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264 Faculty jobs
Browse for Faculty Jobs. Find the job of your dreams on IEEE today!
KENTECH Seeks Global Leaders in Energy Technology
Korea Institute of Energy Technology (KENTECH)
Naju City South Korea
Job Description: Korea Institute of Energy Technology (KENTECH) is seekin...
Assistant/Assosiate/Professor
The School of Engineering and Applied Science (SEAS) at Princeton University invites applications for a faculty position at the junior or senior level (Assistant, tenured Associate or Full Professor rank) in the broadly defined field of robotics. Applicants must hold a Ph.D. in engineering or a rela...
The School of Engineering and Applied Science (SEAS) at Princeton University invites applications for a faculty position at the junior or senior...
IT & Engineering
Teaching-track Faculty Position in Systems and Enterprises
The School of Systems and Enterprises (SSE) at Stevens Institute
Teaching-track Faculty Position in Systems and Enterprises The School of Systems and Enterprises (SSE) at Stevens Institute of Technology invites applications for a teaching-track faculty position, starting Spring 2022 or on a mutually agreed upon date. Successful candidates will contribute to a ...
Teaching-track Faculty Position in Systems and Enterprises The School of Systems and Enterprises (SSE) at Stevens Institute of Technology...
Lecturer Position, School of Systems and Enterprises
The School of Systems and Enterprises (SSE) at Stevens Institute of Technology
Lecturer Position, School of Systems and Enterprises The School of Systems and Enterprises (SSE) at Stevens Institute of Technology invites applications for a 9-month lecturer position, starting Spring 2022. Successful candidates will contribute to a dynamic and growing educational program in the...
Lecturer Position, School of Systems and Enterprises The School of Systems and Enterprises (SSE) at Stevens Institute of Technology invites...
Teaching-track Faculty Positions in Systems and Enterprises
Teaching-track Faculty Positions in Systems and Enterprises The School of Systems and Enterprises (SSE) at Stevens Institute of Technology invites applications for teaching-track faculty positions, starting Fall 2022 or on a mutually agreed upon date. Successful teaching faculty will contribute t...
Teaching-track Faculty Positions in Systems and Enterprises The School of Systems and Enterprises (SSE) at Stevens Institute of Technology...
Assistant Professor of Computer Science
Boston University Metropolitan College
Boston University's Metropolitan College seeks two dynamic and creative faculty members with expertise in data analytics or software development to join its nationally recognized Department of Computer Science (http://www.bu.edu/csmet/) at the rank of Assistant Professor starting July or September 1...
Boston University's Metropolitan College seeks two dynamic and creative faculty members with expertise in data analytics or software development...
Executive in Residence - Institute for Enterprise Engineering
The Institute for Enterprise Engineering in the Pratt School of Engineering at Duke University (Durham, NC) invites applications for a Non Regular Rank Executive in Residence position. The Pratt School of Engineering is seeking a director to lead and mange a new Master of Engineering degree track fo...
The Institute for Enterprise Engineering in the Pratt School of Engineering at Duke University (Durham, NC) invites applications for a Non Regular...
Assistant Professor / Associate Professor / Professor in Computer Science and Engineering Department
Ad Dawhah Qatar
Job Title: Assistant Professor / Associate Professor / Professor Position Start Date: July 2022 Position Summary The Computer Science and Engineering Department is seeking high-caliber candidates for multiple faculty positions at the levels of assistant, associate, and full professor. The applicant ...
Job Title: Assistant Professor / Associate Professor / Professor Position Start Date: July 2022 Position Summary The Computer Science and...
Assistant Professor, Tenure-Track Faculty Position in Electrical Engineering
Assistant Professor, Tenure-Track Faculty Position in Electrical Engineering Job Description Syracuse University's Department of Electrical Engineering and Computer Science (http://eecs.syr.edu) in the College of Engineering and Computer Science (https://eng-cs.syr.edu) invites applicants for a t...
Assistant Professor, Tenure-Track Faculty Position in Electrical Engineering Job Description Syracuse University's Department of Electrical...
The Department of Computer Science and Engineering at the South Dakota School of Mines & Technology invites applications for a full-time, 9-month, benefited, tenure-track position in Computer Science and Engineering with the anticipated start date of August 2022. A doctorate in Computer Scien...
The Department of Computer Science and Engineering at the South Dakota School of Mines & Technology invites applications for a full-time, 9-month,...
Divisional Dean, School of Computing
George Mason University College of Engineering and Computing Divisional Dean, School of Computing The School of Computing at George Mason University invites applications and nominations for the position of Divisional Dean. The Divisional Dean will play a critical leadership role in guiding the evo...
George Mason University College of Engineering and Computing Divisional Dean, School of Computing The School of Computing at George Mason...
Assistant Professor of Computer Science (2 positions – Cybersecurity and Computer Engineering)
Hempstead, New York
The Department of Computer Science at Hofstra University (www.hofstra.edu/compscience) invites applications for two anticipated tenure-track faculty positions at the Assistant Professor level to begin in Fall 2022. Strong candidates in all areas of computer science are welcome to apply. Faculty memb...
The Department of Computer Science at Hofstra University (www.hofstra.edu/compscience) invites applications for two anticipated tenure-track...
W3 PROFESSORSHIP FOR HUMAN-CENTERED SENSING
Bochum, Nordrhein-Westfalen Germany
Ruhr-Universität Bochum (RUB) is one of Germany's leading research universities, addressing the whole range of academic disciplines. A highly dynamic setting enables researchers and students to work across the traditional boundaries of academic subjects and faculties. To create knowledge networks wi...
Ruhr-Universität Bochum (RUB) is one of Germany's leading research universities, addressing the whole range of academic disciplines. A highly...
Professor of Practice - Mechanical Engineering Technology
Purdue University, School of Engineering Technology
Columbus, Indiana
The School of Engineering Technology at Purdue University invites applications for a full-time appointment at either the Assistant or Associate Professor of Practice level in the area of mechanical engineering technology. The Professor of Practice position is contractual non-tenure accruing, but ren...
The School of Engineering Technology at Purdue University invites applications for a full-time appointment at either the Assistant or Associate...
Assistant Teaching Professor - Industrial Engineering & Operations Research -M.Analytics-COE
Assistant Teaching Professor - Industrial Engineering & Operations Research -M.Analytics-COE Assistant Teaching Professor The DEPARTMENT OF INDUSTRIAL ENGINEERING & OPERATIONS RESEARCH (IEOR) at the University of California, Berkeley welcomes applications for a teaching assistant professor ...
Assistant Teaching Professor - Industrial Engineering & Operations Research -M.Analytics-COE Assistant Teaching Professor The DEPARTMENT OF...
Data Analytics Nuclear Threat Detection - Postdoctoral Researcher
We have an opening for a Postdoctoral Researcher to conduct research in nuclear nonproliferation, threat detection and analysis. You will participate in the development of new detection systems and algorithms, and also implementing these new technologies in actively deployed systems. The successful ...
We have an opening for a Postdoctoral Researcher to conduct research in nuclear nonproliferation, threat detection and analysis. You will...
Infrastructure & Climate Analysis - Postdoctoral Research Staff Member
We have multiple openings for highly qualified and motivated scientists and engineers to join us to solve critical climate change problems as a Postdoctoral Research Staff Member in Infrastructure & Climate Analysis. In this role, you will perform original research and participate in multidisciplina...
We have multiple openings for highly qualified and motivated scientists and engineers to join us to solve critical climate change problems as a...
Activity Leader
Branch Lead
Broadcast And Sound Engineering Technician
Communication Systems Engineer
Department Lead
Enterprise Engineer
ERP Analyst
GIS Engineer
Global Commodity Leader
City College Of New York
Department Of Mathematics And Computer Science, SDU
Embry-Riddle Aeronautical University
Faculty Of Computer Science, Dalhousie University
Idiap Research Institute And Ecole Polytechnique Fédérale De Lausanne
LSU Shreveport
Technical University Of Munich (TUM)
The Department Of Biomedical Engineering At The University Of Utah


SAP C_BOCR_11 exam is very popular in SAP field, many SAP candidates choose this exam to add their credentials. There are many resource online to offering SAP C_BOCR_11 exam questions, through many good feedbacks, we conclude that GreatExam can help you pass your test easily with SAP C_BOCR_11 exam questions. Choose GreatExam to get your SAP C_BOCR_11 certification.


The Maplesoft Elite Maintenance Program (EMP) is an annual subscription that provides upgrades to the latest release of Maplesoft products, ensuring that you are always working with the latest technology from Maplesoft.
Save money. Enjoy significant savings over the cost of buying upgrades at a later date.
Help your students. Provide your students with Maple discounts through the Maple Adoption Program, which is available only to EMP customers. As part of the Adoption Program, eligible instructors will also receive a free home-use copy of Maple.
Relax. Obtain new releases automatically, without having to place an order, or take any action at all.
Stay up to date. Remain current so you can always take advantage of the latest new features and product improvements as soon as they are available.
EMP is available for most Maplesoft products, including Maple, MapleSim, and MapleNet. One full year of EMP is included with your product purchase. At the end of that year, simply renew your membership to continue to enjoy the benefits of this program.
Renewing your EMP is the easiest and most cost effective way to keep your products up-to-date.
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The Brooke Owens Fellowship is a non-profit program in the United States that provides paid internships and executive mentorship for undergraduate women seeking a career in aviation or space exploration. The fellowship was created to honor the memory of Brooke Owens, a pilot and space policy expert who died of cancer at the age of 36.

Motivation and overview
The program looks to improve diversity within the aerospace industry. The program offers students paid summer internships at companies (including SpaceX, Avascent, Commercial Spaceflight Federation, Orbital ATK, Virgin Orbit, and Blue Origin), travel stipends and assigned mentors. It was created by Lori Garver, a former NASA deputy administrator, along with aerospace executives William Pomerantz (Virgin Orbit) and Cassie Kloberdanz Lee (Vulcan Inc.).

Fellows received two experienced aerospace mentors, one at their host industry, and another in an associated sector. Mentors include Lori Garver, Diana Trujillo, Charles Bolden, Pamela Melroy, Dava Newman, Danielle Wood, Emily Calandrelli, Will Pomerantz and Cassie Lee. The fellows are connected to a Fellowship class and an alumni network. The program is run with Future Space Leaders, and emphasises creativity. The annual Brooke Owens Fellowship conference happens during the Future Space Conference in Washington, D.C. Whilst the program is open to international students, some institutions can only host US citizens or green card holders.

The program's success has resulted in the creation of several spin-off fellowships, including the Patti Grace Smith Fellowship, Zed Factor Fellowship, and Zenith Canada Pathways Fellowship.

References

External links
Brooke Owens Fellowship

Fellowships
Science policy
Scholarships in the United States
Space industry
Internship programs
Charities based in Washington, D.C.
Organizations established in 2017
2017 establishments in Washington, D.C.

redpajama_set_name: RedPajamaWikipedia


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Q: Needing to count specific values on a report I have an unbound text box in the report footer with expression =Count(IIf([vwPetBreed]="Bichon Frise",1)) with a summary of count running on the report.
When I run the report I get a sum of the total of the report instead of just the couple that matches the criteria.
I have used =Sum(IIf()) as well only to get the total of all of them.
The only times I can get a different outcome is if:

*

*I change the summary to none, I will get on the report =Count(IIf(Boston Terrier="Bichon Frise",1)), or replace Boston Terrier with the breed of the last dog on the report.

*I change the summary to page, I will get "0"

*I change the summary to group, I will get "?"

redpajama_set_name: RedPajamaStackExchange


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Daugavpils Mark Rothko Art Centre Creative Industries Club
Daugavpils Mark Rothko Art Centre
About center
About Rothko
The collection of Daugavpils Mark Rothko Art Centre
Open-air art works
History of Arsenal
Prices for visiting
Conference sector
Residence rooms
The Basil Alkazzi Acquisition Fund established at the Mark Rothko Centre
At the end of 2018, Daugavpils Mark Rothko Art Centre signed a contract with Mr Basil Alkazzi, artist and patron of the arts from Monaco, regarding the establishment of The Basil Alkazzi Acquisition Fund at the Rothko Centre.
Nearly six years into existence, Daugavpils Mark Rothko Art Centre continues to work responsibly towards inclusion of local cultural processes into European and global trends and providing access to prime examples of professional art to inhabitants of Daugavpils and Latvia as well as to tourists from all over the world.
These activities of Daugavpils Mark Rothko Art Centre have been noticed by Basil Alkazzi, artist and patron of the arts and cultural institutions worldwide. By mutual agreement between the parties, a contract was signed regarding the establishment of The Basil Alkazzi Acquisition Fund at the Mark Rothko Art Centre with a view to enriching the centre's painting collection.
The purpose of The Basil Alkazzi Acquisition Fund is to provide financial support to emerging and established Latvian and international artists through the acquisition of their artwork for the Rothko Centre's painting collection. The artwork will be purchased in accordance with the Rothko Centre's strategy, which will include abstract, modern and contemporary art. Acquisitions will be selected at the discretion of the Rothko Centre's curators and artistic board with the advice of the centre's collection committee and decisions ratified by the director. Options will be considered to purchase additional artwork from artists already featured in the centre's collection, thereby giving a broader view of their creative style and enabling future loans of comprehensive assortments of artwork for major exhibitions in Latvia and abroad, which will boost the image of the Rothko Centre and Basil Alkazzi Acquisition Fund as major brands on the global art scene.
Apart from financial means, the British artist Basil Alkazzi has donated to Daugavpils Mark Rothko Art Centre some of his original artwork and a number of Limited Edition photographs by photographer Myoung-Cheul Chung (South Korea), which will add to the Rothko Centre's photography collection. Since 2016, Mr Alkazzi has also repeatedly donated valuable art-themed books to the Rothko Centre's library.
The recognition and support of Basil Alkazzi will help the Rothko Centre in pursuing its goals regarding the purchase of artwork, making it more competitive with contemporary art museums and galleries worldwide.
The acquisition fund will operate throughout 2019 and will constitute a major contribution to replenishing the Rothko Centre's painting collection. It will boost the centre's overall value with major works of art and perform an important social function by providing much needed financial support to artists, which is especially significant in Eastern Europe.
Copyright © Daugavpils Mark Rothko Art Centre 2016. All rights reserved. Design by LatInSoft.
We use cookies to provide you with a more convenient and safer user experience. By continuing the browsing session or clicking the "I Agree" button, you confirm that you agree to the use of cookies. You can revoke your consent at any time by changing your browser settings and deleting the cookies stored. Read moreI Agree

redpajama_set_name: RedPajamaCommonCrawl


One of the coolest new additions to My Tamagotchi Forever in the game's biggest update yet was a brand new character named Neliatchi. What makes this new Tamagotchi stand out isn't just her adorable appearance — she looks sort of like a mermaid, albeit without a tail, so maybe not all that much — but the fact that she was the result of a contest whose lucky winner got to help design the character. The contest ended back in January 2018, but Neliatchi didn't make it into the game until August. Mobile game updates definitely don't happen overnight!
Neliatchi is an adult Tamagotchi, and like the previous eight adult forms, she can be evolved from any of the game's six teen forms. The big question on everyone's mind, though, is the obvious one: How can you be sure you'll end up with the newest character?
As always, the answer is in the diet you feed your teen.
A pretty big hint to what to feed your teen to end up with a Neliatchi is in the character's bio. It states that she "enjoys snacks and green vegetables," and this is indeed what you should be looking to feed your teen.
While you can unlock a variety of snacks, most players who have already acquired Neliatchi report that french fries seem to be the way to go. They're available right away and cost 10 coins each. Hamburgers and pizza may also work for you.
As far as green vegetables go, you've got several options, but broccoli is your best bet if you haven't been playing My Tamagotchi Forever all that long. It only costs seven coins and you have it even when you first start the game. Other green veggies include cucumber (35 coins each, unlocks at level 14) and paksoi (56 coins, unlocks at level 22). None of the new food items to hit the game since the update are green vegetables, so they don't really figure into what we're discussing here.
How much of each kind of food should you feed a teen Tamagotchi? That's difficult to say with 100 percent certainty, but based on what has been proven to work with other adult forms, it seems smart to try for a 50/50 mix between green vegetables and snacks. This ratio has been pretty dependable throughout the game, and of the different adult forms, only Kuchipatchi seems to prefer only one type of food (though with a healthy appetite for plenty of what we would typically call junk food).
The other important tip to remember when attempting to evolve a Neliatchi is not to get discouraged if it doesn't happen on your first try. The veggies/snacks mix has definitely already paid off for other players, so just tinker with that basic formula a bit if necessary and you should get it to work before too long.
Good luck attaining a Neliatchi, as for some of you experienced My Tamagotchi Forever players, it may be the only character you haven't already come across. If you found this article useful, please check out our other guides, including our advanced tips and advice on how to play forever for free.


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Subject: Politics
'The President faces considerable constraints in domestic policy in comparison to the UK Prime Minister' Discuss.
'The President faces considerable constraints in domestic policy in comparison to the UK prime Minister' Discuss. To say that Clinton faced considerable constraints would be to recognise the setbacks he faced during his Presidency, in terms of sleaze and also in terms of his political agenda. Most infamously, Bill & Hilary's failed attempt to reform the healthcare system in 1993/4. Blair's 'Devolution Act 1997' -which was in essence a major constitutional change- was passed with startling simplicity especially when considered with the difficulty Clinton and countless other Presidents have faced in passing the simplest laws. The ways in which both Premiers are constrained must be considered in detail in order to make an effective comparison of the two systems. The constraints faced by the Prime Minister in passing legislation are minimal. With a large enough majority in parliament, a Prime Minister is able to pass the most constitutionally radical laws, (with a one-year delay from the House of Lords being the only formal threat to its passing.) In the USA, any legislative success is dependent almost entirely on congressional approval. The presidents has the solitary legislative power of veto, which is entirely negative, and even this can be overridden with 2/3rds majority in both houses. Law making in the UK is often dependent on the size of the government majority, which is -due to the First-Past-The-Post electoral system- often large. ...read more.
The president often also uses his cabinet to reward loyalty and repay political debts to people. The PM must also have a political and social balance the cabinet (e.g. Prescott and Short were the representatives for old labour ideal in Blair's cabinet,) and must pick an able Cabinet as they will have a job that is constantly in the public eye. A PM who does not include a variety of views in their cabinet can become isolated, as was seen towards the end of Thatcher's government in the late 1980s. If the PM has a small Majority then the amount of people a cabinet can be selected from is minimal. Both the President and the Prime Minister require Cabinet appointees to be ambitious and enthusiastic about the job, in the UK a dissident MP such as Dennis Skinner would not do Blair any good by having his in his Cabinet and in the US, congressmen simply do not see the job as cabinet minister to be important or desirable. The PM is more constrained than the President in terms of Cabinet appointees as there are much fewer people to choose from, however the UK and USA cabinets are very different in terms of domestic power and credence and so perhaps it is justified that the more important Cabinet is the harder to fill with incompetent ministers. ...read more.
This was seen as autocratic and so led to legislation being passed to prevent this from happening again. The PM has distinctly more power than the President in that he has a potentially unlimited time in office. This however, has some advantages as it means that a PM never has a 'lame-duck' period. The UK PM is less constrained than the US President in most matters of domestic policy, and it could be argued that the ones he is more constrained in because the issue is not as important in the US (e.g. the President's cabinet has much less authority and is much less accountable than the PM's cabinet and so the PM is justifiably more constrained in who he appoints into it.) Harry Truman said about the limits of presidential power. "I sit here all day trying to persuade people to do the things they ought to have the sense to do without me persuading them to. That's all the powers of the President amount to." The Prime Minister has whips and party discipline in order to keep people working without this degree of persuasion. The President does face considerably more constraints with regards to domestic policy than the Prime Minister, but the USA is also a considerably larger and more ethnically, socially and geographically diverse country to try to represent domestically without sufficient scrutiny and control than the UK. 1 NATHAN GRIFFIN, 13 LER- POLITICS 1 ...read more.
This student written piece of work is one of many that can be found in our AS and A Level United States section.
Related AS and A Level United States essays
Using examples, explain the limitations on the Supreme Courts powers.How do Presidents veto legislation, ...
from tyranny by establishing a series of 'checks and balances' amongst the President, Congress and the Supreme Court. Why, and to what extent, has there been disagreement about the constitutional importance of federalism? How do Presidents veto legislation, and how significant is the presidential veto?
How far does the president only have the power to pursuade
While these may indeed require Congressional approval, the Constitution actually states that Congress must only object if the nominee is truly not fit for the job, and not on the basis of ideological preference. For example many Republican members of Congress were criticised for opposing the nomination of Elena Kegan
US pressures groups are undemocratic, discuss
As result, people claim that pressure groups are not merely there to cause injustice but to exert justice into the political world. Groups can also enhance the two fundamental rights of freedom of speech and freedom of association. In a country like the Unites States, with a participatory tradition and
Difference in the Prime Minister and President
As a result, the whip is a vital tool for the PM. The PM's power of patronage (ability to appoint/dismiss ministers). Members of parliament usually vote along party lines because they know that their careers depend to a large extent on their loyalty to the government and ultimately the Prime Minister.
The power of the President is limited to the power to persuade. Discuss.
drafted by Woodrow Wilson, but never signed by the United States because of a lack of support in Congress. The Supreme Court also exercises an effective check of Presidential power by declaring acts of the President unconstitutional, perhaps most notably in the case of United States v Nixon.
Critically analyse the appointment and confirmation process for nominees in the US Supreme Court
It allows them to place political allies and sympathisers in another branch of the federal government?[5]. This trait is evident it federal courts too as 93% of Lyndon Johnsons appointments to federal judgeships were Democrats, where was 93% of Richard Nixon?s were Republican[6].
Ethnic minorities in the USA
This is because the USA has so many huge problems to face at the moment. In foreign policy the war in Afghanistan (& Iraq) is unpopular with many Americans. Possibly even more difficult are the problems the US economy is facing due to the world recession which has cost millions
How far do you agree the USA remains a global hegemony today?
Total GDP in 2001 was almost as much as the combined total of the next six top GDP countries in the world. The next closest state was Japan with less than half the GDP of the United States. From 1990 until the end of 2001, real gross domestic product rose from $6,707.9 billion to $10,171.4 billion.
Looking for expert help with your Politics work?
Why has reforming campaign finance been difficult?


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Real name : Kevin David Sorbo
Place of birth : Motley
Date of birth : 24/09/1958
Sorbo Kevin
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Kevin Sorbo (1958)
Kevin David Sorbo
Kevin David Sorbo is an American actor best known for the roles of Hercules in Hercules: The Legendary Journeys, Captain Dylan Hunt in Andromeda and Kull in Kull the Conqueror.
Sorbo was born in Mound, Minnesota, where he attended Mound Westonka High School. He is the son of Ardis, a nurse, and Lynn Sorbo, a junior high school mathematics and biology teacher. He is of Norwegian descent and was raised in a Lutheran family. Sorbo attended Minnesota State University Moorhead and worked as a model for print and television advertising in the 1980s.
Sorbo started his acting career in the late 1980s making guest appearances in several television series such as 1st & Ten, Murder She Wrote and The Commish. He was considered for and lost out to Dean Cain as Superman in Lois and Clark: The New Adventures of Superman and was a possible contender for the role of Agent Mulder in The X Files which went to David Duchovny.
In 1994, he shot to fame when he played the role of Hercules in the television film Hercules and the Amazon Women. This was the first in a series of television films that served as pilots for the TV series Hercules: The Legendary Journeys, which ran from 1995 to 1999.
Sorbo also guest-starred as Hercules in episodes of the 1995-2001 spin-off series Xena: Warrior Princess and provided the voice of Hercules in the 1998 direct-to-video animated film Hercules and Xena - The Animated Movie: The Battle for Mount Olympus.
Other voice-over work followed, with Sorbo providing the voices of Reiko and Quan Chi in the 1997 video game Mortal Kombat 4. In between the years playing Hercules, he played his first leading film role in Kull the Conqueror .
In 1997, while on a publicity tour for Kull the Conqueror and between the 4th and 5th seasons of Hercules, Sorbo experienced an aneurysm in his shoulder, which led to three strokes. As a result, he was weakened for the next several years, a condition that he and the producers of Hercules kept secret from the public. During the last two seasons of Hercules, the 5th and 6th, which aired in 1998 and 1999, Sorbo was given a reduced filming schedule to accommodate his condition, and more guest stars were brought in.
After Hercules came to an end, Sorbo played the starring role of Captain Dylan Hunt in the science-fiction drama series Andromeda from 2000 to 2005. In 2006, he played a recurring role on the final season of The O.C and guest-starred in the sitcom Two and a Half Men. In 2007, he starred in the direct-to-video film Walking Tall: The Payback, which was a sequel to the 2004 film Walking Tall. He reprised his role in the second sequel, Walking Tall: Lone Justice which released later that year. He also starred in the Lifetime Channel film Last Chance Café, the Hallmark Channel film Avenging Angel, co-starring his real life wife Sam Jenkins and guest starred as a bounty hunter in the season-two episode "Bounty Hunters!" of the series Psych. He appeared in the 2008 spoof film Meet the Spartans, which was a box office success despite being universally negatively reviewed by critics. He starred in the Albert Pyun directed SciFi Vampire flick Tales of the Ancient Empire.
Sorbo voiced one of the main protagonists, Prometheus, in the Wii First Person Shooter video game, The Conduit.
Sorbo returned to the role of Hercules, albeit in a more sinister portrayal, in the video game God of War III released for the PlayStation 3 in March 2010.
Sorbo married actress Sam Jenkins, whom he met when she had a guest role on Hercules, on January 5, 1998. Sorbo is the spokesman and chair of A World Fit For Kids! (AWFFK!), a non-profit organization that trains teenagers to become mentors to younger children.
Played movies
Wog Boy 2: Kings of Mykonos
Bitch Slap
Fire from Below
Prairie Fever
Meet the Spartans
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1ª temporada de Xena: Warrior Princess
Wolf Canyon
TV show season
Hercules: The Legendary Journeys (season 6)
Andrómeda (season 5)
TV show episode
War Bride
Two Men and a Baby
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With work in Brazil, if you want your job application to be taken seriously you have to consider all national differences. The work in Brazil require more than just the obvious Brazil cover letter with Brazil CV writing and translation - they require careful preparation.
Expatriates wishing to work in Brazil should find a job prior to their departure as the job market and regulations for foreign employees offer only limited job opportunities for expatriates in Brazil.
You will be confronted with problems that in all probability did not even cross your mind when you decided to start employment in Brazil. Do not take too lightly the influence the work in Brazil can have on the result of your adventure! For example, you will experience the unfamiliar immigration rules and practices, strange job application procedures, bizarre job selection trends and weird management culture.
Brazil is one of the fastest growing economies in the world, however has high unemployment (particularly for ages 15-24: male: 13.9%, female: 23.1%), and visitors who enter the country as tourists are not legally allowed to take jobs.
Working without an appropriate visa is illegal. If caught, you may be subject to imprisonment, a fine and/or deportation. You may also be barred from re-entry to Brazil.
As a Brazil work visa is very hard to obtain, and is only issued in certain cases (see visa section), you should apply for it before leaving for Brazil. Yet in order to do that, you will need a pre-arranged job. You will also need your employer to start the application process for your work permit.
You need to accept that not knowing of local language will put you at real disadvantage from the local job seekers. The basic knowledge of Portuguese is considered necessary to cope with daily office life and life outside work.
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Good luck with your work in Brazil!


text:
Disney challenge coins are real. Here's the story behind them
Some folks will visibly swell with pride as they present their collection of coins, which to the uninitiated look like gilded slammers from that '90s era game Pogs. Standing before those neatly ordered defense industry discuses, all covered and aligned on a handmade display case, they'll cheerfully remark how one time some four-star general or defense official at this one base palmed them a coin for doing something or other. Others will offer little bits of information, like military-grade Snapple Facts. They'll say, "Hey, did you know that there's a drinking game involving challenge coins?" And everyone else will say "Yes, we know."
It's not that I dislike challenge coins; they're fine. It's just that they're everywhere and handed out for everything, often in lieu of a more meaningful reward, to the point that it sometimes feels like they've lost their meaning.
It's with this jaded outlook that I first encountered challenge coins in one place where I never expected them to be, not in a million years — and I can honestly say that this is one coin I actually wish I had:
That's right: The Walt Disney Company can now add "challenge coins" to a list that includes Marvel, Star Wars, and pretty much everything else that defined my childhood.
The badass-looking (albeit confusing) Mickey Mouse/Punisher skull challenge coin appears to have come from security personnel at Disneyland in Anaheim, California. A photo of the coin was provided to Task & Purpose by a reader who did not offer details on when the coin was given out.
At first, we were unsure if this was a one-off occurrence, like a few security guards who were vets decided to make a challenge coin for themselves, or if it was something the magical kingdom had officially sanctioned.
"The Walt Disney Company has an enduring tradition of support for those who support in the military, as well as their families and veterans" and that extends to challenge coins, a spokesman for Walt Disney World in Orlando, Florida told Task & Purpose.
"In our security departments and other areas where military veterans have come to work after their service, it's natural that affinity, that cultural use of coins, came with them and all of the hallmarks of it: unit identity, organizational identity, pride in mission, as well as the use of the coins as a sign of mutual respect and recognition," said the spokesperson, adding that the coins are primarily created for employee recognition and are not available for purchase.
At any given time Disneyland and Disney World have three to four officially sanctioned coins, which are used in much the same way as they are in the military, Disney confirmed to Task & Purpose. The spokesman said that the Punisher/Mickey coin was not an official Disney challenge coin, but added that park personnel often make their own coins for internal use.
Mickey And Friends Christmas Svg
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3. Merida Disney Princess Svg
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7. Goofy Svg
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9. Goofy Angel Svg
10. Donald Duck Svg
Some folks will visibly swell with pride as they present their collection of coins, which to the uninitiated look like gilded slammers from that '90s era game Pogs. Standing before those neatly ordered defense industry discuses, all covered and aligned on a handmade display case, they'll cheerfully remark how one time some four-star general or…
Tags: Donald Duck Disney Svg Mickey And Friends Svg
Disney World Confirms Popular Holiday Show Not Coming Back in 2021
The hidden Disney World spot where you can avoid the crowds


text:
1970-1990s / Horror / K - O
Harry Adam Knight
by Christopher Fulbright May 6, 2017 July 14, 2019
Harry Adam Knight is one of several pseudonyms used by Australian-born writer John Brosnan (7 October 1947 – 11 April 2005). Brosnan wrote four novels between 1983 and 1992 as Knight: Slimer, Carnosaur, The Fungus, and Bedlam. Some of them were co-written by British author Leroy Kettle. Brosnan's 1988 novel Worm was originally published under the pseudonym Simon Ian Childer, but was later reissued under the Knight name. His novel The Fungus was re-released in the U.S. as Death Spore by Pinnacle.
Brosnan was a fairly prolific author, well-liked by his peers. He wrote more than 30 books, ranging from science fiction and horror to humor, including novelizations, and non-fiction books on cinema. He also wrote the SF/pulp/noir comic strip Night Zero for the British magazine 2000 AD from the late 1980s through the early 1990s. He covered TV and film for the UK magazine Starburst for many years. A fanzine piece written on the occasion of his funeral years ago makes interesting reading for his fans and can be found here.
Despite Brosnan's inside joke that Harry Adam Knight was a HAK (ahem), the books met with success relatively few writers see — his novel Carnosaur was made into a 1993 horror film by executive producer Roger Corman and spawned a couple of sequels. Brosnan adapted Slimer for the 1996 horror film Proteus.
The Harry Adam Knight novels have become collectibles in recent years. To see a list of what's available second-hand, click here.
These cover scans are from the library of Christopher Fulbright. Please note that Realms of Night has an eBay page with monthly horror auctions. Follow our page and save us as a favorite seller for updates.
Taggedharry adam knightharry adam knight book coversjohn brosnanproteus
John Halkin
Robert R. McCammon
Carol Ellis


Anadarko Petroleum (APC) issued a quarterly update on operations in the Permian Basin for the third quarter of 2011. The company reported average daily production volume of 15,600 barrels of oil equivalent (BOE) per day in the Permian Basin, up 13% from the third quarter of 2010.
Anadarko Petroleum said that production of liquids increased 180% year over year and 30% sequentially in the most recent quarter.
Anadarko Petroleum entered the fourth quarter of 2011 with eleven rigs (five operated, six non-operated) working in the Permian Basin. The company drilled fifteen wells and completed nineteen wells during the quarter.
"Our West Texas Permian oil poduction nearly tripled in liquids volumes relative to the third quarter of 2010. During the quarter, Anadarko Petroleum participated in fifteen total Bone Spring and Avalon Shale wells as we continued to test our position in these emerging growth plays."


Greve in Chianti is a small and quite charming town located, unusually for a Tuscan village, on the floor of the valley of the Greve stream. It has always been a market place but only in the past few hundred years has it developed as a town. Greve is now probably the most popular centre for holiday-makers staying in the Chianti Classico region. Both the town and the county of Greve are the largest in Chianti, and the surrounding hills offer a considerable range of country accommodation, while apartments and B&B rooms are available within Greve itself. Wine rates high in interest both for the Grevigiani and visitors, there are many restaurants both in town and in the country nearby, restaurant prices being significantly lower outside Greve. Ceramics and Tuscan country-style furniture and fittings are available in speciality shops. There is a good open market in Piazza Matteotti on Saturday morning and a Coop supermarket, as well as numerous speciality food shops.
Important dates for Greve in Chianti.
Greve in Chianti Antiques and Collectors' Fair.
Greve in Chianti Flower Festival – Festa dei Fiori.
Chianti Classico wine fair at Greve in Chianti.
How to get to Greve in Chianti.
Map of Greve in Chianti.
Where is Greve in Chianti?
Where was Greve in Chianti in past times?
Greve in Chianti public swimming pool.
Greve in Chianti public library.
Art, artisans and ceramics in Greve in Chianti.
Furniture and antiques in Greve in Chianti.
Piazza Matteotti in Greve in Chianti.


text:
Q: Solving Stefan's solidification problem - for the case of 3 regions This question heavily related to this question, where the case of two PDE's are solved along with a zipping condition that is a function of time.
Using the link in the code I have solved this set of equations
\begin{equation}
\frac{\partial T_1}{\partial t}=\alpha_1\frac{\partial^2 T_1}{\partial x^2},\quad x\in\left[S\left(t\right),L\right]
\end{equation}
\begin{equation}
\frac{\partial T_1}{\partial t}=\alpha_2\frac{\partial^2 T_1}{\partial x^2},\quad x\in\left[0,S\left(t\right)\right]
\end{equation}
\begin{equation}
\frac{\partial T_1}{\partial x}-\frac{\partial T_2}{\partial x}=a\frac{\partial S}{\partial t}
\end{equation}
Along with the BC's and IC's:
\begin{equation}
T_1\left(0,t>0\right)=1, \quad T_1\left(S\left(t\right),t\right)=T_s, \quad T_2\left(S\left(t\right),t\right)=T_s, \quad
\end{equation}
\begin{equation}
T_2\left(L,t\right)=0, \quad T_1\left(x,0\right)=0, \quad T_2\left(x,0\right)=0 \end{equation}
where $\alpha_1,\alpha_2,L,a$ ,and $T_s$ are known constants.
This equation is known as Stefan's solidification problem and the heat coefficients are different in both solid ($\alpha_2$) and liquid ($\alpha_1$) stats.
I wish to solve the case where after some time, say $t=t^*$,the boundary condition at $x=0$ is changed to $T_1(0,t>t^*)=0$.
The solution assumes $T_1>T_s$ and $T_2<T_s$ at any time, which is now wrong.
I think there are two possible ways to construct that (none of them worked for me):
1) expand the solution, presented by @xzczd in the link above to consist 3 different PDEs, on for each region $(\alpha_1,\alpha_2,\alpha_1)$.
2) use the same solution @xzczd presented and adding a piece-wise function to alpha as $\alpha=\alpha_1$ when $T>Ts$ and $\alpha=\alpha_2$ when $T<Ts$.
If anyone has experience with a related problem or any idea for how to make it work I will be grateful!
Following the comments to this post I add the post to contain the code I have used for this case:
xR = 10; tend = 200; Pxs = 0.5; \[Kappa] = -10;
hyd1 = 2; h1 = 2;
w = 1;
hyd2 = 1; h2 = 1;
k1 = 1; k2 = hyd2^3/hyd1^3; k3 = k1;
\[Alpha]1 = 1; \[Alpha]2 = hyd1^3/hyd2^3;
eqL = D[P1[x, t], t] == \[Alpha]2 D[P1[x, t], x, x];
eqM = D[P2[x, t], t] == \[Alpha]2 D[P2[x, t], x, x];
eqR = D[P3[x, t], t] == \[Alpha]2 D[P3[x, t], x, x];
{icL, icM, icR} = {P1[x, 0] == 1, P2[x, 0] == 0, P3[x, 0] == 0};
{bcL, bcM,bcR} = {{P1[0, t] == 1, P1[S1@(t), t] == Pxs}, {P2[S1@(t), t] == Pxs, P2[S2@(t), t] == Pxs}, {P3[S2@(t), t] == Pxs, P3[xR, t] == 0}};
slopeL = ( k1 D[P1[x, t], x] /. x -> S1[t]);
slopeM1 = ( k2 D[P2[x, t], x] /. x -> S1[t]);
bcmidfunc1 = S1'[t] == (# - #2)/\[Kappa] &;
slopeM2 = ( k2 D[P2[x, t], x] /. x -> S2[t]);
slopeR = ( k3 D[P3[x, t], x] /. x -> S2[t]);
bcmidfunc2 = S2'[t] == - ((# - #2)/\[Kappa]) &;
With[{eps = 10^-10}, icmid1 = S1[0] == eps];
With[{eps = 10^-10}, icmid2 = S2[0] == 1 + eps];
changeL = DChange[#, x/S1@t == \[Xi], x, \[Xi], P1[x, t]] &;
changeM = DChange[#, (x - S1[t])/(S2[t] - S1[t]) == \[Xi], x, \[Xi], P2[x,t]] &;
changeR = DChange[#, (x - S2[t])/(xR - S2[t]) == \[Xi], x, \[Xi], 3[x,t]] &;
toode = With[{sf = 100}, Map[sf # + D[#, t] &, #, {2}] &];
{neweqL, newicL, newbcL, newslopeL} = changeL@{eqL, icL, toode@bcL,slopeL} /. S1[0] -> S1[t];
{neweqM1, newicM1, newbcM1, newslopeM1} = changeM@{eqM, icM, toode@bcM, slopeM1} /. {S1[0] -> S1[t]} // Simplify;
{neweqM2, newicM2, newbcM2, newslopeM2} = changeM@{eqM, icM, toode@bcM, slopeM2} /. {S2[0] -> S2[t]} // Simplify;
{neweqR, newicR, newbcR, newslopeR} = changeR@{eqR, icR, toode@bcR, slopeR} /. S2[0] -> S2[t] // Simplify;
points = 25;
xdifforder = 4;
{\[Xi]L, \[Xi]R} = domain = {0, 1};
grid = Array[# &, points, domain];
ptoo = pdetoode[{P1, P2, P3}[\[Xi], t], t, grid, xdifforder];
del = #[[2 ;; -2]] &;
{odeL, odeicL, odebcL, odeslopeL, odeM1, odeicM1, odebcM1, odeslopeM1, deM2, odeicM2, odebcM2, odeslopeM2, odeR, odeicR, odebcR, odeslopeR} = MapAt[del, ptoo /@ {neweqL, newicL, newbcL, newslopeL, neweqM1, newicM1, newbcM1, newslopeM1, neweqM2, newicM2, newbcM2, newslopeM2, neweqR, newicR, newbcR, newslopeR}, {{1}, {5}}];
odebcmid1 = bcmidfunc1[odeslopeL, odeslopeM1];
odebcmid2 = bcmidfunc2[odeslopeM2, odeslopeR];
odeicmid1 = icmid1;
odeicmid2 = icmid2;
sollst = NDSolveValue[{odeL, odeM1, odeM2, odeR, odeicL, odeicM1, odeicM2, odeicR, odebcL, odebcM1, odebcM2, odebcR, odebcmid1, odebcmid2, odeicmid1, odeicmid2}, {P1 /@ grid, P2 /@ grid, P3 /@ grid, S1, S2} // Flatten, {t, 0, tend}];

The Error i get is
    NDSolveValue::overdet: There are fewer dependent variables,...., than equations, so the system is overdetermined.

Thanks,
Ofek.

A: Important Update
Through a copy-paste mistake, I dropped the temperature dependence on the effective heat capacity, which was the point of the exercise. I have modified the post to correct that mistake.
Update #2
The difference between liquid and solid thermal conductivity can be quite large (4x for water), so I added support for the temperature dependent thermal conductivity.
Modified Original Post
You might find it easier to introduce the concept of a "mushy" zone versus tracking the phase boundaries.  The typical enthalpy versus temperature curve for the melting of ice is shown in the following.

We can approximate this curve with continuous functions and not lose much in the simulation.  Typically, this is done by defining an apparent heat capacity like so
$${\hat C_{p}(T)}={\hat C_{p,s}}\left ( 1-\epsilon(T) \right )+\epsilon(T){\hat C_{p,l}} + \Delta {\hat H_f}\frac{d \epsilon}{dT}$$
Where $\epsilon$ is the phase fraction of liquid.  Any nice shaped S-curve will do so let's try a normalized Tanh function that ranges from 0 to 1.  $T_m$ is the meltpoint and $\delta$ is the width of the phase transition.
$$\epsilon(T)=\frac{{1 + \operatorname{Tanh} \left( {8\frac{{\left( {T - {T_m}} \right)}}{\delta }} \right)}}{2}$$
And the temperature derivative of $\epsilon$ is
$$\frac{d\epsilon}{dT}=\frac{{4\operatorname{Sech} {{\left( {8\frac{{\left( {T - {T_m}} \right)}}{\delta }} \right)}^2}}}{\delta }$$
Now, we can integrate ${\hat C_{p}(T)}$ to see that we recover the enthalpy phase transition curve.
us[m_, t_] := (1 + Tanh[m (t)])/2(* Unit Step *)
eps[tm_, deltaT_, t_] := (1 + Tanh[8 (t - tm)/deltaT])/2
deps[tm_, deltaT_, t_] := (4 Sech[(8 (t - tm))/deltaT]^2)/deltaT
cpeff[deltaHf_, cpl_, cps_, tm_, deltaT_, t_] :=
 cps (1 - eps[tm, deltaT, t]) + cpl eps[tm, deltaT, t] +
  deltaHf deps[tm, deltaT, t]
keff[kl_, ks_, tm_, deltaT_, t_] :=
 ks (1 - eps[tm, deltaT, t]) + kl  eps[tm, deltaT, t]
deltah[deltaHf_, cpl_, cps_, tm_, deltaT_, t_] :=
 1/16 (8 (cpl + cps) t + (cpl - cps) deltaT Log[
      Cosh[(8 (t - tm))/deltaT]] + 8 deltaHf Tanh[(8 (t - tm))/deltaT])
pulseSeq[a_, fac_, m_, t0_, t_] := (
 a (1 + (1 + fac) us[m, t0 - t] (-1 + us[m, -t]) + (-1 + fac) us[
      m, -t]))/fac

Using this phase fraction approach, we only have one temperature equation to solve as shown.
$$\frac{\partial T}{\partial t}=\frac{k}{\rho \hat C_{p}(T)} \frac{\partial^2 T}{\partial x^2}$$
In the following, I start with water at $5^\circ C$ and "instantaneously" imposes a $-5^\circ C$ wall.  After 1800 seconds, the wall returns to $5^\circ C$. The Mathematica code is shown below (note that earlier version of this post contained an error in cpeff).
eqn = D[u[t, x], t] -
    0.555/(1000 cpeff[334000.`, 4180, 2060, 0, 0.2, u[t, x]])
      D[u[t, x], {x, 2}] == 0;
opts = Method -> {"MethodOfLines",
    "SpatialDiscretization" -> {"TensorProductGrid",
      "MinPoints" -> 500}};
ics = {u[0, x] == 5};
bcs = {u[t, 0] == pulseSeq[5, 1, 10, 1800, t], u[t, 0.05] == 5};
eqns = {eqn} ~ Join ~ ics ~ Join ~ bcs;
ifun = NDSolveValue[eqns, {u}, {t, 0, 3600}, {x, 0, 0.05}, opts];
plts = Plot3D[ifun[[1]][t, x], {t, 0, 3600}, {x, 0, 0.0075},
   PlotRange -> All, PlotPoints -> {200, 200}, MaxRecursion -> 4,
   ColorFunction -> (ColorData["MintColors"][#3] &),
   MeshFunctions -> {If[-0.01 < #3 < 0.01, #3, 0] &,
     If[#3 < 0, #3, 0] &, If[#3 > 0, #3, 0] &}, Mesh -> 21,
   AxesLabel -> Automatic,
   MeshStyle -> {{Black, Thick}, {Blue, Thick, Dashed}, {Red, Thick,
      DotDashed}}, Boxed -> False, ImageSize -> Large];
sz = 300;
Grid[{{Show[{plts}, ViewProjection -> "Orthographic",
    ViewPoint -> Front, ImageSize -> sz,
    Background -> RGBColor[0.84`, 0.92`, 1.`], Boxed -> False],
   Show[{plts}, ViewProjection -> "Orthographic", ViewPoint -> Right,
    ImageSize -> sz, Background -> RGBColor[0.84`, 0.92`, 1.`],
    Boxed -> False]}, {Show[{plts}, ViewProjection -> "Orthographic",
    ViewPoint -> Top, ImageSize -> sz,
    Background -> RGBColor[0.84`, 0.92`, 1.`], Boxed -> False],
   Show[{plts}, ViewProjection -> "Perspective",
    ViewPoint -> {Above, Left, Front}, ImageSize -> sz,
    Background -> RGBColor[0.84`, 0.92`, 1.`], Boxed -> False]}},
 Dividers -> Center]

The model seems to behave reasonably well.  There is nice parabolic growth in the ice layer initially.  Once the heating is turned back on, the ice first melts at the wall as expected.  When all the ice is gone, the system starts to heat more rapidly as on would expect.  An elegant way to produce the phase boundary was suggested by @Alex Trounev.
ContourPlot[ifun[[1]][t, x] == 0, {t, 0, 3600}, {x, 0, 0.01}, MaxRecursion -> 4]

Enhancement for Temperature Dependent Thermal Conductivity
Ice is about 4x more thermally conductive than liquid water.  In my initial analysis, the thermal conductivity, $k$, was presumed to be constant.  The original energy balance was given by
$$\frac{{\partial T}}{{\partial t}} - \alpha \frac{{{\partial ^2}T}}{{\partial {x^2}}} = 0$$
To use the "mushy" zone, $\alpha$ is no longer constant, but a function of temperature so we really need to recast it in coefficient form as shown below.
$$m\frac{{{\partial ^2}}}{{\partial {t^2}}}u + d\frac{\partial }{{\partial t}}u + \nabla \cdot\left( { - c\nabla u - \alpha u + \gamma } \right) + \beta \cdot\nabla u + au - f = 0$$
All terms except $d$ and $c$ are zero so the new energy balance becomes:
$$\rho {{\hat C}_p}(T)\frac{\partial u }{{\partial t}} + \nabla  \cdot \left( { - k(T)\nabla u} \right) = \rho {{\hat C}_p}(T)\frac{\partial u }{{\partial t}} + \frac{\partial }{{\partial x}}\left( { - k(T)\frac{\partial u }{{\partial x}}} \right) = 0$$
Where $k(T)$ will be given by the same s-shaped curve $\epsilon(T)$ or
$$k(T) = k_s\left ( 1-\epsilon(T) \right )+k_l\epsilon(T)$$
The Mathematica code for a $-4^\circ C$ to $4^\circ C$ pulse sequence (sans plotting that is the same as above) is shown below.  I needed to supply a small MaxStepFraction to capture the change in wall temperature at 1800s.  This can lead to large file sizes.  Perhaps, someone can comment on better/more robust settings.
rho = 1000;
dhf = 334000.`;
cpl = 4180.0;
cps = 2060;
kl = 0.55575;
ks = 2.22;
tm = 0;
delta = 0.25;
eqn = rho cpeff[dhf, cpl, cps, tm, delta, u[t, x]] D[u[t, x], t] -
    D[keff[kl, ks, tm, delta, u[t, x]] D[u[t, x], x], x] == 0;
opts = Method -> {"MethodOfLines",
    "SpatialDiscretization" -> {"TensorProductGrid",
      "MinPoints" -> 200}};
ics = {u[0, x] == 4};
bcs = {u[t, 0] == pulseSeq[4, 1, 0.0625, 1800, t], u[t, 0.01] == 4};
eqns = {eqn} ~ Join ~ ics ~ Join ~ bcs;
ifun = NDSolveValue[eqns, {u}, {t, 0, 3600}, {x, 0, 0.01}, opts,
   MaxStepFraction -> 1/2000];

Variable Conductivity

The "mushy" zone is fuzzy so I created a contour plot of the $\pm 30\%$ bands using the following Mathematica code.
ContourPlot[{ifun[[1]][t, x],
  ifun[[1]][t, x] == -delta/11.54156032711171`, ifun[[1]][t, x] == 0,
  ifun[[1]][t, x] == delta/11.54156032711171`}, {t, 0, 3600}, {x, 0,
  0.01}, MaxRecursion -> 4]

We expect the spacing between solid and median temperature band to be about 4x that of the liquid and median band because there is 4x the resistance through the liquid layer.  The plot suggests that this is the case.
Constant Conductivity
I changed the pulse sequence, boundary conditions, and the domain dimensions from the previous example.  For completeness, I re-ran the constant liquid conductivity case with the geometry and conditions.

Because the liquid conductivity is lower than the solid, the film does not grow as fast as the variable conductivity case.

A: There is a solution to the problem when the value of the function P1[x,t] on the border does not fall to zero, but to a critical value Pxs. Then the second moving boundary is not needed, and the solution can be obtained using NDSolve (my algorithm)
Nmax = 500; xR = 10; t0 = 1/3; tm = 100; Pxs = 1/2; s0 = 1/10; u0 =
 2/100;

S1[0] = s0; S1[-1] = S1[0];
f[t_] := If[t < tm, 1, Pxs]
f1[t_] := If[t < 10^-6, 0, f[t]]
f2[t_] := If[t < 10^-6, 0, Pxs]
p1[0] = NDSolveValue[{D[P1[x, t], t] == D[P1[x, t], x, x],
    P1[0, t] == f1[t], P1[S1[0], t] == f2[t], P1[x, 0] == 0},
   P1, {x, 0, S1[0]}, {t, 0, t0}];
p2[0] = NDSolveValue[{D[P2[x, t], t] == D[P2[x, t], x, x],
    P2[xR, t] == 0, P2[S1[0], t] == f2[t], P2[x, 0] == 0},
   P2, {x, S1[0], xR}, {t, 0, t0}];
p3[0][x_, t_] := 0

Table[T[i] = t0 + i*t0, {i, 0, Nmax}];

Do[p1[i] =
   NDSolveValue[{D[P1[x, t], t] == D[P1[x, t], x, x],
     P1[0, t] == f1[t], P1[S1[i - 1], t] == f2[t],
     P1[x, T[i - 1]] ==
      If[x < S1[i - 2], p1[i - 1][x, T[i - 1]], f2[T[i - 1]]]},
    P1, {x, 0, S1[i - 1]}, {t, T[i - 1], T[i]}] ;
  p2[i] =
   NDSolveValue[{D[P2[x, t], t] == D[P2[x, t], x, x], P2[xR, t] == 0,
     P2[S1[i - 1], t] == f2[T[i - 1]],
     P2[x, T[i - 1]] == p2[i - 1][x, T[i - 1]]},
    P2, {x, S1[i - 1], xR}, {t, T[i - 1], T[i]}];
  S1[i] = S1[i - 1] -
    u0*( Derivative[1, 0][p1[i]][S1[i - 1], T[i]] -
       Derivative[1, 0][p2[i]][S1[i - 1], T[i]]), {i, 1,
   Nmax}] // Quiet
P12 = Interpolation[
    Flatten[Table[{{x, T[i]},
       If[x < S1[i - 1], p1[i][x, T[i]], p2[i][x, T[i]]]}, {x, .01,
       xR, .01}, {i, 0, Nmax}], 1], InterpolationOrder -> 3]; // Quiet

pp1[i_] :=
  Table[{x, If[x < S1[i - 1], p1[i][x, T[i]], p2[i][x, T[i]]]}, {x, 0,
     xR, .01}];

{ListLinePlot[Table[pp1[i], {i, 0, 290, 10}], PlotRange -> All,
  AxesLabel -> {"x", "P"}],
 ListLinePlot[Table[pp1[i], {i, 300, 320, 1}], PlotRange -> All,
  AxesLabel -> {"x", "P"}],
 ListLinePlot[Table[pp1[i], {i, 320, Nmax, 10}], PlotRange -> All,
  AxesLabel -> {"x", "P"}]}
{ListPlot[Table[{T[i], S1[i]}, {i, 0, Nmax}],
  AxesLabel -> {"t", "S1"}],
 Plot3D[P12[x, t], {x, 0, xR}, {t, 0, T[Nmax]}, PlotRange -> {0, 1},
   Mesh -> None, ColorFunction -> "TemperatureMap", PlotPoints -> 40,
   AxesLabel -> {"x", "t", "P"}] // Quiet}

Unexpectedly, I managed to debug the code that @Ofek Peretz  wrote. Corrections had to be done a lot. The result is the curve that I received in part using my code, and Tim Laska received in full. The solution uses two wellknown functions that I will present for the convenience of readers. The first function is called pdetoode introduced by @xzczd and DChange introduced by @Kuba
Clear[fdd, pdetoode, tooderule]
fdd[{}, grid_, value_, order_, periodic_] := value;
fdd[a__] := NDSolve`FiniteDifferenceDerivative@a;

pdetoode[funcvalue_List, rest__] :=
  pdetoode[(Alternatives @@ Head /@ funcvalue) @@ funcvalue[[1]],
   rest];
pdetoode[{func__}[var__], rest__] :=
  pdetoode[Alternatives[func][var], rest];
pdetoode[front__, grid_?VectorQ, o_Integer, periodic_: False] :=
  pdetoode[front, {grid}, o, periodic];

pdetoode[func_[var__], time_, {grid : {__} ..}, o_Integer,
   periodic : True | False | {(True | False) ..} : False] :=
  With[{pos = Position[{var}, time][[1, 1]]},
   With[{bound = #[[{1, -1}]] & /@ {grid},
     pat = Repeated[_, {pos - 1}],
     spacevar = Alternatives @@ Delete[{var}, pos]},
    With[{coordtoindex =
       Function[coord,
        MapThread[
         Piecewise[{{1, # === #2[[1]]}, {-1, # === #2[[-1]]}},
           All] &, {coord, bound}]]},
     tooderule@
      Flatten@{((u : func) |
            Derivative[dx1 : pat, dt_, dx2___][(u : func)])[x1 : pat,
          t_, x2___] :> (Sow@coordtoindex@{x1, x2};

          fdd[{dx1, dx2}, {grid},
           Outer[Derivative[dt][u@##]@t &, grid],
           "DifferenceOrder" -> o,
           PeriodicInterpolation -> periodic]),
        inde : spacevar :>
         With[{i = Position[spacevar, inde][[1, 1]]},
          Outer[Slot@i &, grid]]}]]];

tooderule[rule_][pde_List] := tooderule[rule] /@ pde;
tooderule[rule_]@Equal[a_, b_] :=
  Equal[tooderule[rule][a - b], 0] //.
   eqn : HoldPattern@Equal[_, _] :> Thread@eqn;
tooderule[rule_][expr_] := #[[Sequence @@ #2[[1, 1]]]] & @@
  Reap[expr /. rule]

Clear@pdetoae;
pdetoae[funcvalue_List, rest__] :=
  pdetoae[(Alternatives @@ Head /@ funcvalue) @@ funcvalue[[1]], rest];
pdetoae[{func__}[var__], rest__] :=
  pdetoae[Alternatives[func][var], rest];

pdetoae[func_[var__], rest__] :=
 Module[{t},
  Function[pde, #[
       pde /. {Derivative[d__][u : func][inde__] :>
          Derivative[d, 0][u][inde, t], (u : func)[inde__] :>
          u[inde, t]}] /. (u : func)[i__][t] :> u[i]] &@
   pdetoode[func[var, t], t, rest]]
ClearAll[DChange];

DChange[expr_, transformations_List, oldVars_List, newVars_List,
   functions_List] :=
  Module[{pos, functionsReplacements, variablesReplacements,
    arguments, heads, newVarsSolved},
   pos = Flatten[
     Outer[Position, functions, oldVars], {{1}, {2}, {3, 4}}];
   heads = functions[[All, 0]];
   arguments = List @@@ functions;
   newVarsSolved = newVars /. Solve[transformations, newVars][[1]];
   functionsReplacements =
    Map[Function[i,
      heads[[i]] -> (Function[#, #2] &[arguments[[i]],
         ReplacePart[functions[[i]],
          Thread[pos[[i]] -> newVarsSolved]]])],
     Range@Length@functions];
   variablesReplacements = Solve[transformations, oldVars][[1]];
   expr /. functionsReplacements /. variablesReplacements //
     Simplify // Normal];

DChange[expr_, functions : {(_[___] == _) ..}] :=
 expr /. Replace[
   functions, (f_[vars__] == body_) :> (f ->
      Function[{vars}, body]), {1}]

DChange[expr_, x___] :=
  DChange[expr, ##] & @@
   Replace[{x}, var : Except[_List] :> {var}, {1}];

DChange[expr_, coordinates : Verbatim[Rule][__String], oldVars_List,
   newVars_List, functions_] :=
  Module[{mapping, transformation},
   mapping =
    Check[CoordinateTransformData[coordinates, "Mapping", oldVars],
     Abort[]];
   transformation = Thread[newVars == mapping];
   {DChange[expr, transformation, oldVars, newVars, functions],
    transformation}];

Below is the debugged code from which @Ofek Peretz  began the discussion
xR = 10; tend = 286.288; t0 = 200; Pxs = 0.5; \[Kappa] = 10;
hyd1 = 1; h1 = 2;
w = 1;
hyd2 = 1; h2 = 1;
k1 = 1; k2 = hyd2^3/hyd1^3; k3 = k1;
\[Alpha]1 = 1; \[Alpha]2 = hyd1^3/hyd2^3;
fp10[t_] := (1 - Tanh[20*(t - t0)])/2
fp11[t_] := (1 + Pxs - (1 - Pxs)*Tanh[20*(t - t0)])/2
fs1[t_] := (1 + Tanh[20*(t - t0)])/2
eqL = D[P1[x, t], t] == \[Alpha]2 D[P1[x, t], x, x];
eqM = D[P2[x, t], t] == \[Alpha]2 D[P2[x, t], x, x];
eqR = D[P3[x, t], t] == \[Alpha]2 D[P3[x, t], x, x];
{icL, icM, icR} = {P1[x, 0] == 1, P2[x, 0] == 1, P3[x, 0] == 0};
{bcL, bcM,
   bcR} = {{P1[0, t] == 1, P1[1, t] == 1}, {P2[0, t] == 1,
    P2[1, t] == Pxs}, {P3[0, t] == Pxs, P3[1, t] == 0}};

With[{eps = 10^-3}, icmid1 = S1[0] == eps];
With[{eps = 2*10^-3}, icmid2 = S2[0] == eps];
changeL = DChange[#, x/S1@t == \[Xi], x, \[Xi], P1[x, t]] &;
changeM =
  DChange[#, (2*x - S1[t] - S2[t])/(S2[t] - S1[t])/2 + 1/2 == \[Xi],
    x, \[Xi], P2[x, t]] &;
changeR =
  DChange[#, (x - S2[t])/(xR - S2[t]) == \[Xi], x, \[Xi], P3[x, t]] &;
toode = With[{sf = 100}, Map[sf # + D[#, t] &, #, {2}] &];
neweqL = changeL@eqL // Simplify;
neweqM1 = changeM@eqM // Simplify;

neweqR = changeR@eqR // Simplify;
bc = {newbcL, newbcM1, newbcR} = {toode@bcL, toode@bcM, toode@bcR};
points = 25; h = 1/(points - 1);
xdifforder = 2;
{\[Xi]L, \[Xi]R} = domain = {0, 1};
grid = Array[# &, points, domain];
ptoo = pdetoode[{P1[\[Xi], t], P2[\[Xi], t], P3[\[Xi], t]}, t, grid,
   xdifforder];
del = #[[2 ;; -2]] &;
{newicL, newicM1,
   newicR} = {{P1[\[Xi], 0] == 1}, {P2[\[Xi], 0] ==
     1}, {P3[\[Xi], 0] == 0}};
{odeL, odeicL, odebcL, odeM1, odeicM1, odebcM1, odeR, odeicR,
   odebcR} = {neweqL // ptoo // del, del /@ ptoo@newicL,
   newbcL // ptoo, neweqM1 // ptoo // del, del /@ ptoo@newicM1,
   newbcM1 // ptoo, neweqR // ptoo // del, del /@ ptoo@newicR,
   newbcR // ptoo};
eqS1 = S1'[t] ==
   fs1[t]*(k1*Derivative[1, 0][P1][1, t]/S1[t] -
       k2*Derivative[1, 0][P2][0, t]/(S2[t] - S1[t]))/\[Kappa];
eqS2 = S2'[
    t] == (k3*Derivative[1, 0][P3][0, t]/(xR - S2[t]) -
      k2*Derivative[1, 0][P2][1, t]/(S2[t] - S1[t]))/\[Kappa];
odeicmid1 = icmid1;
odeicmid2 = icmid2;
op = {
\!\(\*SuperscriptBox[\(P1\),
TagBox[
RowBox[{"(",
RowBox[{"1", ",", "0"}], ")"}],
Derivative],
MultilineFunction->None]\)[1, t] -> (P1[1][t] - P1[1 - h][t])/h,
\!\(\*SuperscriptBox[\(P2\),
TagBox[
RowBox[{"(",
RowBox[{"1", ",", "0"}], ")"}],
Derivative],
MultilineFunction->None]\)[0, t] -> (P2[h][t] - P2[0][t])/h,
\!\(\*SuperscriptBox[\(P2\),
TagBox[
RowBox[{"(",
RowBox[{"1", ",", "0"}], ")"}],
Derivative],
MultilineFunction->None]\)[1, t] -> (P2[1][t] - P2[1 - h][t])/h,
\!\(\*SuperscriptBox[\(P3\),
TagBox[
RowBox[{"(",
RowBox[{"1", ",", "0"}], ")"}],
Derivative],
MultilineFunction->None]\)[0, t] -> (P3[h][t] - P3[0][t])/h};
eq0 = {P1[0][0] == 1, P2[0][0] == 1, P3[0][0] == Pxs, P1[1][0] == 1,
   P2[1][0] == Pxs, P3[1][0] == 0};

eqsop = {odeL, odeM1, odeR, odeicL, odeicM1, odeicR, odebcL, odebcM1,
    odebcR, odeicmid1, odeicmid2, eqS1, eqS2} /. op;
op1 = {eqsop[[
     7]] -> {-100*fp10[t] + 100 P1[0][t] + Derivative[1][P1[0]][t] ==
      0, -100*fp11[t] + 100 P1[1][t] + Derivative[1][P1[1]][t] == 0},
   eqsop[[8]] -> {-100*fp11[t] + 100 P2[0][t] +
       Derivative[1][P2[0]][t] ==
      0, -50.` + 100 P2[1][t] + Derivative[1][P2[1]][t] == 0}};

eqs = eqsop /. op1;

sollst3 =
  NDSolveValue[{eqs, eq0}, P3 /@ grid // Flatten, {t, 0, tend}];

sol3 = ListInterpolation[
   Developer`ToPackedArray@#["ValuesOnGrid"] & /@ sollst3 //
    Transpose, {Flatten@sollst3[[1]]["Grid"], grid}];
sollst1 =
  NDSolveValue[{eqs, eq0}, P1 /@ grid // Flatten, {t, 0, tend}];
sol1 = ListInterpolation[
   Developer`ToPackedArray@#["ValuesOnGrid"] & /@ sollst1 //
    Transpose, {Flatten@sollst1[[1]]["Grid"], grid}];
sollst2 =
  NDSolveValue[{eqs, eq0}, P2 /@ grid // Flatten, {t, 0, tend}];
sol2 = ListInterpolation[
   Developer`ToPackedArray@#["ValuesOnGrid"] & /@ sollst2 //
    Transpose, {Flatten@sollst2[[1]]["Grid"], grid}];

{ContourPlot[sol1[t, x], {t, 0, tend}, {x, 0, 1}, Contours -> 20,
  ColorFunction -> Hue, FrameLabel -> {"t", "\[Xi]"},
  PlotLegends -> Automatic, PlotRange -> All, PlotLabel -> "P1"],
 ContourPlot[sol2[t, x], {t, 0, tend}, {x, 0, 1}, Contours -> 20,
  ColorFunction -> Hue, FrameLabel -> {"t", "\[Xi]"},
  PlotLegends -> Automatic, PlotRange -> All, PlotLabel -> "P2"],
 ContourPlot[sol3[t, x], {t, 0, tend}, {x, 0, 1}, Contours -> 20,
  ColorFunction -> Hue, FrameLabel -> {"t", "\[Xi]"},
  PlotLegends -> Automatic, PlotRange -> All, PlotLabel -> "P3"]}
S11 = NDSolveValue[{eqs, eq0}, S1, {t, 0, tend}]; S21 =
 NDSolveValue[{eqs, eq0}, S2, {t, 0, tend}];
Plot[{S11[t], S21[t]}, {t, 0, tend}, AxesLabel -> {"t", "S1,S2"}]

Add a couple of pictures for clarity of what P1,P2,P3 looks like in the coordinates x, t.
 F[t_, x_] :=
     If[x >= S21[t], sol3[t, (x - S21[t])/(xR - S21[t])],
      If[x <= S11[t], sol1[t, x/S11[t]],
       sol2[t, (2*x - S11[t] - S21[t])/(S21[t] - S11[t])/2 + 1/2]]]
    l1 = Table[{t, x, F[t, x]}, {t, 0, 1.9, .05}, {x, 0, 5, .1}];
    l2 = Table[{t, x, F[t, x]}, {t, 2, tend, .5}, {x, 0, 5, .1}];
    ff = Interpolation[Join[Flatten[l1, 1], Flatten[l2, 1]],
       InterpolationOrder -> 4];

    {ContourPlot[ff[t, x], {t, 0, tend}, {x, 0, 5}, Contours -> 38,
      PlotPoints -> 50, FrameLabel -> {"t", "x"},
      PlotLegends -> Automatic, ColorFunction -> "TemperatureMap"],
     ListPlot3D[Join[Flatten[l1, 1], Flatten[l2, 1]], Mesh -> None,
      InterpolationOrder -> 4, ColorFunction -> Hue,
      AxesLabel -> {"t", "x", ""}]}

A: Inspired by Tim's excellent answer I was wondering if it is not possible to use the FEM for this. In Version 12.0 there is no way to do this from top level. However, we still can solve this phase change problem with the low level FEM functions, which I'd like to show here. Why bother? In this specific case we look at a 1D spatial plus time PDE and there is not much to be gained by making use of the FEM. In two spatial dimensions, things are different as the FEM will then allow us to model phase change in arbitrary shaped regions.
Since Tim covered the theory so well in his post I am going to focus on the FEM part. The basic idea is to write a function discretizeResidual the returns the residual of the PDE and then have NDSolve do the time integration. Variants of this approach are documented in the FEMProgramming tutorial.
We start by setting up the parameters.
Needs["NDSolve`FEM`"]
(*latent heat*)
Lm = 3.335*10^5;
(* melt point *)
Tm = 0;
(*temperature interval for phase change*)
dT = 0.25;
Tc = -5;
Th = 5;
r1 = 918;
r2 = 997;
Cp1 = 2052;
Cp2 = 4179;

Next we set up some derived parameters and some helper functions:
SmoothedStepFunction[fmin_, fmax_, ts_, m_] :=
 Function[t, (fmin*Exp[ts*m] + fmax*Exp[m*t])/(Exp[ts*m] + Exp[m*t])]

theta = SmoothedStepFunction[1, 0, 0, 50];

rRatio = r1/r2;
(*convertion from space coord. to material coord*)
r = r2*rRatio;

k1 = 2.31;
(*convertion from space coord. to material coord*)
k2 = 0.613*rRatio;
k[T_] := theta[T]*k1 + (1 - theta[T])*k2

Setting up CL with a mass fraction a
a[T_] := (1 - 2 theta[T])/2;
CL[T_] := Evaluate[Lm*D[a[Temp], Temp] /. {Temp -> T}]

An alternative method is to use a regularized delta function
(* RegularizedDelta[g_,T_,Tm_]:=Piecewise[{{1/(4*g)(1+Cos[Pi/(2*g)(T-Tm)]),RealAbs[T-Tm]\[LessEqual]2*g},{0,True}}];
CL[T_]:=Lm*RegularizedDelta[dT/4,T,Tm]
*)

We perform a basic check that the integral over CL matches the latent heat.
(* check *)
NIntegrate[CL[T], {T, Tc, Th}] == Lm

Set up Cp with latent heat.
Cp[T_] := theta[T]*Cp1 + (1 - theta[T])*Cp2 + CL[T]

For completeness we have Cp without latent heat
(* Cp[T_]:=theta[T]*Cp1+(1-theta[T])*Cp2 *)

Set up the temperature profile on the left boundary:
TL[t_] := Piecewise[{{SmoothedStepFunction[Th, Tc, 0.5, 20][t], t <= 1}, {Tc,
     1 < t <= 1800}, {SmoothedStepFunction[Tc, Th, 1800.5, 20][t],
     1800 < t <= 1801}, {Th, True}}];

(*Plot[TL[t],{t,0,3600},PlotTheme\[Rule]"Detailed",PlotLabel\[Rule]\
"TLeft",FrameLabel\[Rule]{"time [s]","temperature \
[\[Degree]C]"},PlotLegends\[Rule]None,LabelStyle\[Rule]Directive[14],\
ImageSize\[Rule]Medium,Exclusions\[Rule]None]*)

Now we start to set up the low level FEM functions.
dampCoef[t_, T_] := r*Cp[T]
diffuCoef[t_, T_] := k[T]
ll = 0;
ic = T[0, x] == Th;
bc = {DirichletCondition[T[t, x] == TL[t], x == 0.],
   DirichletCondition[T[t, x] == Th, x == 0.01]};
tEnd = 3600;

Initialize the BCs and method data:
vd = NDSolve`VariableData[{"DependentVariables" -> {T},
    "Space" -> {x}, "Time" -> t}];
nr = ToNumericalRegion[FullRegion[1], {{0, .01}}];
sd = NDSolve`SolutionData[{"Space" -> nr, "Time" -> 0.}];
initBCs = InitializeBoundaryConditions[vd, sd, {bc}];
methodData =
  InitializePDEMethodData[vd, sd,
   Method -> {"FiniteElement",
     "MeshOptions" -> {"MaxCellMeasure" -> 0.01/50}}];

We initialize the coefficients:
initCoeffs = InitializePDECoefficients[vd, sd,
   "DampingCoefficients" -> {{dampCoef[t, T[t, x]]}},
   "DiffusionCoefficients" -> {{-diffuCoef[t, T[t, x]]*
       IdentityMatrix[1]}}, "LoadCoefficients" -> {{ll}}];

We discretize the stationary components once before everything else and make use of these during the time integration such that we do not have to recompute them at every step.
sdpde = DiscretizePDE[initCoeffs, methodData, sd];
sbcs = DiscretizeBoundaryConditions[initBCs, methodData, sd];

What follows is the heart of the idea. The function discretizePDEResidual gets the time t, dependent variable u and the time derivative of u as an argument. From there we update the solution data with the current time and dependent variable. We extract the stationay components computed previously and add the transient and nonlinear components. After that we deploy the boundary conditons and finally compute the residual.
discretizePDEResidual[t_?NumericQ, u_?VectorQ, dudt_?VectorQ] :=

 Module[{l, s, d, tdpde, tbcs, nldpde, nlbcs, sdTemp},

  NDSolve`SetSolutionDataComponent[sd, "Time", t];
  NDSolve`SetSolutionDataComponent[sd, "DependentVariables", u];

  l = sdpde["LoadVector"];
  s = sdpde["StiffnessMatrix"];
  d = sdpde["DampingMatrix"];

  tdpde = DiscretizePDE[initCoeffs, methodData, sd, "Transient"];
  tbcs = DiscretizeBoundaryConditions[initBCs, methodData, sd,
    "Transient"];
  l += tdpde["LoadVector"];
  s += tdpde["StiffnessMatrix"];
  d += tdpde["DampingMatrix"];

  nldpde = DiscretizePDE[initCoeffs, methodData, sd, "Nonlinear"];
  nlbcs =
   DiscretizeBoundaryConditions[initBCs, methodData, sd,
    "Nonlinear"];
  l += nldpde["LoadVector"];
  s += nldpde["StiffnessMatrix"];
  d += nldpde["DampingMatrix"];

  DeployBoundaryConditions[{l, s, d}, nlbcs];
  DeployBoundaryConditions[{l, s, d}, tbcs];
  DeployBoundaryConditions[{l, s, d}, sbcs];

  d.dudt + s.u - l
  ]

To allow for a fast time integration we write a small help function to construct a damping matrix at a specific point in time. From this damping matrix we extract the sparsity pattern. Details can be found in the FEMProgramming tutorial.
initializeDampingMatrix[t_, u_?VectorQ] := Module[
  {d, tdpde, nldpde},

  NDSolve`SetSolutionDataComponent[sd, "Time", t];
  NDSolve`SetSolutionDataComponent[sd, "DependentVariables", u];

  d = sdpde["DampingMatrix"];

  tdpde = DiscretizePDE[initCoeffs, methodData, sd, "Transient"];
  d += tdpde["DampingMatrix"];

  nldpde = DiscretizePDE[initCoeffs, methodData, sd, "Nonlinear"];
  d += nldpde["DampingMatrix"];

  d
  ]

One thing to keep in mind with this function is that we should choose a time that allows transient components to be picked up. The exact time does not matter and it could be t=0 just make sure that possible transient components are picked up.
sparsity = initializeDampingMatrix[10^-6, init]["PatternArray"];

Create the initial conditions:
init = #[[1]] & /@ methodData["ElementMesh"]["Coordinates"];

Do the time integration:
measure =
  AbsoluteTiming[
   MaxMemoryUsed[
     Monitor[tTfun =
       NDSolveValue[{discretizePDEResidual[t, T[t], T'[ t]] == 0,
         T[0] == init}, T, {t, 0, tEnd}
        , Method -> {"EquationSimplification" -> "Residual"}
        , Jacobian -> {Automatic, Sparse -> sparsity}
        , EvaluationMonitor :> (monitor = Row[{"t = ", CForm[t]}])],
      monitor]]/(1024.^2)];
Print["Time -> ", measure[[1]], "\nMemory -> ", measure[[2]]]

On my computer this takes about 130 seconds and 55MB of memory.
Create final the interpolating function:
Tfun = ElementMeshInterpolation[{tTfun["Coordinates"][[1]],
    methodData["ElementMesh"]}, Partition[tTfun["ValuesOnGrid"], 1]];

Visualize the result:
TRange = {Tc, Th};
legendBar =
  BarLegend[{"TemperatureMap", TRange}, 50,
   LegendLabel -> Text[Style["[C]", Opacity[0.6`]]]];
options = {PlotRange -> TRange,
   ColorFunction -> ColorData[{"TemperatureMap", TRange}],
   ColorFunctionScaling -> False, ContourStyle -> Opacity[0.1`],
   Contours -> 30, PlotPoints -> 50,
   FrameLabel -> {"time [s]", "x [m]"}, LabelStyle -> Directive[14],
   PlotLabel -> Text[Style["Temperature: T(t,x)", 18]],
   ImageSize -> Medium};
tempField =
 Legended[ContourPlot[Tfun[t, x], {t, 0, 3600}, {x, 0, 0.01},
   Evaluate[options]], legendBar]; phaseBoundary =
 ContourPlot[{Tfun[t, x] == 0}, {t, 0, 3600}, {x, 0, 0.01},
  MaxRecursion -> 5]; Show[tempField, phaseBoundary]

As many of you know, posts like these, were I get an opportunity to translate the stuff into the low level FEM functions, form the basis for what will be doable in NDSolve. Once more I'd like to take the opportunity to thank Tim for his great post (and this is certainly not the only one!) Well done and thanks!


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Waiting for a response…. since April 7th, 2017.
Be innovative with how you ask for Testimonials [or other favours]. How about offering a charity donation, an internship, some free consulting with your experts…. so many choices and so little cost to the business.
I am sick and tired of corporations taking advantage of their hapless customers and when the ONE TIME that I have some influence over the situation – they expect me to roll over and act dumb.


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Die Gmina Nowe Brzesko, jiddisch Bzhisk, ist eine Stadt-und-Land-Gemeinde im Powiat Proszowicki der Woiwodschaft Kleinpolen in Polen. Ihr Sitz ist die gleichnamige Stadt mit etwa 1650 Einwohnern. Zum 1. Januar 2011 wurde Nowe Brzesko zur Stadt erhoben.

Gliederung
Zur Stadt-und-Land-Gemeinde (gmina miejsko-wiejska) gehören neben der Stadt Nowe Brzesko folgende 16 Dörfer mit einem Schulzenamt:

 Grębocin
 Gruszów
 Hebdów
 Hebdów Stary
 Kuchary
 Majkowice
 Mniszów
 Mniszów-Kolonia
 Nowe Brzesko
 Pławowice
 Przybysławice
 Rudno Dolne
 Rudno-Józefów
 Sierosławice
 Szpitary
 Śmiłowice

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Einzelnachweise

Powiat Proszowicki


The benefits of sound walls are many for the overall community. Those that live or work near busy highways, loud railways or other industrial noise sources seem to be happier when unwanted noise levels are reduced. A quieter environment reduces stress, hearing impairments, high blood pressure created by loud noise. There have been numerous studies done on the use of sound barriers their benefit to the overall quality of life for affected residents. The federal government has spent hundreds of millions of dollars on sound walls nationwide to reduce noise pollution for its citizens. So sound walls play an important role in our country and provide a tangible benefit to us all.
There have been numerous cases where concrete sound walls, once installed, exacerbated the problem due to the unpredictable reflective noise. Research shows that reflective parallel sound walls (walls running parallel and across the roadway from each other) often send reflective noise far beyond the noise source and can actually increase the noise within the area of the traffic by 6 decibels or more.
Learn more about the benefits of Sound Walls in this article from Environmental Psychology.


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ADD UPDATE, 9 July 2017: Less than two weeks before Eastleigh Borough Council (EBC) makes a key decision on a massive 6,200 housing development, it has been hit by a double whammy. Problems are piling up one after another. In one case, Network Rail wants a ransom of millions of pounds for improving a road under a deathtrap bridge. And Southern Water has now admitted it would have to find alternative supplies if the scheme goes ahead. If it can't find them then the scheme is, literally, dead in the water.
In the case of the bridge, EBC has been warned by Network Rail that trying to squeeze a new road under a very old road bridge could cost lives. In recent years, lorries have hit the bridge no less than 18 times. Fixing it could also cost the council millions of pounds because Network Rail will only allow improvements to be made to the bridge to accommodate the huge housing development if it gets a share of the developers' profits. It's demanding a share of the uplift in value from agricultural to residential land. And, say experts, that could cost so many millions that it would make the whole scheme unviable. And as if that wasn't enough, the council has already been warned by an MEP that if the planned new road damages the River Itchen's floodplain then the UK could be taken to court and fined many millions of euros.
In an official statement that now confirms the dangers, Network Rail said: "This bridge is already prone to bridge strikes, with 18 recorded since 2008, and an increase in the volume of traffic would increase the risk of such incidents. Bridge strikes not only present a safety risk to road users and pedestrians, they also delay thousands of rail passengers and cost the taxpayer significant amounts of money. In addition, an increase in the volume of traffic may require changes to the road and bridge in order for it to be compliant with safety standards designed to protect road users and pedestrians, and generally to reduce the risk of bridge strikes should a housing development of this scale proceed."
One solution being considered is to ban HGVs from the bridge, together with pedestrians. But that would divert even more heavy traffic onto near roads and increase congestion. And all this even if engineers found a way of squeezing the new road between protected ancient woodlands.
And now even EBC admits the scheme could have vast funding problems. A council statement confirms Network Rail "are under a best-value obligation from the Department for Transport to ensure that any rights granted (or other related work needed to enable the scheme) are appropriately valued and take into account the uplift in land value (from agricultural to residential) that such works will unlock. The value secured by Network Rail in that scenario would then be reinvested back into the railway network. This could result in a significant value being due to Network Rail which could significantly impact upon the viability of the development option."
But apart from money problems there is now a new question: how to supply thousands of new residents with water. The Environment Agency (EA) has ordered Southern Water to drastically reduce the amount of water it takes from both the Test and the Itchen. The EA is forced to restrict how much water is taken from the rivers because of the EU Habitats Directive which has ruled that the rivers are not up to par. The decision will be finally made by a public inquiry next year. But in the meantime the water company has admitted: "We will consider all the options (including desalination, water recycling and transfers from neighbouring water companies) for the alternative new supplies we need and how long it will take to implement these schemes."
EBC is due to make a key decision about the plan at a public meeting on 20 July (7pm at Kings Community Church, Upper Northam Road, Hedge End, Southampton, SO30 4BZ) when hundreds of protestors are due to attend. More details on this meeting can be found here. We look forward to seeing you there!
Your ticket for the: Eastleigh's monster housing plan hit by rail and water double whammy


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Mirabelle Plums
Mirabelle Plums Puzzle Details:
About: The Mirabelle plum, also known as mirabelle prune or cherry plum is identified by its small, oval shape, smooth-textured flesh, and especially by its red,or dark yellow color which becomes flecked in appearance. Mirabelle plums are known for being sweet and full of flavour. They are used in fruit preserves and dessert pies, and its juice is commonly fermented for wine or distilled into plum brandy.
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Case Of Plums
Plums come in a wide variety of colors and sizes. Plums are produced around the world, and China is the world's largest producer. Some are much firmer-fleshed than others, and some have yellow, white, green or red flesh, with equally varying skin color. Plums can be eaten fresh or used in jam-making or other recipes. Dried plums are also sweet and juicy and contain several antioxidants. Dried, salted plums are used as a snack, sometimes known as saladito or salao.
Freshly Picked Cherries
In today's fun and challenging puzzle we feature some freshly picked cherries. Cherries are a good source of fibre, vitamins and minerals, including potassium, calcium, vitamin A and folic acid. They also contain antioxidants that are vital for good health as they protect our cells from damage caused by oxidants. Cherries blossom in April (in the Northern Hemisphere) and the peak season for the cherry harvest is in the summer. In southern Europe in June, in North America in June, in England in mid-July, and in southern British Columbia (Canada) in June to mid-August. In the Southern Hemisphere, cherries are usually at their peak in late December and are widely associated with Christmas.
Freshly Backed Cinnamon Rolls
A cinnamon roll is a sweet roll served commonly in Northern Europe and North America. Its main ingredients are flour, cinnamon, sugar, and butter, which provide a robust and sweet flavor. In some places, it is eaten as a breakfast food and is served with cream cheese or icing. The size of a cinnamon roll varies from place to place.
A new fun and challenging puzzle featuring a bunch of different colored peppercorns. The peppercorn is the dried berry of a climbing vine, used whole as a spice or crushed or ground to make pepper.
Freshly Picked Produce
We've just got back from the greengrocer's with some delicious, freshly picked produce -carrots, tomatoes, apples, strawberries, grapes, peaches, kiwis. Click start and put the fruits and vegetables in today's new puzzle back together as fast as you can and get your spot on our leader boards.
Apples Ripening In The Sun
Click start and join us in the apple orchard. Put the pieces of this fun puzzle back together and see juicy apples ripening in warm summer sun. Apple crops ripen at different times of the year according to the cultivar. Apple cultivars ripen at different times of the year; in the summer include 'Gala', 'Golden Supreme', 'McIntosh', 'Transparent', 'Primate', 'Sweet Bough', and 'Duchess'; fall producers include 'Fuji', 'Jonagold', 'Golden Delicious', 'Red Delicious', 'Chenango', 'Gravenstein', 'Wealthy', 'McIntosh', 'Snow', and 'Blenheim'; winter producers include 'Winesap', 'Granny Smith', 'King', 'Wagener', 'Swayzie', 'Greening', and 'Tolman Sweet'. So what's your favorite type of apple? Solve this fun and colorful puzzle and let us know. have fun!
Red Camargue Rice
Another fun and challenging puzzle is here. In this new one we feature lots and lots of red Camargue rice grains. If you didn't know, Camargue red rice is a variety of red rice cultivated in the wetlands of the Camargue region of southern France. Red rice is a variety of rice that is usually eaten unhulled or partially hulled, and has a red husk, rather than the more common brown. It has a nutty flavor and the highest nutritional value of rices eaten with the germ intact.
Grapes, Apples And Bananas
Get your vitamins and minerals the natural way with a delicious piece of fruit. In this fun new game we have some apples, green and red grapes and a couple of ripe bananas. If you didn't know by know regular consumption of fruit is generally associated with reduced risks of several diseases and functional declines associated with aging. Most fruit are high in fiber, vitamins, and water. Pick a difficulty level, start the game and put the fruit plate back together one piece at a time for a relaxing puzzle solving time.
Freshly Brewed Coffee
Put the freshly brewed coffee mugs, and the coffee beans around them, back together piece by piece and complete today's challenge. Coffee is one of the most popular drinks in the world. It is darkly colored, bitter, slightly acidic and has a stimulating effect in humans, primarily due to its caffeine content. Sugar, milk or cream are often used to lessen the bitter taste.
Today's puzzle features a bunch of juicy peach fruits. The peach, Prunus persica, is a deciduous tree, native to China and South Asia, where it was first cultivated. It bears an edible juicy fruit also called a peach. Peaches and nectarines are closely related, even though they are regarded commercially as different fruits. Nectarines belong to the same species as peaches. Nectarines have smooth skin, while peaches have fuzzy skin; genetic studies suggest nectarines are produced due to a recessive allele, whereas peaches are produced from dominant allele for fuzzy skin.
The cucumber originated in India. It has been cultivated for at least 3,000 years, and was probably introduced to other parts of Europe by the Greeks or Romans. The cucumber is listed among the foods of ancient Ur, and the legend of Gilgamesh describes people eating cucumbers. Cucumbers are classified as accessory fruits. Much like tomatoes and squash they are often also perceived, prepared and eaten as vegetables.
In this new jigsaw puzzle you will have to piece back together lots and lots of pistachios. The pistachio, a member of the cashew family, is a small tree originally from Central Asia and the Middle East. The tree produces seeds that are featured in this jigsaw.The kernels are often eaten whole, either fresh or roasted and salted, and are also used in pistachio ice cream, kulfi, spumoni, historically in Neapolitan ice cream, pistachio butter and confections such as baklava, pistachio chocolate, pistachio biscotti and cold cuts such as mortadella. Some people even make pistachio salad, which includes fresh pistachios or pistachio pudding, whipped cream, and canned fruit.
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Home Back Issues Volume 1 - 10 Volume 10
Volume 1 - 10
Volume 11 - 20
Garden Updates
Musa Species and Related Plants
Bananas or scientifically known as Musa species belonging to the family Musaceae are known to originate from Southeast Asia and wild bananas can still be found in Malaysia, Philippines, Indonesia and Papua New Guinea. The genus name Musa commemorates the Roman physician Antonius Musa.
Sometimes in mid 18th century, Carl Linnaeus, a Swedish medical professor turned Botanist named the cooking banana or plantain as Musa paradisiaca L and the dessert banana as Musa sapientum L. These names were used for almost two centuries until later when various cultivars or varieties were produced which deviated from the typical plantains and dessert bananas in their morphological characteristics. Due to the complications caused by these variations, a new classification system was recommended and it was concluded that the edible bananas originated from two wild bananas with seeds, that is, Musa acuminata Colla and Musa balbisiana Colla endemic to Southeast Asia. A mixture of natural selection and cross breeding involving these two species of bananas gave rise to the many cultivars or varieties of edible bananas of today. From Southeast Asia bananas were brought to India, east Africa and the islands of the Pacific and today banana is one of the world's important food crops.
Feature Garden
A Collector's Garden
When I assigned the photographer to Puan Juriah's house to take pictures of her garden I was guilty of not telling him that there is no theme to look out for the garden. It is a garden with plants that fascinate me! And the lady collects begonias.
Having to direct the reshoot, to ensure that we do not miss the ambience of the garden, feel the harmony in the little ecosystem that the plants have created was a good excuse to return to Juriah's house. Apart from the excellent tea she served, I enjoyed discussing with her pure gardening, with tips on how to keep your plants 'happy' in the garden.
The plot for the single detached house in Kepong in the vicinity of the Forest Reserve Institute Malaysia, is not very large and the house occupy most of the land. However, our lady gardener has made full use of her available space and she has landscaped the road reserve as well. The African daisies growing out there are in bloom, adding cheerful colours to the surrounding greenery.
Garden Gallery
Kuala Lumpur Orchid Garden
Grammatophyllum, Bulbophyllum, Paphiopedilum what frightful words! Ah…, but if you will allow me, I would like to take you up the hill where we can put some identity to these strange names. This hill, in the heart of the city of Kuala Lumpur, is the home of the largest family of flowering plants - the orchids whose many relatives are located all over the world. From the wild species to the current special hybrids, members of this family have spread to different parts of the world. Come and I will introduce you to a few more popular varieties living at the Orchid Garden on the hill so you won't fight shy of the names they have adopted through their 'cross marriages'. Shall we get started?
Here, at the Orchid Garden, many of the orchid members sit around busking in their glory while others perch on branches and tree trunks waiting to be admired and loved. Look over here, isn't this flower beautiful? Look at the striking colours and size of the blooms. The largest member here has been commonly named "Tiger Orchid"- perhaps because of the coloration. Well, this is the Grammatophyllum. Over here is the native terrestrial orchid with its very prominent lips. These are the Bulbophyllum. Then there are the more common and numerous members with their voluptuous round flowers of various colours. These belong to the genus Vanda with Vanda Miss Joaquim as an example. Many other members will be looking forward to the days for relatives from all over the world to come together for a grand reunion at the 17th World Orchid Congress to be held on 24th April – 2nd May 2002 at the Mines International Exhibition Centre. Imagine what a show that will be!!!
Young Gardener
Inspiration from Nature - What inspires you?
From the mighty red wood trees in America to the smallest worker ants in the tropics, nature and its splendor has inspired and taught us amazing things. Nature has brought to us ideas that have changed our way of life; let's face it, if it were not for that apple that fell on Newton's head, we would still not know what gravity was. Nature has also stirred the souls of artists to create masterpieces such as the wildlife paintings by Janet N. Heaton:
Garden Science
Guide To Flowering Potted Plants
Lantana is a very popular bedding plant here and they are very easy to care for. There are now many colours to chose from and can be free flowering.
Care: When in bloom they are striking but after the blooms have dropped the stems and leaves look straggly so they should be cut back and pruned to encourage new growth. Propagation is through seeds or stem cutting.
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