Getting to Tempe is Easy for Arizona Meetings & Events Tempe, Arizona is located just four miles from Phoenix Sky Harbor International Airport in the heart of the Phoenix/Scottsdale metro area. It's easy for meeting attendees to get to Tempe and this classic college town is full of activity year-round. With all the meeting spaces, local eateries, full-service and limited service hotels and things to do, Tempe is an excellent choice for Arizona group travel. Tempe's location makes it easy for meeting planners who want to boost attendance at their next event, while minimizing transportation planning hassles, headaches and costs. Phoenix has a lower domestic itinerary fare than the U.S. average, and flights from Phoenix Sky Harbor International Airport travel to 80 domestic locations and 20 international locations. PHX has nonstop flights from many major cities like Denver, San Francisco, Los Angeles, Miami, El Paso, Cleveland, Portland and many more. This makes it quite convenient and inexpensive to get to Tempe, even for an international group. The destination experts at the Tempe Tourism Office are committed to helping you make your meeting a success. We offer an array of free services to meet all of your meeting planning needs and program requirements. Proposal Requests and Site Selection: Each RFP is submitted only to the hotels and/or venues that fit your requests. Site inspection itineraries can be arranged for group meeting and travel planners. You may conduct your own site tour, or your Tempe Tourism Office destination expert will be happy to create and confirm your schedule as well as accompany you. Formal Bid Proposals: The Tempe Tourism Office will prepare and present a customized proposal to your board of directors or decision makers. Services and Promotional Materials: To help increase attendance, we offer enticing destination guides, videos and photography. An order form is available at tempetourism.com. Activity Ideas and Sample Itineraries: Each staff member at the Tempe Tourism Office is all about fun; so we will help you create memorable events, original theme parties and find fun activities. We can also suggest the perfect spouse, family and children's programs and much more.
Tempe's college town atmosphere allows for artistic expression from all aspects of the arts and cultural spectrum, from the Broadway productions at ASU's Gammage theatre to concerts at the Marquee Theatre in Tempe.
Dive into SEA LIFE Arizona Aquarium! Discover more than 5,000 creatures, walk through the amazing 360-degree ocean tunnel and marvel at 30 incredible displays. It's the perfect stop for family fun!
Experience Arizona's original walkable urban district for great dining, shopping, nightlife and more. The Mill Avenue District features over 100 shops and restaurants, world renowned events, arts, culture, hiking, biking, boating, sports and lodging. Find your way at MillAvenue.com.
Founded in 1962, the Phoenix Zoo is one of the largest privately-owned, non-profit zoos in the country. Home to more than 1,100 animals including 200 endangered or threatened birds, mammals and reptiles, the Zoo always entertains and delights. Meeting and banquet facilities with professional catering and meeting planning. Indoor and outdoor facilities can accommodate 10 - 10,000 for private events.
Arizona's largest attraction, Arizona Mills, features a mile of Outlet stores, retail stores, and entertainment venues all under one roof. Everyday you can take advantage of savings up to 70% off at designer and name brand stores such as Neiman Marcus Last Call, Saks Fifth Avenue OFF 5th, NIKEFactory Store, Aeropostale, Justice, Nine West, Conn's and many more! And while you're shopping, check out the largest IMAX theater in Arizona and the only SEA LIFE Aquarium and GameWorks you can find in the state.
Tempe Town Lake, located adjacent to the Mill Avenue District, provides a two-mile recreational haven for kayaking, sailing, rowing, jogging, skating or picnicking. The heart of Tempe Town Lake is historic Tempe Beach Park. The park provides five miles of pathways and ample room for festivals or events, such as Ironman Arizona, various charity walks, Oktoberfest and the July 4th Tempe Town Lake Festival.
Discover over 100 retail, dining and entertainment offerings including Target, Gap, Bath & Body Works, The Keg Steakhouse & Bar, Harkins Theatres, Dave & Buster's and so much more. Enjoy unique water features, outdoor fireplaces, bright lights and live music as you stroll through the District. Conveniently located in Tempe on Loop 101 & 202, Tempe Marketplace is just minutes from the surrounding communities of Phoenix, Scottsdale, Mesa, Chandler and Gilbert.
Living museum featuring 50,000 desert plants from around the world. Enjoy tours, concerts, seasonal exhibits, special events and family activities.
Tempe, Arizona, home to Arizona State University, is located less than 10 minutes from Phoenix Sky Harbor International Airport. Situated in the heart of the Metropolitan Phoenix area, it is easily accessible by Metro light rail and several freeways. Tempe is the perfect year-round destination, offering exciting events, Broadway shows, live music, professional sports and some of the Southwest's best dining, nightlife and shopping. We invite you to plan your next meeting at one of the many premier Tempe, Arizona resorts and hotels. From gorgeous mountaintop views to a dynamic downtown setting, the Tempe first class resorts and unique venues offer something for every taste and budget.


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Architect: Jean-Baptiste Lassus
Jean-Baptiste Lassus
Jean-Baptiste Lassus1 August 2016
By Martin Bressani
After a brief passage at the École des Beaux-Arts in Paris in the studio of Henri Labrouste from 1828 to 1830, French architect Jean-Baptiste Lassus fell under the sway of the romantic cult of history and turned toward the middle ages. Together with his life-time associate Eugène-Emmanuel Viollet-le-Duc (1814–1879), he… Read More
Tags elevation presentation civic & municipal religion
Jean-Baptiste Lassus1 October 2015
The watercolour of the Sainte-Chapelle drawn by Lassus dates from the first years of the restoration, when the desire to restore the monument to its original thirteenth-century form was still very strong. The chapel is shown without its fifteenth-century flamboyant rose window and its exterior staircase built by Louis XII,… Read More
Tags elevation topographic/cartographic presentation religion
Displaced persons
Displaced persons3 October 2012
By Niall Hobhouse and Nicholas Olsberg
Architects are extraordinarily reluctant to incorporate into their visual descriptions of buildings any evidence that the real subject their structures serve, and around whose activities they are so carefully formulated, is people. Here's a look at a few of the moments when this unspoken rule has been broken. DISTANCES: Using… Read More
Tags section exhibition design health & leisure memorial & monument urban form education public space theatre interior work on paper (series)

redpajama_set_name: RedPajamaCommonCrawl


Why don't I see my DEP device in Fleetsmith?
How do I assign a device to Fleetsmith manually in the Apple DEP portal?
How do I get a list of DEP eligible devices from the Apple DEP portal?
Where can I find a DEP device's temporary password?
1. Visit the DEP portal at deploy.apple.com and sign in.
3. Select "Serial Number" under "Choose Devices By".
4. Paste the Serial Number of the device you want to assign to Fleetsmith in the box. If you have multiple, separate the Serial Numbers with commas.


Best known for: Luxurious rooms & suites to stimulate your senses.
Stylish and warm, Boutique Hotel La Posada de Bucerias offers a peaceful and relaxing setting with all the comforts of home. Relax in tranquil and lush, tropical surroundings at this new, small hotel is an ideal destination for business and leisure travelers alike. Located only two blocks from the beach! Enjoy the longest, uninterrupted beach on the bay. This Boutique Hotel is within walking distance to town, restaurants, and shopping.
Inventively contemporary & unexpectedly traditional in mexican design! The chic La Posada de Bucerias is ideally located near downtown Bucerias, close to golf and other area activities and attractions.
From the moment you step into the beautiful lobby you will be impressed with your surroundings - even more so when you settle into your suite. All of the suites feature a comfortable sitting and work area with plenty of space to relax or work. It's all about comfort at La Posada de Bucerias, and they provide it with style!
Discover La Posada de Bucerias Bucerias Hotel and start planning your next trip today!


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Enomoto (written:  or ) is a Japanese surname. Notable people with the surname include:

, Japanese baseball player
, Japanese voice actress and singer
, Japanese model and actress
, Japanese painter
, Japanese footballer
, Japanese business executive and space tourist
Isami Enomoto (1929-2016), American ceramicist
, Japanese footballer
, Japanese actress
, Japanese comedian
, Japanese footballer
, Japanese singer-songwriter
, Japanese manga artist
, Japanese poet
, Japanese basketball player
, Japanese manga artist
, Admiral of the Imperial Japanese Navy
, Japanese footballer
, Japanese footballer
, Japanese ice hockey player
, Japanese Blogger

Fictional characters
, a character in the manga series First Love Limited
, a character in the manga series Love Lab

See also
Enomoto: New Elements that Shake the World, a manga series by Shunji Enomoto

Japanese-language surnames

redpajama_set_name: RedPajamaWikipedia


I am learning so much about allowing everything to be what it is, with no fault, no judgment, no expectation. The times when I feel a sense of unease on this journey, when I am agitated or that familiar sense of anxiety starts trickling up my limbs, it is because there is a disconnect between the way things are, and the way I expected them to be.
The boat ride is rough, the shower is cold, the street is crowded. These are facts, my resistance to them creates nothing but a lack of harmony to the world around me. I restate the facts, lacking judgment and they lose their power to push me into a negative space. Yes, the world is all of these things, but what else is it at the same time? And if I can catch myself, and realign the thought process, suddenly the street is crowded, the ride is rough, the shower is cold and they are just brilliant details of where I am at that moment.
I have never before been so sure of how fleeting everything is. My place, and my feelings, pass as quick as the afternoon rains. It reminds me sometimes of how it was to be heartbroken, that reminder that I wold feel something else in ten minutes, to ride it out, to press on.
Yesterday was hard. It was no different than today other than the fact that I let it be that way. There was nothing truly wrong just a general sense of unease, a longing to be with the person I love, and lack of gratitude for where I was. While I think it is alright to have a hard day, there is something increasingly detrimental in the way it can take over when you are this alone in the world.
I am impressed by myself on the daily, and yet always expecting more. It keeps me moving, it keeps me watching, and it me writing. I am stretched thin in all of the best ways, and full of things I have never had before. Whatever it was I wanted when I decided to do this, this might have been it. You have to learn how to see yourself in the dark.


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Q: Why and how does the 'clock rule' of electromagnetism (i.e. current flows clockwise as seen from the south pole of an electromagnet) work? Can anybody explain why the 'clock rule' has been designed the way it is?
I mean, why is it that the polarity is North pole, if current flows in the anticlockwise sense as viewed from above and vice-versa.
What is the reason behind assigning the different fingers in Fleming's left or right hand rule? Why do we assign the thumb to the motion of conductor, the finger for the magnetic field and the middle finger for current?

A: By observing the direction of current in the anticlockwise direction, you see a capital N (for North Pole); in clockwise direction, you see a capital S (for South Pole). Try it on a piece of paper.
However, as stated above, it's just a convention.

redpajama_set_name: RedPajamaStackExchange


text:
Institute for Medical Technology Assessment (iMTA) /
Annals of the Rheumatic Diseases: an international peer-reviewed journal for health professionals and researchers in the rheumatic diseases /
Van Mulligen, E., Weel, A.E.A.M., T.M. Kuijper (Martijn), Denissen, N.H.A.M., Gerards, A.H.M., De Jager, M.H., Lam-Tse, WK, J.M.W. Hazes (Mieke), Van Der Helm-Van Mil, A., De Jong, P.H.P., et al. J.J. Luime (Jolanda)
Two-year cost effectiveness between two gradual tapering strategies in rheumatoid arthritis: Cost-utility analysis of the TARA trial
Annals of the Rheumatic Diseases: an international peer-reviewed journal for health professionals and researchers in the rheumatic diseases , Volume 79 - Issue 12 p. 1550- 1556
Objective The aim of the current study was to evaluate the 2-year cost-utility ratio between tapering conventional synthetic disease-modifying antirheumatic drugs (csDMARD) first followed by the tumour necrosis factor (TNF)-inhibitor, or vice versa, in patients with rheumatoid arthritis (RA). Methods Two-year data of the Tapering strategies in Rheumatoid Arthritis trial were used. Patients with RA, who used both a csDMARD and a TNF-inhibitor and had a well-controlled disease (disease activity score ≤2.4 and swollen joint count≤1) for at least 3 months, were randomised into gradual tapering the csDMARD first followed by the TNF-inhibitor, or vice versa. Qualityadjusted life years (QALYs) were derived from the European Quality of life questionnaire with 5 dimensions. Healthcare and productivity costs were calculated with data from patient records and questionnaires. The incremental cost-effectiveness ratio and the incremental net monetary benefit were used to assess cost effectiveness between both tapering strategies. Results 94 patients started tapering their TNF-inhibitor first, while the other 95 tapered their csDMARD first. QALYs (SD) were, respectively, 1.64 (0.22) and 1.65 (0.22). Medication costs were significantly lower in the patients who tapered the TNF-inhibitor first, while indirect cost were higher due to more productivity loss (p=0.10). Therefore, total costs (SD) were €38 833 (€39 616) for tapering csDMARDs first, and €39 442 (€47 271) for tapering the TNF-inhibitor (p=0.88). For willingness-to-pay (WTP) levels <€83 800 tapering, the csDMARD first has the highest probability of being cost effective, while for WTP levels >€83 800 tapering the TNF-inhibitor first has the highest probability. Conclusion Our economic evaluation shows that costs are similar for both tapering strategies. Regardless of the WTP, tapering either the TNF-inhibitor or the csDMARD first is equally cost effective.
Persistent URL doi.org/10.1136/annrheumdis-2020-217528, hdl.handle.net/1765/133923
Journal Annals of the Rheumatic Diseases: an international peer-reviewed journal for health professionals and researchers in the rheumatic diseases
Organisation Institute for Medical Technology Assessment (iMTA)
Van Mulligen, E., Weel, A.E.A.M., Kuijper, T.M, Denissen, N.H.A.M., Gerards, A.H.M., De Jager, M.H., … Luime, J.J. (2020). Two-year cost effectiveness between two gradual tapering strategies in rheumatoid arthritis: Cost-utility analysis of the TARA trial. Annals of the Rheumatic Diseases: an international peer-reviewed journal for health professionals and researchers in the rheumatic diseases, 79(12), 1550–1556. doi:10.1136/annrheumdis-2020-217528


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Kristen Stewart, Katy Perry, and Cara Delevingne Stole the Chanel Couture Show With Their Matching Buzz Cuts
By Sophia Panych
For Chanel's fall 2017 couture show in Paris, designer Karl Lagerfeld managed to pull off a feat of architectural ingenuity by placing a life-size version of the Eiffel Tower in the middle of the Grand Palais. Okay, so it wasn't technically the whole Eiffel Tower — it was just the first two levels that disappeared into a gray fog that covered the ceiling of the Grand Palais, creating the illusion that the structure was stretching far up into the clouds. But while the set was impressive, it didn't compare to the celebrity moment that practically stole show: Katy Perry, Cara Delevingne, and Kristen Stewart all sitting front row, all with head-turning, bright-blonde buzzcuts.
The buzz cut has become increasingly more mainstream over the past year with a surge of models sporting the crop on the runways in New York, Milan, and Paris. Catwalkers like Ruth Bell, Adwoa Aboah, Grace Bol, and Kris Gottschalk all took risks when they shaved their heads, but are now cast specifically for their distinctive hairstyles and aesthetic. Victoria's Secret took notice and, for their 2016 show, cast multiple models with closely-shorn crops, a major step for the brand known for basically inventing the notion of beachy waves. And how most trends go, this one has now trickled down from runway to red carpet, with multiple celebrities getting buzzed in the past few months. Our June cover star, Zoë Kravitz, did it, so did 13-year-old Millie Bobby Brown for her role in Stranger Things, you have singer Halsey, and of course, the three stars who all made an appearance front row at Chanel couture: Katy, Cara, and Kristen.
What makes this such a major moment isn't just because the three women all look freakin' amazing with their short, bleached-out styles — Stewart with frosted tips, Perry an cool platinum, and Delevingne so icy her hair's nearly white. It's because it's proof that the fashion industry and Hollywood are slowly but surely widening their definition of beauty (although, each field still has a long way to go). Even as close as five years ago, you'd have never seen an A-list actress or top-selling pop star shave their head unless it was for a role, as it's often been a style associated with the anti-establishment, whether that be angsty teenagers or punk rockers. The image of the three women sitting front row in Paris at a haute couture fashion show will surely help bash that stereotype — and have many of us contemplating going shorter than we ever have before.
Watch three models talk about taking major hair risks:


SQL injection & LFIMarco's SQL Iniection - LFI protection for Joomla!
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Marco's component maker for Joomla is based on plain text templates, so you can edit the them to improve the code or to add new features. Templates are stored in the templates directory.
This article is being written and is under revision, errors may occur. sorry!
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At present time default is not used. It is reserved for future implementation of the not cms Joomla! framework: please, do not use it.
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So file that are common between j3x and j25 are stored only in j25 directory. If j3x template differs from the j25 one you can save only this one in the j3x directory (in the exact position).
Here the directory structure. Please remember the structure is very important, only the file here listed (and in this exact position) can be used. Other files added to structure are ignored, modifiaction of structure will result in a program fault.
Directories are in Italics, files in bold, strike through file are not used at present time.
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text:
SouthwestFamily Vacations
Beyond Disneyland: Things to Do in Orange County with Kids
By Laura Ishmael, May 24th, 2017
Millions of families make the trek to Southern California each year with one goal in mind: Disneyland. It's the mecca of family travel and a rite of passage that most children should experience at least once.
But while Disneyland may be the most magical place on earth, there really is so much more to Orange County, California than its most famous theme park. With year-round sun, a string of gorgeous beaches, and plenty of family-friendly activities, Orange County is the ideal destination for any vacation– family, Disneyland and beyond.
So if you're really wanting to make the trip, but not quite sure you can handle "It's a Small World" day after day, here are a few other things to do in Orange County with Kids (beyond Disneyland):
Learn to Surf in Huntington Beach
Photo from Unsplash.
There are so many great beaches in Orange County, but undoubtedly the most famous is Huntington Beach. It's your classic California beach: sands that stretch for miles and fill up end-to-end with visitors and locals alike in the summertime. If you're feeling adventurous, why not try your hand at the OC's favorite pastime: surfing! Banzai Surf School and HB Surf School both offer 1-2 hour private lessons to get your feet wet and have you standing up in no time. After your lesson, don't miss a stroll down Main Street for some beach gear or lunch at Ruby's on the pier.
Visit the Mission at San Juan Capistrano
Photo by the author.
Non-California natives will probably know little about the important role the missions of California played in shaping the state. Visit one of the most well-preserved missions right in Orange County at Mission San Juan Capistrano. The affordable admission price includes an audio tour which retells the story of the mission's inhabitants.
Explore the Trails at Crystal Cove State Park
Certainly not hidden, but often overlooked, Crystal Cove State Park is an OC favorite tucked between the cities of Newport and Laguna Beach. Start your trek into the park near Newport Coast Drive and explore the grassy trails and ocean views as they lead you down toward the beach. If you arrive early enough, try to claim a table at Beachcomber Cafe, an old beach cottage that's been converted into a restaurant with a beautiful ocean-view.
Ride the Ferris Wheel at the Balboa Fun Zone
Though it may be small in size, the Balboa Fun Zone, with its signature Ferris Wheel, has been around for over 80 years. The old school boardwalk brings the nostalgia of Coney Island to the west coast, with Newport Bay on one side of the Fun Zone, and the Balboa Peninsula on the other. After exploring the Fun Zone, families can rent boats to cruise around Newport Harbor or take the Balboa Island Ferry across the bay for some shopping on Balboa Island. No matter which side you stick to, you can't go home without a famous Balboa Bar or frozen dipped banana!
Go Horseback Riding in the Canyons
Not all that far beyond the beach is a whole different side of Orange County. Bordered to the east by the Santa Ana Mountains, the OC is home to many cities along the foothills and the canyon trails leading up through the mountains offer some of the best views. Visit Country Trails and Riding School in Irvine Regional Park for scenic guided trail rides on horseback.
Take a Boat to Catalina Island
About 30 minutes from the Orange County coastline is another must-see gem: Catalina Island! Making a quick day trip to the island is quite simple, with the Catalina Flyer leaving from Newport Beach to Avalon in the morning and returning by dinnertime. The quaint town of Avalon can be easily explored on foot or by bike, and there are several hotels in the small village if you wish to extend your stay. While on the island for the day, enjoy snorkeling at Lover's Cove, biking the village on beach cruiser rentals or relaxing at Descanso Beach Club.
Check out the Tide Pools in Corona del Mar
Corona del Mar State Beach (located in the city of Newport Beach) is another favorite beach for a low-key afternoon. Much less touristy than Balboa or Huntington, not only does it have stellar ocean views and a nice sandy beach, but a wonderful collection of tide pools just beyond the rocks as well. Kids will be thrilled to spot sea urchins, starfish, and plenty of other colorful sea creatures quite easily at low tide. It's no wonder this spot is a favorite among the locals!
Where to Stay in Orange County with Kids
Laguna Cliffs Marriott Resort
Photo from trivago.
View on trivago
Located in southern Orange County, Laguna Cliffs Marriott Resort is the ultimate in resort living. The hotel's parlor suites are perfect for families needing some extra space. That is, of course, when not busy utilizing the resort's many outdoor activities and complimentary rentals of boogie boards, sand toys, board games, sports equipment and more!
Hyatt Regency Newport Beach
Situated near the Back Bay of Newport Beach, the Hyatt Regency is minutes from both the sand and John Wayne Airport, while also being ideally located in central OC. This upscale hotel also boasts three outdoor swimming pools and an on-site restaurant.
SpringHill Suites Irvine
At the doorstep of the South Coast Plaza shopping center, families will find plenty of dining options within walking distance of this hotel. The thoughtfully laid-out suites with contemporary decor will help families feel right at home on their trip.
With so much to do in Orange County, California with kids and year-round gorgeous weather to welcome you, the only question is: when will you be booking your trip?
5 Places Your Kids Will Get A Taste of Californ...
Best California Wineries To Visit With Kids
Weekend Getaways in New Mexico


Naveeen Rajdev from Wipro and Allan Valahu from Accenture gave their views on new and old forms of influence to Phil Fersht in the AR Forum's first fire-side chat. Many AR people agree on the tiring nature of signature research like the Quadrants, and the debatable value in the stale research formats. More consolidation of the quadrants would be interesting, and better perspective is needed about the real role that we can expect analysts to perform. Dogs are colour-blind, but they can still help us cross the road. AR people need to understand how they can do well enough to be invited into deals, and quality services is clearly primary to these charts. Even so, you need to be on the quadrant to be taken seriously in market segments which are consolidated and clearly categorised. Integrators are struggling with transformative and new areas, which the major analysts don't cover so well. The diagrams are well used, but there's little coverage in the segments that are really growing strategically. Executives want to bring analysts into conversations with clients: the signature research does not help you to do that.
To get relationships-building and dialogue more in the centre, organisations need to focus on the analysts who can bring something to the table, not only those who can write research. Relationships are getting warmer with analysts, quite often, but the challenge is to have spokespeople who focus on each firm and can give an across-the-board picture of the vendor that supplements the personal connections that are also needed for success. More proactive relationships are also needed with the leaderships in analyst firms to see how relationships can turn into cooperations, and to really engage each analyst firm in a way which tempts it to maximise value rather than simply maximise revenue. That can mean pushing back against salespeople in analyst firms, who often don't really introduce themselves to the vendors' top executives, and when they do often don't clarify their roles as industry analysts.
Pushing back against the legacy analysts firms isn't as hard, or as one sided, as it sounds. Long-run business is till influenced strongly by the legacy firms, and if legacy analysts don't get your market then it's easier than ever to go around them and find other analysts who are keen to make a mark in a market, even a new segment that is hard to understand.
To the vendors, analysts are obviously much more than a media channel: their value lies in helping firms to define and position and to come to the market more effectively. Mapping the analysts and reaching out in more structured and effective ways means that analysts can better help vendors to reshape themselves, to reshape the market and to help customers shape up for the future.
Relationships with sales reps can help relationships with analysts and analyst firm leaders to also develop. The turnover of salespeople gets strained, especially when salespeople struggling with their numbers start to sell above the budget-holders. Increasingly it's hearing from customers, rather than salespeople, that is encouraging vendors to decide on which analyst firms need to be invested in.
How far will automation influence the analyst industry, given the need for relationships. Talking and testing is essential. Much of the process can be automated and social media in particular can produce stackable content: one or two pages to allow analysts to produce prolific, more regular, earlier insight using podcasts and webinars that can flag up trends early. Executives get exhausted by long production schedules when research is out of date by the time is emerges. So, can analysts have a short questionnaire and more intensive and accelerated research processes that are completed in weeks rather than months. Of course, this means that analysts need a different tolerance for risk, and to reduce any single-point dependency on vendor participation.


Barnett, C. (2007). Mirage: Florida and the Vanishing Water of the Eastern U.S. The University of Michigan Press.
Book Review on Mirage by Cynthia Barnett Essay - Brainbasket. https://brainbasket.net/essay/book-review-mirage-by-cynthia-barnett-1117183.
"Book Review on Mirage by Cynthia Barnett Essay - Brainbasket", n.d. https://brainbasket.net/essay/book-review-mirage-by-cynthia-barnett-1117183.


We are hosts. We are events.
The Stadthalle Braunschweig Betriebsgesellschaft mbH as a municipal company of the City of Braunschweig operates the Stadthalle, the Volkswagen Halle Braunschweig and the Eintracht Stadium. As the market leader in the Braunschweig-Wolfsburg region, the operating company offers around 1 million visitors per year a diverse programme consisting of concerts, shows, congresses, business events, trade fairs and markets as well as sporting events. A significant characteristic of the three facilities is their specific suitability for particular types of events.


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We must kick coal, and here's how we'll do it: Australia Institute
18th June, 2020 | Renewables, Solar, Storage, Wind |
The pulse of the energy markets will tell you coal is in terminal decline. But with economies around the world still heavily reliant on the polluting energy source its demise will be a scrappy, drawn out affair.
Major coal exporters, such as Australia, will sense real anguish as they weigh the possibilities of transitioning to clean sources of generation against a rich history of revenue.
It needn't be that way.
New research from The Australia Institute's Climate & Energy program has shown that an orderly approach to phasing-out thermal coal would shield Australian workers, communities and the economy from the negative consequences of an unmanaged transition.
Half Australia's coal exports by value are metallurgical coal, a premium product used in steelmaking. Thermal coal, which accounts for the great majority of production and is used in electricity plants, is battling to remain competitive as the costs of solar, wind and hydro fall.
The study, written by John Quiggin, Professor of Economics at The University of Queensland, found that a managed transition out of thermal coal should be prioritised to reduce Australia's carbon output. If coordinated action is taken early the outcome can be achieved with relatively modest measures.
Key findings of the report include:
A transition out of thermal coal is going to occur, because the world is moving to other sources of energy – our choice is whether that transition is planned and orderly, or delayed and disorderly.
In the context of Australia's economy, the thermal coal industry accounts for a small share of total economic activity and around one-quarter of 1% of overall employment.
The phase-out of thermal coal production and use over 10 years could be achieved with minimal disruption to coal workers, regional communities and the Australian economy.
"Australia's transition away from excessive carbon pollution must begin with an urgent and coordinated phase-out of thermal coal production and use," Quiggin says.
"Fortunately, with enough advance notice and an appropriate transition plan, the thermal coal industry can be phased-out over time without any significant dislocation to workers."
The development and widespread adoption of a carbon-free technology for steel production is unlikely to take place before the 2030s, the report says. This implies that the need for Australian metallurgical coal will continue, and that the focus for the 2020s must be on phasing out thermal coal.
A well-planned and coordinated phase-out of coal would be based on targeted development of the renewable energy resources abundant in many coal-mining regions. It would include transition supports for early retirements, retraining for employees and economic diversification for affected communities.
"Through a managed transition, Australia can wean itself off coal by 2030, while also protecting the interests of workers, communities and the economy at a very modest cost. The costs of not acting, by contrast, are both huge and long-term," said Richie Merzian, climate and energy program director at The Australia Institute.
"A well-managed phase-out of coal would be the best way forward, but it can only be achieved through a coordinated approach involving the private sector, government and the unions who represent workers."
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The first few weeks of January have been super busy for us here at Check 4 Houses. Paul has been out on lots of property valuations. Clearly local people in Fleet, Farnborough and Aldershot are keen to maximise the Spring sales window.
We love getting out and about meeting people and supporting them on the journey of selling their property – which can be stressful. We are often reminded, as we have been this week, that even just choosing which estate agent to use can be a real minefield.
On the one hand, the rise of online agents has brought greater competition into the estate agency market and helped to bring down prices. On the other hand it seems to have led to increased confusion. In the old days, perhaps you knew what you were getting. But now with so many agents available, all with slightly different packages, it can be difficult to know which to choose.
At Check 4 Houses we do our best to make things simple. We urge people to always check the small print of the sales contract. Ask the questions about any nagging doubts and make sure you really understand what you are signing up for. For example, many people do not realise they have signed in to long exclusivity deals, leaving them stuck with what they might feel is an underperforming agent for months. In a property market such as ours that could cost you valuable time and money. Some online agents (especially those advertising heavily on TV) might seem like they offer a great deal, but do you realise that you may have to do viewings yourself? Some people might be very uncomfortable with this, having to deal with buyers directly.
Another area of confusion is around 'Buy now, pay later' options. For years the estate agency market was based on no sale, no fee. You only paid an estate agent once your house sale had completed. So if a sale fell though (which unfortunately it sometimes did), you hadn't lost anything. This gave you security that you were only paying the money to the agent when you had it – once the property had sold. Then came online agents (including ourselves) offering much lower fees if you paid upfront. "Pay just £499 now and save yourself thousands compared to standard agency fees." Of course there was a risk that the property wouldn't sell and you would lose your money. But for many people the risk was well worth taking based on the financial gain. For example, we sold one property in Wokingham last year for £850,000. The owners had decided to pay upfront and use our standard package. As a result they saved themselves nearly £15,000 in fees. A third option has now appeared with some agents suggesting that you can 'Pay Later', meaning that you can still take advantage of a low sale price without having to pay it up front. However what some people don't realise is that pay later does not mean pay once the property has sold. If you change your mind and do not sell the property then you still have to pay the fees. It isn't the same as a no sale, no fee option, even if it might appear to be.
What is the fee and what is included?
Do you do accompanied viewings or do I have to?
Does the fee include a For Sale board or not?
Is there any limit on the number of photographs you take, or websites you will advertise my property on?
Am I tied in to using any of your other services, such as an EPC, solicitor or mortgage broker?
Please can I read the full Terms & Conditions of the sales contract?
Asking these questions of each agent should ensure you have a level playing field to assess the agents on. You can then choose the right one for you.


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Bruno Aveillan, born in Toulouse, is one of the most distinguished and sought-after commercials directors in the world today. What inevitably sets Bruno's work apart is his highly developed artistic sensibility and innate talent for capturing extraordinary images that speak to the pursuit of perfection in every frame.
Early in his career, Bruno worked as an art director for Ogilvy and Publicis in Paris. By the mid-90's, he made the transition to commercial directing, shooting spots for clients including Time Warner, Thermasilk, Nintendo, Nissan, and Acura. Bruno's first major recognition came in 1998 with an award-winning spot for Perrier, in which he brought a fresh, fantastical approach to a traditional brand. By 2001, he was directing alongside Martin Scorsese, Wong Kar-Wai and Oliver Stone on the high-profile Orange spots for audiences overseas.
Having initially studied painting, his success can be attributed to his meticulous attention to detail and to his dexterous choice and devotion in unveiling the exquisite subject. His ability to blend this artistry with the most sophisticated visual effects with spots for Audi, Coca Blak, Baileys, Philips and Asics has made Bruno's work memorable to viewers worldwide.
In 2008, Bruno directed the first ever brand campaign for Louis Vuitton, asking viewers "Where will life take you? The 90-second spot evoking the soul of travel has since been translated into 14 languages. It received 14 international awards including the 2008 Gold Clio Award and the Gold at the London International Awards.
In 2012, Cartier announced the international release of "L'Odyssee de Cartier," a three-and-one-half minute film directed by Bruno. The award-winning film chronicling Cartier's 165-year history was first screened at The Metropolitan Museum of Art in New York. In 2014, Bruno presented his latest opus for Cartier with "Shape Your Time." Epic and complex, the film pays tribute to the brands rich heritage and its future with wondrous vfx.
In 2014, Bruno took home the Bronze Clio in Film Technique for his captivating Samsung spot "Life in Every Pixel." With his always-cinematic approach, Bruno turns the lens on the complex beauty of organic life forms in nature, immersing us into a vivid, magical world teeming with color and clarity.
Bruno has set the benchmark for the luxury genre with his refined aesthetic and superbly arresting images. His oeuvre of exquisite Clio and Cannes Lion-winning films for the houses of Cartier, Swarovski, Lanvin and Guerlain have become the touchstone for the highest level of cinematographic sophistication, and as such have been internationally acclaimed. In 2014, he was honored with the film retrospective Bruno Aveillan: Then Retrospective of a World Master at the 5th annual La Jolla Fashion Festival, which celebrates the most brilliant minds in fashion filmmaking internationally.


text:
Home / NEWS / Newsletter Archive, 2006-2021 / 2010-2011 / April 1, 2011
Faculty Governance News
vol. 5.6
From the UNC Office of Faculty Governance
200-204 Carr Building
UNC-CH Campus Box 9170
Contact: Anne M. Whisnant (anne_whisnant@unc.edu)
Boxill, Steponaitis are candidates for Chair of the Faculty; elections are April 13-22, 2011
Faculty members will vote in April to choose a new Chair of the Faculty to succeed current Chair McKay Coble, who will step down June 30. Two longtime faculty members, Jan Boxill (Philosophy) and Vin Steponaitis (Anthropology), have agreed to run for this visible faculty leadership post.
The University Gazette this week ran profiles of both candidates, along with a Q&A in which they each discussed their vision and preparation for the role of Faculty Chair. You can read the fully story at: http://gazette.unc.edu/file.2.html
The faculty elections will be held April 13-22, 2011 via electronic ballot emailed to all members of the Voting Faculty.
Office of Faculty Governance invites you to meet the candidates in the 2011 Faculty Elections, April 7, 3:00 pm at Campus Y
Faculty elections season is now in full swing, and with our ballot nearly complete, our office invites all faculty to join us for the 2011 Candidate Meet and Greet on Thursday, April 7th, 2011 from 3:00-4:30 pm in the Anne Queen Room in the Campus Y building!
Drop in for some light refreshments, informal chatting with our candidates (including the candidates for Chair of the Faculty), and a chance to pick up a copy of your Voter Information Guide. If you have any questions, contact Kathryn Turner in the Office of Faculty Governance at Katie_turner@unc.edu. We look forward to seeing you!
Faculty members asked to complete brief Sakai survey in which you choose when to migrate!
You are invited to complete a brief five-question survey intended to help the university plan for the switch from Blackboard to Sakai. The survey will ask you to identify your preferred: (1) semester to begin teaching using Sakai and (2) method to learn to use Sakai. For more information and a link to the survey, please visit: http://tinyurl.com/prefs. If you are unable to log in, please submit a help request (choose "Sakai Support") or call 962-HELP to be added.
The survey closes April 11, 2011.
Final draft of the 2011 Academic Plan online; calls faculty the "irreducible ingredient for transformative student experiences"
The Provost's Office has released a final draft version of The Academic Plan 2011: Reach Carolina. The Plan outlines the challenges, opportunities, and recommendations for the university over the next ten years. Its Executive Summary notes that "the irreducible ingredient for transformative student experiences is our faculty. Carolina must make strategic investment in faculty a priority." Read more at the link above.
AAUP President to speak at Duke, April 8th
Cary Nelson, president of the American Association of University Professors (AAUP) will give a free public lecture, "How to Save the University, " on Friday, April 8, 2011 at 7pm in Richard White Lecture Hall at Duke University. The talk, which is part of the statewide annual meeting of the North Carolina State Conference of the AAUP, will address what we can do individually and collectively to save higher education. These steps involve reforming the campus, making common cause with all faculty, staff, and students — and increasing strategic public outreach. Open to the public; wine and hors d'oeuvres reception to follow. Sponsored by the North Carolina Conference of the AAUP (http://www.nc-aaup.org).
Call for Proposals: IAH Innovation Fund Deadline, April 8
The Institute for the Arts and Humanities (IAH), in partnership with the Office of the Vice Chancellor for Research and Economic Development and with support from the Hyde Family Foundations, announces the IAH Innovation Fund, a $100,000 fund for research and creative activities in the arts and humanities.
The Innovation Fund exists to support faculty work that falls within the broad outlines of the roadmap for innovation at UNC. It supports projects that venture beyond traditional practices in arts and humanities research and teaching. The IAH encourages projects, collaborative or individual, from faculty across the University as long as the work is within the presented guidelines.
All UNC fixed term, tenure-track and tenured faculty are eligible to apply as individuals or in collaboration with other faculty, staff, students, community partners and/or professionals as long as the work has relevance to arts and humanities teaching and/or practice. While each project must be led by a UNC faculty member, the team may include members who are not affiliated with UNC. The IAH encourages faculty applying for proposals to collaborate across and beyond campus.
Full information is available at http://iah.unc.edu/innovation/cfp. Deadline: April 8, 2011, and winners will be notified by May 20, 2011.
Upcoming Trainings:
Virtual Technology Training (Elluminate, Chat, Phone, etc.)
Would you like help with websites, blackboard, Sakai, Word, Powerpoint, or some other software? Every Wednesday from 1-4 pm, OASIS offers Virtual Instructional Technology Training! Learn more: http://oasis.unc.edu/get-help/
Sakai Informational Meetings
Monday, April 4, 10am, Peabody Hall 08; Monday, April 18, 1:00 pm, Toy Lounge, Dey Hall
These session will give a brief overview of Sakai, present the migration timeline and support processes and invite questions, suggestions and ideas. To learn more about this and upcoming information sessions, please visit http://sakai.unc.edu/.
Faculty Governance reading room
Articles, books, reports, or other resources of interest to faculty. This week's selections:
"Gains, Drawbacks, for Female Professors" (New York Times, 21 March 2011). Article discusses new "Report on the Status of Women Faculty in the Schools of Science and Engineering at MIT, 2011" just released.
"'Academic Freedom' Offers Little Protection Against New Efforts to Obtain Professors' E-Mails" (Chronicle of Higher Education, 29 March 2011). Article discusses issues emerging from recent efforts by conservative-leaning groups to obtain emails of Michigan and Wisconsin public-university faculty members, including the President of the American Historical Association, William Cronon.
About Faculty Governance News
The Faculty Governance News is published approximately every two weeks throughout the academic year, and approximately monthly during the summer, by the Office of Faculty Governance. Information to be considered for inclusion should be sent to Anne Whisnant (anne_whisnant@unc.edu) on Monday before an issue is scheduled to appear.
2022-23 Newsletters


Telia was the first company to install NetClean ProActive on its company network.
A few years later, the company also took the step as an Internet service provider to block CSAI sites. "We must accept our social responsibility," says Marie Ehrling, Chairman of the Board at Telia.
Marie Ehrling first came into contact with NetClean during her time as CEO of TeliaSonera Sweden. In the NetClean ProActive program, management at Telia recognised an opportunity to introduce protection against child sexual abuse images (CSAI) in its network without needing to make the decision itself on what was right or wrong.
"There's a deep-rooted resistance to anything that restricts, and the unique feature of NetClean ProActive was that we as a company didn't need to adopt a position. That was done by a system that had been developed together with the police and other authorities," says Marie Ehrling.
She recounts that when management at Telia decided in 2005 to introduce ProActive, there was a high level of understanding in the organisation.
Three years later Telia also introduced NetClean Whitebox, which helps Internet service providers to block sites containing CSAI. This was a big decision, as it concerns how customers use the company's network. According to Marie Ehrling, blocking content is a sensitive issue, and Telia's basic position is that it should be free of regulation.
She points out that even if the Internet has meant a lot for developments over the last 10-15 years, it's also important to be aware of its negative effects.
Marie Ehrling has been back at TeliaSonera since this spring, as Chairman of the Board. She's proud that Telia was the first company to introduce protection against CSAI, both internally and in its external networks, and that the company is a good role model for the industry.


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text:
\section{Introduction}
	\label{intro}

	The study of relativistic collisions of heavy ions at various beam energies provides a unique tool to study the fundamental properties of strongly interacting matter in different regions of the QCD phase diagram \cite{Busza:2018rrf}. Some of these regions may be accessed with current and future facilities dedicated to the experimental realization of heavy-ion collisions (HICs). At low to intermediate beam energies these include the HADES experiment at the Facility for Antiproton and Ion Research (FAIR) \cite{Wilczek:2010ae} or the NICA experiment at the Joint Institute for Nuclear Research (JINR) \cite{article}, as well as the Beam Energy Scan program by the Relativistic Heavy Ion Collider (RHIC). The low energy regime is well known to be dominated by hadronic interactions and, therefore, it is successfully described by transport approaches that consider hadronic degrees of freedom \cite{Weil:2016zrk, Buss:2011mx, EHEHALT1996449, Nara:1999dz, Bass:1998ca}.

	In this range of collisional energies, the experimental detection of a non-vanishing polarization of $\Lambda$ hyperons lead to the breakthrough discovery that the medium created during heavy-ion collisions has a strong vortical structure \cite{Karpenko:2017lyj,Jiang:2016woz,Becattini:2015ska,McInnes:2018ibt,HADES:2022enx}. This polarization is induced by the spin-orbit coupling of the hyperons to the non-zero local rotation, the so called vorticity \cite{Liang:PolarizedQGP,Gao:2007bc,Betz:Polarization}.
	This can be directly thought to be a consequence of the initial configuration of the ions, which travel close to the speed of light generally with a non-vanishing offset distance, the so-called impact parameter. This initial condition grants the system a large amount of initial orbital angular momentum. For example, an AuAu collision at $\sqrt{s_{\rm NN}} = 39 \text{ GeV}$ and an impact parameter of $b=5$ fm carries an initial angular momentum of $|L_0| \sim A\,b\sqrt{s_{\rm NN}}/2\sim 2 \times 10^5\hbar$, where $A$ denotes the atomic mass number.
	As the early out-of-equilibrium medium created by the collision evolves, such large global angular momentum is rapidly broken down into smaller rotational domains, which can eventually be described in the hydrodynamical limit by vorticity.

	While the total angular momentum is fully conserved and it scales almost linearly with the energy of the collision, its deposition in the interacting region exhibits a more complex behavior. As the energy increases, the relative deposition of angular momentum into the medium is reduced, making the nuclei more transparent \cite{Becattini_2008}. There is therefore a maximum angular momentum deposition to energy ratio, which can be traced to be within the low-to-intermediate energy regime. This argument is supported by the energy dependence of the measurements of the $\Lambda$ hyperon polarization, where the total polarization signal decreases with the collision energy \cite{STAR:2017ckg}. Understanding the dynamics of angular momentum at intermediate beam energies is not only important to guide experimental programs in selecting systems and centralities for the deeper understanding of observables related to angular momentum, but also provides constraints on the dynamical evolution itself. Well understood dynamical approaches are the basis for the future solid identification of phase transition signals.

	In this work we investigate the dynamical deposition of angular momentum into the medium using the hadronic transport approach SMASH \cite{Weil:2016zrk,SMASHweb}. This grants us the possibility to access the out-of-equilibrium nature of the deposition of energy and angular momentum in the initial stages of a heavy-ion collision. Even though purely hadronic dynamics is restricted to low beam energies, we can use a hadron-string approach at higher beam energies. This renders the full approach valid for a large range of collisional energies, opening the window to study the energy dependence of angular momentum. Additionally, this kinetic approach allows us to build on previous geometric studies \cite{Becattini_2008} by not only being able to assess the conversion of initial angular momentum to the medium, but also to resolve the evolution of angular momentum with time.

	This work is organized as follows: In section \ref{sec:model} we briefly review the hadronic transport model SMASH, the basics of angular momentum transfer, as well as giving the definitions we use to quantify the in-medium angular momentum. In section \ref{sec:results} we present the results of the study, where we explore and discuss the impact parameter, energy and system size dependence of the deposited angular momentum. We also discuss the evolution of angular momentum, total and in-medium. As it is widely known \cite{sym13101852,Cheng_2002,Kodama:Causality,Zhang:Causality}, angular momentum conservation is broken in transport approaches. However, we not only show that the local broken angular momentum conservation has only a minor impact on the overall evolution of angular momentum, but also that our results display a good qualitative agreement with theoretical predictions and experimental data. Finally we present a short summary and outlook.

	\section{Angular momentum in SMASH}
	\label{sec:model}

	In this work, the model applied to study angular momentum transfer in heavy-ion collisions is the hadronic transport approach SMASH in version 2.0 \cite{Weil:2016zrk, SMASHweb}, which has been shown to be successful in the description of particle production in numerous setups \cite{Weil:2016zrk,Staudenmaier:2020xqr,Mohs:2019iee,Steinberg:2019wgm}. It provides the full phase-space evolution of every particle by providing an effective solution of the relativistic Boltzmann equation
	\begin{equation}\label{Boltzmann Equation}
		p^\mu \partial_\mu f_i(x,p)+m_i F^\alpha\partial^p_\alpha f_i(x,p) = C^i_\text{coll}
	\end{equation}
	in the non-equilibrium dynamics regime, where $C^i_\text{coll}$ denotes the collision term, $F^\alpha$ is an external force acting on each particle species $i$ with mass $m_i$ and its corresponding single particle distribution $f_i(x,p)$.
	The relevant degrees of freedom in SMASH include most of the well-established hadrons and hadronic resonances listed in the Particle Data Group \cite{Zyla:2020zbs}, up to a mass of $m\approx 2.3\,\text{GeV}$. In SMASH, resonances are treated with their vacuum spectral functions according to a Breit-Wigner distribution with mass-dependent widths following the Manley-Saleski ansatz \cite{Manley:1992}. The interface to high-energy hadronic interactions, by means of hard scattering processes and string fragmentation, is realized within the string model Pythia 8 \cite{Sjostrand:2006za,Sjostrand:2007gs}. A detailed overview of our approach including a complete list of incorporated degrees of freedom can be found in Ref. \cite{Weil:2016zrk}.

	At the basis of each interaction is the collision search based on the total cross-sections. The geometric collision criterion, as it is employed in the UrQMD (Ultra-relativistic Quantum Molecular Dynamics) approach \cite{Bass:1998ca,Bleicher:1999xi} is based upon determining the transverse distance of closest approach $d_T$ between two incoming particles. If $d_T$ undershoots a threshold distance $d_{int}$,
	\begin{equation}\label{collision criterion}
		d_T<d_{int}=\sqrt{\frac{\sigma}{\pi}}\, ,
	\end{equation}
	given by a geometrical interpretation of the corresponding total cross-sections, the particles collide. In this work we apply a modified version of the geometric collision criterion in a covariant formulation, as presented in Ref. \cite{Hirano:2012yy}.
	Eq. (\ref{collision criterion}) is responsible for the well-known broken angular momentum conservation in transport approaches, as it encodes an immediate finite range interaction which breaks Poincaré invariance \cite{sym13101852,Cheng_2002,Kodama:Causality,Zhang:Causality}. As a direct consequence, angular momentum cannot be conserved locally. However, the concept of test particles provides us with a tool to restore locality and remedy angular momentum conservation in the limit $N_{\rm test}\rightarrow \infty$.

	SMASH applies the test particle method, which means that cross-sections $\sigma$ and initial particle number $N$ are scaled as
	\begin{align}\label{test_particle_method}
		N &\rightarrow N_{\text{test}} N\\
		\sigma &\rightarrow N^{-1}_{\text{test}} \sigma \label{testparticle_sigma_scaling}
	\end{align}
	while keeping the scattering rate fixed. The factor $N_{\text{test}} $ thereby defines the number of test particles. Increasing N has two effects in particular. On the one hand, the cross-sections are decreased, which causes interactions to become more local and suppresses non-conservation of angular momentum. The corresponding increase of particle number results in a significant increase in computational time. For the following considerations, a test particle number of $N_{\text{test}}=20$ is chosen as a compromise between relevance for the results and computational time.

	Furthermore, to simulate nucleus-nucleus collisions, it is necessary to define initial conditions for the phase-space distributions of the initial nuclei. In coordinate space, spherical nuclei (e.g. gold) are sampled with nucleons according to a Woods-Saxon profile \cite{Woods:1954}.\\
	The momentum space distribution of the nuclear ground state, on the other hand, gives rise of the so-called Fermi motion. This distribution is reflected in a uniformly filled sphere in momentum space, also known as Fermi sphere, with radius
	\begin{equation}\label{Fermi Radius}
		p_F(\textbf{r})=\hbar\,c\left(3\pi^2 \rho(\textbf{r}) \right)^{1/3}\,,
	\end{equation}
	where $\rho(\textbf{r})$ is the spatial nucleon density at the point $\textbf{r}$. The Fermi momentum will typically be of order $p_F\approx 300\,\text{MeV}$ which corresponds to an excess kinetic energy of roughly $p_F^2/2m_N \sim 45\, \text{MeV}$. Even though the energy contribution originating from Fermi momenta is comparably small, for low beam energy setups it is important to take it into account as it gives a non-negligible contribution to the transverse mass spectra. In this work, we apply the frozen Fermi approximation in which Fermi momenta are neglected during propagation and the additional momentum is only considered for the collisions. The Fermi motion contributes to the total angular momentum of the system as will be shown in the following.\\

	To study the evolution of angular momentum in heavy-ion collisions, the relevant quantities are the initial angular momentum $L_0$, defined as the total angular momentum $L_{\text{tot}}$ of all nucleons at time $t<0\,\text{fm}$, and the final angular momentum $L_f$ at a time when no secondary collisions occur any more. Unless stated otherwise, we choose the final time to be $t_F=200\,\text{fm}$. To investigate which fraction of the initial angular momentum is transferred to the fireball, we further distinguish between the remaining angular momentum $L_r$ in the interaction medium carried by the participants and the contribution of spectators $L_{\text{sp}}$, such that

	\begin{equation}
		L_{\text{tot}}=L_{\text{r}}+L_{\text{sp}}\,.
	\end{equation}
	The generation of angular momentum in a heavy-ion collision is predominantly driven by the initial geometry of the collision setup which is dictated by the chosen impact parameter. In SMASH, nuclei are propagated along the z-axis while a non-zero impact parameter creates a relative offset between the nuclei centers in x-direction. Consequently, the main contribution of the orbital angular momentum points in the y-direction of the computational frame and all other components are negligible for qualitative analysis.
	\begin{figure}[t]
		\centering
		\includegraphics[width=0.52\textwidth]{figures/L_of_b_sqrtsnn8_7/lyAuAu8_7Fr_binned_analyt.pdf}
		\caption{Angular momentum as a function of impact parameter for AuAu collisions at $\sqrt{s_{\rm NN}}= 8.7$ GeV. Shown is the angular momentum of the participants, spectators, the total value and the analytical approximation of the total angular momentum.}
		\label{fig:total_spec87}
	\end{figure}

	\begin{figure*}[t]
		\centering
		\includegraphics[width=0.342\textwidth]{figures/Lr_of_b/2_4_Lr/lyAuAu2_4FrOffTest_binned.pdf}\hspace{-10pt}
		\includegraphics[width=0.342\textwidth]{figures/Lr_of_b/8_7_Lr/lyAuAu8_7FrOffTest_binned.pdf}\hspace{-10pt}
		\includegraphics[width=0.342\textwidth]{figures/Lr_of_b/200_Lr/lyAuAu200FrOffTest_binned.pdf}
		\caption{Angular momentum as a function of impact parameter for AuAu collisions at $\sqrt{s_{\rm NN}}=2.41, 8.7$ and $200$ GeV within the fireball. Compared are three calculations with and without Fermi motion, as well as including 20 test particles depicted by the gray dashed line.}
		\label{fig:imp_energy}
	\end{figure*}

	We can estimate the behavior of the orbital angular momentum $L_y$ as function of the invariant mass $\sqrt{s}$ by considering two identical initial nuclei with 4-momenta $P=(\sqrt{s}/2, 0, 0, m \gamma v_z)^T$. The square of this 4-momentum then determines the z-component of the velocity and the $\gamma$-factor
	\begin{equation}
		v_z^2=1-\frac{4m^2}{s}\,, \qquad \gamma=\frac{\sqrt{s}}{2m}\,,
	\end{equation}
	where we used that for two identical nuclei $\sqrt{s}=2\gamma m$. For large energies, i.e. $s >> 4m^2$, the orbital angular momentum becomes a linear function in $\sqrt{s}$:
	\begin{equation}\label{L as function of sqrt(s)}
		L_y=-\frac{b \sqrt{s}}{2} \sqrt{1-\frac{4 m^2}{s}} \approx -\frac{b}{2} \sqrt{s}\,.
	\end{equation}
	This result provides us with an estimate against which we can test our results from the next section for plausibility.
	\section{Results for global angular momentum} \label{sec:results}
	Unless otherwise stated, the following results obey the convention that all plots show as default our findings for which the Fermi motion was turned off.

	\subsection{Impact parameter dependence}\label{subsec:results_impact_parameter}
	In this section, we study the orbital angular momentum of AuAu collisions for different centralities and energies, ranging from $\sqrt{s_{\rm NN}}=2.41\,\text{GeV}$ to $\sqrt{s_{\rm NN}}=200\,\text{GeV}$.

	In Fig. \ref{fig:total_spec87} we show our results for the angular momentum of an AuAu collision at $\sqrt{s_{\rm NN}}=8.7\, \text{GeV}$ as a function of the impact parameter including frozen Fermi motion.
	The blue and green curves show the angular momentum carried by participants and spectators, respectively. The total angular momentum, depicted by the red line, on the other hand, is compared to the dashed gray line, which shows the analytical estimate from Eq. (\ref{L as function of sqrt(s)}).
	Our findings for the fraction of angular momentum contained in the interaction region show a distinct maximum in mid-central collisions $b_{max}\approx 6.7\, \text{fm}$, while decreasing for even larger impact parameters until the angular momentum generation drops to zero beyond $b=17.0\text{ fm}$, where the nuclei no longer have an overlap on average. This result coincides with predictions by Becattini \textit{et al} \cite{Becattini_2008,Becattini_2020} that have shown the same qualitative behavior in a geometric Glauber model approach. The maximum of $L_r$ thereby indicates the configuration for which the orbital angular momentum in the impact area is largest and for which we therefore expect the strongest vorticity in the QGP \cite{Becattini_2008, Deng_2016,STAR:2017ckg}. Considering also spectators, the total angular momentum of the whole system, as expected, follows the linear behavior we predicted with Eq. (\ref{L as function of sqrt(s)}). In general, the global angular momentum has to be zero in central collisions due to symmetry arguments. It is then increasing for mid-central collisions due to the off-set of the nuclei that work like spinning a top, while going to peripheral collisions the interaction rate decreases and eventually no angular momentum is transferred anymore to the fireball.

	To understand the impact of Fermi motion on the remaining angular momentum in the medium, we compare calculations for AuAu collisions with and without frozen Fermi motion for different beam energies in Fig. \ref{fig:imp_energy}. Displayed as curves are fits to our calculations of the impact parameter dependence of the angular momentum of the participants. The blue curve shows the angular momentum of the system as function of the impact parameter when Fermi motion is turned off, while the dashed gray curve additionally includes $N_{\rm test}=20$ test particles. With the pink curve we show our results without test particles but taking Fermi motion into account. In general, the curves qualitatively show the same characteristic shape for all energies, i.e. for every beam energy we find a unique impact parameter $b_{max}$ for which $L_r$ reaches its maximum. As Fermi motion is incorporated by sampling additional momenta for each nucleon isotropically, it increases the deposited angular momentum of the system and therefore increases the orbital angular momentum. The pink curve lies above the blue curve for all values of $b$ and for all calculated beam energies, while the relative difference between both curves becomes smaller for higher beam energies as expected. Besides increasing the absolute value of angular momentum, Fermi motion also slightly shifts $b_{max}$ towards more peripheral collisions. Since in the frozen Fermi approximation Fermi momenta are considered in the moment of collision, they increase the momentum diffusion at the edge of the interaction region turning some spectators into participants and thus effectively increase the overlap area. In turn, the maximum impact parameter is shifted to slightly larger values.

	In contrast, with test particles that are incorporated to ensure conservation of angular momentum locally, we see that $b_{max}$ is pushed towards more central collisions. Following Eq. (\ref{testparticle_sigma_scaling}), the cross-sections inversely scale with $N_{\rm test}$ making interactions more local. The reduced interaction range has to be balanced by moving the nuclei closer to each other to recover the maximum angular momentum transfer. Overall the qualitative behavior and even the magnitude of angular momentum is only mildly affected at all beam energies.

	\subsection{Time evolution} \label{subsec:time_evolution}
	\begin{figure*}[t]
		\centering
		\includegraphics[width=0.342\textwidth]{figures/timedep/2_4_FMfr/ly_AuAu2_4timedev_b5_8.pdf}\hspace{-10pt}
		\includegraphics[width=0.342\textwidth]{figures/timedep/8_7_FMfr/ly_AuAu8_7timedev_b6_6.pdf}\hspace{-10pt}
		\includegraphics[width=0.342\textwidth]{figures/timedep/200_FMfr/ly_AuAu200timedev_b4_6.pdf}
		\caption{Time evolution of the angular momentum in AuAu collisions at $\sqrt{s_{\rm NN}}=2.4, 8.7$ and $200$ GeV including frozen Fermi motion. For each energy, the corresponding impact parameter was chosen such that it maximizes the angular momentum deposition in the interaction region. The dashed lines depict the result for the same simulations including 20 test particles.}
		\label{fig:time_evolution}
	\end{figure*}
	With each interaction of two or more nucleons, the orbital angular momentum of the initial state is dynamically transferred to the participants of the heavy-ion collision over time until all secondary collisions have ceased.
	In particular, this means that we expect a large deposition of angular momentum at times of highest interaction rates, which can be traced to the initial to very early collision stages for which a transport description is still valid. Although SMASH does not incorporate QGP formation, it is still relevant to understand how angular momentum is generated in initial hadronic interactions.\\
	Fig. \ref{fig:time_evolution} shows the time evolution of angular momentum in an AuAu collision with frozen Fermi motion at the impact parameter where the highest angular momentum transfer happens within the hadronic transport approach.
	As in Sec. \refeq{subsec:results_impact_parameter}, the red curve indicates the total angular momentum of the system, while the blue and green curves show the angular momentum evolution of participants and spectators, respectively. The dashed lines indicate our calculation with $N_{\rm test}=20$ test particles, where locality is restored approximately. Without test particles, we observe a loss of total angular momentum for each beam energy.

	The broken conservation does not have a single reason, but is an effect composed of two separate contributions:
	as stated in Sec. \ref{sec:model}, our hadronic transport approach is based upon a geometrical interpretation of cross-sections as a maximum threshold for performing an interaction between incoming particles. Such an immediate finite range interaction breaks Poincaré invariance in binary interactions locally. Therefore, it also violates angular momentum conservation which can be seen from the kink in the total angular momentum and the subsequent undershooting during evolution \cite{Cheng_2002}. If test particles are added, the picture changes considerably. The time evolution of the angular momentum in Fig. \ref{fig:time_evolution} shows that the test particle method improves the non-conservation of angular momentum already for 20 test particles by correcting the participant contribution significantly, while the spectator's evolution stays nearly unchanged within error bars. This is particularly evident at early collision times, for which the initial kink is clearly smoothed out. We find that the non-conservation is purely driven by the participant evolution, which is consistent with our previous statement that the geometrical interpretation of cross-sections in binary interactions induces a spurious contribution to the angular momentum.
	\begin{figure}[t]
		\centering
		\includegraphics[width=0.52\textwidth]{figures/b_max/bmaxLog_yaxis0to10.pdf}
		\caption{Impact parameter at which transfer of angular momentum is maximal as a function of the beam energy in AuAu collisions. Shown is the angular momentum of the participants with frozen Fermi motion and without Fermi motion. Additionally, the dashed line shows our results taking into account 20 test particles while Fermi motion is turned off.}
		\label{fig:energy_dep}
	\end{figure}
	However, especially for small beam energies as in the leftmost plot of Fig. \ref{fig:time_evolution}, we observe that the conservation of angular momentum can only be improved to a certain extent with the test particle method and a residual contribution exists that breaks the conservation, which does not appear to originate from the non-locality of binary interactions. This part is due to the frozen Fermi approach. With frozen Fermi motion, Fermi momenta are neglected for initial propagation of the nuclei and are considered only for interactions. This treatment leads to a discontinuity in the nucleon momenta, which consequently also contributes to the violation of angular momentum conservation. Accordingly, if this assertion is true, the angular momentum of the system must be conserved if, in addition to the test particle method, Fermi momenta are either neglected (off) or considered for the entire evolution, including initial propagation (on). Our statement is supported by Fig. \ref{fig:time_evolution_fermi_motion}. Here, similar to Fig. \ref{fig:time_evolution}, we show the angular momentum evolution of on AuAu collision at $\sqrt{s_{\rm NN}}=2.41\text{ GeV}$ with (dashed lines) and without test particles (solid lines). In each plot we applied Fermi motion in a different approach (frozen, off, on). As claimed earlier, we observe that conservation of angular momentum can be fully recovered with test particles if Fermi momenta are either neglected or considered throughout the whole evolution, starting from the initial state.
	In general, we find that the impact of broken conservation on the global behavior is not relevant for medium to high beam energies even without test particles. Nevertheless, as a conclusion, we can define optimal configurations for angular momentum studies in transport approaches.
	\begin{figure*}[t]
		\centering
		\includegraphics[width=0.342\textwidth]{figures/timedep/2_4_FermiMotion/FMfr_testparticles100/ly_AuAu2_41_fermi_frozen.pdf}\hspace{-10pt}
		\includegraphics[width=0.342\textwidth]{figures/timedep/2_4_FermiMotion/FMoff_testparticles100/ly_AuAu2_41_fermi_off.pdf}\hspace{-10pt}
		\includegraphics[width=0.342\textwidth]{figures/timedep/2_4_FermiMotion/FMon_testparticles100/ly_AuAu2_41_fermi_on.pdf}
		\caption{Time evolution of the angular momentum in AuAu collisions at $\sqrt{s_{\rm NN}}=2.41$ GeV. Compared are three different approaches for Fermi motion (frozen, off, on)
			The dashed lines depict the result for the same simulations including 100 test particles. It can be seen that the violation of angular momentum has a contribution originating solely from the frozen Fermi approach.}
		\label{fig:time_evolution_fermi_motion}
	\end{figure*}
	In the low energy range, the test particle method in combination with Fermi motion taken into account over the entire evolution has proven to be the optimum in our studies. In this setup, however, potentials need to be taken into account to prevent the nuclei from flying apart.
	For medium to high beam energies, on the other hand, we see that the violation of angular momentum conservation predominately arises from the non-locality of the binary interactions and is thus remedied by the test particle method alone, while the contribution from the frozen Fermi approach is negligible.
	\subsection{Energy and system size dependence}
	\begin{figure}[t]
		\centering
		\includegraphics[width=0.52\textwidth]{figures/system_size/syssizedepRatio.pdf}
		\caption{Ratio of the transferred angular momentum to the initial value as a function of system size and beam energy for two different fixed impact parameters.}
		\label{fig:system_size}
	\end{figure}
	From Fig. \ref{fig:imp_energy} we already concluded that we expect a single impact parameter that maximizes the angular momentum transfer at a given beam energy. However, we also want to understand whether such a maximum impact parameter is a generic characteristic that only depends on the structure of the initial state or if it changes as a function of the beam energy.
	Therefore, we extract for each simulated beam energy, i.e. $\sqrt{s_{\rm NN}}=\left\lbrace 2.41, \,3.0, \,8.7, \,39.0, \,120.0,\, 200.0\right\rbrace \, \text{GeV}$, the corresponding $b_{max}$ and plot it as function of $\sqrt{s_{\rm NN}}$, as seen in Fig. \ref{fig:energy_dep}. The green and yellow curve depict our findings for the maximum impact parameter with Fermi motion and without, respectively, while the dashed gray line represents our findings without Fermi motion and including 20 test particles. Our simulations show that the impact parameter of maximum angular momentum transfer depends weakly on the beam energy, precisely it varies within a range of $b_{max}\in \left[ 4.3\, \text{fm}, 6.2\, \text{fm}\right]$ without Fermi motion and $b_{max}\in \left[ 4.6\, \text{fm}, 6.6\, \text{fm}\right]$ including frozen Fermi motion.
	As already stated in Sec. \ref{subsec:results_impact_parameter}, also Fig. \ref{fig:energy_dep} reinforces our observation that Fermi motion shifts the point of maximum angular momentum transfer towards slightly more peripheral collisions.
	On the other hand, the curve for test particles consistently lies slightly below those without test particles, as we have also already seen in Sec. \ref{subsec:results_impact_parameter} due to the reduced cross-sections of the nucleons.\\
	Another quantity that determines the deposition of angular momentum in the fireball is the system size. In Fig. \ref{fig:system_size} we show our results for the system size dependence of the relative angular momentum transfer at mid-rapidity for different sets of fixed beam energies and impact parameters. To obtain Fig. \ref{fig:system_size}, we simulate a heavy-ion collision for nuclei with varying nucleon number in the range of $A = 16$ $(^{16}_8O)$ to $A = 208$ $(^{208}_{82}Pb)$. For each event we choose every combination between $\sqrt{s_{\rm NN}}={8.7\text{ GeV}, 200.0\text{ GeV}}$ and $b={2.0\text{ fm}, 6.0\text{ fm}}$. We calculate the relative transfer by normalizing the participant angular momentum to the angular momentum of the initial state.
	Thereby, the solid lines belong to our results for $\sqrt{s_{\rm NN}}=8.7\text{ GeV}$ and the dashed lines depict the case of $\sqrt{s_{\rm NN}}=200.0\text{ GeV}$.
	Although one might make the intuitive assumption that the deposition of angular momentum increases at higher beam energies due to the higher particle production and interaction rate, we see a clear trend towards lower beam energies and more central collisions for a higher relative angular momentum transfer. \\
	This result sets an important orientation marker to guide future experiments in the choice of systems and centralities, with the aim of identifying potential signals of a phase transition.

	\section{Conclusions}
	\label{sec:conclusions}
	The evolution and transfer of angular momentum in heavy-ion collisions has been studied applying the hadronic transport approach SMASH. It was shown that the angular momentum of the fireball exhibits a distinct maximum for one unique impact parameter which is, furthermore, found to be a system specific parameter that is approximately beam energy independent. This is consistent with Glauber model predictions by Becattini \textit{et al} \cite{Becattini_2008}. System size studies at mid-rapidity suggest that the relative transfer and deposition of angular momentum in the interaction volume is larger for lower beam energies and in more central collisions. This observation is made equally for all studied nucleus sizes.
	Furthermore, our results show that the impact of the non-conservation of angular momentum due to Poincaré violations originating from the geometrical interpretation of cross-sections and the frozen Fermi approach are insignificant, especially in the medium to high beam energy regime.
	However, in order to restore locality fully, we applied the test particle method as a simple tool to guaranty angular momentum conservation in the limit $N_\text{test}\rightarrow\infty$. Even though finite Fermi momenta increase the angular momentum at all beam energies, we found that they are most relevant for low beam energies as expected.
	Our results indicate under which conditions the highest transfer of angular momentum in a heavy-ion collisions is expected, which is relevant to guide experimental programs and help to identify possible signals of a phase-transition of hadronic matter by constraining the dynamical evolution. In the future, the determination of vorticity based on coarse-graining the transport evolution could be interesting to compare to experimental data for $\Lambda$ polarization.

	\begin{acknowledgments}
		This work was funded by the Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) – Project number 315477589 – TRR 211. Computational resources have been provided by the GreenCube at GSI. H.E. and N. S. acknowledge the support by the State of Hesse within the Research Cluster ELEMENTS (Project ID 500/10.006).
	\end{acknowledgments}

	\pagebreak

redpajama_set_name: RedPajamaArXiv


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text:
Poema Arcanvs post a music video for the song »Straits Of Devotion«
Chilean doom veterans Poema Arcanvs post a music video for »Straits Of Devotion«, taken from the upcoming album, »Stardust Solitude«, to be released on August 28th via Transcending Obscurity Records.
01. Stardust Solitude
02. Orphans
03. Haven
04. The Lighthouse Keeper
05. Straits Of Devotion
06. Pilgrim
07. Kingdom Of Ruins
08. Brave
Chilean doom metal band Poema Arcanvs have built up a legendary status over the years, having been around since the '90s to be precise and releasing one impressive album after the other. Inspired originally by the UK doom bands such as Paradise Lost, Anathama and My Dying Bride, they've forged a powerful, soulful sound which they have perfected over the years. »Stardust Solitude« is their sixth full length album where they take things to a different level, adding better dynamics and expanding the scope of the music. This is a beautiful album that unravels gracefully, revealing a wealth of variations and moods that few bands are able to create and sustain for the entire duration of the album. The more you listen to it, the more it entrances you with its gentle yet plaintive melodies and entreating vocals that remain with you like warnings from the other side. Dive into this immersive album and emerge a changed person, one rich with profound sensations and a more sentient outlook on life.


These fun mosaic blue leggings have cobalt blue swirls on them, faux button cuffs and a sweet little flower with a bow at one ankle. They pair great with the entire Fairies Believer Line. Made of 95% cotton and 5% spandex. Elastic waist for a comfortable fit. Imported.


S&OP is often pictured as a largely standard process; textbook S&OP starts with agreeing an unconstrained demand plan that is handed over to supply planning who need to ensure product availability. In case of important bottlenecks, the S&OP meeting is the final escalation step in the process, where all remaining imbalances should be resolved.
For many companies in the agribusiness this is only half the story, as they often have to deal with a supply side with very specific characteristics. Product or ingredient supply in agri often has limited responsiveness and in some cases high levels of uncertainty.
Let's for example take a look at harvest products, where supply volumes often have to be contracted long in advance. Volume or mix adjustments cannot be made afterwards, or only against significant costs. The actually harvested volumes and quality can deviate significantly from the contracted volumes though, impacting the company's ability to fulfil its originally anticipated demand plan.
Dairy products are another example where supply volumes often have to be fixed over longer periods of time. The contracted volumes may be driven by long term demand projections, but market circumstances will change whereas supply volumes remain fixed. The challenge that arises is how to still balance demand and supply.
The diversity in agribusiness is so high that there can be no standard S&OP process here either, even when making it specific to this segment. There is a common framework though, that will have to be detailed by the specific supply characteristics.
For the mid to long term, the planning process in most cases is driven by the "demand side"; strategic plans, projected market developments and shares, innovations, competitor activities, etc. In this phase, supply planning's objective is to enable the fulfilment of these demand plans. Many agribusiness companies reach a point in their planning horizons though where supply takes over. Demand planning still has a role, but supply volumes and qualities are more or less fixed now and therefore put serious constraints on what can an cannot be produced and sold.
Impact on S&OP: how to maximise value?
The limited short term supply responsiveness must have an impact on how S&OP is set-up. Somewhere in the process from long to mid to short term planning, the decision focus in S&OP has to change, from demand to supply driven. From: "how do we ensure sufficient supply to fulfil all demand?" to: "how can we get maximum value from the given supply volumes and mix?".
The levers that companies have to maximise value from the (more or less) fixed supply volumes are very different, and this will have to drive the way the S&OP process is designed. What are important phases in the planning horizon, what can and cannot be changed, what information do we need and which persons are required to take key decisions? Understanding these design parameters is essential when setting-up the S&OP process. A standard Demand-Supply-S&OP cycle therefore will not do in all but the simplest cases.
S&OP is a means to an end, not a textbook process that can be implemented as a commodity. It is a decision making process, and its design therefore should match the key decisions that it has to support.
The agribusiness has a number of specific characteristics, mainly on the supply side. A linear and demand driven process therefore will not meet all requirements here. Failing to recognise that companies operating in the agribusiness have to cope with very specific and inflexible supply volumes will lead to flawed S&OP processes. Pity, since a well-designed S&OP process can add huge value, specifically in agri!


text:
Dabang Delhi end home leg with a win after Sheykh and Mane's splendid show
Dabang Delhi K.C. fought off a strong second-half show by Tamil Thalaivas' captain Ajay Thakur to win their final home game 37-33 at the Thyagaraj Indoor Stadium in Delhi on Thursday. Thakur scored 14 raid points on the night but a combined effort by Meraj Sheykh and Vishal Mane took the home team to victory.
Much like the rest of their home leg matches, Dabang Delhi K.C. started the contest in an aggressive fashion, with their defence and raiders both performing well. Meraj Sheykh led the offence in this period as the only point Tamil Thalaivas managed in the first six minutes was through Chandran Ranjit's self out where he stepped into the lobby without a touch. This helped the home team open up a 5-1 lead in the contest.
Check out the photos from the match here.
Reduced to three men on the mat, Tamil Thalaivas kept the scoreboard ticking through bonus points but weren't able to avoid the All-Out as Sheykh reduced them to a solitary player on the mat before a Block by Vishal Mane gave the home side a 10-4 lead in the 10th minute.
Sukesh Hegde and Ajay Thakur then took on the responsibility of bringing Tamil Thalaivas back into the contest and were helped by the defence which put in a strong effort to hold down Sheykh, reducing the deficit to four points. However, a successful raid by Naveen Kumar brought momentum back on Dabang Delhi K.C.'s side and Mane's tackle to send Thakur to the bench helped then take a 5-point lead, going into halftime with the scores favouring them 16-11.
The second half saw Dabang Delhi K.C. increase their lead to six points by sending Thakur to the bench once again. Sheykh's three successive successful raids followed by an Athul MS self out helped Dabang Delhi K.C. inflict another All-Out on Tamil Thalaivas in the 8th minute to gain a sizeable 10-point lead at 27-17.
Dabang Delhi K.C. picked up the next three points in the contest before a combined effort by Ponparthiban Subramanian and Anil Kumar put Tamil Thalaivas on the board. Thakur's 2-point raid then brought Dabang Delhi K.C. down to three men on the mat before the Tamil Thalaivas captain helped his side inflict an All-Out and claw back into the game at 33-26. Tamil Thalaivas then rode that momentum to pick up the next three points of the contest. Thakur was spectacular in this phase as he continued scoring freely, reaching his Super 10 in the process and reducing Dabang Delhi K.C. to four men on the mat.
Visit the matchcentre to relive the contest here.
With a little more than a minute left on the clock, the score difference was down to four points when Dabang Delhi K.C. finally managed to send Thakur to the bench and pick up a Super Tackle in the process. That tackle sealed the match in their favour as they ran down the clock to win by a 4-point margin and become the only team so far to win five matches of their home leg.
Top Performers –
Best Raider: Meraj Sheykh (9 raid points)
Best Defender: Vishal Mane (5 tackle points)
Best Raider: Ajay Thakur (14 raid points)
Best Defender: Manjeet Chhillar (2 tackle points)
Tamil ThalaivasDelPro Kabaddi League Season 6, 2018NewsEnglish


text:
A Gnome-Rhône 14K Mistral Major egy 14-hengeres, léghűtéses kétkoszorús csillagmotor. Meghatározó csillagmotor volt a második világháború előtt és alatt. Többezres darabszámban épült, tucatnyi repülőtípusnál alkalmazták. Licenc alapján Európa számos országában és Japánban is gyártották. Magyarországon a Weiss Manfréd Acél- és Fémművek gyártotta WM K–14 típusnéven.

Története

Alkalmazás

Franciaország
Amiot 143
Aero A.102
Bloch MB.200
Bloch MB.210
Breguet 460
Breguet 521
Farman F.222
Loire 46 C1
Potez 62
Potez 651

Licenc alapján más országokban
Magyarország
WM–16 Budapest
WM–21 Sólyom
WM–23 Ezüst Nyíl
MÁVAG Héja
He 46
He 170
Ju 86K–2
SM.75

Lengyelország
PZL P.24

Németország
Me 323 Gigant

Olaszország
Breda Ba.65
Breda Ba.75
Breda Ba.88
Caproni Ca.135
Caproni Ca.161
CANT Z.1007
Piaggio P.XI
Reggiane Re.2000
Savoia-Marchetti S.M.79-II
Savoia-Marchetti S.M.84

Románia
IAR K.14
IAR.37
IAR 80

Svédország
Saab 17C

Szovjetunió
Polikarpov I–180
DB–3
Szu–2

Műszaki adatok (14 Kdrs)

Általános jellemzők
Típus: Tizennégy-hengeres, kétkoszorús, léghűtéses csillagmotor
Furat: 146 mm
Löket: 165 mm
Hengerűrtartalom: 38,72 l
Átmérő: 1296 mm
Száraz tömeg: 540 kg

Segédberendezések
Vezérmű: Alul vezérelt, felül szelepelt
Feltöltő: egyfokozatú centrifugális típusú turbófeltöltő
Üzemanyagrendszer: Stromberg karburátor
Üzemanyag: 87-es oktánszámú benzin
Hűtőrendszer: léghűtés
Reduktor áttéele: 2:3

Teljesítményadatok
743 kW (996 LE) 2390-es percenkénti fordulatszámon a felszállásnál
821 kW (1100 LE) 2390-es percenkénti fordulatszámon 2600 m-en
Fajlagos teljesítmény: 21,23 kW/l
Kompresszióviszony: 5,5:1
Fajlagos üzemanyagfogyasztás: 328 g/(k·•h)
Kenőolajfogyasztás: 20 g/(kW·h)
Teljesítmény-tömeg arány: 1,52 kW/kg

Források

Haditechnika folyóirat XX. évfolyam április-június
https://web.archive.org/web/20090324160448/http://base13.glasnet.ru/text/aviamotory/t.htm
Danel, Raymond és Cuny, Jean. L'AVIATION française de bombardement et de renseignement 1918-1940 Docavia n ° 12, Edition Larivière

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