text:
Bernadette Marie
A Tropical Christmas
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Series & Trilogies
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Vist my AllAuthor.com Page
Sweet Home Alabama ~ Romantic Comedy Film Week
I can say that Sweet Home Alabama has probably influenced my writing more than I thought. Just looking at the tag line...yep...I wrote one of those books. Go back and find the man you loved right where you left him. It's a common love story theme. But what I loved about this story is you loved both the men and you wanted the best for both of them.
Melanie (Reese Witherspoon) is about to marry the son of New York City's mayor, Andrew (Patrick Dempsy.) But wouldn't you know it, the secret she's been hiding all these years is about to come full circle and bite her in the butt! She's a small town Alabama girl, who even changed her name when she became some big name designer in the city. She leaves behind a small town reputation, parents in a double-wide, and wouldn't you know it...a high-school sweetheart/ex-husband (or so she thought.) When it comes right down to it, she never did get that divorce.
The journey of this movie is one we all relate to in one way or another. The whom-you've-become vs. whom-you-once-were. In Melanie's case she was a little untamed, a little bit of a bully, and a whole lot in love with Jake (Josh Lucas.)
When she returns to Alabama to finalize the divorce she has a lot of demons to face and the hardest one is the loving Jake. On many occasions, as an author, I have drawn from Jake's calm demeanor when creating caring men that readers want to fall in love with. His ego is in check. His mouth is too. And he loves the heroine even as she tries her hardest to bury him in her deceit.
I suppose this story could have gone both ways. We would have been okay had she left Jake and continued on and married Andrew. He was in a good place and had lots of friends to catch him if he fell. Andrew, also a sweet man who adored Melanie, would have been a fine catch if she continued to pursue her New York life. The true story was about Melanie finding her true self, because there were times we wanted to shake it out of her. But that only makes it all that more appealing to me as a writer. The heroine people aren't in love with the whole time. It doesn't always make for good reviews, but I think women relate to that.
This movie has some great one liners that you can use everyday. But all in all, it's just a real good, feel good movie.
#WiseWords
Bernadette Marie is an Internationally Bestselling author of Contemporary Romance as well as a mother of 5, and owner of 5 Prince Publishing and Illumination Author Events. Read her full bio here.
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text:
Pradelles-en-Val (okzitanisch Pradèlas en Val) ist eine Ortschaft und eine ehemalige französische Gemeinde mit  Einwohnern (Stand: ) im Département Aude in der Region Okzitanien. Sie gehört zum Arrondissement Carcassonne und zum Kanton La Montagne d'Alaric.

Mit Wirkung vom 1. Januar 2019 wurden die ehemaligen Gemeinden Montlaur und Pradelles-en-Val zur Commune nouvelle Val-de-Dagne zusammengeschlossen und haben in der neuen Gemeinde der Status einer Commune déléguée. Der Verwaltungssitz befindet sich im Ort Montlaur.

Lage
Nachbarorte von Pradelles-en-Val sind Comigne im Nordosten, Montlaur im Südosten, Arquettes-en-Val im Südwesten und Barbaira im Nordwesten.

Bevölkerungsentwicklung

Weblinks

Einzelnachweise

Ort in Okzitanien
Weinbauort in Frankreich
Val-de-Dagne
Commune déléguée im Département Aude
Gemeindeauflösung 2019

redpajama_set_name: RedPajamaWikipedia


text:
Title: Qantara
Subject: Six-Day War, Yom Kippur War, Presidency of Religious Affairs, Raid on the Suez Canal, Ahmet Davutoğlu, Southern Lebanon, Timeline of the 2006 Lebanon War (mid August)
Al Qantarah El Sharqiyya
Location in Egypt
Coordinates: 30°51′N 32°19′E / 30.85°N 32.31°E / 30.85; 32.31
Governorate
EST (UTC+2)
Al Qantarah El Sharqiyya (30.85° N 32.31° E) is a northeastern Egyptian city on the eastern side of the Suez Canal located in the Egyptian governorate of Ismailia. 160 kilometers northeast of Cairo and 50 kilometers south of Port Said.
Alternate Names: Mahattat al qantarah ash sharqiyah, El Qantara, El Qantara East, El-Qantara East Station, El-Qantara El-Sharqiya Station, Mahattat al Qantarah al Sharqiyah, Qantarah esh Sharqiya, Al Qantarah Ash Sharqiyah, El Kantara, Kantara, or Al Qantarah.
In Al Qantarah there is a high-level fixed road bridge, the Mubarak Peace Bridge over the canal. The Arabic al qantara means "the bridge".
During World War I, Kantara, as it was referred to by the Allied troops, was the site of Headquarters No. 3 Section, Canal Defences and Headquarters Eastern Force during the latter stages of the Defence of the Suez Canal Campaign and the Sinai Campaign of 1916. It became the main supply depot for all British, Australian and New Zealand operations in the Sinai from 1916 until final demobilization in 1919. A massive distribution warehouse and hospital centre was located in the town that supplied and supported the numerous units in the area.
Beginning in January 1916 a new railway was constructed from the town to Romani and eastwards through the Sinai to El Arish and Rafa on the border with the Ottoman Empire.
Outside of town there is located a Commonwealth War Graves Commission Cemetery and Memorial. The cemetery was begun in February 1916 and was in use until late 1920. After the war, the cemetery was doubled in size to accommodate graves brought from other cemeteries and desert battlefields, notably those from Qatia, Rumani, Magdhaba, El Arish and Rafa. The cemetery contains 1,562 Commonwealth burials of the First World War and 110 from the Second World War. There are also 341 war graves of other nationalities in the cemetery. The Kantara Memorial bears the names of 16 New Zealand World War I servicemen who died in action at Rafa and Rumani and have no known grave. In 1961, 283 World War I Indian serviceman who were interned in the now inaccessible Kantara Indian Cemetery were commemorated with panels bearing the names of the dead affixed to the wall behind the Stone of Remembrance to form the Kantara Indian Cemetery Memorial.
The town's importance as a hospital centre was renewed during World War II when General Hospital No. 1 was located there from July 1941 to December 1945 and General Hospitals Nos. 41 and 92 were located there for differing periods. No. 8 Polish General Hospital was constructed adjoining the war cemetery.
During the 1967 Six Day War Israel captured the town. Egypt recaptured the town at the start of the 1973 Yom Kippur War during The Crossing and held the town until the ceasefire was negotiated. Egypt regained formal control over the town in 1974.
Six-Day War
Israel, West Bank, Egypt, Syria, Gaza Strip
Yom Kippur War
Israel, Egypt, Syria, Damascus, Israeli Air Force
Presidency of Religious Affairs
Quran, Turkey, Germany, Istanbul, Turkish language

redpajama_set_name: RedPajamaCommonCrawl


text:
Festival slipknot 2015 portland
By Zolojar 08.06.2020 2
Slipknot This is a past event. Thursday, October 22, at pm Memorial Coliseum One Center Court, Portland, OR One Center Court, Portland, OR Oct 24, · Get the Slipknot Setlist of the concert at Gibson Ranch, Elverta, CA, USA on October 24, from the Road to Knotfest Tour and other Slipknot Setlists for free on longlovetabs.biz! Slipknot Concert Setlist at Aftershock on October 24, | longlovetabs.biz Oct 22, · Get the Slipknot Setlist of the concert at Portland Memorial Coliseum, Portland, OR, USA on October 22, from the Road to Knotfest Tour and other Slipknot Setlists for free on longlovetabs.biz!
[Oct 22, · Get the Slipknot Setlist of the concert at Portland Memorial Coliseum, Portland, OR, USA on October 22, from the Road to Knotfest Tour and other Slipknot Setlists for free on longlovetabs.biz! Slipknot Tour - 22/10/ - Portland - Oregon - United States - Event Information - LINEUP - Slipknot, Beartooth, Suicidal Tendencies. Oct 24, · Get the Slipknot Setlist of the concert at Gibson Ranch, Elverta, CA, USA on October 24, from the Road to Knotfest Tour and other Slipknot Setlists for free on longlovetabs.biz! Slipknot Concert Setlist at Aftershock on October 24, | longlovetabs.biz Slipknot began touring North America in support of the album on October 25 at the second iteration of Knotfest. The tour dubbed the "Prepare for Hell" was co-headlined by Korn with King as support. 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Slipknot Book Fall Dates With Suicidal Tendencies + Beartooth Leading Up to Knotfest Just prior to Knotfest, Slipknot will also take part in the Aftershock Festival in Sacramento, Calif. Slipknot 10/22 -- Portland, Ore. and very first for Nuclear Blast worldwide, 's The Concrete Confessional. support to Slipknot on a Spring run in between festival appearances at. North America Fall Tour was a North American concert tour in headlined by Slipknot in October 22, , Portland · Portland Memorial Coliseum October 24, , Elverta, United States, Aftershock Festival. With: Bring Me the. The Hell Not Hallelujah Tour is the fourteenth concert tour by American rock band Marilyn Manson. It launched in support of their ninth studio album, The Pale Emperor, which was released on January 20, in the United States. Beginning on January 21, , the tour includes eleven legs spanning " Download festival review – Kiss, Muse and Slipknot rock out in the. Buy tickets for an upcoming Slipknot concert near you. Slipknot Nova Rock Festival .. Saturday 05 November – Sunday 06 November ] Festival slipknot 2015 portland Get the Slipknot Setlist of the concert at Portland Memorial Coliseum, Portland, OR, USA on October 22, from the Road to Knotfest Tour and other Slipknot Setlists for free on longlovetabs.biz!. Slipknot Tour - 22/10/ - Portland - Oregon - United States - Event Information - LINEUP - Slipknot, Beartooth, Suicidal Tendencies. Get the Slipknot Setlist of the concert at Gibson Ranch, Elverta, CA, USA on October 24, from the Road to Knotfest Tour and other Slipknot Setlists for free on longlovetabs.biz!. longlovetabs.biz concert page for Slipknot at Memorial Coliseum (Portland) on Oct. 22, Discuss the gig, get concert tickets, see who's attending, find similar events. Slipknot This is a past event. Thursday, October 22, at pm Memorial Coliseum One Center Court, Portland, OR One Center Court, Portland, OR. Slipknot Tour - 26/08/ - Concord - New Hampshire - United States - Event Information - LINEUP - Bullet For My Valentine, Lamb Of God, Motionless In White, Slipknot. SLIPKNOT Live – Portland, OR Posted on October 26, by Matt Walsh If there's a Happy Hour in Hell, it probably looks a lot like a Slipknot concert — or at least the one the nonet put on Thursday night, October 22nd, at the Veteran's Memorial Coliseum in Portland, Oregon. Slipknot began touring North America in support of the album on October 25 at the second iteration of Knotfest. The tour dubbed the "Prepare for Hell" was co-headlined by Korn with King as support. The band also performed at 's Soundwave festival in Australia. This blog is a great collection of high quality bootlegs, live & rare performances. I decided to put this blog to share all of the bootlegs I've collected over the years. Genre: tickets , concerts, concert ticket, tour dates, concert dates, tickets, cheap tickets. Anyone know who is opening for the fall leg of the tour? I know they're with Lamb of God right now, and I've heard possibly Suicidal Tendencies. privacy policy | © longlovetabs.biz | © longlovetabs.biz Slipknot - Tour Dates for their current Tour! Includes Slipknot's current concert schedule and past tour dates for your convenience!. March 30, Slipknot Announce Spring Tour Dates. Slipknot has announced tour dates for Joining them on the road will be drummer Jay Weinberg, who has been helping to fill in on the instrument since Joey Jordison departed the band back in Slipknot - Live Download Festival [FULL HD ] ROCK PARTY. Loading Unsubscribe from ROCK PARTY? Cancel Unsubscribe. Working Subscribe Subscribed Unsubscribe 22K. Unlimited recording storage space. Live TV from 60+ channels. No cable box required. Cancel anytime. Music Festivals Music Festivals in with lineups, tickets, dates & video. Your guide to music festivals in for indie rock, alternative & electronic music for music festivals in Fall / Winter / Spring and Summer.
Slipknot -ME INSIDE- live in Portland Oregon 2015
2006 hl accounting marking scheme, cascada 2012 wrzuta er, wahrheit tanz der vampire karaoke s, modeselektor thom yorke this is not authorized, pp no 53 tahun 2012 tentang jamsostek
Tebei
Malanris 08.06.2020 23:49
nice upload great


text:
You are here: Home / News / New Journal Article: "Manuscript Study in Digital Spaces: The State of the Field and New Ways Forward"
New Journal Article: "Manuscript Study in Digital Spaces: The State of the Field and New Ways Forward"
The following article appears in issue 12.2 of Digital Humanities Quarterly (DHQ).
Manuscript Study in Digital Spaces: The State of the Field and New Ways Forward
Bridget Almas
The Alpheios Project, Ltd.
Emad Khazraee
School of Information, Kent State University
Matthew Thomas Miller
Roshan Institute for Persian Studies, University of Maryland College Park
Joshua Westgar
University Libraries, University of Maryland College Park
Digital Humanities Quarterly (DHQ)
In the last decade tremendous advances have been made in the tools and platforms available for the digital study of manuscripts. Much work, however, remains to be done in order to address the wide range of pedagogical, cataloging, preservation, scholarly (individual and collaborative), and citizen science (crowdsourcing) workflows and use cases in a user-friendly manner. This study (1) summarizes the feedback of dozens of technologists, manuscript experts, and curators obtained through survey data and workshop focus groups; (2) provides a "state of the field" report which assesses the current tools available and their limitations; and, (3) outlines principles to help guide future development. The authors in particular emphasize the importance of producing tool-independent data, fostering intellectual "trading zones" between technologists, scholars, librarians, and curators, utilizing a code base with an active community of users, and re-conceptualizing tool-creation as a collaborative form of humanistic intellectual labor.
Direct to Full Text Article
http://www.digitalhumanities.org/dhq/vol/12/2/000374/000374.html


text:
\section{Introduction}
Neutral beam injection (NBI) is widely adopted in tokamaks for heating plasma
and driving flow{\cite{Scoville2019,Hu2015,Schneider_2011,ASUNTA201533,Heidbrink_2009}}.
Modeling the neutral beam heating, which involves neutral particle ionization
and fast ion collisional transport, is a mature field where simulation results
usually agree reasonably with experiments{\cite{pankin2004}}. One of the
uncertainties in the modeling is how electromagnetic perturbations, if
present, affect the heating and fast ion transport process. These
electromagnetic perturbations can be various intrinsic modes such as
Alfv{\'e}n eigenmodes, and can also be externally imposed perturbations such
as resonant magnetic perturbations (RMPs).

This work numerically studies the influence of RMPs on the Deuterium neutral
beam heating in the EAST tokamak{\cite{Wan_2017,Wan_2019}}. EAST is equipped
with RMP coils which are designed for the control of edge localized modes
(ELMs){\cite{Sun_2016,sun2016prl}}. This coils turn out to also have effects
on the transport of neutral beam fast
ions{\cite{Xu_2020,yxu2019,He_2019,he2020a,he2020b}}. The effects of RMPs on
fast ion transport and loss have been extensively investigated on AUG
{\cite{Garcia_Munoz_2013,Garcia_Munoz_2013b,Sanchis_2018}},
KSTAR{\cite{kim2018}}, DIII-D{\cite{Van_Zeeland_2013,Van_Zeeland_2015}}, and
MAST{\cite{McClements_2015}} tokamaks.

In this work, we consider RMPs of $n = 1$ with linear resistive
magnetohydrodynamics (MHD) plasma response, where $n$ is the toroidal mode
number of the RMP coil current. The configurations with $n = 0, 2, 3, 4$ were
also examined (not shown in this paper). The results indicate that $n = 0$ RMP
has negligible effects on the confinement of fast ions, as is expected, and
the deleterious effects of configurations with $n = 2, 3, 4$ on the
confinement of fast ions are generally smaller than that of the $n = 1$ RMP.
Therefore we will focus on the $n = 1$ configuration in this paper.

We consider one of the four neutral beams on EAST that is injected in the
co-current direction, with the tangent radius being $1.26 m$ and the full
(kinetic) energy being $51 \tmop{keV}$. The number ratio between neutrals of
the full energy, half energy and $1 / 3$ energy is chosen to be $80 : 14 : 6$.
NBI power after neutralizing is assumed to be 1MW. Further details on the
neutral beam modeling are provided in Appendix \ref{21-4-14-p1} and
\ref{21-4-14-p2}. In this paper, fast ions are defined as those ions that are
born from the neutral beam ionization and have not yet been slowed down to the
energy $2 T_{i 0}$, where $T_{i 0}$ is the temperature of background thermal
ions at the magnetic axis.

We found that the internal redistribution of fast ions by RMPs can induce
local accumulation of fast ions, resulting in larger local fast ion pressure
than the case without RMPs. It is also found that the toroidal phasing of the
RMP with respect to the fast ion source has slight effects on the steady-state
radial profile of fast ions. The dependence of fast ion loss fraction on the
RMP up-down phase difference $\Delta \Phi$ is found to show similar behavior
as the dependence of the radial width of chaotic magnetic field on $\Delta
\Phi$.

A simple statistical method for identifying resonances between RMPs and lost
fast ions is proposed, in which resonances are identified by examining peaks
in the graph of $p$ versus $\Delta f$, where $p = n \omega_{\phi} /
\omega_{\theta}$ is called resonance order with $\omega_{\phi}$ and
$\omega_{\theta}$ being the toroidal angular frequency and poloidal angular
frequency of lost fast ions, respectively, and $\Delta f$ is the difference of
the lost fast ion distribution function between the case with RMP and that
without RMP. By taking the difference, we exclude all the fast ions that are
lost due to the first-orbit prompt loss and pure collision loss. The results
indicate that some resonances may be of non-integer fractional order, rather
than the usual integer order.

In the process of studying the effects of RMP on NBI heating, we developed a
new Monte-Carlo code which models continuous neutral beam injection,
ionization, and the resulting fast ions transport under the influence of RMPs.
This code (referred to as {\codestar{TGCO}}) is similar to the established NBI
modeling code {\codestar{NUBEAM}}{\cite{pankin2004}} and many other test
particle orbit-following codes such as {\codestar{OFMC}}{\cite{Tani1981}},
{\codestar{ASCOT}}{\cite{HIRVIJOKI2014}},
{\codestar{ORBIT}}{\cite{White_2010}},
{\codestar{SPIRAL}}{\cite{Kramer_2013}},
{\codestar{VENUS-LEVIS}}{\cite{PFEFFERLE20143127}},
{\codestar{GYCAVA}}{\cite{yxu2019}}, {\codestar{SOFT}}{\cite{he2020b}}.
{\codestar{TGCO}} has been used as a NBI module in Ref.
{\cite{Xu_2020,he2020a,xyXU_2020}}. The guiding-center drift model, edge loss
model, and fast ion collision model adopted in this work are well known, and
the details of these models are provided in the Appendix. The finite Larmor
radius (FLR) effect is taken into account when pushing particle guiding center
drift, depositing markers to compute density and pressure, and checking
whether particles are lost to the boundary. The simulation includes the
X-points of equilibrium magnetic field and uses the first wall as the particle
loss boundary. For simplicity, we assume a pure Deuterium plasma with no
impurities.

The remainder of this paper is organized as follows. Section \ref{19-12-26-5}
describes the equilibrium configuration, bulk plasma profiles, and neutral
beam ionization profiles. Section \ref{21-5-30-a1} introduces the RMP coils on
EAST and the resulting 3D magnetic perturbations with/without plasma response.
Section \ref{21-6-2a1} discusses effects of RMPs on the steady state radial
profiles of neutral beam heating and fast ion pressure. Section \ref{21-6-2a4}
examines the dependence of volume integrated heating power, fast ion stored
energy, and fast ion loss fraction on the up-down phase difference of RMP coil
currents, where radial width of chaotic magnetic region is computed and is
found to be closely related to the fast ion loss fraction. Section
\ref{21-6-2a5} use a statistical method to identify the resonance between RMPs
and fast ions. A brief summary and some discussions are given in Sec.
\ref{19-12-26-8}.

\section{Equilibrium and fast ion source}\label{19-12-26-5}

EAST is a superconducting tokamak with a major radius $R_0 = 1.85 m$, minor
radius $a \approx 0.45 m$, typical on-axis magnetic field strength
$B_{\tmop{axis}} \approx 2.2 T$ and plasma current $I_p \approx 0.5
\tmop{MA}${\cite{Wan_2017,Wan_2019}}. The magnetic configuration and plasma
profiles used in this work (Fig. \ref{17-2-22-p1m}) were reconstructed by EFIT
code from EAST tokamak discharge \#52340@3.4s with constrains from experiment
diagnostics.

\begin{figure}[htp]
  \includegraphics[scale=0.5]{./1.eps}
  \caption{\label{17-2-22-p1m}Left panel: profiles of electron number density
  $n_e$ , electron temperature $T_e$, ion temperature $T_i$, and safety factor
  $q$ of EAST discharge \#52340@3.4s. The radial coordinate $\rho =
  \sqrt{\overline{\Psi}_p}$ is the square root of the normalized poloidal
  magnetic flux, with $\overline{\Psi}_p = (\Psi - \Psi_0) / (\Psi_b -
  \Psi_0)$, where $\Psi \equiv A_{\phi} R$ is the poloidal flux function,
  $\Psi_0$ and $\Psi_b$ are the values of $\Psi$ at the magnetic axis and
  last-closed-flux-surface, respectively. Right panel: magnetic configuration.
  This is a low single null configuration with $B_{\tmop{axis}} = 2.2 T$, $I_p
  = 404 \tmop{kA}$, $q_{\tmop{axis}} = 0.95$, and $q_{95} = 5.05$.}
\end{figure}

The neutral beam ionization is modeled by the Monte-Carlo method and the
details are provided in Appendix \ref{21-5-30-a3}. Figure \ref{17-4-13-p1}
plots the two-dimensional distribution of ionized particles in the poloidal
plane (averaged over the toroidal direction) and in the toroidal plane
(averaged over the vertical direction). The results indicate most fast ions
are born on the low-field-side.

\begin{figure}[htp]
  \includegraphics[scale=0.75]{./2a.eps}\includegraphics[scale=0.7]{./2b.eps}
  \caption{\label{17-4-13-p1}Neutral beam ionization profiles in the poloidal
  plane (left) and toroidal plane (right) computed by {\codestar{TGCO}}. This
  is for the neutral beam injection with $R_{\tan} = 1.26 m$ in EAST discharge
  \#52340@3.4s. The loss fraction of neutral particles to the inner first wall
  (shine-through loss) is 14\% in this case.}
\end{figure}

Figure \ref{20-9-14-e1} plots the distribution of ionized particles in
$(\Lambda, P_{\phi})$ plane and $(\lambda, R)$ plane, where $\Lambda = \mu
B_{\tmop{axis}} / \varepsilon$, $\lambda = v_{\parallel} / v$, $\varepsilon$
is ion kinetic energy, $P_{\phi}$ is the canonical toroidal angular momentum.
The trapped/passing boundary in $(\Lambda, P_{\phi})$ plane is plotted, which
indicates that most ions born in this case are in the passing region, with a
small number of ions being near the trapped/passing boundary.

\begin{figure}[htp]
  \includegraphics[scale=0.6]{3.eps}
  \caption{\label{20-9-14-e1}Distribution of ionized particles in $(\Lambda,
  P_{\phi})$ plane (left) and $(\lambda, R)$ plane (right), where $\Lambda =
  \mu B_{\tmop{axis}} / \varepsilon$, $\lambda = v_{\parallel} / v$, $P_{\phi}
  = m_f g v_{\parallel} / B_0 + Z_f e \Psi$ is the canonical toroidal angular
  momentum, $\mu$ is the magnetic moment, $v_{\parallel}$ is the parallel (to
  the magnetic field) velocity, $B_0$ is the equilibrium magnetic field, $m_f$
  and $Z_f e$ are the mass and charge of fast ions, respectively, $g =
  B_{\phi} R$, $B_n = 1 T$, $L_n = 1 m$. The trapped/passing boundary in
  $(\Lambda, P_{\phi})$ plane is indicated (the region to the left side of the
  curve is the trapped region).}
\end{figure}

\section{Three dimensional magnetic perturbations}\label{21-5-30-a1}

EAST has 16 RMP coils consisting of two arrays of 8 coils with up-down
symmetry located on the low field side and uniformly distributed along the
toroidal direction. Figure \ref{19-9-24-1} shows the setup of the RMP coils on
EAST tokamak{\cite{Sun_2016}}.

\begin{figure}[htp]
  \includegraphics[scale=0.6]{4a.eps}\includegraphics[scale=0.6]{4b.eps}
  \caption{\label{19-9-24-1}RMP coils on EAST tokamak in 3D view (left) and
  poloidal view (right). Each coil has 4 turns with maximum current $2.5
  \tmop{kA}$ per turn. The maximum frequency of alternating current (AC)
  operation is $1 \tmop{kHz}$ (usually operating at less than $10 \tmop{Hz}$).
  This paper considers only direct current (DC) operation, i.e. static RMP. In
  the left panel, red color denotes current circulating in the clockwise
  direction and blue denotes current circulating in the anti-clockwise
  direction, viewed from the outside of the torus. The magnitude of currents
  are set to be the same. The setup shown here is called $n = 1$ and
  $\Delta \Phi = 0$ configuration, where $\Delta \Phi$ is the up-down
  phase difference.}
\end{figure}

The vacuum magnetic perturbations produced by the RMP coils are numerically
calculated by using the Biot-Savart law. The magnetic perturbations including
the the effect of plasma response are computed, using the linear resistive MHD
model, by MARS-F code {\cite{liu2000,liu2010}} as a boundary value problem,
taking into account of a given toroidal flow. The RMP coil current, located in
the vacuum region outside the plasma, is directly modeled in the code as a
source term {\cite{liu2010}}.

In this work, we use the $n = 1$ RMP with a current amplitude of $10
\tmop{kAt}$ unless otherwise specified. To perceive the magnitude of the
resulting magnetic perturbation (without plasma response) relative to the
equilibrium field, Figures \ref{21-11-15-p1}(a,d) show the two-dimensional
distribution of $\delta B / B_0$ on the $\rho = 0.96$ magnetic surface. Figs.
\ref{21-11-15-p1}(b,e) show the poloidal dependence of $\delta B / B_0$ at a
series of toroidal locations at $\rho = 0.96$ and Figs. \ref{21-11-15-p1}(c,f)
show the toroidal dependence of $\delta B / B_0$ at a series of poloidal
locations at $\rho = 0.96$. The results indicate that the maximal value of
$\delta B$ at $\rho = 0.96$ is about 0.3\% of the equilibrium field $B_0$. The
corresponding minimal value of $\delta B$ is small (0.03\% of $B_0$) but is
not exact zero.

\begin{figure}[htp]
  \includegraphics[scale=0.55]{5.eps}
  \caption{\label{21-11-15-p1}(a) and (d): Two-dimensional distribution of
  $\delta B / B_0$ on the $\rho = 0.96$ magnetic surface. (b) and (e):
  Poloidal dependence of $\delta B / B_0$ at a series of toroidal locations at
  $\rho = 0.96$. (c) ad (f): Toroidal dependence of $\delta B / B_0$ at a
  series of poloidal locations at $\rho = 0.96$. The upper panels are for the
  full vacuum field and the lower panels are for filtered vacuum field
  (keeping only $n = \pm 1$ Fourier harmonics). $\delta B = | \delta
  \mathbf{B} |$ is the magnetic perturbation magnitude and $B_0$ is the local
  value of the equilibrium magnetic field. $\phi$ is the toroidal angle in the
  $(R, \phi, Z)$ cylindrical coordinates. The poloidal angle $\theta$ is
  chosen to be of the PEST type{\cite{cheng1987}}, i.e., magnetic field lines
  are straight in $(\theta, \phi)$ plane (the positive direction of $\theta$
  is chosen to be counterclockwise when viewed along $\nabla \phi$ direction;
  $\theta \in [- \pi, \pi]$ with $\theta = - \pi$ being in the high field side
  midplane.) The two peaks of $\delta B / B_0$ in the poloidal direction
  appears near the poloidal locations of the RMP coils. The RMP up-down
  phasing $\Delta \Phi = 0$ in this case.}
\end{figure}

The magnetic perturbation component that is perpendicular to the 2D
equilibrium magnetic surface (i.e., the radial component) is of most interest
to magnetic confinement since it creates magnetic islands at resonant surfaces
and thus changes the topology of magnetic field. Define the normalized radial
component of the magnetic perturbation by
\begin{equation}
  \delta B_N = \frac{\delta \mathbf{B} \cdot \nabla \rho}{\mathbf{B}_0 \cdot
  \nabla \phi} .
\end{equation}
Fourier expansion of $\delta B_N$ is written as
\begin{eqnarray}
  \delta B_N (\rho, \theta, \phi) & = & \sum_{n = - \infty}^{\infty} \delta
  B_N^{(n)} (\rho, \theta) \exp [- i n \phi] \\
  & = & \sum_{n = - \infty}^{\infty} \sum_{m = - \infty}^{\infty} \delta
  B_N^{(m n)} (\rho) \exp [i (m \theta - n \phi)],
\end{eqnarray}
where $m$ and $n$ are the poloidal and toroidal mode numbers, respectively,
$\delta B_N^{(n)}$ and $\delta B_N^{(m n)}$ are the Fourier expansion
coefficients.

Figure \ref{20-12-29-p1} compares the amplitude of $n = 1$ harmonic of $\delta
B_N$ in the poloidal plane between the vacuum RMP and the response RMP. The
results indicates that the amplitude of perturbation are enhanced by the
plasma response at some poloidal locations, which might be related to the kink
response{\cite{boozer2001prl}}. The results also show that there is also some
minor perturbation appearing near the top region in the case of response RMP
and there is twist effect on the distribution of $| \delta B_N^{(1)} |$ by the
plasma response.

\begin{figure}[htp]
  \includegraphics[scale=0.7]{6.eps}
  \caption{\label{20-12-29-p1}Amplitude of $n = 1$ harmonic of $\delta B_N$,
  i.e., $| \delta B_N^{(1)} |$, in the poloidal plane. The left panel is for
  the vacuum RMP and the right panel is for the response RMP.}
\end{figure}

Figure \ref{20-12-14-a1} shows the distribution of magnetic perturbation
$\delta B_N$ over $(\phi, \theta)$ on the $\rho = 0.96$ magnetic surface.
Three kinds of perturbations are shown: the full vacuum RMP, the filtered
vacuum RMP (keeping only the $n = \pm 1$ Fourier components) and the filtered
response RMP. One-dimensional distributions along $\phi$ at fixed values of
poloidal angle $\theta$ are also show in Fig. \ref{20-12-14-a1} to compare the
amplitude and phase along the toroidal direction between the three kinds of
magnetic perturbations. The results indicate that the amplitude of
perturbation are enhanced by the plasma response at at some poloidal locations
(Fig \ref{20-12-14-a1}d, f) but are slightly reduced at others (Fig.
\ref{20-12-14-a1}e). The results also indicate that the response RMP has a
toroidal phase shift relative to the vacuum one, which ranges from minor
difference (in Fig. \ref{20-12-14-a1}d) to major difference (anti-phasing in
Fig. \ref{20-12-14-a1}g).

\begin{figure}[htp]
  \includegraphics[scale=0.7]{7.eps}
  \caption{\label{20-12-14-a1}Distribution of magnetic perturbation $\delta
  B_N$ over $(\phi, \theta)$ on the $\rho = 0.96$ magnetic surface. (a)-(c)
  are for the two-dimensional distributions. (d)-(g) are for the
  one-dimensional distributions along $\phi$ at fixed values of poloidal angle
  $\theta$. Specifically, (d) is for $\theta = 0$, (e) is for $\theta = 0.09
  \pi$, (f) is for $\theta = 0.18 \pi$, and (g) is for $\theta = 0.29 \pi$.
  Three kinds of perturbations are shown: magnetic perturbation produced by
  the coils (full vacuum), the filtered vacuum field, and the filtered
  perturbation when the plasma response is considered (filtered response). (a)
  is for the full vacuum field, (b) is for the filtered vacuum field, and (c)
  is for the filtered field with plasma response.}
\end{figure}

To clearly distinguish the resonant components from the non-resonant ones, \
Figure \ref{20-12-28-a1} gives the heatmap of Fourier components of $\delta
B_N$ in the $(m, \rho)$ plane. Figure \ref{20-12-28-a1} compares the poloidal
Fourier spectrum of the $n = 1$ harmonic of $\delta B_N$ between the vacuum
RMP and response RMP. The main difference between vacuum and response RMPs is
that plasma response reduces the perturbation amplitude at resonant locations
(shielding effects) and enhances the amplitude of non-resonant components, as
is shown in Fig. \ref{20-12-28-a1}, where the resonant locations $m = n q$ are
indicated.

\begin{figure}[htp]
  \includegraphics[scale=0.7]{8a.eps}\includegraphics[scale=0.7]{8b.eps}
  \caption{\label{20-12-28-a1}Amplitude of the poloidal Fourier spectrum of
  the $n = 1$ harmonic of $\delta B_N$ for different radial locations, i.e.,
  $| \delta B_N^{(m n)} (\rho) |$ with $n = 1$. The left panel is for the
  vacuum field and the right panel is for the field with plasma response. RMP
  coil configuration of $\Delta \Phi = 0$ is used. The black curves are $m = n
  q$, which indicate the resonant locations.}
\end{figure}

To more clearly show the effects of plasma response, Figure \ref{21-11-4-a1}
compares the radial profiles of amplitude of poloidal harmonics between vacuum
RMP and response RMP. The results indicate that the peaks of the harmonics are
shifted inward to the core by the plasma response and the peak values near the
edge are enhanced. The results also show that plasma response reduces the
magnitude of harmonics near their respective resonant locations (e.g., $m = 2$
at $\rho = 0.76$ and $m = 3$ at $\rho = 0.89$).

\begin{figure}[htp]
  \includegraphics{9a.eps}
  \includegraphics{9b.eps}
  \caption{\label{21-11-4-a1}Radial profile of amplitude of various poloidal
  Fourier harmonics of $n = 1$ RMPs of phasing $\Delta \Phi = 0$ for the
  vacuum case (a) and plasma response case (b). Only $m > 0$ harmonics are
  shown here. The differences of the $m \leqslant 0$ harmonics between the
  vacuum RMP and response RMP are minor (which can be roughly recognized from
  Fig. \ref{20-12-28-a1}) and are thus not shown here.}
\end{figure}

Using $\delta B_N^{(m n)}$ defined above, the width of magnetic island
generated by a magnetic perturbation at a rational surface $q = m / n \equiv
q_s$ is given by{\cite{Sun_2015}}
\begin{equation}
  \label{21-4-28-1} w_{m n} = 4 \sqrt{\left| \frac{\rho \delta B_N^{(m n)}}{n
  S} \right|_{q = q_s}},
\end{equation}
where $S \equiv \rho q' / q$ with $q' = d q / d \rho$ being the magnetic
shear. Formula (\ref{21-4-28-1}) will be used later in this paper to calculate
the Chirikov parameter to determine whether adjacent islands overlap. The
Chirikov parameter is defined by
\begin{equation}
  \sigma = \frac{w_{m_1 n} + w_{m_2 n}}{2 | \rho_2 - \rho_1 |},
\end{equation}
where $\rho_1$ and $\rho_2$ are the radial coordinates of two adjacent
rational surfaces, $w_{m_1 n}$ and $w_{m_2 n}$ are the width of magnetic
islands at the two radial locations. Then the two islands overlap if $\sigma >
1$, which further indicates that magnetic stochasticity appears.

In the remainder of this paper, RMPs refer to the RMPs with plasma response
unless otherwise specified.

\section{Modification of radial profile of ion heating power density by
RMPs}\label{21-6-2a1}

\

With continuous beam injection into a time-independent background plasma, a
steady state of fast ions can be reached on the time scale of slowing-down
time ($\sim 100 \tmop{ms}$ for typical parameters of EAST tokamaks). A steady
state is reached when there is a balance between the source (beam injection
and ionization) and sink (thermalization and edge loss). In this section, we
examine the steady state of the radial profiles of NBI heating power density
and fast ion pressure.

Fig. \ref{21-4-12-p1}a compares the radial profiles of the NBI heating power
density delivered to bulk ions between the case without RMP and those with
RMPs of $\Delta \Phi = 0, \pi$. To clearly show the difference, Fig.
\ref{21-4-12-p1}b plots the power density difference $\Delta H_i$, where
$\Delta H_i \equiv H_i^{(\tmop{rmp})} - H_i^{(\tmop{normp})}$ is the power
density difference between the case with RMP and that without RMP. The results
indicate that the ion heating power density is significantly reduced near the
edge (around the radial location $q = 3$) by the RMPs of $\Delta \Phi = 0$
while very marginal reduction is induced by the the RMP of $\Delta \Phi =
\pi$. The results also show that the heating power density is slightly
increased around $q = 2$ by the RMPs.

\begin{figure}[htp]
  \includegraphics[scale=0.75]{10a.eps}\includegraphics[scale=0.75]{10b.eps}
  \caption{\label{21-4-12-p1}(a) Radial profiles of NBI heating power density
  delivered to bulk ions. (b) Difference of ion heating power density between
  the case with RMP and that without RMP. The locations of $q = 2$ and $q = 3$
  rational surfaces are indicated. The FLR effect is included in the
  simulations.}
\end{figure}

The radial profile of NBI heating power density is determined by the radial
profile of fast ion pressure (see Appendix \ref{21-5-17-a1} for the formula of
computing the power density). Figure \ref{21-5-17-a2}a plots the radial
profile of fast ion pressure for the three cases: without RMP, with RMP of
$\Delta \Phi = 0$, and with RMP of $\Delta \Phi = \pi$. To clearly show the
difference, Fig. \ref{21-5-17-a2}b plots the pressure difference $\Delta P_f$,
where $\Delta P_f \equiv P_f^{(\tmop{rmp})} - P_f^{(\tmop{normp})}$ is the
power density difference between the case with RMP and that without RMP. The
results indicate that the influence of RMPs on fast ion pressure is similar to
that of RMPs on the ion heating power, i.e., the pressure is significantly
reduced near the edge (around the radial location $q = 3$) by the RMPs of
$\Delta \Phi = 0$ while very marginal reduction is induced by the the RMP of
$\Delta \Phi = \pi$ and the pressure is slightly increased around $q = 2$ by
the RMPs.

\begin{figure}[htp]
  \includegraphics[scale=0.75]{11a.eps}\includegraphics[scale=0.72]{11b.eps}
  \caption{\label{21-5-17-a2}(a) Radial profiles of fast ion pressure. (b)
  Difference of fast ion pressure between the case with RMP and that without
  RMP.}
\end{figure}

As is shown in Fig. \ref{21-5-17-a2}, the pressure increasing around $q = 2$
surface induced by RMPs is quite small. It is reasonable to doubt whether the
increasing is physical or due to numerical errors. As a partial verification
of this issue, we perform convergence studies over some numerical parameters
used in the simulations such as the maker numbers and time step sizes. Figure
\ref{21-5-17-a3} shows that the radial profiles of $\Delta P_f$ agree with
each other for two different values of the time step size and marker number.
Also shown in Fig. \ref{21-5-17-a3} is the dependence of values of $\Delta
P_f$ at a specified radial location ($\rho = 0.755$) over the time step size
and marker number, which shows reasonable convergence.

\begin{figure}[htp]
  \includegraphics[scale=0.65]{12a.eps}\includegraphics[scale=0.65]{12b.eps}
  \includegraphics[scale=0.65]{12c.eps}\includegraphics[scale=0.65]{12d.eps}
  \caption{\label{21-5-17-a3}Comparison of radial profiles of fast ion
  pressure perturbation for different values of time step sizes (a) and marker
  number (b). Panel (c) plots the $\Delta P_f$ at $\sqrt{\overline{\Psi}_p} =
  0.755$ as a function of number of markers used in the simulation. Panel (c)
  plots the $\Delta P_f$ as a function of the inverse of the time step size $1
  / (\Delta t / T_n)$, where $T_n = 2 \pi / (B_n Z_f e / m_f)$ with $B_n = 1
  T$. RMP of $\Delta \Phi = 0$ is used in the simulations. In (a) and (d),
  marker number $N = 2 \times 10^5$. In (b) and (c), time step size $\Delta t
  / T_n = 1.0$.}
\end{figure}

It is not surprising to observe the local increasing of fast ion pressure when
a RMP is imposed. RMPs generally have pump out effects on fast ions. However
the pump out effects can be non-uniform along the radial direction, which
implies that some radial locations may accumulate fast ions, resulting higher
fast ion pressure than the no RMP case.

The results in Fig. \ref{21-5-17-a2}b indicate that the radial fluctuation of
fast ion pressure relative to the no RMP case depends on the RMP up-down phase
difference $\Delta \Phi$: radial fluctuation for $\Delta \Phi = 0$
is larger than the case of $\Delta \Phi = \pi$. To understand this, we
compare the resonant and non-resonant components for the two phasings. The
amplitude of resonant components is related to the width of magnetic islands
[Eq. (\ref{21-4-28-1})], which can be inferred from Poincare sections of
magnetic field lines. Figure (\ref{21-4-28-p1}) shows the Poincare plots of
magnetic field line for RMPs of $\Delta \Phi = 0$ and $\Delta \Phi = \pi$. The
results indicate that magnetic islands for RMP of $\Delta \Phi = 0$ are wider
than those of $\Delta \Phi = \pi$. The magnetic island width can also be
directly calculated by using Eq. (\ref{21-4-28-1}). The results are plotted in
Fig. \ref{21-4-28-p2}a, which confirm the conclusion draw from the Poincare
plots.

\begin{figure}[htp]
  \includegraphics[scale=0.8]{13a.eps}\includegraphics[scale=0.8]{13b.eps}
  \caption{\label{21-4-28-p1}Comparison of magnetic field line Poincare plots
  between RMP of $\Delta \Phi = 0$ and that of $\Delta \Phi = \pi$.}
\end{figure}
\begin{figure}[htp]
  \includegraphics[scale=0.9]{14.eps}
  \caption{\label{21-4-28-p2}Magnetic island width (upper panel) and Chirikov
  parameter values (low panel) for RMPs of $\Delta \Phi = 0$ and $\Delta \Phi
  = \pi$. The safety factor profile is also shown to indicate the radial
  locations of rational surfaces. The island width is calculated by using
  formula (\ref{21-4-28-1}).}
\end{figure}

The values of Chirikov parameter $\sigma$ at the rational surfaces $q = 2, 3,
4, 5$ are plotted in Fig. \ref{21-4-28-p2}b, which indicates $\sigma > 1$ at
$q = 5$ for $\Delta \Phi = 0$ RMP while $\sigma$ is still less than one at $q
= 5$ for $\Delta \Phi = \pi$ RMP. This implies that the radial width of
stochastic magnetic field is larger for $\Delta \Phi = 0$ RMP than that of
$\Delta \Phi = \pi$ RMP.

The width of magnetic islands characterizes the amplitude of resonant
components. To characterize the non-resonant components, Fig. \ref{21-5-26-p3}
plots the radial profiles of amplitude of various poloidal Fourier harmonics.
The radial peaks of the harmonics can be used as a measure of magnitude of
non-resonant harmonics. The results clearly show that amplitude of the
non-resonant components (except for $m = 1$) for $\Delta \Phi = 0$ are larger
than those of $\Delta \Phi = \pi$.

\begin{figure}[htp]
  \includegraphics[scale=0.9]{15a.eps}
  \includegraphics[scale=0.9]{15b.eps}
  \caption{\label{21-5-26-p3}Radial profiles of poloidal Fourier harmonics of
  $n = 1$ RMPs of $\Delta \Phi = 0$ (a) and $\Delta \Phi = \pi$ (b).}
\end{figure}

The above results indicate that both resonant components and non-resonant
components of RMP of $\Delta \Phi = 0$ are larger than those of $\Delta \Phi =
\pi$. Both the resonant components and non-resonant components can contribute
to the redistribution of fast ions. Therefore the larger fluctuation of fast
ion pressure for the case of $\Delta \Phi = 0$ is probably due to the larger
resonant and non-resonant components for this coil current configuration.

Plasma response usually helps heal magnetic islands, i.e., reduces the
resonant components, as is shown in Figs. \ref{20-12-28-a1} and \
\ref{21-11-4-a1}, and thus is believed to be beneficial to fast ion
confinement{\cite{he2020b}}. Figure \ref{21-11-8-e1} compares the steady-state
fast ion profiles (subtracted by the profile when no rmp is imposed) between
the vacuum RMP and response RMP. The results shows that the fast ion pressure
around $q = 2$ for the response RMP is higher than that for the vacuum RMP,
which suggests that plasma response is beneficial to fast ion confinement
around the $q = 2$ surface. However, the results also show that the fast ion
pressure within $\sqrt{\overline{\Psi}_p} \approx 0.65$ for the response RMP
case is lower than the vacuum RMP case. This may be due to the enhancement of
$m = 1$ and $m = 2$ harmonics at their non-resonant locations by the plasma
response, as is shown by Fig. \ref{21-11-4-a1}.

\begin{figure}[htp]
  \includegraphics{16.eps}
  \caption{\label{21-11-8-e1}Difference of steady-state fast ion pressure
  between the case with RMP and that without RMP. The blue curve is for the
  RMP with plasma response while the red curve is for the vacuum RMP. Both the
  RMPs are of up-down phasing $\Delta \Phi = 0$.}
\end{figure}

Since fast ion source from NBI is localized in a narrow toroidal span, it is
natural to ask whether the toroidal phasing of RMPs relative to the fast ion
source can have effects on the steady-state radial profile of fast ions. To
answer this question, we compute the steady-state radial profile of fast ion
pressure under various toroidal phasings while fixing the up-down phase
difference $\Delta \Phi$. The results are plotted in Fig. \ref{21-5-17-a3m}
for $\Delta \Phi = \pi / 2$, which indicate that the toroidal phasing has
slight effects on the steady-state radial profile. One interesting observation
is that the profiles around $q = 2$ are almost identical among the cases of
different toroidal phasings.

\begin{figure}[htp]
  \includegraphics[scale=0.65]{17a.eps}\includegraphics[scale=0.65]{17b.eps}
  \caption{\label{21-5-17-a3m}(a) Radial profiles of fast ion pressure under
  RMPs of various toroidal phasings relative to the fast ion source, $\Phi_s$.
  Also shown in (a) is the radial profile when RMPs are absent. (b) The
  difference between the case with RMP and that without RMP for various values
  of $\Phi_s$. The up-down phase difference $\Delta \Phi$ is fixed at $\pi /
  2$. \ The results indicate that the toroidal phasing has slight effect on
  the steady-state radial profile of fast ions.}
\end{figure}

The effect of toroidal phasing on radial profile being slight may be valid
only for passing fast ions resulted from the tangential injection considered
in this paper. In Ref. {\cite{Sanchis_2021}}, the toroidal phasing is found to
have significant effects on the fast ion confinement, where both passing and
trapped particles are significant in the fast ion source.

\section{Up-down phase dependence of volume integrated
quantities}\label{21-6-2a4}

This section investigates the dependence of spatially integrated heating
power, fast ion stored energy, and loss fraction on the RMP up-down phase
difference $\Delta \Phi$. The results are shown in Fig.
\ref{21-5-26-a1}.

\begin{figure}[htp]
  \includegraphics[scale=0.5]{18a.eps}\includegraphics[scale=0.5]{18b.eps}
  \includegraphics[scale=0.5]{18c.eps}\includegraphics[scale=0.5]{18d.eps}
  \caption{\label{21-5-26-a1}The up-down phasing dependence of (a) ion heating
  power, (b) electron heating power, (c) fast ion stored energy, and (d) fast
  ion loss fraction. The corresponding values in the no RMP case are shown for
  comparison. The results for three kinds of magnetic perturbations are shown,
  namely full vacuum magnetic perturbation generated by the coils (without
  filtering), filtered vacuum field (keeping only the $n = \pm 1$ Fourier
  harmonic), and the filter response RMP.}
\end{figure}

The first observation from Fig. \ref{21-5-26-a1} is that the heating power and
fast ion stored energy are reduced relative to the no RMP case and the loss
fraction is increased relative to the no RMP case. Fig. \ref{21-5-26-a1} shows
that the results for full vacuum RMP and the filtered vacuum RMP (keeping only
the $n = \pm 1$ Fourier harmonic) agree with each other well, indicating
harmonics other than $n = \pm 1$ have negligible effects. The results also
indicate that the heating powers and fast ion stored energy are roughly
decreasing functions of the loss fraction in all the three cases, as is
expected.

As is mentioned above, plasma response usually helps heal magnetic islands
and thus is believed to be beneficial to fast ion confinement. Comparing
between the response RMP case and the vacuum RMPs, however, we found the loss
fraction in the response RMP case is not always smaller the corresponding
vacuum case. This may indicate that non-resonant components, which can be
enhanced when plasma response is included, have significant effects on fast
ion confinement.

To more accurately describe the magnetic stochasticity, we use a purely
numerical method to determine the radial width of stochasticity (rather than
using the approximate analytical formula of magnetic island width and the
Chirkikov magnetic island overlap criteria discussed above). Figure
\ref{21-5-5-p1} plots the radial width of stochastic magnetic field as a
function of the RMP coil up-down phase difference $\Delta \Phi$. The radial
width is determined numerically by tracing a series of field lines starting
from the low field side midplane (i.e., $\theta = 0$, $\phi = [0 : 2 \pi]$,
and $\rho_p = [0 : 1]$). If a field line touches the wall during its first
3000 toroidal transits, then the magnetic field is considered as stochastic at
the initial radial location. At each toroidal location, scanning the initial
points from the core to the edge, the radial innermost location where magnetic
field becomes stochastic determines the width of the stochastic region. This
will give different value of radial width at different toroidal locations. The
reasonable radial width of stochasticity should be the toroidal maximal
values. This width is denoted by $w_{s 1}$ in Fig. \ref{21-5-5-p1}. As a
comparison, the toroidal minimal values and toroidal average values of the
width of stochasticity, denoted by $w_{s 2}$ and $w_{s 3}$, respectively are
also shown in Fig. \ref{21-5-5-p1}. The results show that the dependence of
fast ion loss fraction on $\Delta \Phi$ roughly agrees with those of the
radial width of stochasticity on $\Delta \Phi$.

\begin{figure}[htp]
  \includegraphics[scale=0.6]{19.eps}
  \caption{ \label{21-5-5-p1}Radial width of stochastic magnetic field as a
  function of the RMP coil up-down phase difference $\Delta \Phi$. The width
  is defined in terms of the square root of the normalized poloidal magnetic
  flux, $\rho = \sqrt{\overline{\Psi}_p}$ and is defined as the difference of
  $\rho$ between the stochastic radial location and the unperturbed
  last-closed-flux-surface. Three possible radial width, namely $w_{s 1}$,
  $w_{s 2}$, $w_{s 3}$, are plotted. Also plotted is the dependence of the
  loss fraction on the phase difference $\Delta \Phi$.}
\end{figure}

\section{Resonance between RMPs and lost fast ions}\label{21-6-2a5}

Fast ion loss induced by RMP is often related to the resonance between fast
ions and RMPs. Generally, the resonance condition in tokamaks between a wave
and a particle drift is given by
\begin{equation}
  \label{3-8-e4m1} n \omega_{\phi} - \omega = p \omega_{\theta},
\end{equation}
where $n$ and $\omega$ are the toroidal mode number and angular frequency of
the wave, respectively, $\omega_{\phi}$ and $\omega_{\theta}$ are the toroidal
angular frequency and poloidal angular frequency of the particle drift,
respectively, and $p$ can be called resonance order, which is an arbitrary
rational number. When $p$ is an integer, it is the usual resonance condition.
When $p = j / k$ is a non-integer fraction ($j$ and $k$ are integers), the
resonance is called fractional resonance
{\cite{heidbrink2021,chen2019,kramer2012,Todo2018}} , where the (unperturbed)
drift motion reach the same phase of the wave when it finish $k$ times of
poloidal periods. The fractional resonance is often considered to be important
when the wave amplitude is large and thus might be related to the nonlinear
effects. However, the definition of resonance given above is essentially
linear because we are using the unperturbed motion in defining $\omega_{\phi}$
and $\omega_{\theta}$.

For RMPs with $\omega = 0$ and $n = 1$ considered in this work, the resonance
condition in Eq. (\ref{3-8-e4m1}) is simplified as
\begin{equation}
  \label{21-10-25-p1} p = \frac{\omega_{\phi}}{\omega_{\theta}} .
\end{equation}

To show how important the resonant effects are in generating fast ion loss, we
propose to use the graph of $\omega_{\phi} / \omega_{\theta}$ versus $\Delta
f$, where $\Delta f = f_{\tmop{rmp}} - f_{\tmop{normp}}$ is the difference of
the lost fast ion distribution function between the case with RMP and that
without RMP. By taking the difference, we exclude all the fast ions that are
lost due to the first-orbit prompt loss and pure collision loss.

For the tangential NBI considered in this work, the results indicate that lost
particles are dominated by passing particles and we will consider only passing
particles here. The graph of $\omega_{\phi} / \omega_{\theta}$ versus $\Delta
f$ for lost passing ions are plotted in Fig. \ref{21-4-13-a1} for RMPs of
$\Delta \Phi = 0, \pi / 2, \pi, 3 \pi / 2$. The values of $\omega_{\phi} /
\omega_{\theta}$ at peaks of $\Delta f$ are indicated in Fig.
\ref{21-4-13-a1}, which shows that some of them can not be well approximated
by integers.

\begin{figure}[htp]
  \includegraphics[scale=0.8]{20.eps}
  \caption{\label{21-4-13-a1}The difference of distribution of lost passing
  particles relative to the no RMP case for various RMP up-down phasings
  $\Delta \Phi$. The results show that some peaks of $\Delta f$ appear at
  non-integer values of $p$. The small peak at $p = 2$ is probably due to
  resonance of integer order. The peaks at $p = 2 + 3 / 4$ can be roughly
  regarded to be due to resonance of integer order, considering that the peaks
  are of finite width and are close to $p = 3$. The peaks at $p = 3 + 2 / 5$,
  $p = 2 + 2 / 3$ and $p = 4 + 1 / 2$ can not be well approximated as near
  integer values of $p$.}
\end{figure}

\

As is indicated in Fig. \ref{21-4-13-a1}, some peaks of $\Delta f$ seem to
appear at non-integer fractions. It is usually believed that fractional
resonances are associated with nonlinear effects and thus amplitude of the
perturbation matters. In the work of Kramer et al.{\cite{kramer2012}}, the
fractional resonance appears when the amplitude of the wave exceeds a
threshold and thus it is natural to connect the fraction resonance with
nonlinear effects. Here we examine how peaks of $\Delta f$ change with the
changing of amplitude of coil currents. The results are plotted in Fig.
\ref{21-6-1a2}, where the peaks remain at the same non-integer values when the
current amplitude is changed from $10 \tmop{kA}$ (the designed maximal total
current in RMP coils on EAST) to $2 \tmop{kA}$. The fact that these peaks
persist even when the RMP amplitude is very small (2kA) may imply that the
peaks at these non-integer values of $\omega_{\phi} / \omega_{\theta}$ are not
related to nonlinear effects.

\begin{figure}[htp]
  \includegraphics[scale=0.8]{21.eps}
  \caption{\label{21-6-1a2}The same as Fig. \ref{21-4-13-a1} except that the
  RMP up-down phasing is fixed at $\Delta \Phi = 0$ and the amplitude of the
  coil current is scanned.}
\end{figure}

We note that linear resonances can be of non-integer fractional orders (it is
easy to demonstrate this by deriving the resonance condition from
scratch{\cite{Todo2018}}). Since, as mentioned above, it is hard to relate the
peaks at non-integer fraction with nonlinear effects, a plausible
interpretation for these peaks is that they are due to linear resonances of
non-integer fractional orders.

We note that resonance is not a necessary condition for RMP to induce fast ion
loss (resonance is only a beneficial case for perturbation to have large
impact). Any perturbation that breaks the axisymmetry can potentially generate
radial particle transport and hence loss. Therefore, we can not exclude the
possibility that the peaks at non-integer values are caused by non-resonant
effects of RMPs on fast ions. This is one of the limitations of this crude
statistical method in identifying resonance.

Another observation from Fig. \ref{21-6-1a2} is that the peaks are of nonzero
expansion width, so that the consecutive peaks are not well separated, which
makes it difficult to identify all peaks in some cases (e.g., for the case of
10kA RMP, only the peaks near $p = 2, 3$ show up and all the other peaks merge
and are blurred).

Since there are obvious statistic noises in the results of Figs.
\ref{21-4-13-a1} and \ref{21-6-1a2}, we need to make sure that the dominant
peaks identified above are not sensitive to the noise. We perform a numerical
convergence study over the number of markers $N$ used in the simulation (which
is the most important numerical parameter in reducing noise). The results are
plotted in Fig. \ref{21-6-1a3}, which shows that the statistic noise does no
significantly change the peaks in $\Delta f$, i.e., the results are well
converged, in terms of the dominant resonant peaks.

\begin{figure}[htp]
  \includegraphics[scale=0.5]{22a.eps}\includegraphics[scale=0.5]{22b.eps}
  \caption{\label{21-6-1a3}Convergence of $\Delta f$ over number of markers
  $N$ for RMPs of currents $10 \tmop{kAt}$ (left) and $6 \tmop{kAt}$ (right).
  RMPs of $\Delta \Phi = 0$ are used in the simulation.}
\end{figure}

In the above, $\Delta f$ is the difference of the lost fast ion distribution
function between the case with RMP and that without RMP. Collisions are
included in both the cases. By taking the difference, we expect to cancel the
collision effect and obtain the pure RMP effect. However collision may blur
the resonance between RMPs and fast ions if the collision effects are not
exactly canceled out in the simple subtraction. Thus it is desirable to do a
simulation with collisions turned off. The results are plotted in Fig.
\ref{21-11-2-p1} for RMPs of $\Delta \Phi = 0, \pi / 2, \pi, 3 \pi / 2$, which
show similar behavior as that in Fig. \ \ref{21-4-13-a1}. Specifically, there
are peaks at non-integer values of $p$ (e.g., peaks between $p = 3$ and $p =
4$ for the $\Delta \Phi = \pi$ and $\Delta \Phi = 3 \pi / 2$ RMPs). There are
also some peaks which are very near to integer values of $p$ (e.g., the peak
near $p = 3$ for the $\Delta \Phi = \pi / 2$ RMP).

\begin{figure}[htp]
  \includegraphics[scale=0.8]{23.eps}
  \caption{\label{21-11-2-p1}The same as Fig. \ \ref{21-4-13-a1} except that
  collisions are turned off in this case. The peaks of $\Delta f$ roughly
  agree with those in Fig. \ref{21-4-13-a1}. The results also show that the
  amplitude of $\Delta f$ in the collisionless case is much smaller than that
  in the collisional case (Fig. \ \ref{21-4-13-a1}). The unit of $\Delta
  f$ is the same as that of Fig. \ \ref{21-4-13-a1}. }
\end{figure}

\section{Summary and discussion}\label{19-12-26-8}\label{19-9-18-1}

The effects of resonant magnetic perturbation on the steady-state radial
profile of neutral beam heating and fast ion pressure are studied
computationally in a realistic tokamak configuration. It is observed in the
simulations that RMPs can accumulate fast ions at some radial locations,
giving a higher fast ion pressure than the case without RMP. RMPs generally
have pump out effects on fast ions. The pump out effects are non-uniform along
the radial direction, which implies that some radial locations may accumulate
fast ions. Therefore it is not surprising to observe the local increasing of
fast ion pressure when a RMP is imposed.

It is also found that the toroidal phasing of the RMP with respect to the fast
ion source has slight effects on the steady-state radial profile of fast ions.
The effect being slight is expected, considering that most particles resulted
from the tangential injection are passing particles which quickly traverse a
full toroidal loop, making the relative location between neutral beam source
and RMP coils almost irrelevant. For trapped particles resulted from
perpendicular NBI whose toroidal procession frequencies are low, the toroidal
phase of RMP coils relative to the source can be important since the trapped
particles can remain in a limited toroidal range for a sufficient time. The
toroidal phasing can be a useful free parameter for fast ion control using
RMPs, considering that ELMs control is not sensitive to the toroidal phasing.

The dependence of fast ion loss fraction on the RMP up-down phase difference
is found to show similar behavior as the dependence of the radial width of
chaotic edge magnetic field on the up-down phase difference.

A simple numerical statistical method, which uses the lost fast ion
distribution over $\omega_{\phi} / \omega_{\theta}$, is proposed to identify
resonance between lost fast ions and RMPs. Using this method, we found that
the RMP induced loss of passing particles may be partially due to resonance of
fractional orders. However, the reliability and usefulness of this statistic
method in identifying resonance between lost fast ions and RMPs needs to be
further explored. Most authors analyze fast ion transport in terms of the
variation of the toroidal canonical momentum, $\delta P_{\phi}$, which is a
more informative figure of merit than the simple condition of loss or not
(used in this work), in revealing the resonance between fast-ions and magnetic
perturbations{\cite{Sanchis_2018}}.

\section{ACKNOWLEDGMENTS}

One of the authors (Y. Hu) acknowledges useful discussions with Dr. Nong Xiang
and Dr. Wei Chen. Numerical computations were performed on Tianhe at National
SuperComputer Center in Tianjin and the ShenMa computing cluster in Institute
of Plasma Physics, Chinese Academy of Sciences. This work was supported by
National Key R\&D Program of China under Grant No. 2017YFE0300400, by
Comprehensive Research Facility for Fusion Technology Program of China under
Contract No. 2018-000052-73-01-001228, by users with Excellence Program of
Hefei Science Center CAS under Grant No. 2021HSC-UE017, and by the National
Natural Science Foundation of China under Grant No. 11575251.

\subsection{Conflict of interest}

The authors have no conflicts to disclose.

\section{DATA AVAILABILITY}

The data that support the findings of this study are available from the
corresponding author upon reasonable request.

redpajama_set_name: RedPajamaArXiv


Renesas Electronics Corporation which specializes in advanced semiconductor solutions has partnered with Airbiquity to develop a secure, high-performance automotive solution. This solution has over-the-air (OTA) capabilities and is suitable for use as part of advanced driver assistance systems (ADAS), vehicle-to-everything (V2X), and automated driving applications that are likely to be used on a widespread basis in the future.
The two companies are working on integrating Airbiquity's OTAmatic cloud-based OTA software and data management service delivery solution with Renesas' high-performance, low-power R-Car H3 automotive computing platform. The combined solution will be based on the R-Car H3 system-on-chip (SoC). It confirms with ISO 26262 safety functionality (FuSa) standard, and will serve as a powerful, efficient, and secure automotive computing platform with highly targeted and scalable on-demand OTA software update and data management capabilities.
Vehicles are increasingly depending on software, electronic control units (ECUs), sensors, and microprocessors (MCUs) as they come with more connectivity features. The age of autonomous vehicles is not too far off and soon there will be a need to securely manage OTA software updates and data collection for millions of vehicles simultaneously. All these factors have led to greater demand for an automotive-grade solution comprising high-performance telematics processors that is backed by a robust OTA software update and data management solution.
Commenting on the collaboration, John Tuttle, Vice President of Engineering at Airbiquity said that connected vehicles of the future will need a combination of sophisticated on-board processing power and the ability to securely perform software updates remotely. He added that the integration of Renesas SoC technology and Airbiquity OTA service delivery will provide automotive customers with a market-leading option.


text:
Q: Docker-compose connect multiple projects As the title explains i'm trying to connect 2 instances of docker-compose together.
One is the data api, and the other is the actual application.
The solutions i've found are all docker-compose v2 or v1, nothing for version 3.
I've so far tried a normal docker-compose, but cant ping from one to the other.
I've also tried adding networks, but this creates networks like this:
DataAPI_network
FrontEnd_network
So they're not connecting to the same network.
I don't think i need to share actual code for this, if you want to know something more, please just leave a comment.

A: Mark your network as external in your compose files.
The network will need to be pre-existing (create it using docker network create before calling docker-compose up).
See documentation, at the end of this page : https://docs.docker.com/compose/networking/#configure-the-default-network
BTW there is the same concept of external volumes.

redpajama_set_name: RedPajamaStackExchange


text:
/**
 */
package xtext.scoping.adventures.xscope1;

/**
 *
 * A representation of the model object 'Variable'.
 *
 *
 *

 * The following features are supported:
 *

 *
{@link xtext.scoping.adventures.xscope1.Variable#getName Name}

 *

 *

 *
 * @see xtext.scoping.adventures.xscope1.Xscope1Package#getVariable()
 * @model
 * @generated
 */
public interface Variable extends Statement
{
  /**
   * Returns the value of the 'Name' attribute.
   *
   *

   * If the meaning of the 'Name' attribute isn't clear,
   * there really should be more of a description here...
   *

   *
   * @return the value of the 'Name' attribute.
   * @see #setName(String)
   * @see xtext.scoping.adventures.xscope1.Xscope1Package#getVariable_Name()
   * @model
   * @generated
   */
  String getName();

  /**
   * Sets the value of the '{@link xtext.scoping.adventures.xscope1.Variable#getName Name}' attribute.
   *
   *
   * @param value the new value of the 'Name' attribute.
   * @see #getName()
   * @generated
   */
  void setName(String value);

} // Variable

redpajama_set_name: RedPajamaGithub


The function of examination representative at Linköping University was created in 2006 by decision of the university president. Each department has its own examination representative, as does the Faculty of Health Sciences.
Here you can get help with questions concerning the set of rules for examinations. The examination representative at the Faculty of Health Sciences answers questions from both students and teachers within degree courses, stand-alone courses, and commissioned courses.
Below, you will find a link to the local set of rules so that you can find the answer to your question before you contact the examination representative.
Only questions sent from an liu.se address will be answered.
You must be registered, or have a teaching assignment in the course concerned. Give the course name and number. You may not ask questions anonymously. In the even the examination representative judges it necessary to inform the the teacher responsible for the course or the examiner, the person who asked the question will remain anonymous. Any questions concerning evaluation and marking of examinations will be referred to the examiner for the current course. All questions and answers will be archived at Linköping University.


Peace of Mind, Don't Look Back, More Than a Feeling, Foreplay/Long Time, and Amanda are a few of the many classic rock anthems that Boston can lay claim to and will be playing live when the band makes a stop on their current tour to Columbus on August 1st. They will be playing the Celeste Center at the Ohio State Fair. I didn't hesitate when I was given the opportunity to interview the newest member of the band, bass player Tracy Ferrie.
The bands publicist, Gail Parenteau, was gracious enough to organize the interview and Tracy was the real deal. During my time with him on the phone I got to know a little more about him, I got a better understanding to the inner workings of Boston and the music they play, and we even got to do a little bit of old fashioned rock 'n roll discussion.
Me: Tell me about how you got into playing music?
Tracy: I'm from Elkhart, Indiana and it is known as the band instrument capital of the world. There was lots of access there and I got started in my public school. I learned to play the guitar, tuba, standup bass, electric bass, and percussion.
Me: I know that you grew up on classical music, so what were some of the bands that got you into rock 'n' roll?
Tracy: As a roller skating champion as a kid you perform to classical music. My big brother actually introduced me to bands like Ted Nugent, KISS, Queen, and Boston of course. As I got older I started finding my own tastes like Steely Dan. Then I went to Berkley, where a lot of those people were famous for. I liked jazz influenced pop and gravitated towards that.
Me: Who were some of your influences that got you into playing the bass full time rather than another instrument?
Tracy: I can name some off the top of my head; John Paul Jones from Led Zeppelin and John Deacon from Queen. There is one that a lot of people aren't familiar with, a guy named Mars Cowling from the Pat Travers Band. Their album Go for What You Know features some phenomenal bass work. It's one of those things that when you meet somebody else that has heard it and appreciates it; you're kind of in the brotherhood. Then there is Michael Anthony from Van Halen. I've never really been into the virtuoso type of bass players. I always thought if you want that much spotlight, play the piano or the guitar. Why are you playing the bass?
Me: You stated that you were a fan of Boston when you were younger, is there a time that you can pinpoint when you discovered them?
Tracy: Prior to the release of that first record. I was 11 or 12 at the time. Being into roller skating you always had to keep up on new music and that's where I was introduced to that first Boston record. I'll never forget hearing that sound and those songs. Its sound and production was light-years beyond anything that had been recorded before.
Me: Tell me about how the position in Boston came about for you?
Tracy: I have a lot of experience as a studio musician and I played in Stryper. In their later years I recorded a couple of albums with Stryper and we did a cover of "Peace of Mind" with Tom Scholz on it. I believe it's the only record he has played on outside of Boston. We performed it live at a benefit for the Station nightclub fire in Rhode Island. Later on he contacted me about playing bass with Boston.
Me: So, what's it like playing in a band with Tom Scholz? I mean, he gives me the impression that he is a perfectionist; he's been known to take many years in between records. Is he a perfectionist and does he expect perfection from the rest of you guys?
Tracy: He does. He expects perfection but more importantly your direction. Everything has to work together in Boston's music; it's not a free for all. Everyone makes mistakes, misses a note, but it's that we are trying our hardest to get to where it needs to be. Specific parts all gel together to form this sort of orchestra of music. We need to all be on the same page and we strive for that.
Me: Ok, now that you guys have been back on the road for a couple weeks, how has the crowd reaction been on this current round of tour dates?
Tracy: It's been overwhelmingly positive and energetic. The crowd hears those songs and this is what they expected to see and hear. One of the most commons comments we get at the meet and greets after the shows is that it "exceeded our expectations". The excitement during "Long Time", people are literally coming out of their skin. It's a great time had by all.
Me: Is the Boston crowd much different than what you experienced as a member of Stryper?
Tracy: Not really. Stryper isn't brand new either and they have a very diverse crowd like Boston. There have been people of all ages at these shows, a lot of fathers and their sons. The longtime fans are saying "I have great memories of this music and you guys brought that back." The kids though, it's refreshing to have teenagers telling you that they aren't really into newer music and that we are their favorite band. Seeing them appreciate what Boston does musically and lyrically, it shows you how timeless this music is.
Me: What has been your favorite Boston song to play live?
Tracy: We do a song from the Walk On record called "Surrender to Me". It's got kind of an 80's flavor to it. Maybe that's why I like it, and then when the whole thing comes together during "Long Time" it leaves no doubt. The crowds become frenzy like.
Me: On August 1st, you guys will be playing the Ohio State Fair with opening act Kansas. Tell me, what are your expectations for when you guys come to Columbus?
Tracy: Everybody knows that Columbus is a rock 'n roll town. If the reaction is the same to what we've been getting in other cities, we aren't going to kid anyone. The shows we're playing are the real deal.
Me: Obviously it's great for the fans when they get another classic band on the bill, like we will be getting when Kansas opens for you guys. On your side though, is it more difficult to play when the opener is an established act like Kansas? Is there added pressure to perform at a high level?
Tracy: Absolutely there is. People are coming to hear two great bands of that era and are wondering "Who's going to deliver?" People want to know, but at the same time it's an added bonus for everybody getting to sample these two flavors of music.
Me: Boston is a marquee act. Do you prefer playing to larger crowds in arena and amphitheater settings or the more intimate smaller venues?
Tracy: Each one has its own reward. In the intimate ones you can connect with the crowd more and see facial expressions that you wouldn't be able to see with a guy at the top of an arena. So it can translate better in smaller venues. It's a different feeling though. There is a different energy when you are playing a big show and there are ten thousand people singing along to the chorus of "Peace of Mind".
Me: Are there any surprises in the set list this year that should get fans extra excited about August 1st?
Tracy: "Foreplay" is extended and has an almost orchestral element to it. It's great; there really is no dead time between songs. I've played in other bands where there is that awkward pause between songs and you are hoping the singer says something good, but we are just go, go, go.
Me: Are there any plans for new material when you guys get back off the road?
Tracy: I know there is an album in the works. With me being a newcomer and very late notice arrival to the tour that would be a better question for Tom. I know he was working on stuff but it was put on hold. He wanted to take his time on it and wants to wait until after the tour.
Me: Ok, I have one last question, for you as a fan, who put on the best concert that you ever saw?
Tracy: Roger Waters on his Pros and Cons of Hitch Hiking tour. I love when theater and rock come together. KISS was one of my all-time favorite bands but Roger Waters topped it all. Eric Clapton was playing guitar on that tour. One half of the show was songs from The Wall and the other half was from his solo album Pros and Cons of Hitch Hiking. That really is an easy one for me.
With that I thanked him for his time and told him how excited I am for the tour to hit Columbus in a few weeks. I wished him well and he thanked me as well and made sure to say that he is looking forward to their show here also. He seemed to be a very genuine class act and was a true rock 'n roll gentleman in affording me the opportunity to talk to him. Not all established bands are so generous to their fans. Get ready Columbus; find your way to the fair for the Boston and Kansas show on August 1st, even if you have to Hitch a Ride. Boston's back in the capital city for the first time since 2003. I attended that show at the Schottenstein Center nine years ago and it was one of the best live performances I have ever seen. Tickets are on sale now at all Ticketmaster outlets for $30.


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A musician from the age of 9, Pianist/Composer/Educator Sam Pasco received his degree in performance from the prestigious Berklee College of Music in Boston. Since graduating, he has worked as a staff writer with Otis Blackwell ("Don't Be Cruel," All Shook Up") in Nashville, and performed as a session musician, playing with some of the Music City's finest artists. As a private teacher with over fifteen years experience, Sam incorpora...
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Marcia generated lots of interest in the Mystery Quilt. You can see several of the first installment blocks posted on our Proper Bostonian Facebook page. Take a look and get inspired to start yours if you haven't jumped in yet.
Kace presented the guild with proposals for the season. She gave an update on our charity quilt projects. Preschool nap quilts in the 40"-50" range are needed. We give them to a variety of places including Horizons for Homeless Preschool, Project Linus (delivery each October), andCasa Nueva Vida in Jamaica Plain, a shelter for battered women and their children. Casa Nueva Vida can use quilts in all sizes: infant to adult. MARE (Mass Adoption Resource Exchange) needs twin bed quilts.
PBQ is also committed to providing quilts to our service men and women through the Veterans Administration. Quilts with a red, white, and blue focus are particularly appropriate, but any color-way is appreciated. Sizes can range from lap size to bed size. A suggestion was made that if we make an extra Block of the Month in patriotic fabrics each month, we will have a good start on a patriotic sample quilt by the end of the year.
We will be having an upcoming project for ovarian cancer.
Kace brought lots of fabric for the taking to make charity quilts.
Quilters should bring all their comfort/charity quilts in for show and tell before they are sent off to these organizations.
Kace does an amazing job of organizing quilters for these important causes throughout the year as well as making quilts along with the rest of the volunteers.


First, RPM staff will be heading just south of Phoenix to Wild Horse Pass Motorsports Park in Chandler AZ to hook up with US DRAGCAR and their Arizona Race Company StreetCar Showdown Series to get an inside look at the series and its racers, and develop photoshoots for upcoming issues of RPM!
Right after racing's done, the RPM team will be heading slightly north to Glendale AZ to catch all of the street car, muscle car and hot rod action they can handle for the Saturday night Mixteca cruise night at 67th Ave and Bell Rd. "For this ROAD TRIP we are guests of two very cool existing events and are there for one reason, to gather info on badass cars for RPM. We're face-to-face people and prefer to catch horsepower in it's natural habitat rather than over the internet only," joked Biro.
RPM senior staff will be on hand for this inaugural ROAD TRIP, including Biro himself along with Toby Brooks, RPM Special Projects Director and builder of the RPM aPocalypSe Horse; the world's first Twin ProCharged Kaase Boss Nine Hemi Ford Mustang!


They're still girls, not yet women. Britney-esque Norwegian teens Marit and Marion continue to sing about cliques and crushes, though they exhibit some musical growth since their debut, which spawned the hit "Don't Say You Love Me." The best uptempo tracks — "Everything," "Miss Popular" — recall the acoustic pop of Hanson (that's a compliment). But the gals' wispy vocals can't carry the ballads. A set of hits and misses, with little in between.


Long-time Top Hat strategic partner, Community Elf, decided to re-name and re-brand to position themselves as leaders in creating results-driven customer-centric content. We took the reigns from there, delivering a mark and a website of custom, engaging interactions to play on their spacey name without being overly-explicit.
COSMITTO HAS THE BRAND AND THE WEBSITE TO LAUNCH THEMSELVES INTO INTO NEW STRATOSPHERES.


As you all know: foobar2000 is a very unique and fantastic music player. It comes with couple of different user interfaces from witch you can choose freely what to use. They are good, but have you ever wondered how to customize foobar's interface by yourself? If you have, you have to read this article!


text:
Mr. Ubaidullo Nazriev, a farmer from village Chapaev, jamoat Rudaki, Vaksh district, Khatlon province, was born in 1954. He is an accountant-financial specialist with a big family of 17 members, including 8 grandchildren (Photo 8). He owns 2.3 ha of land, producing mostly cotton. A small area was cultivated under potato with unknown variety procured on the local fresh market.
Photo 8. Mr. Ubaidullo Nazriev's family, Khatlon.
Mr. Nazriev became a project beneficiary in 2015 and started producing potato by using of CIP varieties and innovative potato production technologies. That same year, his potato productivity increased by 53%, thanks to the high productivity and resistance of CIP varieties. As a result, his income also increased.
Since 2016 he started selling potato on the market, as his family's consumption was fully satisfied and potato was available for sale. Mr. Nazriev's high-quality seed potato costs are much higher, but has brought in additional income and has had very positive impact on his family's economic situation. After introduction of the technique to artificially break dormancy of newly harvested potato, Mr. Nazriev solved the no. 1 problem in potato production, as seed potato is a big deficit in the second growing season. Accordingly, he received additional income from double-cropping through potato production in the second growing season.
Photo 9. Mr. Nazriev's commercial potato production farm, Khatlon.
After 3 years of working with CIP potatoes, Mr. Nazriev decided to become a seed producer, because during last three years, he found that potato seed production has become highly profitable by using resistant
varieties, high-quality seeds, and innovative technologies. To support him, in 2017 CIP created a storage facility (cool rooms equipped with the CoolBot) for treating potato seed to artificially break dormancy at his farm. To create full value chain of seed potato production, CIP established a demo plot of commercial potato production in Khatlon at Mr. Nazriev's farm. The advantages of introduced innovations will be commercialized through scalingup of introduced varieties and technologies that bring high profits to beneficiary farmers (photos 9 and 10).
Photo 10. Ubaidullo Nazriev's CoolBot, Khatlon
Mr. Nazriev has also attended several trainings on table and seed potato production. He increased his own skills in this sector and now provides consultancy service to other farmers in the region.
On his farm 2,368 m2 land was cultivated under CIP potato and innovative technologies; 5.127 MT of potato was harvested, from which 2.5 MT was sold for 2 TJS and 513 kg (10%) was kept as seed for next growing year and 2.115 MT used as food for family. Mr. Nazriev's family got 10,254 TJS ($1,367.20) total income from potato production. His farm can be seen as model farm of successful potato value chain in Khatlon Province.


Whenever walking in the port, pedestrians are advised to use marked paths whenever available, and also always make sure to use the most safe passages. Entry or exit to/from the area by foot is to be made through gate B4. Admission for entry is issued by the harbour office on request. High visibility clothing (classification mark 2) and a helmet (classification CE EN 397) must be worn.
Entrance to the harbour office, the customs office and the canteen is possible without entering the port area through the pedestrians´gate (B1), from the nearby carpark, and further entrance to the port area is enabled by obtaining a access permit from the harbouroffice. Gate B1 is open daily (weekdays) 07.00 to 17.00.


WRITTEN ON Friday, September 25th, 2009 BY William Heath AND STORED IN Foundation of Trust, Identity, We told you so..., What do we want?
WRITTEN ON Wednesday, September 9th, 2009 BY William Heath AND STORED IN Foundation of Trust, Identity, We told you so..., What do we want?
WRITTEN ON Friday, September 4th, 2009 BY William Heath AND STORED IN Foundation of Trust, Official fibbing/bad stats, Political engagement, We told you so..., What do we want?
Having dumped controversial former chief executive Wally O'Dell in 2005Diebold has now finally dumped its e-voting unit. This was a deeply unpleasant history, and the new buyer Election Systems & Software (ES&S) is far from Ideal.
WRITTEN ON Thursday, August 13th, 2009 BY William Heath AND STORED IN Foundation of Trust, Identity, Save Time and Money, We told you so..., What do we want?
WRITTEN ON Tuesday, August 11th, 2009 BY William Heath AND STORED IN Foundation of Trust, Identity, We told you so..., What do we want?
WRITTEN ON Thursday, August 6th, 2009 BY William Heath AND STORED IN Foundation of Trust, Identity, We told you so..., What do we want?


I have just been in France where I was privileged to visit a number of WW1 British and Commonwealth War cemeteries with a friend who was visiting the grave of their Great Uncle who was killed at the age of 19 just before the battle of the Somme, when a wall fell on him.
This afforded me the opportunity to try and take photos in what is, I suppose, the closest British people can get to "Holy Ground". I don't have any ancestors buried in any War Cemetery but there were other family connections with the First World War.
The first cemetery we visited was at Roeux, where I came across the grave of 266066 Private A. Gordon, of the Gordon Highlanders. This regiment was raised in Huntly, Aberdeenshire which is where one side of my family comes from. Private Gordon, could well have gone to school with my Father's Uncle or known my Grandfather's shop in the town.
In Huntly a young man is known as a "Loon" and this is one Huntly Loon who never went home. More poignant yet was the grave of another Gordon Highlander who was one of the many graves where they were simply labelled "Known Unto God".


October 18, 2018: Welcome to the MaxFH-Zag Holland Tour website. We hope you can join us on this life & game changing tour to Holland, where you will be able to learn from some of the greatest hockey coaches in the world. Coming off of a gold medal at the World Cup in London in 2018, the Dutch style of hockey is exciting and mesmerizing. You will have the opportunity to meet and play against local Dutch clubs and learn firsthand what skills and tactics the Dutch are using to produce some of the the best hockey players in the world. You will also have a chance to explore the rich Dutch culture and participate in leadership exercises to help you maximize your potential as a hockey player, leader and person.


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Q: are objects in every stack-based-only VM allocated on heap Say, we have a VM, which has a stack. The stack's length must be variable. Then the stack itself must be allocated on heap, because the VM needs to request memory for the stack at runtime. So all the objects in that stack are actually allocated on heap, too. I wonder if this guess holds true for all stack-based languages.
This not a questing specifically for JVM. I just learned that JVM is both stack and register based. My question is that, for languages of only stack-based VMs, is it possible to allocate objects on the OS stack? And if possible, how can that be implemented?