Everyone knows that the way to make coins is to play the minigames in Club Penguin but some games are better for playing coins than others. A lot better. If you want to earn coins quickly in Club Penguin you should be playing these three games. They are the best way to take advantage of the limited Club Penguin money cheats in the game.
Puffle Round Up is easy to play and fun. In this game you help round up puffles. Click on the Employees Only door in the Pet Shop and use your mouse to herd puffles into the fenced area.
A round ends when all the puffles are herded into the pen or have run away. Coins are awarded based on the number of puffles you catch in the shortest amount of time.
You will get a lot of coins playing this game and it is really easy. The games go by pretty quickly so it doesn't get too boring.
In Cart Surfer you will speed along a mine track in a cart. You earn points for doing tricks in the cart while you are going down the track. You use the keyboard arrows and spacebar to discover trick combinations. Cart Surfer is a single-player game and you play it by clicking on the carts inside the Mine.
The best way to make coins quickly in Cart Surfer is to do just two moves, the backflip and the spin. They give you 100 points and 80 points. Just remember to always alternate between them to get the full points. If you repeat the same move twice or more in a row, you only get half points each time.
Go to the Pizza Parlor and click on the beaded doorway to become a pizza chef. Use your mouse to drag and drop the toppings that show up on the order screen. Get paid coins for every correct pizza you make. The more correct pizzas you make in a row, the more coins you get. If you have a perfect game in Pizzatron 3000, you will get a lot of coins. A perfect game lasts about 6 minutes so if you are good and fast, you can get a lot of coins very quickly.
There are a lot of other minigames in Club Penguin, but these three are the best for making coins quickly. But if you get bored and want to try other games, here is a list.
I played pizzatron and had a perfect game, and one pizza left. I then pressed a button on my mouse that refreshed.
thanks for all the tips but could you pleaseget some more in there,i've been there for over 80 times so i relley neen some more!
It didn't work 4 me!!!!
I think GO FISHING is the best game 4 money.u get 100 coins for catching the mullet,to get it u use the normal fish for bait instead of reeling it in.
thx for the list, it realy helped!


text:
how gold is formed in the earth
Gold on Earth formed in collision of exotic stars - USA TODAY
· Gold on Earth formed in collision of exotic stars. The gold glinting from jewelry store windows, or in your wedding band, astronomers report Wednesday,was likely born in …
How Gold Gets Out Of The Ground | ETF.com
The Earth's crust contains approximately 0.004 grams of gold per ton, and there is even a lot of gold in saltwater - but concentrating the trace amounts just doesn't make economical sense.
How was gold formed in the earth? | Socratic
When universe formed only hydrogen and helium was there..Rest all elements were cooked up in stars.Sun and solar system got its matter from the remnants of a star which exploded as supernova..So gold not formed in earth but came from the supernova of parent star pof the Sun.
Prospecting Encyclopedia: Geology of how Gold Deposits ...
The effort to understand the geology of gold was perhaps man's first serious effort at understanding the earth's rocks and minerals. Gold is actually a relatively scarce element on the crust of the earth, but it occurs in trace quantities spread throughout many different kinds of rocks and in many different geological environments.
How is gold formed ers.com
Gold is an element and is formed in the core of large stars, especially during a nova. On Earth, veins of gold are formed by separation from liquid rock after gravity agglomerates the molecules.
The Mysterious Origin of Our Galaxy's Gold - The Atlantic
Across history and folklore, the question of where Earth's gold came from—and maybe how to get more of it—has invited fantastical explanation.
Earth's Inner Fort Knox | DiscoverMagazine.com
Earth formed from a series of smaller planetesimals that crashed together over the course of 30 million to 40 million years. Wood deduced how much gold ought to be present in Earth's crust by comparing the crust's composition to that of meteorites similar to the planetesimals.
How does Gold Naturally Form on Earth's Crust - Veins
Gold is not formed on the Earth like diamonds and many other gems and minerals. Instead, most scientists now believe that gold actually came to earth from outer space in large meteorites that have struck the planet over billions of years. In fact, most of the gold on Earth is actually located in its core where its heavy properties caused it to ...
extracting gold from the earth s crust
Gold Extraction / Mining Gold . Even though the precious metal gold only occurs very rarely indeed, it can be found almost everywhere on the planet in the 16 kilometre thick Earth's crust.
EARTH SCIENCE FACTS - Explorit Science Center
Earth not only orbits the sun but spins on its own axis as it does so. At the equator the Earth is spinning on its axis at a speed of about 1,038 miles (1,670 kilometres) an hour. Earth's spin or rotation is a relic of its origin as a hot, spinning mass when it was first formed. Earth science or geology is the science of the Earth.
Formation of gold | Ergo
Ancient Greeks believed that gold was formed by the rays of the sun transforming common metals in the earth. Scientists today still think that gold formation is related to stars, specifically dying stars.
Geology of Gold Mineralization & How Gold Deposits are Formed
Gold is relatively scarce in the earth, but it occurs in many different kinds of rocks and in many different geological environments. Though scarce, gold is concentrated by geologic processes to form commercial deposits of two principal types: lode (primary) deposits and placer (secondary) deposits.
Gold - USGS
Gold is called a "noble" metal (an alchemistic term) because it does not oxidize under ordinary conditions. Its chemical symbol Auis derived from the Latin word "aurum." In pure form gold has a metallic luster and is sun yellow, but mixtures of other metals, such as silver, copper, nickel, platinum, palladium, telluri-
How Is Gold Formed and Where Does it Come From ...
Gold isn't truly formed—at least, not on Earth. Gold Comes From Outer Space Gold, the shiny yellow metal prized for its beauty and malleability and used in many different industries, is actually created inside massive stars when they explode into a supernova.
Chemistry for Kids: Elements - Gold - Ducksters
Gold is an extremely rare element on Earth. Because it doesn't react with very many other elements, it is often found in its native form in the Earth's crust or mixed with other metals like silver. It can be found in veins underground or in small fragments in sandy riverbeds.
How is gold formed in earth? | Yahoo Answers
· The amount of gold in the earth has been constant since the earth was formed 4.5 billion years ago after the "Big Bang" (except for maybe a little bit that has left the earth on some deep space probes like Explorer).
How Is Quartz Formed? | Sophisticated EDGE
How quartz is formed depends on two of the most prevalent materials in the earth's crust, silicon and oxygen. Quartz is an abundant element appearing in many forms within the earth's crust; known as silicon dioxide or Si02.
Where is gold found on earth? - Gold-Traders (UK) Ltd
Despite the fact that gold can be found almost everywhere, there is very little gold in comparison to other elements on earth. In fact, if all the gold ever discovered were collected and melted down and formed into one cube, it would measure just 20 meters on each side.
How is gold formed in the Earth's crust ers.com
As gold isn't a compound (it's an element), it's not formed in the earth's crust. Because of this, there is a pre-existing, set amount of gold on earth.
How Is Quartz Formed? | Our Pastimes
Quartz is present in many other types of rock, including granite, sandstone, shale, schist, gneiss, quartzite and various other rocks in all three major categories--igneous, metamorphic and sedimentary. Natural Formation. Quartz can be formed naturally from the silica which collects in the earth.
How is gold formed? - Quora
Gold atoms are not formed in the earth, but existed before the earth was formed. I have read somewhere that gold atoms were formed in stars or supernovae or so, and that remnants of those explosions became the raw material for new systems, like our solar system.
How Is Gold Formed – American Mining Rights Association
Gold is an inert element therefore it is not actually formed, but instead exists in its natural state contained within the earth's crust. When referring to the formation of gold we are actually discussing gold deposits such as gold flakes, nuggets, ores, and veins.
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redpajama_set_name: RedPajamaCommonCrawl


Reserving your adventure with Appalachian Adventures is just the first step! Upon Arrival at Mines and Meadows you'll need to come check-in at our main office to pay for your normal admission separately. (We left that part out of the rental prices just to keep things a little simpler on our end) Once you're checked-in and ready to go, our Appalachian Adventure rep will get you squared up with your machine!
They will teach you the basics on everything you need to know to operate your rental machine safely! Rentals include DOT Approved helmets and protective eyewear. Once you feel that you are comfortable on your rental, you're off to have the adventure of a lifetime!
Renters still must fill out a Mines and Meadows Waiver!
Appalachian Adventures now offers us ATV rentals, and we took full advantage of it! After a short time of not having rentals available, we knew that you, the people, wanted to come ride with us at Mines and Meadows. But not everyone has their own machine. Soon to be on-site in mid April, Appalachian Adventures has your machine here and ready for you! Check out their website or call to for more information and to reserve your rental date!


Ensure that your Amazon Lambda functions do not share the same AWS IAM execution role in order to promote the Principle of Least Privilege (POLP) by providing each individual function the minimal amount of access required to perform its tasks. There should be always a one-to-one relationship between your AWS Lambda functions and their IAM roles, meaning that each Lambda function should have its own IAM execution role, therefore this role should not be shared between functions.
The permissions assumed by an AWS Lambda function are determined by the IAM execution role associated with the function. Using this IAM role with more than one Lambda function will violate the Principle of Least Privilege. With the right IAM execution role you can control the privileges that your Lambda function has, thus instead of providing full or generic permissions you should grant each execution the permissions that your function really needs.
05 Select the Configuration tab then click Execution role to expand the panel with IAM role that defines the permissions for the selected function.
06 Within Execution role section, check the name of the IAM role assigned to the selected function, available in the Existing role dropdown list.
07 Go back to the AWS Lambda Functions page and repeat steps no. 4 – 6 for the rest of the functions provisioned within the selected AWS region. If two or more Amazon Lambda functions share the same IAM execution role, the permissions configuration of your AWS Lambda functions available within the selected region violates the Principle of Least Privilege (POLP).
05 Repeat step no. 3 and 4 for the rest of the functions available within the selected AWS region and compare the IAM role ARNs. If two or more Amazon Lambda functions share the same IAM execution role, the permissions configuration of your AWS Lambda functions available within the selected region defies the Principle of Least Privilege (POLP).
04 Choose the Lambda function that you want to reconfigure then click on the function name to access its configuration page.
To apply an existing execution role, select Choose an existing role from the first dropdown list, then select the name of the existing IAM role from the second dropdown list. The chosen IAM role cannot be associated with another Lambda function and must adhere to the Principle of Least Privilege by providing only the access permissions required by the selected function.
To apply a new execution role, built using Lambda policy templates, select Create new role from template(s) from the first dropdown list, enter a unique name for the IAM role within Role name box and select one of more templates from the Policy templates dropdown list.
To apply a custom execution role, select Create a custom role from the dropdown list to redirect you to the AWS Lambda requires access to your resources page where you can create your own IAM execution role for the selected Lambda function. Once your new custom role is defined, click Allow to add the custom IAM role to the current function configuration.
07 Click the Save button from the dashboard top menu to update the function configuration and apply the individual IAM execution role.
08 Go back to the AWS Lambda Functions page and repeat steps no. 4 – 7 for the rest of the Amazon functions available in the selected AWS region. Make sure each Lambda function uses its own individual IAM execution role with the right set of permissions.
09 Change the AWS region from the navigation bar and repeat the entire process for the other regions.
08 Repeat steps no. 1 – 7 for the rest of the Amazon functions available within the selected AWS region. Make sure each Lambda function uses its own individual IAM execution role with the right set of permissions to promote the Principle of Least Privilege.
Cloud Conformity allows you to automate the auditing process of Using An IAM Role For More Than One Lambda Function. Register for a 14 day evaluation and check your compliance level for free!


text:
//
//  gdt.h
//  Firedrake
//
//  Created by Sidney Just
//  Copyright (c) 2012 by Sidney Just
//  Permission is hereby granted, free of charge, to any person obtaining a copy of this software and associated
//  documentation files (the "Software"), to deal in the Software without restriction, including without limitation
//  the rights to use, copy, modify, merge, publish, distribute, sublicense, and/or sell copies of the Software,
//  and to permit persons to whom the Software is furnished to do so, subject to the following conditions:
//  The above copyright notice and this permission notice shall be included in all copies or substantial portions of the Software.
//  THE SOFTWARE IS PROVIDED "AS IS", WITHOUT WARRANTY OF ANY KIND, EXPRESS OR IMPLIED,
//  INCLUDING BUT NOT LIMITED TO THE WARRANTIES OF MERCHANTABILITY, FITNESS FOR A PARTICULAR
//  PURPOSE AND NONINFRINGEMENT. IN NO EVENT SHALL THE AUTHORS OR COPYRIGHT HOLDERS BE LIABLE
//  FOR ANY CLAIM, DAMAGES OR OTHER LIABILITY, WHETHER IN AN ACTION OF CONTRACT, TORT OR OTHERWISE,
//  ARISING FROM, OUT OF OR IN CONNECTION WITH THE SOFTWARE OR THE USE OR OTHER DEALINGS IN THE SOFTWARE.
//

#ifndef _GDT_H_
#define _GDT_H_

#include <types.h>
#include "tss.h"

#define GDT_FLAG_DATASEG 	0x02
#define GDT_FLAG_CODESEG	0x0A
#define GDT_FLAG_TSS    	0x09

#define GDT_FLAG_SEGMENT	0x10
#define GDT_FLAG_RING0   	0x00
#define GDT_FLAG_RING3   	0x60
#define GDT_FLAG_PRESENT 	0x80

#define GDT_FLAG_4K      	0x800
#define GDT_FLAG_32_BIT  	0x400

#define GDT_ENTRIES 		6

void gdt_init(uint64_t *gdt, struct tss_s *tss);

#endif /* _GDT_H_ */

redpajama_set_name: RedPajamaGithub


text:
(+263) (242) 704118 | 706260
info@jsc.org.zw
Labour Court
Magistrate's Court
Sheriff of the High Court
Master's Office
The Judicial Service Commission as a policy making body is supported by a Secretariat headed by the Secretary whose responsibility shall, subject to the Commission's directions, supervise and manage the Commission's staff, activities, funds and property and perform such other functions on behalf of the Commission as the Commission may assign to him or her. The Secretary is ably supported by two Deputy Secretaries.
Administratively there are two main sections each headed by a Deputy Secretary. One section is primarily concerned with court services. Under this section there are registrars of the Superior and Specialised Courts, the Magistracy, the Office of the Master of the High Court and the Legal Research department.
The other division offers necessary support services such as finance, administration, human resources, procurement and information services. In line with its policy of decentralising decision making authority, the structure of the Secretariat described above is replicated at provincial level to the extent where this is practicable with the Provincial Magistrate acting as the provincial heads of administration.
CONSTITUTIONAL COURT JUDGEMENTS INDEX
SUPREME COURT JUDGEMENTS INDEX
HIGH COURT JUDGEMENTS INDEX
THE CONSTITUTION OF ZIMBABWE
Zimbabwe Republic Police
Zimbabwe Prisons and Correctional Services
Attorney General's Office
African Law
Namibian Law
Malawi Law
Laws of South Africa
Ghana Law
Law Society of Zimbabwe
Legal Resources Foundation
Zimbabwe Legal Information Institute
Zimbabwe Law Reports
Ministry of Justice,Legal and Parliamentary Affairs
© 2018 Judicial Service Commission of Zimbabwe. All Rights Reserved.


text:
\section*{Introduction}

Mesoscale coarse-grained mechanical modeling \cite{Buehler2006, Volkov2010, Ostanin2013, Ostanin2014} is an important tool for \textit{in silico} characterization of nanostructures. The typical coarse-grained modeling approach is based on the idea of the representation of a nanostructure (\textit{e.g.} nanotube, nanoparticle, \textit{etc.}) as a set of elements, which are treated either as point masses or solid bodies (rigid or deformable), interacting via bonding or non-bonding potentials. Compared to regular molecular dynamic (MD) approaches, such models are easily as scalable as MD, while rendering much higher computational efficiency. For example, they can be used for accurate mechanical modeling of the representative volume elements of complex nanostructured materials. However, such models require the efficient and reliable description of van der Waals (vdW) interaction potentials between complex-shaped elements. Such potentials depend on multiple parameters. For example, the interaction between two rigid bodies of a fixed size requires tabulation of six-dimensional array with good precision. The description of interactions between the bodies of variable size, which is required for adaptive models, or interactions between deformable elements, requires even more degrees of freedom and leads to larger multidimensional arrays of data. This makes simple tabulation of such potentials impractical, since the time to construct such a table and the memory to store it grows exponentially with the number of dimensions (the problem known as ``curse of dimensionality''). The approach that is often used in the field is to design relatively simple analytical approximations for such interaction potentials, representing the potentials sought as separable functions \cite{Volkov2010, Ostanin2013}. Such an approach may be efficient in some situations, but in many cases it leads to over-simplifications and incorrect mechanics on the larger scale.
In this work we suggest the reliable and universal approach for storing arbitrarily complex mesoscale potentials as compressed multidimensional tables (following the terminology accepted in data science and computational linear algebra communities, such tables will be referred to as tensors below). The compression is reached via tensor-train cross approximation \cite{Oseledets2011, Oseledets2010}. It allows to construct the approximation of a tensor with the desired precision, using relatively small number of explicitly computed potential values. Such approaches were applied earlier in the field of computational chemistry \cite{Baranov2015}, however, they are still widely unknown to the community of multiscale mechanical modeling.
In order to demonstrate the pipeline of tensor approximation in application to mesoscale models, we consider relatively simple yet pratically important problem of the vdW interaction between two equal-sized cylinders. This problem is important in a context of mesoscale mechanical modeling of large assemblies of carbon nanotubes (CNTs). As has been showed earlier, the use of simple pair potentials for the description of intertube interactions between cylindrical CNT segments leads to significant artifacts in model's behavior. In the previous works \cite{Volkov2010, Ostanin2013} the problem was addressed with sophisticated analytical approximations. However, these approximations can not be transparently generalized onto more complex situations  - CNTs of different diameters, curved CNT segments \textit{etc.} Our approach presented here does not suffer from such a lack of generality and can be used in a number of similar problems of the description of interactions between complex-shaped nanostructures.

\section*{Method}

In this section we describe our technique of construction of the compressed table of the interaction potential between complex-shaped bodies with the example of vdW interactions between two equal-sized cylindrical segments of CNTs. Following the coarse-graining approach developed in \cite{Ostanin2013, Ostanin2014}, we idealize CNT segments as interacting cylindrical surfaces of uniform density. Total vdW interaction between two segments is found via the integration of standard Lennard-Jones (LJ) potential:

\begin{equation}
u_{LJ}(r)=4\varepsilon\left( \left(
\frac{\sigma}{r}\right)^{12}-\left(
\frac{\sigma}{r}\right)^{6}\right)
\end{equation}

where $r$ is the distance between particles, $\sigma\sqrt[6]{2}$ is the equilibrium distance, $-\varepsilon$ is the energy at the equilibrium distance. For carbon-carbon interaction, we accept $\sigma=3.851\ \angstrom$, $\varepsilon=0.004\ eV$. In order to avoid the integration of an artificial singular part of LJ potential, we replace the potential in near-singular region $(0,r_0), r_0 = 3.8 \angstrom $, with the cubic spline $u(r)$, satisfying $u(0)=3\ eV, u'(0) = 0, u(r_{0}) = u_{LJ}(r_{0}), u'(r_{0}) = u'_{LJ}(r_{0}) $.

We assume that carbon atoms are uniformly distributed over
surfaces of cylinders with the surface density
$\rho=\frac{4}{3\sqrt3a_{C-C}}$, where
$a_{C-C}=1.42\angstrom$ is the equilibrium carbon-carbon
bond length. The potential between cylindrical segments of
nanotubes is then represented as the integral over the
surface of each cylinder:

\begin{equation}
\label{integral}
U_t=\int\limits_{S_1}{\int\limits_{S_2}{\rho^2u_{LJ}\left(r\right)dS_1dS_2}}
\end{equation}
where $S_1$ and $S_2$ are cylinders side surfaces, $dS_1$
and $dS_2$ are the elements of surfaces, $r$ is the
distance between $dS_1$ and $dS_2$. The shapes of function
$r$ for different parametrizations are given in the Appendix.
In order to describe the mutual position and orientation of two cylinders one needs four independent variables - six variables for general rigid bodies are reduced by two due to axial symmetries of the cylinders. Since the choise and order of these four variables is important for the approximation technique we intend to use, we compare two different parameterizations. The first one includes one distance and three angles ($R,  \alpha_1,  \alpha_2,  \alpha_{12} $ ( Fig. 1(a))), whereas the second utilizes three distances and one angle ( $ t_1, t_2, H, \gamma  $(Fig. 1(b))). For both choices of independent variables, we specify the regular grid in four-dimensional space with the appropriate tabulation limits. We sample $n$ points along each independent variable, which results in $n^4$ tabulated potential values.

\begin{figure}[h]
	\centering
	\includegraphics[height=0.2\textheight]{param.eps}
	\protect\caption{\label{1 param} Two possible parameterizations of mutual position of two cylinders}
\end{figure}

Clearly, it is impossible to perform such expensive calculations ``on the fly'' for millions of interacting bodies. Therefore, within the direct approach we have to tabulate this potential function on multidimensional dense grid. It is possible for our rather simple example, but becomes computationally prohibitive in terms of required time and memory for more complex structures and corresponding potentials. Below we describe a general approach that is capable to compute such multidimensional tables fast and store them in a compact form.

Our approach is based on tensor train decomposition (TT) and tensor train cross approximation \cite{Oseledets2011, Oseledets2010}. In the TT format each element of $d$-dimensional tensor $U\left(i_1,i_2,\ldots,i_d\right)$ is
represented as the product of $d$ matrices:
\begin{equation}
\label{TT}
U\left(i_1,i_2,\ldots,i_d\right)=\sum\limits_{\alpha_0,\alpha_1,\ldots,\alpha_d}G_1\left(\alpha_0,i_1,\alpha_1\right)G_2\left(\alpha_1,i_2,\alpha_2\right)\ldots
G_d\left(\alpha_{d-1},i_d,\alpha_d\right)
\end{equation}
Here indices $\alpha_k$ are changing from $1$ to $r_k$,
which are called TT-ranks. Each matrix
$G_k\left(\alpha_k-1,i_k,\alpha_k\right)$ has the size
$r_{k-1}\times r_k$, depends on only one index of the original tensor, and these
matrices form the three-dimensional tensors, which are
called cores of the TT-decomposition. $r_0$ and $r_d$
are assigned to $1$. Intermediate TT ranks $r_k$ are determined by the TT approximation procedure to provide given approximation precision $\epsilon_{tt}$ and are conditioned by the structure of the approximated tensor.

Since tensors generated by the discretization of physically meaningful functions are typically ether low-rank or well approximated by the low-rank tensors, the decomposition (\ref{TT}) provides a powerful tool to represent such tensors in a compact form. The technique of construction of the best approximation in TT format with a given precision is described in \cite{Oseledets2010}. In this work we use the standard package TT toolbox for construction of the low-rank approximation of our potential.
In application to mesoscale modeling, TT decomposition can be used in two different ways. The first way is to accelerate the design of a full potential table and the second - to store it in a compact form. In the latter case the calculation of a single value of the potential in a nodal point would require computation of $d$ matrix-vector products, with matrix dimensions  $r_{k-1}\times r_k$.

\section*{Results and discussion}

We constructed TT decompositions for a tensor of
cylinder-cylinder interactions, for few different values of
mesh refinement and accuracy. The potential of interaction between two cylindrical segments of (10,10) CNTs with the radius $R_c = 6.78 \angstrom$  and height $2 R_c = 13.56 \angstrom$  was considered. The four-dimensional
integral (\ref{integral}) was computed using regular
rectangle quadratures over azimuthal angles of cylinders,
and Gauss quadratures over cylinders axial directions. The
number of integration points was chosen adaptively to
provide the desired integration precision $\epsilon_i = 10^{-3}$. In order to keep
our computations fast, we restricted ourselves with the best
integration precision $\epsilon_i = 10^{-3}$. In our case of
four-dimensional tensor TT-decomposition contains two
matrices and two three-dimensional tensors as TT-cores. The tensor indices correspond to the sampling of the continuous potential function on a regular grid: $U(i_1,i_2,\ldots,i_d)=U_t(x_1, x_2,\ldots, x_d)$, where
$x_d = x_d^{min} + i/n \cdot  (x_d^{max} - x_d^{min} )$. The tabulation limits $(x_d^{min}$, $x_d^{max})$ for both parametrizations are given in Table \ref{table1}.

\begin{table}[h!]
	\caption{\label{table1} Tabulation limits for two paremetrizations used.}  \centering
	\begin{tabular}{|l|l|l|l|}
		\hline
		\multicolumn{2}{c|}{Parametrization 1} &
		\multicolumn{2}{c}{Parametrization 2}\\

		\hline

		\multicolumn{1}{c|}{$R$} & \multicolumn{1}{c|}{$(2  R_c, 5  R_c)$} & \multicolumn{1}{c|}{$H$} & \multicolumn{1}{c}{$(2  R_c, 5  R_c)$}  \\

		\hline

		\multicolumn{1}{c|}{$\alpha_1$} & \multicolumn{1}{c|}{$(0, \pi)$} & \multicolumn{1}{c|}{$t_1$} & \multicolumn{1}{c}{$(-5  R_c, 5  R_c)$} \\

		\hline

		\multicolumn{1}{c|}{$\alpha_2$} & \multicolumn{1}{c|}{$(0, \pi)$} & \multicolumn{1}{c|}{$t_2$} & \multicolumn{1}{c}{$(-5  R_c, 5  R_c)$}  \\

		\hline

		\multicolumn{1}{c|}{$\alpha_{12}$} & \multicolumn{1}{c|}{$(0, \pi)$} & \multicolumn{1}{c|}{$\gamma$} & \multicolumn{1}{c}{$(0, \pi)$} \\

		\hline
	\end{tabular}
\end{table}

We
can define the compression of the tensor as the ratio of the
numbers of elements in the initial tensor and in all the
cores of the resulting TT-decomposition. The TT compression
was performed for two different parameterizations of
cylinders mutual position and different orders of variables
(TT decomposition is not invariant with respect to
permutation of tensor indices, our results are given for TT decompositions with the permutation of variables providing the lowest ranks of TT cores and the best compression). Tables \ref{table2} and
\ref{table3} give the compression number obtained for the
first and second parametrizations respectively, as a
function of the grid refinement (number of points per each
dimension) and the requested approximation precision $\epsilon_{tt}$. It
appears that even black-box application of the TT algorithm
gives significant compression of the original tensor (which
also roughly corresponds to the time needed to construct
this tensor approximation).

\begin{table}[h!]
\caption{\label{table2} The compression for the first
parameterization} \centering
\begin{tabular}{|l|l|l|l|l|}
\hline \multicolumn{1}{c|}{} & \multicolumn{4}{c}{TT approximation precision $\epsilon_{tt}$} \\
\hline \multicolumn{1}{c|}{} &
\multicolumn{2}{c|}{$10^{-3}$} &
\multicolumn{2}{c}{$10^{-2}$}\\
\hline \multicolumn{1}{c|}{$n$} & \multicolumn{1}{c|}{Max
rank} & \multicolumn{1}{c|}{Compression, $\%$} &
\multicolumn{1}{c|}{Max rank} &
\multicolumn{1}{c}{Compression, $\%$}\\
\hline \multicolumn{1}{c}{$10$} & \multicolumn{1}{c}{$20$}
& \multicolumn{1}{c}{$29.4$} & \multicolumn{1}{c}{$13$} &
\multicolumn{1}{c}{$18.2$}\\
\hline \multicolumn{1}{c}{$20$} & \multicolumn{1}{c}{$41$}
& \multicolumn{1}{c}{$13.6$} & \multicolumn{1}{c}{$16$} &
\multicolumn{1}{c}{$3.4$}\\
\hline \multicolumn{1}{c}{$30$} & \multicolumn{1}{c}{$47$}
& \multicolumn{1}{c}{$5.3$} & \multicolumn{1}{c}{$16$} &
\multicolumn{1}{c}{$1$}\\
\hline \multicolumn{1}{c}{$40$} & \multicolumn{1}{c}{$48$}
& \multicolumn{1}{c}{$2.4$} & \multicolumn{1}{c}{$16$} &
\multicolumn{1}{c}{$0.4$}\\
\hline
\end{tabular}
\end{table}

\begin{table}[h!]
\caption{\label{table3} The compression for the second
parameterization} \centering
\begin{tabular}{|l|l|l|l|l|}
\hline \multicolumn{1}{c|}{} & \multicolumn{4}{c}{TT approximation precision $\epsilon_{tt}$} \\
\hline \multicolumn{1}{c|}{} &
\multicolumn{2}{c|}{$10^{-3}$} &
\multicolumn{2}{c}{$10^{-2}$}\\
\hline \multicolumn{1}{c|}{$n$} & \multicolumn{1}{c|}{Max
rank} & \multicolumn{1}{c|}{Compression, $\%$} &
\multicolumn{1}{c|}{Max rank} &
\multicolumn{1}{c}{Compression, $\%$}\\
\hline \multicolumn{1}{c}{$10$} & \multicolumn{1}{c}{$27$}
& \multicolumn{1}{c}{$44.8$} & \multicolumn{1}{c}{$19$} &
\multicolumn{1}{c}{$30$}\\
\hline \multicolumn{1}{c}{$20$} & \multicolumn{1}{c}{$65$}
& \multicolumn{1}{c}{$24.7$} & \multicolumn{1}{c}{$33$} &
\multicolumn{1}{c}{$10.2$}\\
\hline \multicolumn{1}{c}{$30$} & \multicolumn{1}{c}{$85$}
& \multicolumn{1}{c}{$12.1$} & \multicolumn{1}{c}{$38$} &
\multicolumn{1}{c}{$3.4$}\\
\hline \multicolumn{1}{c}{$40$} & \multicolumn{1}{c}{$96$}
& \multicolumn{1}{c}{$6.3$} & \multicolumn{1}{c}{$39$} &
\multicolumn{1}{c}{$1.5$}\\
\hline
\end{tabular}
\end{table}

Figure \ref{slices} illustrates the quality of the approximation of a complex potential relief at few cross-sections that correspond to in-plane (a) and out-of-plane (b) rotaton of one cylinder with respect to another for different intercenter distances. As we can see, the compressed potential representation fully reproduce original tensor.

\begin{figure}[h!]
\centering
\includegraphics[height=0.2\textheight]{slices.eps}
\protect\caption{\label{slices} The potential in the first parametrization ($U( R, \alpha_1, \alpha_2, \alpha_{12} )$, solid red) and its TT approximation (dotted blue, $n=50$, $\epsilon_{tt}= 10^{-2}$), as a function of one of parametrization angles and few different values of $R$: (a) $\alpha_1 \in (0, \pi)$, $\alpha_2 = 0$, $\alpha_{12}=0$, $R = 19.8, 20.6, 21.4, 22.2$, (b) $\alpha_{12} \in (0, \pi)$, $\alpha_1 = 0$, $\alpha_2=0$, $R = 14.4, 14.8, 15.2, 15.6$.}
\end{figure}

\section*{Conclusion}

In this note we have demonstrated the successful application of the technique that have recently emerged in the community of computational multilinear algebra - tensor-train cross approximation - to the problem of representation of the interaction potentials in modern mesoscale models. Within this approach the multidimensional potential table can be constructed based on just few direct calculations of the potential values, which dramatically accelerates construction of such a table. In the case when memory efficient representation is required, this table can be stored in a compact form and then each required value of the potential can be recovered at a moderate computational cost. In case when performance of on-the-fly computations is the highest priority, our approach can be used for fast construction of the full multidimensional table. The instruments for such approximaiton are freely available as components of  the open source software TT-toolbox (\url{https://github.com/oseledets/ttpy}),  and our code, performing the approximation of cylinder-cylinder vdW interaction potential, can be found at \url{https://bitbucket.org/iostanin/cnt_potential_tt_compression/}. The resulting approximations can be easily stored in either full or compact form, and further used in the framework of such existing mesoscale models as MDEM \cite{Ostanin2013, Ostanin2014, Ostanin2015}. Our approach appears to be particularly useful for the problems involving interactions between complex deformable shapes - \textit{e.g.} CNT segments with variable length, radius, curvature and flatness.

\section*{Acknowledgements}

Authors gratefully acknowledge partial financial support from Russian Foundation for Basic Research under grants RFBR 16-31-00429, RFBR 16-31-60100. This work was partially supported by an Early Stage Innovations grant from NASA's Space Technology Research Grants Program.

\section*{Appendix}

Here we give the explicit shapes for the functions $r$ for two parameterizations used. In both cases the distance depends on four variables describing the mutual position of two cylinders, and four more variables - axial coordinates $z_1, z_2$ and azimuthal angles $ \varphi_1, \varphi_2 $, describing the positions of surface elements $dS_1$ and $dS_2$ on cylinders' side surfaces.
First parameterization:
$$r(dS_1,dS_2)=r( R, \alpha_1, \alpha_2, \alpha_{12}, z_1,z_2,\varphi_1,\varphi_2)=$$
$$\Big(\big(z_2
\sin{\alpha_{12}}\sin{\alpha_2}-R_c\left(\cos{\alpha_2}
\cos{\varphi_2}\sin{\varphi_2}+\sin{\varphi_1}\right)\big)^2+$$
$$+\big(R\sin{\alpha_1}+z_2\left(\cos{\alpha_2}\sin{\alpha_1}
-\cos{\alpha_1}\cos{\alpha_{12}}\sin{\alpha_2}\right)+$$
$$+R_c\big(\cos{\varphi_2}\sin{\alpha_1}\sin{\alpha_2}+
\cos{\alpha_1}\cos{\alpha_{12}}\cos{\alpha_2}\cos{\varphi_2}-$$

$$\cos{\alpha_1}\sin{\alpha_{12}}\sin{\varphi_2}-\cos{\varphi_1}
\big)\big)^2+$$
$$+\big(R\cos{\alpha_1}+z_2\left(\cos{\alpha_1}\cos{\alpha_2}+
\cos{\alpha_{12}}+\cos{\alpha_{12}}\sin{\alpha_1}
\sin{\alpha_2}\right)+$$
$$+R_c\big(\cos{\alpha_1}\cos{\varphi_2}\sin{\alpha_2}-
\cos{\alpha_{12}}\cos{\alpha_2}\cos{\varphi_2}
\sin{\alpha_1}+ $$
$$\sin{\alpha_1}\sin{\alpha_{12}}\sin{\varphi_2}
\big)-z_1\big)^2\Big)^{1/2}$$

Second parameterization:
$$r(dS_1,dS_2)=r(t_1, t_2, H, \gamma, z_1,z_2,\varphi_1,\varphi_2)=$$
$$\Big(
\big(\left(t_2+z_2\right)\sin{\gamma}+R_c\left(\sin{\varphi_1}-
\cos{\gamma}\sin{\varphi_2}\right)\big)^2+$$
$$+\big(H+R_{c}\left(\cos{\varphi_2}-\cos{\varphi_1}
\right)\big)^2+$$
$$+\big(\left(t_2+z_2\right)\cos{\gamma}-R_c\sin{\gamma}\sin{\varphi_2}-
\left(t_1+z_1\right)\big)^2\Big)^{1/2}$$

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Brown one pound chili meat in 2 oz. suet. Add one heaping tablespoon Bolner's Fiesta Brand Chili Mix Seasoning and one pint water. Cook slowly 45 minutes. Thicken if desired. For higher seasoning, add more Chili Mix.


Moynihan, Sinéad: ""Watch me go invisible". Representing Racial Passing in Mat Johnson and Warren Pleece's Incognegro." In: South Central Review 32.3 (2015), S. 45–69.
This essay examines the potential of the graphic novel as a vehicle to explore one of the most enduring tropes in American culture: racial passing. As what Hillary Chute and Marianne DeKoven term a "hybrid project," graphic narrative has the potential to pose "a challenge to the structure of binary classification that opposes a set of terms, privileging one." Since passing narratives are themselves devoted to unsettling binaries – racial binaries – this essay considers the marrying of the graphic novel and the passing narrative in Mat Johnson and Warren Pleece's Incognegro (2008). How, in other words, can what Scott McCloud terms "the art of the invisible" (comics) depict what Joel Williamson memorably calls "invisible blackness"?
The essay is particular interested in two aspects of Incognegro's hybridity, one of which relates content, the other to form. First, in terms of content, the collaborators make several significant revisions to the comic book's signature character, the superhero, amalgamating the conventions of the superhero story with those of passing narratives in order to destabilise some of both genres' most telling assumptions. Second, in terms of formal devices, this essay examines the particular combination of visual and textual vocabularies deployed in Incognegro to portray the ambiguously-raced subject, comparing it to the ways in which such subjects have been racially-encoded in more conventional literary and cinematic narratives of passing. Ultimately, this essay considers whether Incognegro's hybrid properties offer new political possibilities for the narrative of racial passing.


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Haas part number BBK-75-500630-WI shown above. Download technical drawings for each stock part number on the right. Download free Adobe PDF reader and SolidWorks Viewer on the left.


The "Food" section on the New York Times has to be one of my favorite free-time reads. I read it all: the recipes, the restaurant reviews, the random opinion pieces… you name it, I probably read it! Not only is it well-written, but it can also be surprisingly interesting. I mean, I've learned about so many random things ranging from traditions and ingredients, all the way to chefs and hottest trends. Most recently, I stumbled upon a fun little article about Marcella Hazan's favorite beans. I told you… random. But I still read it! Apparently, nothing comes close to a warm plate of these white beans with a drizzle of good olive oil. Yet, her favorite variety could only be found in Italy, so the owner of California-based Rancho Gordo decided to grow them there for her. They are apparently the only ones growing them in the US and decided to call them "Marcella's" in honor of the chef.
After reading this piece, two beans-related thoughts came to my mind. The first was that I really wanted to come up with more recipes for them. Sure, I could make traditional cassoulet or a side of French flageolets, but that was the extent of my experience with beans. Right then, I was craving something more modern and fresh. The second was Heidi Swanson's pan fried giant white beans recipe. Adding one to the other, I rushed to the kitchen and created my twist on Heidi's recipe. I had some giant butter beans in my pantry, and some spinach in my fridge. I added mushrooms and onions because one can never go wrong with those, and what resulted is pictured right below.
Now this is totally different from Marcella Hazan's beans (and way to cook them, which I shall both try eventually) but it's pretty damn good! Once pan fried, the skin around these beans gets golden and crispy while their center remains creamy. The freshly grated cheese brings the dish to the next level. It's veggie comfort food at its best!
I'll be sure to experiment more with different varieties and recipes throughout winter. Let me know if you have your own favorites (varieties or recipes) in the comments – I'd love to learn more about these gems. After trying a recipe on my own, I'm further convinced that beans are completely underrated. Not only do they taste really great, but they are also incredible nutrition-wise for people trying to cut down/replace animal protein. They're packed with nutrients and good carbs, and keep you full for long. So dig in, and bon appétit!
Rinse and slice the mushrooms and roughly mince the onion.
Heat some olive oil in a pan and add the mushrooms and onions with some salt. Let it all sweat for a couple minutes, until lightly brown. Then, add a splash of water and let it evaporate to soften it all.
Add a bit more oil and the giant butter beans in a single layer. Let them fry until golden for 4-5 minutes. Then flip them and let the other side brown.
Finally, add the lemon juice and spinach. Let the greens wilt quickly.
Serve in a deep plate and garnish with some freshly grated cheese and a drizzle of spicy oil. Enjoy!
Rincez et tranchez les champignons. Emincez l'oignon.
Faites chauffer de l'huile dans une poèle et ajoutez les champignons et l'oignon avec une bonne pincée de sel. Laissez le tout suer un moment jusqu'à ce que les légumes dorent. Puis, ajoutez un filet d'eau et laissez-le s'évaporer.
Ajoutez un peu d'huile, et disposez les haricots en une seule couche dans la poèle. Faites-les dorer pendant 4-5 minutes, puis tournez les pour dorer l'autre côté.
Ajoutez enfin le jus de citron et les épinards. Mélangez délicatement juste pour ramollir les feuilles.
Servez le tout dans une assiette creuse, et garnissez de parmesan fraichement rapé et d'un filet d'huile pimentée. Bon appétit!
Posted on February 15, 2016 by julieadPosted in Dinner, Fridge Friday, Lunch, Main, RecipesTagged butter beans, crispy, dinner, golden, lemon, lima, lunch, mushrooms, pan fried, spinach, vegetarian.
Yum yum yum, this looks delicious!!


CMs or Content management systems is becoming an essential part for all businesses. They help in designing and managing the websites. Also, they prove to be of great help making it more attractive.
Managing the content is significant in the present world. This will basically decide how well engaged you are able to keep your customers. However, selecting the best WordPress Development Company can prove to be a tedious task.
Read the article to know more about some points that can help in deciding the right kind of content management system.
It is very important to identify the business needs before you start evaluating diverse CMS platforms. There is no dearth of CMS platforms out there. But you need to be sure of the features that you require.
You need to be sure if your website will be inter-connected sites, simple brochure site, or multiple sites or the need of third-party software integration.
For instance, WordPress will work the best in your case if 'easy to use' is your precedence.
It's important to add new content to your website to grab the attention of the visitors to your page. Thus, scalability plays an integral role.
In such cases, platforms like Drupal, Magento or Sitecore will be the best for you.
You need to identify the core functionality of the CMS platform. These are characteristically multi-functionality, but each one is associated with a set of functionalities.
For example, WordPress, is the perfect platform for all those who are interested in blogging. And for e-commerce there is nothing better than Magento.
You need to be serious about security aspects of your CMS platform as hacking and malicious attacks are pretty common these days. So with every update security cover for CMS should also be enhanced.
This is something that cannot be taken lightly at all. You need to be sure of the budget before you choose a CMS platform.
Kentico is an affordable option, especially for all those who have recently set up their business.
It is very important for your website is to be responsive in the modern era of smartphones and smart gadgets. It means that the same websites needws to be accessible across several devices.
WordPress offers one of the best content management system that efficiently supports mobile responsive website.
The world of web development is highly dynamic. It means that you need to constantly keep working on the designs and content. It is important that making the changes is manageable and easy. Also, aspects like accessibility and usability cannot be avoided. Thus, you need for look for platforms that have extensions.
User interaction is something that cannot be avoided while selecting the CMS platform for your business. You need to ensure that the selected CMS platform supports plugins like social media, chat tools, and so on. All this will make the site more interactive.
You can select open source model as it can be easily customized and as per your requirement. Also, you can go for proprietary CMS platforms. It means that the company that owns the platform can modify it based on your needs and will be charging a licensing fee.
The support system for the chosen CMS platform will be of great importance, especially when you face a problem. In case of open source CMS platforms you will be receiving more support as there is greater community interaction. And SaaS platform like Wix or Squarespace will be offering their own support.
Always carry out thorough research in selecting the right kind of professionals offering Durpal Development Services. The right content management system plays an integral role in making your presence felt on the internet.


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Lawyers Blog
Four Medical Problems That Are More Common in Summer
March 12, 2018 AdminGeneral
Summers are filled with picnics, barbecues, beach trips and other fun activities, but they can also be a time of increased risks for specific types of disease. While it may seem like most illnesses occur during the cold months of winter, summer brings its own health issues, including these four common problems:
Summer staples like campfires and smoke from barbecue grills, significant changes in the weather including increases in humidity – even chlorine – can all increase the risk of asthma problems and allergic reactions, according to the American College of Allergy, Asthma and Immunology.
Swimmer's ear
Whether you swim in a pool, the ocean or a lake, the ear can trap water, and that can lead to infections. Swimmer's ear is responsible for about 2.4 million trips to the doctor each year. Drying your ears thoroughly is the best way to prevent swimmer's ear from occurring.
The warm summer weather provides ideal conditions for bacterial growth, and that means the risk for food poisoning increases dramatically. If you're planning a barbecue or picnic, use these tips from the USDA to avoid food-borne illnesses.
Carried by tiny deer ticks hardly larger than the head of a pin, the CDC says Lyme disease affects tens of thousands of people each year. The agency provides tips on how to prevent tick bites and how to remove ticks once they've latched on.
Enjoying lazy summer days doesn't mean being trapped indoors. Being aware of the risks of illness and disease that are most likely to occur in the summer is the best way to stay healthy and enjoy fun in the sun.
Six Surprising Facts about Heat Stroke
Understanding the Difference Between Absolute Risk and Relative Risk
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Q: Intercepting and modifying the JavaScript code from PhoneGap Android apps Context
I'm currently trying to design a model generator for hybrid Android apps. The goal is as follows: given any hybrid Android app developed using PhoneGap, generate a UI model that describes the UI states (in this case, I'm treating the UI state as equivalent to the DOM state) and the transitions to these UI states (denoted by actions - e.g., click on DOM element X). The model is represented by a finite state machine, where the nodes are the UI states and the edges are the transitions.
Problem
My current task is to come up with a way to figure out whether a DOM element has an event handler registered to it (let's assume for now that we're only interested in the initial DOM state). With the help of this StackOverflow answer, I was able to come up with a solution that uses webView.loadURL("javascript:" + ....) to determine if an element has an event registered to it either by using, for example, element.onclick, or by using methods provided by libraries like jQuery and Prototype. However, I am currently unable to determine if an element has an event registered to it via addEventListener(), for reasons specified in that same StackOverflow answer. (Again, for simplicity, let's assume we're only interested in events registered right after the page loads, prior to any user interactions).
Questions

*

*The approach I'm planning to take is as follows: I plan to intercept the JavaScript code from the PhoneGap app. Once intercepted, I will instrument the code (e.g., using Rhino) such that after each call to addEventListener(), I will place a "marker" for the DOM element involved in that call. I will then pass this instrumented code to the WebView so that it is this instrumented JavaScript code that gets loaded instead of the original JavaScript code. By doing so, I can determine which elements addEventListener() was called on. This seems pretty straightforward, but the problem is, I can't figure out a way to intercept the JavaScript code for instrumentation, and to pass the instrumented code so that it gets loaded in lieu of the original. Are there any tools that would allow me to do this intercepting and passing, as described? By the way, I'm using the Android emulator to run the PhoneGap app.

*Are there any other approaches that are perhaps simpler (or more elegant) and I should consider?

A: The solution I came up with is as follows. I created a new CordovaWebViewClient (passing the same activity and webView object to the CordovaWebViewClient constructor) in which the onPageStarted() method is overriden. The onPageStarted() code will execute once an HTML page in the hybrid app has begun loading. The overriding code does the following:

*

*Retrieve the URL of the page that just started loading, relative to the assets folder (file:///android_asset/) where all HTML/JS/CSS files are assumed to be located. The URL is one of onPageStarted()'s parameters, so you can retrieve it by simply accessing the value of this parameter. Example: If the HTML file is located in assets/www/foo.html, the relative URL is www/foo.html

*Retrieve the HTML code by setting up an input stream via activity.getAssets().open(relativeUrl), where activity is the current DroidGap activity and relativeUrl is the relative URL found in the previous step.

*Parse the HTML code into a Document object (I used Jsoup to do this).

*Prepare the JS code you want to add as instrumentation (e.g., by storing the new code in a String object) and insert that new JS code as part of a new script tag in the Document object. (In my case, I inserted the new script tag at the beginning of the HTML's head element)

*Re-convert the modified Document object into a String (say we call this string newHTML), and call the loadDataWithBaseURL() method as follows: webView.loadDataWithBaseURL("file:///android_asset/www/", newHTML, "text/html", "UTF-8", null). This essentially reloads the page, albeit with the instrumented code included.

I then set this extended CordovaWebViewClient as the webView object's new webView client (using the webView.setWebViewClient() method). Finally, I called webView.reload() so that the web view client change above takes into effect. As a result, each time a new HTML page loads in the web view, the onPageStarted code I wrote would execute.
Note that since item #5 above uses "file:///android_asset/www/ as the base URL and the HTML is loaded by string, you should also include a check at the beginning of your overriding onPageStarted() method to make sure that the URL of the page that just started loading is not equal to the base URL (i.e., check that the URL is not exactly equal to file:///android_asset/www/). Otherwise, you'll encounter an infinite loop. (I also directed the onPageStarted not to execute whenever the url does not begin with file:///android_asset, which is the expected base folder).

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