       - the number of records to skip (useful for pagination)
 * @param {String} sort        - the order of returned records, e.g. `name ASC` or `age DESC`
 * @param {String} callback - default jsonp callback param (i.e. the name of the js function returned)
 */

module.exports = function findRecords (req, res) {

  // Look up the model
  var Model = actionUtil.parseModel(req);

  // If an `id` param was specified, use the findOne blueprint action
  // to grab the particular instance with its primary key === the value
  // of the `id` param.   (mainly here for compatibility for 0.9, where
  // there was no separate `findOne` action)
  if ( actionUtil.parsePk(req) ) {
    return require('sails/lib/hooks/blueprints/actions/findOne')(req,res);
  }

  // Lookup for records that match the specified criteria
  var query = Model.find()
  .where( actionUtil.parseCriteria(req) )
  .limit( actionUtil.parseLimit(req) )
  .skip( actionUtil.parseSkip(req) )
  .sort( actionUtil.parseSort(req) );
  query = actionUtil.populateRequest(query, req);

  var queryCount = Model.count().where(actionUtil.parseCriteria(req));

  async.parallel({
    data: getData,
    count: getTotalCount
  }, function (err, results) {
    res.ok(results);
  });

  //////////////////

  function getTotalCount(cb) {
    queryCount.exec(function (err, count) {
      cb(null, count);
    });
  }

  function getData(cb) {
    query.exec(function found(err, matchingRecords) {
      if (err) return res.serverError(err);

      // Only `.watch()` for new instances of the model if
      // `autoWatch` is enabled.
      if (req._sails.hooks.pubsub && req.isSocket) {
        Model.subscribe(req, matchingRecords);
        if (req.options.autoWatch) { Model.watch(req); }
        // Also subscribe to instances of all associated models
        _.each(matchingRecords, function (record) {
          actionUtil.subscribeDeep(req, record);
        });
      }

      cb(null, matchingRecords);
    });
  }

};


Base class for nearly all descriptors, providing common functionality.
The file this descriptor was declared in.
The fully qualified name of the descriptor's target.
The index of this descriptor within its parent descriptor.
Returns the name of the entity (field, message etc) being described.