I took the terrain squares to the club this afternoon for a game of Spearhead.
First up, they went together OK (well just about) on one table. There was a sizable overlap which meant that there was no leaning on the table. There were no serious accidents.
My opponent Jon asked to be Germans. I knocked up 2 different defend lists and a German list I had prevously used here. This one has Pz Iv's. Keith seems to be the only person I know that likes PzIV's. I brought my Russian Cavalry division as I've never used it on table, and as an afterthought packed my US army if I had to defend (I have yet to think out a defend list for the Russians).
So of course I am defending.
2 infantry battalions with M36 TD's and M15/M16 AA as infantry choppers. A tank battalion at the rear completed the deployment.
Deployment on the right flank. Infantry battalion at right top, with the tank battalion bottom left.
Left flank with most of the support troops deployed forward.
Jons list had 4 battalions of ~11 stands. 1 Pz IV H, 1 Pz grenadier and 2 infantry. His plan was a frontal attack across the front. He used the infantry units on the flank and the armoured units in the center.
As the game developed on the left the german infantry launched an all out assault on the US positions. The US tank battalion attempted to envelope the center thrust at the bottom right.
In the center the german armoured attack was flanked by the US armoured battalion. Lead by an M4 Jumbo (US players, don't lead your tank units with anything else) and aided by some bad luck with the dice on the German end the Pz IV's died as usual.
I forgot to record the rest of the game, but the German infantry units were eventually broken by the US infantry. For a change my dice were not abysmal and I didn't manage to slaughter my troops.
Takeway lessons? 4 small German battalions in an attack list doesn't work that well, and Pz IV's are crap.
I enjoyed reading this. PzIVs aren't crap but they are going to struggle in frontal attacks, especially when encountering M36s and Jumbos!


Please join us Sunday, October 16th, from 3PM-6PM for the Sansom Street Block Party - hosted by Liberti! This year we are encouraging our friends and neighbors on the block to help make this year's Block Party a huge community event! Federal Donuts, The Happy Rooster and Dizengoff are all going to be helping to serve food and drinks this year! Find out more and how you can connect here!
We are hosting a ministry fair after the service on Sunday 9/25! If you are looking for a place to serve using your God-given talents and gifts, please come check out all of the ways that you can get involved in what God is doing through Liberti Church! There will be plenty of material available to help you find the perfect place to serve in-our-church or in-our-neighborhoods!
The first step in becoming a member at Liberti Church is to attend an In-covenant class, an informal time to meet with church leaders to discuss Liberti's mission and vision. If you attend Liberti and are considering becoming a member, please join us on October 9th immediately following the service to explore becoming In-covenant! Lunch will be provided. We hope to see you there! Contact Ken if you would like to attend or would like more information!
MLCF is designed to help our kids develop Christian fellowship, a deep identity in Christ, a posture of worship, a heart for service, and a relationship with God that extends beyond us, the parents. We are happy to include kindergarten through 6th graders, as well as preschoolers who turned 4 by Sept. 1. Children will participate in a small group specific to their age. Our upper elementary class is expanding to include 4-6th grade. For more information click here!
Liz Spiegler leads an international student ministry through Intervarsity Christian Fellowship at Temple University, where she offers Bible studies for non-Christian international students. This ministry has been an incredible opportunity to spread the Gospel among the nations that are coming to the US, many of which still have large numbers of unreached and hard-to-reach people groups. Liz is currently building a team of prayer partners and financial supporters. If you missed Liz during coffee hour you can email her if you are interested in learning more about this ministry and ways of supporting it!
We look forward to our home groups getting started again this fall, during the week of September 11th-17th. There will be sign-ups online and at our services starting Sunday, August 28th. For more info, please check out our groups page on our website here.


I think it's probably a good thing that social media was not a thing when I was a new mum. Like most parents I believed that my babies were adorable angels. I probably (definitely) would have totally spammed all of my channels with endless baby photographs.
OK I admit it I still adore them even thought they are all mostly taller than me. And I may do a bit of spamming anyway.
I even have olde worlde paper photographs of of my eldest child aged about three weeks having a poo on his blanket in the garden while he was enjoying some nappy-free time! (sorry Jacob) Imagine if I could have shared those on Instagram instead of just those geographically close to me? Luckily for him Instagram was not in existence back then. Hashtag #gross #poo #WhatDidIEat?
Although I think my children are the most precious and wonderful people in the world it's actually true of course that all babies are amazing!
They bring their own special form of magical happiness to everyone around them, and they always know how to somehow put a smile on your face or make you laugh. You may know that babies can help save lives by doing nothing more than wearing Pampers because Pampers donates 1 vaccine against maternal and newborn tetanus for every pack of Pampers nappies and wipes sold through the "1 Pack = 1 Vaccine" Pampers-UNICEF campaign.
And now, if you share a photo of your amazing baby with #1photo1vaccine or #PampersUNICEF, on Facebook, Twitter or Instagram – Pampers® will also donate the equivalent cost of one vaccine!
The vaccination donation campaign is now in its 11th year, and during that time, amazing babies (with help from their amazing parents) around the world have helped Pampers and UNICEF to eliminate maternal and newborn tetanus in 19 countries – with only 19 more to go, they are halfway towards the goal of global elimination!
Thanks to the support of families, since the Pampers-UNICEF "1 pack=1 vaccine" campaign began, an estimated 500,000** newborn babies have been saved (** Based on Child Health Epidemiology Reference Group (CHERG) of WHO and UNICEF (Lancet, October 2014) and a vaccine has reached a mother and her baby every second.
If that doesn't make you feel warm and fuzzy, check out the video below for some cute baby-ness.
Campaigns like this make me proud to be a blogger with my own little corner of the internet where I am able to share news about campaigns like this.
I am not alone in my pride - celebrity mum and former Girls Aloud singer Kimberley Walsh who is supporting the Pampers-UNICEF campaign said: "I feel hugely honoured to be supporting the Pampers-UNICEF campaign in its 11th year. As a mum to Bobby, and expecting my second child later this year, I feel great empathy with other mothers around the world who, just as I do, want nothing more than to deliver a happy, healthy baby.
She added:"The reason I'm so passionate about this campaign is that mums and dads here in the UK can make a very real difference by doing nothing more than buying the Pampers that they need for their little ones. It's phenomenal and makes me feel very proud of what we can achieve together."
It really is that simple - buying nappies and sharing photos can make a real impact on the lives of tiny babies across the globe.
So, to recap -there are 3 ways YOU can help save newborn babies and their mums.
1. Share a photo of your amazing baby with the hashtags #1photo1vaccine #PampersUNICEF on Facebook, Twitter or Instagram.
3. Donate to UNICEF. Sign up to donate to UNICEF today and you can join thousands of other parents who give to improve the lives of these vulnerable children. This is something people like me with older children past the nappy-wearing and cute baby pic years can do to help.
It really is that simple - buying nappies, sharing photos and making even small donations can make a real impact on the lives of tiny babies across the globe as with our help Pampers® and UNICEF can help protect the world's amazing babies against newborn tetanus.
Disclaimer: Post produced in collaboration with Pampers.


text:
+++
Talk_date = ""
Talk_start_time = ""
Talk_end_time = ""
Title = "The Kubernetes Hype - Do you really need it?"
Type = "talk"
Speakers = ["renata-rocha"]
+++

K8S is everywhere today, and if you don't LOVE it, you're not cool. But does your infra really NEED it? A quick check on what K8S is, what it isn't, what is it used for, why people love it and why it may not solve your problems at all!

redpajama_set_name: RedPajamaGithub


Just six weeks after the global reveal of the all-new 2017 Honda Ridgeline at the 2016 North American International Auto Show, the SEMA Garage is proud to announce the aftermarket industry's first measuring session. Don't miss this opportunity to get up-close and personal with this exciting new player in the midsize pickup truck segment. With dramatically improved design and packaging, as well as an industry first in-bed audio system, this second generation Ridgeline will once again set new standards for truck innovation. This session is sure to be well attended, so reserve your space now to attend this one-day-only measuring session. This event is limited to SEMA members only.
Honda staff will be on-hand to assist with any product disassembly, as well as answer any technical questions. Photography will be permitted for product development needs only. Vehicles present will be pre-preduction, so some limitations may exist. Feel free to contact Jim Moore ahead of time should you have any questions.


Scientists increasingly agree with the poem about the direct human experience: we are more than just atoms and molecules that make up the body of us, we are beings of light. Biophotons are emitted from the human body, can be released by mental intention, and could modulate the fundamental processes within the communication between cells and DNA.
Nothing is more amazing than the fact extremely improbable that we exist. Often we ignore this fact, forgetting the reality that instead of being something there, could there be anything, that is why there is a universe (pithy of conscious of himself through us) and not some completely unconscious of the vacuum itself?
Keep in mind that light, air, water, and minerals of the earth's crust, and from information at least 3 billion years contained in the cell nucleus of a diploid zygote is formed, the human body, and the body of a soul able at least to try to understand his bodily and spiritual origins.
Given our existential condition, insanity and bodily incarnation as a whole, and considering that our earthly existence is partially composed of sunlight and require continuous consumption of light condensed in the form of food, would not sound too exaggerated as our body emits light.
Indeed, the human body emits biophotons, also known as ultra-weak photon emission (ultraweak photon emissions-UPE), with a visibility of 1 000 times lower than our eye sensitivity. Though not visible to us, these particles of light (or where depends on how do you measure them) are the visible part of the electromagnetic spectrum (380-780 nm) and are detectable by sophisticated modern instrumentation.
The eye itself, which is continually exposed to strong ambient photons that pass through the various ocular tissues, emits the photon emission induced by ultra weak light visible. It was released even hypothesize that visible light induces bioluminescent delayed within the eye tissue exposed, providing an explanation for the origin of the remaining retinal image.
The hypothesis of Bókkon suggests that photons released by chemical processes within the brain produce images during visual imagery biophysical, and a recent study has found that when subjects were actively imagining light in a very dark medium, their intention has produced a significant increase in photon emissions ultraweak.
This is consistent with an emerging point of view according to which biophotons are not only the cellular-metabolic byproducts but rather because the intensity of the biophotons can be higher inside the cell than outside. It is possible that the mind can access this gradient (difference) energy to create the intrinsic perception of biophysical during visual imagery.
Cells and our DNA uses biophotons to store and communicate information.
Apparently, biophotons are used by the cells of many living organisms in order to communicate, which facilitates the transfer of energy/information that is a couple of orders of size faster than diffusion. According to a study from 2010, "Communication from cell to cell by biophotons has been demonstrated in plants, bacteria, granulocytes neutrophils and the renal cells.
The researchers were able to prove that ".. .the specter through the stimulation of light (infrared, red, yellow, blue, green and white) at one end of the sensor or spinal nerve root engine resulted in a significant increase in biophotonics activity at the other end. " Researchers have interpreted their discovery suggesting that stimulation by light could generate biophotons that circulate along nerve fibers, perhaps as the neural communication signals ".
Because your body's metabolism change in a circadian manner, biophotons emissions also vary along the time axis. Research has been made, distinct anatomical locations of the biophotonics where the emissions are stronger and weaker, depending on the time of day.
Photon counting fluctuations in general within the body were lower in the morning than the afternoon. Thorax-abdomen region is less and more steadily. Upper limbs and head region broadcast most and ever more intense throughout the day.
Spectral analysis of low emissions and high intermediate from the top front of the right foot, the forehead and palms in the range of sensitivity of fotomultiplicatorului showed a wider contribution to the emission spectrum of the domain 420-470 spontaneous than a hand in autumn/winter. Luminescent spectrum shifted from hand showed a significant release in the same domain as the spontaneous emission.


Robert "Bob" Pierce, age 65, of Sioux Rapids, Iowa died on Monday, March 18, 2019 at the Buena Vista Regional Medical Center in Storm Lake.
Memorial services will be held on Saturday, March 23, 2019 at 10:30 a.m. at the Sliefert Funeral Home in Sioux Rapids. Burial will be in the Lone Tree Cemetery in Sioux Rapids. Visitation will take place Friday, March 22, 2019 from 4:00-7:00 p.m. at the Sliefert Funeral Home in Sioux Rapids. The Sliefert Funeral Home in Sioux Rapids is in charge of the arrangements.
Robert Ray Pierce, the son of Charles and Margaret (Reed) Pierce, was born on February 2, 1954 in Cherokee, Iowa.
Bob was baptized as an infant at the Methodist Church in Sutherland in 1954. He was later confirmed at the Sioux Rapids Methodist Church where he remained a member.
As a child, Bob lived in rural Calumet and Sutherland. He and his family later moved to Sioux Rapids where he attended school from 4th grade until 10th grade. He spent his last two years of high school at Storm Lake High graduating in 1972. After high school, he attended Northwest Iowa Community College.
On June 19, 1976, Bob was united in marriage to Teresa Kirkpatrick in the First Baptist Church in Storm Lake. The couple was blessed with three children: Matthew, Bobbi Jo, and Ashley.
In his earlier years, Bob was a Mason, member of the Sioux Rapids Fire Department, and a part of the Swimming Pool Board.
In his free time, Bob enjoyed going to auctions to collect rakes and shovels, sitting on the deck enjoying nice sunny days, and going to grandkids school concerts and sports activities. He was always helping friends and family with projects of all kinds, especially on Junk Day.
Those left to cherish his memory include his wife, Tess of Sioux Rapids, Iowa; children: Matthew (Christina) Pierce of Spencer, Iowa; Bobbi Jo Butler of Storm Lake, Iowa; Ashley (Juan Fernando) Pierce of Sioux Rapids, Iowa; brother, Ron (Denise) Pierce of Sioux Rapids, Iowa; sister, Becky (Keith) Diersen of Sac City, Iowa; grandchildren: Aria Petersen, Makenna Pierce, Tanner Pierce, Jaley and Jenna Butler, Noah, Gabriela, Esabella Pierce; sisters and brothers-in-law: Karen (Ron) Gifford of Naples, Florida; Connie (Eldon) Dyke of Aurora, Colorado; Jane (Ken) Fedde of Elkhorn, Nebraska; Kerry (Kathy) Kirkpatrick of Ankeny, Iowa; and many nieces and nephews.
Bob was preceded in death by his parents, Craig and Margaret; parents-in-law, Wayne and Mavis Kirkpatrick; brother and sister-in-law, Terry (Rose Mary) Kirkpatrick; grandparents, aunts, and uncles.


text:
The glory days of Reykjavík - 5 places we miss
We have spoken in another article about the must-sees of Reykjavík, those places that have been there forever and continue to prosper. But the Icelandic capital is a changing city, and the tourist influx in recent years has transformed its face. Here we guide you through the streets of Reykjavik of a few years ago to talk about the cafes and places we miss ... and what they have become today.
Tiú drópar - The castle of the ten drops - Laugavegur 27
This café was known and loved for its brunches, waffles and jazz music. In the evening after 6 pm, the café had the appearance of a brasserie and offered wine and cheese platters to be shared. The delightful atmosphere of Tiú drópar made it a fascinating place! It closed in 2016 after 30 years of service Today, it is a Vietnamese restaurant.
Sirkus - Klapparstígur 30
This small house that has sheltered Sirkus for many years is well known to those who know the Icelandic capital well. In the 19th century, it was a grocery store, then it became a bar in 1990. The names and owners followed one after the other, from N1 to Grand Rokk, until Sigga "Boston" bought the venue for 4 million crowns (35,000 euros) in 2000. The bar was then called Sirkus and it became a stage for Icelandic performers and groups. It's audience consisted mainly of musicians and artists from Reykjavík. Björk played and danced regularly, and this certainly helped to make it a place known to travellers – who would spend hours queuing to get in on weekend nights.
This legendary bar closed its doors in February 2008, after eight years of music and crazy nights. The owner of the place, Sigga, opened the bar "Boston" on Laugavegur, after the closing of Sirkus. Sirkus has grown into a Macland store selling computer products and is now part of the Hilton hotel complex.
Faktory - Smiðjustígur 6
This bar, which used to be a concert hall, opened its doors in 2010 and closed again in 2013. It was a short time but long enough to make a name for itself. Faktory was one of the best places to enjoy live music in The Icelandic capital, especially for electro fans. The bar was located right in the heart of a small graffiti covered square where young people enjoyed spending time in fine weather. Their last night in August 11, 2013 was hosted by members of the group GusGus. Today, Faktory no longer exists and all of the buildings in the heart of Smiðjustígur have become a Hilton hotel.
Bakkus - Tryggvagata 22
Bakkus was a bar and nightclub that served cheap beer and offered an impressive selection of vodka. There was always something in Bakkus - a concert, a movie night, a quiz, an organized gathering ... Today, the bar Húrra, which replaces it, keeps a little of that good-natured spirit.
Hemmi og Valdi - Laugavegur 21
Nowadays replaced by the excellent Reykjavik Roasters, Hemmi og Valdi resembled your grandmother's living room and was a nice place to have a coffee or a beer. The choice of music depended on the bartender who worked that day, and with a little luck you could hear a few pieces of the excellent bands A Silver Mount Zion or HangedUp.
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redpajama_set_name: RedPajamaCommonCrawl


text:
Dump Truck Driver Killed in US 50 Crash in Grasonville
Jim Russ
Credit: WBAL's Jim Russ
A fatal crash involving an overturned dump truck closed all lanes of US 50 Westbound on Maryland's Eastern Shore for several hours on Wednesday.
Maryland State Police report that the crash happened in the westbound lanes of US 50 between Nesbit and Hissey Roads in Grasonville in Queen Anne's County just after 9 a.m. on Wednesday.
The driver of the truck, Terry Cox, 43, of White Hall, Maryland was the driver and sole occupant of the truck.
He was pronounced dead at the scene of the crash.
State Police say that the truck, which was loaded with gravel and other debris, ran off the road to the left and overturned in the median.
The majority of load spilled out of the roadway.
State Troopers from the Centreville Barrack and the Crash Team are investigating the cause of the wreck.
Nesbit Road is located between US 301 in Queenstown and the Kent Narrows Bridge.
Follow @JimWBALTraffic
UPDATE: Warren Road Bridge Scheduled To Reopen In September
Growing Concern Over Growing Backups On Eastern Shore
Northbound Harbor Tunnel Reopens
Pedestrian Struck, Critically Hurt By MARC Train In Odenton
Overturned Tractor Trailer Snarls Morning Rush Hour on I-70


The Monastic Martyr Philothea was born in Athens in 1522. Her parents, Syriga and Angelos Benizelos, were renowned not only for being eminent and rich, but also deeply devout. Often the kind-hearted Syriga had implored the Most Holy Theotokos for a child. Her fervent prayers were heard, and a daughter was born to the couple. They named her Revoula.
The parents raised their daughter in deep piety and right belief, and when she was twelve years old they gave her away in marriage. Her husband turned out to be an impious and crude man, who often beat and tormented his wife. Revoula patiently endured the abuse and she prayed to God, that He might bring her husband to his senses.
After three years Revoula's husband died, and she began to labor in fasting, vigil and prayer. The saint founded a women's monastery in the name of the Apostle Andrew the First-Called (November 30 and June 30). When the monastery was completed, the saint was the first to accept monastic tonsure, with the name Philothea.
During this time Greece was suffering under the Turkish Yoke, and many Athenians had been turned into slaves by their Turkish conquerors. Saint Philothea utilized all her means to free her fellow countrywomen, ransoming many from servitude. Once, four women ran away from their Turkish masters, who demanded that they renounce their Christianity, and took refuge in the monastery of Saint Philothea.
The Turks, having learned where the Greek women had gone, burst into the saint's cell, and beat her. They took her to the governor, who threw the holy ascetic into prison. In the morning, a mob of Turks had gathered, and they led her out of the prison. The governor said that if she did not renounce Christ, she would be hacked to pieces.
Just when Saint Philothea was ready to accept a martyr's crown, a crowd of Christians assembled by the grace of God. They pacified the judges and freed the holy ascetic. Returning to her monastery, Saint Philothea continued with her efforts of abstinence, prayer and vigil, for which she was granted the gift of wonderworking. In Patesia, an Athens suburb, she founded a new monastery, where she struggled in asceticism with the sisters.
During the Vigil for Saint Dionysius the Areopagite (October 3), the Turks seized Saint Philothea and tortured her. Finally, they threw her down on the ground half-dead. The sisters tearfully brought the holy martyr, flowing with blood, to Kalogreza, where she died on February 19, 1589. Shortly thereafter, the relics of the holy Monastic Martyr Philothea were brought to the Athens cathedral church.


text:
Q: Distribution of two independent random variables a) If $Z_1$ and $Z_2$ are independent standard normal random variables, what is the distribution of $Z^2_1 +Z^2_2$?
b) Let $X$ and $Y$ be independent exponential random variables with mean $3$. What is the c.d.f of $X/Y$ ?
I understand that when two r.v. are independent, you can say that the joint c.d.f is the product of the two c.d.f.. But after that I'm lost with the squared r.v. or $X/Y$.

redpajama_set_name: RedPajamaStackExchange


text:
Q: longformer-base-4096 (pytorch transformers) RuntimeError: grad can be implicitly created only for scalar outputs I am trying to fine-tune longformer with a custom dataset. I created a basic example with the documentation from hugging-face transformers. I receive the mentioned error. "
RuntimeError: grad can be implicitly created only for scalar outputs "
train_data = load_dataset('csv', data_files='C:/Users/user/Desktop/result/train.csv')

test_data = load_dataset('csv', data_files='C:/Users/user/Desktop/result/test.csv')
model = LongformerForSequenceClassification.from_pretrained('allenai/longformer-base-4096',
                                                   gradient_checkpointing=False,
                                                       attention_window = 512,
                                                       num_labels=2)

tokenizer = LongformerTokenizerFast.from_pretrained('allenai/longformer-base-4096', max_length = 1024)

def tokenization(batched_text):
   return tokenizer(batched_text['msg'], padding = 'max_length', truncation=True, max_length = 1024)

train_data = train_data['train'].map(tokenization, batched = True, batch_size = len(train_data))

test_data = test_data['train'].map(tokenization, batched = True, batch_size = len(test_data))

train_data.set_format('torch', columns=['input_ids', 'attention_mask','bull'])

test_data.set_format('torch', columns=['input_ids', 'attention_mask','bull'])

# define the training arguments
training_args = TrainingArguments(
    output_dir = 'Z:/crypto/aa/',
    num_train_epochs = 2,
    per_device_train_batch_size = 1,
    gradient_accumulation_steps = 16,
    per_device_eval_batch_size= 16,
    evaluation_strategy = "epoch",
    disable_tqdm = False,
    load_best_model_at_end=True,
    warmup_steps=200,
    weight_decay=0.01,
    logging_steps = 4,
#fp16 = True,
    logging_dir='Z:/crypto/aa//logs',
    dataloader_num_workers = 0,
    run_name = 'longformer-classification-updated-
    rtx3090_paper_replication_2_warm'
)

trainer = Trainer(
    model=model,
    args=training_args,
    train_dataset=train_data,
    eval_dataset=test_data
)
device = 'cuda' if torch.cuda.is_available() else 'cpu'
device

trainer.train()


text:
HomeHarley Davidson NewsPOLICE NEWS: Man attacked, beaten by group
POLICE NEWS: Man attacked, beaten by group
January 20, 2018 Craig Ballantyne Harley Davidson News 0
A Goshen man was injured after he was beaten by a group of people Thursday night.
Goshen police said the 24-year-old, whose name they did not release, was attacked by several suspects he knows around South 14th Street and College Avenue around 9:30 p.m. Thursday.
The man was taken to Goshen Hospital to receive treatment for a minor cut over his left eye and scratches on his legs, police said.
• Angela Vance, 46, 53945 Cedarcrest Court, Bristol, was arrested by Elkhart County police on a charge of operating a vehicle while intoxicated at C.R. 39 and Ind. 119 in Goshen around 7:15 p.m. Thursday.
• Starlin Hicks, 19, 104 S. Franklin St., Goshen, was arrested by Goshen police on a charge of possession of marijuana following a traffic stop in the 2500 block of East Kercher Road around 9:30 a.m. Thursday. Hicks was released at the scene with a citation to appear in court.
• Danilo Diaz, 19, Elkhart, was arrested by Goshen police on charges of illegal consumption of an alcoholic beverage by a minor and driving without a license after police said he drove his vehicle onto railroad tracks near Ninth and Madison streets around 5:15 a.m. Friday. Diaz was released at the scene with a citation to appear in court.
• Goshen police arrested a juvenile after receiving a call the child was being incorrigible at Chamberlain Elementary School, 428 N. Fifth St., around 1:45 p.m. Thursday. The juvenile was released to a parent with a citation.
• Elizabeth Wortinger, Goshen, reported to Elkhart County police she was battered by someone she knows at a home in the 68000 block of C.R. 33 around 7:45 p.m. Wednesday.
• A juvenile was arrested by Goshen police on a charge of battery after staff at Goshen High School reported a fight at the school, 401 Lincolnway East, around 8 a.m. Thursday.
The suspect was released to a parent with a citation, police said. The injured student was treated at the school for moderate injuries.
An employee at Interra Credit Union in Goshen reported to Goshen police a bank member cashed three fraudulent checks at three different branches on Jan. 4. The report was made Thursday from the branch at 300 W. Lincoln Ave.
• Reece Barrett, Elkhart, reported to Elkhart County police Thursday his Harley Davidson motorcycle was stolen from a location at 13183 Ind. 120 in Bristol in November.
• An employee at Wellington & Weddell Eye Care reported to Goshen police a pair of sunglasses was stolen by a known suspect from the store, 116 W. Washington St., around 12:45 p.m. Thursday.
ABSENT WITHOUT LEAVE
Phillip Estes, 37, Elkhart, was deemed absent without leave after staff at the Elkhart County Work Release Center reported to Elkhart County police Wednesday Estes failed to return to custody around 10 a.m. Tuesday.
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August 18, 2017 Craig Ballantyne Harley Davidson News 0
We've always imagined police officers doing the rounds of any city in India on either Royal Enfields or other commuter bikes but Harley-Davidsons? The Kolkata police has recently inducted brand new Harley-Davidson bikes into their […]
Jefferies Group LLC Reaffirms "Hold" Rating for Harley-Davidson Inc (HOG)
May 4, 2017 Craig Ballantyne Harley Davidson News 0
Harley-Davidson Inc (NYSE:HOG)'s stock had its "hold" rating restated by research analysts at Jefferies Group LLC in a research note issued to investors on Thursday, April 6th. They presently have a $ 49.00 price target […]


text:
Burnaby society giving away 6,000 computers to low-income families
Janaya Fuller-Evans / Burnaby Now
Tech wanted: Mary-Em Waddington, executive director of the B.C. Technology for Learning Society, says they need more computers to help low-income families.
Photograph By File photo/BURNABY NOW
Computers for Schools, run by the British Columbia Technology for Learning Society, will be distributing about 6,000 computers to low-income families in British Columbia.
It's part of the Connecting Families initiative by the federal government, which aims to provide low-income families with $10 monthly Internet service and give up to 50,000 computers to those in need.
Computers for Schools is a partnership between the provincial and federal governments and private industry, and collects and refurbishes donated used computers for B.C. schools.
The initiative launches in October and is expected to wrap up by March 2022, according to Mary-Em Waddington, the executive director of B.C. Technology for Learning Society.
"It's going to mean a lot to students and their families in the school year, but we can't have success without donations," she said. "So this is a call to action for companies and even individuals that when they have computers they'd like to get rid of, that they think to donate to us so that we can repurpose them and put them back into family homes."
The program accepts desktop computers, monitors, smartphones and tablets, printers, networking devices, laptops, and more. They are always looking for laptops, she added.
This initiative is an opportunity for the technology sector, as more young people will have access to technology, meaning more potential employees in the future, Waddington said.
"We have an opportunity for B.C. to expand its technical skills; in particular the IT sector is always looking for new talent," she said. "So this is just opening up another door to find that talent as well."
To donate to the initiative, go to www.reusetechbc.ca/donate.html to learn the donation requirements.
11% of Burnaby food businesses got 'high' risk ratings in 2019 inspections
11% of Burnaby food businesses got 'high' risk ratings in ...


Slim pants with zip pockets.
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Print Page - What are the two PWM pins on the Tinilily?
Title: What are the two PWM pins on the Tinilily?
What are the two PWM pins on the Tinilily?
Are they just the pin labeled "3", and the one pad in the center named "MOSI" (which when coding, would be called as pin 11, I believe). Are those the two?
Title: Re: What are the two PWM pins on the Tinilily?
Sorry this sat so long! Yes, pin 3 is the only easily accessible PWM pin, MOSI/11 is one as well and seems to be labeled correctly in the image!


text:
\section{Introduction}
Accurate prediction of energy radiation from compact object binaries emitted via gravitational waves (GW), is one of the crucial inputs to predict dynamics of the binary system. The behavior of gravitational field at future null infinity is not just dependent on \textit{instantaneous} dynamics of the binaries  at the same retarded time, but also dependent on the past history of the system due to non-linearity of Einstein's field equation \cite{blanchet2014}. The latter contribution is called \textit{hereditary} \cite{Blanchet:1987wq,Blanchet:1992br,Blanchet:1993ec} understood within the framework of post-Newtonian (PN) theory and multipolar post-Minkwoskian (MPM) expansion \cite{Blanchet:1985sp, Blanchet:1989ki} and effective field theory approach \cite{Galley:2015kus}.
Since more attention has been paid on bound orbits \cite{abbott2017gw170817,abbott2017multi, abbott2019gwtc,abbott2021gwtc,venumadhav2020new} in GW/multi-messengers astronomy, energy radiation as well as angular momentum radiation from bound orbits were already computed upto the third post-Newtonian (3PN) order, which indicates $1/c^6$ ($c$ is speed of light) correction to leading order term, in \cite{arun2008inspiralling,arun2009third,Arun:2007rg} long ago in both instantaneous/hereditary contributions. On the other hand, highly accurate description on unbound orbits is getting more attention today in several complementary methodologies \cite{Cho:2018,thefirst,Kalin:2020lmz,Dlapa:2021vgp,Dlapa:2021npj,Liu:2021zxr}, because of its direct usages such as for detection in LIGO, LISA and IPTA \cite{garcia2018gravitational,mukherjee2020detectability,kocsis2006detection,burke2019astrophysics}, and its astronomical applications to gravitational captures \cite{bae2020},  and also the fact that analytic solutions describing dynamics of unbound orbits have comprehensive information on both bound and unbound orbits \cite{Kalin:2019rwq,Kalin:2019inp,Cho:2021arx}.  \\
In this work, we compute the hereditary contribution of energy radiation ($\Delta {\cal E} $) during hyperbolic and parabolic scattering of non-spinning compact objects upto 3PN order. This is a sequel of Ref.~\cite{thefirst}, where 3PN instantaneous contribution of $\Delta {\cal E} $ and angular momentum  radiation ($\Delta {\cal J} $) were computed. By Ref.~\cite{thefirst} and this work, we complete 3PN energy radiation. Historically, the leading (Newtonian) order energy radiation was computed in \cite{Hansen:1972jt}, and the extension to 1PN order was made in \cite{blanchet1989}. And post-Minkowskian (PM) result was computed at the leading $G^3$ order in \cite{Herrmann:2021} ($G$ is Newton's constant).
Recently, the hereditary contribution of both $\Delta {\cal E} $ and $\Delta {\cal J} $  was tackled in \cite{Bini:2021qvf} partially upto  $1/j^7$ order, at the leading order of each tail, tail-of-tail, tail-squared pieces. In independent way, we compute all pieces of the hereditary contribution upto 3PN order including next-leading order of tail piece, and provide upto $1/j^{15}$ or $1/j^{16}$ order in large-$j$ (or, large eccentricity) expansion. Since taking large angular momentum approximation after PN approximation sequentially is equivalent to small energy approximation after PM expansion, this is corresponding to compute upto $G^{15}$ (for tail), and $G^{16}$ (for tail-of-tail, tail-squared) orders. The reason that the aimed $G$ order is different is that our purpose is not only providing a truncated solution in a certain $G$ order, but provide a decent approximation with 12 terms for practical usages. Since tail piece starts at $G^{4}$ order, while tail-of-tail and tail-squared pieces start at $G^{5}$ order, they could end at the different orders. Also, for this reason, we work with two variables, angular momentum and eccentricity to characterize hyperbolic orbits. We will see that this choice exhibits remarkable convergence in Sec.\ref{sec:parab}.
\par
This paper is organized as what follows. In Sec.\ref{sec:formalism}, we explain all inputs needed for entire computation. Next, we do the main computation. The three different pieces are solved via several strategies adopted for each pieces, leading order of tail in Sec.\ref{sec:tail}, leading order of tail-of-tail, tail-squared in Sec.\ref{sec:tails} and 1PN correction of tail in Sec.\ref{sec:1PNtail}. In Sec.\ref{sec:parab}, we provide exact value of energy radiation from parabolic orbits, and it will be compared to hyperbolic energy radiation. In Appendix.\ref{elementaryintegral}, some required integrals are computed exactly. In Appendix.\ref{sec:fullresult}, we collect all contributions upto 3PN and from $G^3$ to $G^{15}$ including the instantaneous part. In the ancillary file accompanied with this paper, every results are provided in \textit{Wolfram} language.

\section{Formalism \& Notations}\label{sec:formalism}
\iffalse
In an effort of solving Einstein's field equations for binaries, we usually assume gravitational field $g$ perturbed from Minkowskian background $\eta$ as
\begin{align}
g(x)=\eta+h(x)\,,
\end{align}
with $|h|\ll1$ and $x$ being space-time coordinates. (Here, we omit indices of tensors).
Here, we attempt further decomposition of the perturbation $h$,
\begin{align}
h(x) = \bar{h}(x)+\tilde{h}(x)\,,
\end{align}
where $\bar{h}$ represents short-distance while $\tilde{h}$ represents long-distance mode. In harmonic gauge $\partial_\mu h^{\mu\nu}=0$, Einstein's field equation $$G[g]=\frac{8\,\pi\,G}{c^4} T[g,\phi]$$ with a matter field $\phi(x)$, reduces down to a d'Alembertian equation
\begin{align}
\Box h\sim T [h,\phi]+\Lambda [h]
\end{align}
where $\Box=\eta^{\mu\nu}\partial_\mu\partial_\nu$ and $\Lambda$ represents all non-linear combination of $h$, and $[\cdots]$ means functional dependence. By solving $\bar{h}$ as a functional of $\tilde{h}$ and $\phi$,  $\bar{h}=\bar{h}[\tilde{h},\phi]$, and inserting it back into the original equation of motion, one will get a wave equation only for $\tilde{h}$, and its solution is written schematically as
\begin{align}
\tilde{h}=\Box^{-1}\, \hat{T}_{0} (x)+ \sum_{n=1}^{\infty}\,\Box^{-1}\,\big[(\tilde{h})^n\,\hat{T}_{n} (x)\big]\,,
\end{align}
where $(\tilde{h})^n$ stands for some algebraic combinations including derivatives between $n$ $\tilde{h}$, and $\Box^{-1}$ is the anti-derivative of d`Alembertian operator with retarded boundary condition. Any fluxes $\mathcal{F}$ can be computed by integrating squared terms $\sim(\tilde{h})^2$ over sphere at infinity
[kipthorne, ross]. In [], we ignored  all $\hat{T}_{n}=0$ except $\hat{T}_{0}$. The contribution that is computed only by $\Box^{-1}\hat{T}_0(x)$ is called instantaneous, and otherwise it is called hereditary. Upto 1PN order, the instantaneous contribution is sufficient, whereas starting from 1.5PN order, we cannot ignore $\hat{T}_1$ and $\hat{T}_2$ contributions appearing at 1.5PN and 3PN respectively,
\begin{align}
&\mathcal{F}\sim \int R^2\,d\Omega (\tilde{h})^2\notag\\[1ex]
&=\underbrace{\big(\Box^{-1}\hat{T}_0\big)^2}_{\text{instantaneous}}+\underbrace{2\,\big(\Box^{-1}\hat{T}_0\big)\,\Box^{-1}[\big(\Box^{-1}\hat{T}_0\big)\hat{T}_1]}_{\text{tail}}\\[1ex]
&+\underbrace{\Big(\Box^{-1}[\big(\Box^{-1}\hat{T}_0\big)\hat{T}_1]\Big)^2}_{(\text{tail})^2}+2\,\big(\Box^{-1}\hat{T}_0\big)\,\Box^{-1}[\big(\Box^{-1}\hat{T}_0\big)^2\hat{T}_2]\notag\\[1ex]
&+
\end{align}

This has been done in []. Energy flux in terms of multipole moments is given in[], and multipole moments in terms of dynamical elements of binaries $r, \phi, \frac{dr}{dt}, \frac{d\phi}{dt}$ where $r$ is coordinate distance between two components in the binaries and $\phi$ is azimuthal angle can be given . Because the tail contribution starts at 1.5PN, we need leading and next-leading order (2.5PN) of tail and $(\text{tail})^2$ and tail-tail effect appear at 3PN for the first time.
\fi
We are computing total energy radiation from scatterings of compact binaries of which each components of which masses are $m_1$, $m_2$, and their positions are $x_1^i$, $x_2^i$ in an almost Minkowskian coordinate. Since total energy radiation $\Delta\mathcal{E}$ is composed of several pieces schematically,
\begin{align}
\Delta\mathcal{E}=\Delta\mathcal{E}_\text{inst}+\Delta\mathcal{E}_\text{hered}\,,
\end{align}
where $\Delta\mathcal{E}_\text{hered}$, of our interest, is consist with sub-pieces,
\begin{align}
\Delta\mathcal{E}_\text{hered}=\Delta\mathcal{E}_\text{tail}+\Delta\mathcal{E}_{(\text{tail})^2}+\Delta\mathcal{E}_\text{tail(tail)}\,.
\end{align}
Since $\Delta\mathcal{E}_\text{tail}$ starts at 1.5PN order, we need the leading term and its 1PN correction (2.5PN), while only leading contribution of $\Delta\mathcal{E}_{(\text{tail})^2}+\Delta\mathcal{E}_\text{tail(tail)}$ is required, because they start at 3PN order. To do this, we need 1PN quadrupole mass moment $I_{ij}$, Newtonian octupolar mass moment $I_{ijk}$ and Newtonian quadrupole current moment $J_{ij}$ in terms of relative position $x^i=x_1^i-x_2^i$ of binaries in the center of mass frame, which can be found in \cite{arun2008inspiralling}, and we present them here for convenience,
\begin{widetext}
\begin{subequations}\label{moments}
\begin{align}
I_{ij}&=M\,\nu\,\Big(x_i\,x_j\Big)_\text{STF}\,\Bigg[1+v^2\,\Big(\frac{29}{42}-\frac{29}{14}\nu\Big)+\frac{G\,M}{R}\Big(-\frac{5}{7}+\frac{8}{7}\nu\Big)\Bigg]\notag\\
&+\frac{M\,\nu}{c^2}\,\Big(v_i\,v_j\Big)_\text{STF} \,R^2\,\Big(\frac{11}{21}-\frac{11}{7}\,\nu\Big)+\frac{M\,\nu}{c^2}\,\Big(x_i\,v_j\Big)_\text{STF}\,\frac{d(R^2)}{d\hat{t}}\,\Big(-\frac{2}{7}+\frac{6}{7}\,\nu\Big) \,,\\[1ex]
I_{ijk}&=-M\,\nu\,\sqrt{1-4\,\nu}\,\Big(x_i\,x_j\,x_k\Big)_\text{STF}\,,\\[1ex]
J_{ij}&=M\,\nu\,\sqrt{1-4\,\nu}\,\,\Big(x^i (x\times v)^j\Big)_\text{STF}\,.
\end{align}
\end{subequations}
Therein, the followings are defined : $v^i=\frac{dx^i}{d\hat{t}}$ where $\hat{t}$ stands for the physical time, total mass $M=m_1+m_2$, symmetric mass ratio $\nu=\frac{m_1\,m_2}{M^2}$,  $R=\sqrt{x^ix^j\delta_{ij}}$, and  $()_\text{STF}$ means the symmetric and trace-free (STF) part.  And $x^i$ in terms of physical time $\hat{t}$ upto 3PN can be found in Ref.~\cite{Cho:2018} (we need only 1PN), and is written here with introducing reduced variables such as $r:=\frac{R}{G\,M}$ and $t:=\frac{t_\text{phys}}{G\,M}$. Note that $r$ has a dimension of $\frac{\text{time}^2}{\text{length}^2}$ while $t$ has $\frac{\text{time}^3}{\text{length}^3}$. And we define the azimuthal angle as $\phi:=\arctan(\frac{x^2}{x^1})$ assuming that $x^3=0$. The analytic expressions for these dynamical variables are given in time implicitly via eccentric anomaly $u$ ($-\infty\leq u\leq\infty$) characterized by $e_t$ (time eccentricity) in 1PN relation,
\begin{subequations}\label{qk}
\begin{align}
r&=j^2\,\frac{e_t\,\cosh u-1}{e_t^2-1}+\frac{1}{c^2}\,\frac{8+4\,e_t^2\,(-3+\nu)-e_t\,\big(e_t^2\,(-4+\nu)+3\,\nu\big)\,\cosh u}{2\,(e_t^2-1)}\,,\\[1ex]
\phi&=2 \arctan\left(\sqrt{\frac{e_t+1}{e_t-1}} \tanh \left(\frac{u}{2}\right)\right)+\frac{1}{c^2\,j^2} \left(6 \arctan\left(\sqrt{\frac{e_t+1}{e_t-1}} \tanh \left(\frac{u}{2}\right)\right)-\frac{e_t \sqrt{e_t^2-1} \,(-4+\nu ) \sinh (u)}{
   (e_t\, \cosh (u)-1)}\right)\,,\\[1ex]
   t&=\frac{1}{n}(e_t\,\sinh u-u)\,,
\end{align}
\end{subequations}
where
\begin{align}
n=\frac{(e_t^2-1)^{3/2}}{j^3}+\frac{1}{c^2\,j^5}\,\frac{(e_t^2-1)^{3/2}\,(3+\nu+e_t^2\,(-9+5\,\nu))}{2}\,,
\end{align}
and $e_t$ is dimensionless and given in reduced energy $E=\frac{\mathcal{E}}{M\,\nu}$, reduced angular momentum $j=\frac{\mathcal{J}}{G\,M^2\,\nu}$ as,
\begin{align}
e_t^2=1+2\,E\,j^2+\frac{E}{2\,c^2}\,\Big(8-8\,\nu+(17-7\,\nu)(2\,E\,j^2)\Big)\,.
\end{align}
Note that we will adopt $e_t$ and $j$ to characterize hyperbolic orbits, because $e_t$ gives the simplest structure in $t$ which makes the following computations easier, and also large-$e_t$ expansion (which is equivalent to large-$j$ expansion) with $j$ exhibits great convergence rate even at $e_t=1$ as reported in \cite{thefirst}.
\iffalse
Note that two variables $\frac{E}{c^2}$ and $\frac{1}{c\,j}$ are both dimensionless PN parameters used throughout this paper under the assumption that their numerical values are small. Finally, we end this section by presenting the time eccentricity $e_t$ in terms of $E$ and $j$ upto 1PN,
\fi
\end{widetext}
\section{Leading order Tail Contribution}\label{sec:tail}
In this section, we are going to get the analytic expressions of the Newtonian contribution of each tail contributions of energy radiation. The computation done in this section is influenced by \cite{Bini:2017wfr,Bini:2020hmy,Bini:2020rzn}. The tail contribution up to 3PN order, the explicit expressions \cite{Arun:2007rg} are given as
\begin{widetext}
\begin{align}
\Delta\mathcal{E}_\text{tail} &=\frac{1}{c^8}\,\frac{4\,G^2\,\mathcal{M}}{5}\,\frac{1}{G^6\,M^6} \int^\infty_{-\infty} \,dt \,\int^\infty_0\,d\tau\, I^{(3)}_{ij}(t)\,I^{(5)}_{ij}(t-\tau)\,\Bigg[\,\log\Big(\frac{c\,\tau \,G\,M}{2\,r_0}\Big)+\frac{11}{12}\Bigg]\notag\\[1ex]
&+\frac{1}{c^{10}}\frac{4\,G^2\,\mathcal{M}}{189}\,\frac{1}{G^8\,M^8} \int^\infty_{-\infty} \,dt \,\int^\infty_0\,d\tau\, I^{(4)}_{ijk}(t)\,I^{(6)}_{ijk}(t-\tau)\,\Bigg[\,\log\Big(\frac{c\,\tau \,G\,M}{2\,r_0}\Big)+\frac{97}{60}\Bigg]\notag\\[1ex]
&+\frac{1}{c^{10}}\frac{64\,G^2\,\mathcal{M}}{45}\,\frac{1}{G^6\,M^6} \int^\infty_{-\infty} \,dt \,\int^\infty_0\,d\tau\, J^{(3)}_{ij}(t)\,J^{(5)}_{ij}(t-\tau)\,\Bigg[\,\log\Big(\frac{c\,\tau\,G\,M}{2\,r_0}\Big)+\frac{7}{6}\Bigg]\,,
\end{align}
\end{widetext}
where $\mathcal{M}$ is ADM mass
\begin{align}
\mathcal{M}=M\,\Bigg(1+\frac{\nu}{c^2}\, \frac{e_t^2-1}{2\,j^2}\Bigg)\,.
\end{align}
Note that the extra $G\,M$s in the above expressions, which cannot be found in \cite{Arun:2007rg} appear because of using $t$ and $\tau$ as the reduced time variable. In favor of computation, we decompose $\Delta\mathcal{E}_\text{tail}$ into several pieces in Fourier domain such as
\begin{subequations}\label{decomposition}
\begin{align}
&\Delta\mathcal{E}_{(0)}+\Delta\mathcal{E}_{(1)} =\frac{2}{5}\frac{n^6\,\mathcal{M}}{c^8\,G^4\,M^6\,e_t^6}\int^\infty_0 dp\,|\hat{I}_{ij}(p)|^2\, p^7\,,\\[1ex]
&\Delta\mathcal{E}_{(2)} =\frac{2}{189}\frac{n^8\,\mathcal{M}}{c^{10}\,G^6\,M^8\,e_t^8}\, \int^\infty_0 \,dp\,|\hat{I}_{ijk}(p)|^2\,p^9\,,\\[1ex]
&\Delta\mathcal{E}_{(3)}=\frac{32}{45}\,\frac{n^6\,\mathcal{M}}{c^{10}\,G^4\,M^6\,e_t^6}\, \int^\infty_0 \,dp\,|\hat{J}_{ij}(p)|^2\,p^7\,,
\end{align}
\end{subequations}
where $\Delta\mathcal{E}_{(0)}$, $\Delta\mathcal{E}_{(2)}$ and $\Delta\mathcal{E}_{(3)}$ denote the leading(Newtonian) order contributions of the right hand sides respectively, whereas $\Delta\mathcal{E}_{(1)}$ refers to 1PN correction of the right hand side.
Therein, we have defined the Fourier transform as
\begin{subequations}
\begin{align}
\hat{K}(p)&:=\int^{+\infty}_{-\infty}d\bar{l}\, \text{e}^{i\,p\,\bar{l}} K(\bar{l})\,,\\[1ex]
K(t)&=\frac{1}{2\,\pi}\int^{+\infty}_{-\infty}dp\, \text{e}^{-i\,p\,\bar{l}}\hat{K}(p)\,,
\end{align}
\end{subequations}
where the reduced mean anomaly is defined as $\bar{l}:=\sinh u-\frac{u}{e_t}=\frac{n}{e_t}\,(t-t_0)$ in the preparation of large $e_t$ expansion, and $p$ and $l$ are both dimensionless for the convenience of forthcoming computation. Also, we should mention that we use the following integration reported in \cite{Arun:2007rg} (with $\gamma$ being Euler's constant),
\begin{align}\label{log1}
\int^{+\infty}_0 dt\,\text{e}^{i\,\sigma\,t}\log (t)=-\frac{1}{\sigma}\,\Bigg[\frac{\pi}{2}\,\text{sign}(\sigma)+i\,\Big(\log\big(|\sigma|\big)+\gamma\Big)\Bigg]
\end{align}
in the middle of obtaining the Fourier domain expressions in Eqs.~(\ref{decomposition}). \\
Among them, we compute three of them $\Delta\mathcal{E}_{(0)}$, $\Delta\mathcal{E}_{(2)}$ and $\Delta\mathcal{E}_{(3)}$ here, because they have analytic expressions in Fourier domain, whereas it is not the case for $\Delta\mathcal{E}_{(1)}$. We will come back to $\Delta\mathcal{E}_{(1)}$ in Sec.~\ref{sec:1PNtail}.\\

Using Eqs.~(\ref{qk}), we can write all components of multipole moments in terms of the eccentric anomaly $u$ (particularly  the form of $\text{e}^{k u}$ with integers $k$).
\iffalse
For instance, $I_{11}$ at Newtonian order looks
\begin{align}
I_{11}&=\frac{G^2\,M^3\,\nu\,j^4}{3}\Bigg[-\frac{2 e_t \,\text{e}^{-u}}{ \left(e_t^2-1\right)^2}-\frac{2 e_t \,\text{e}^u}{ \left(e_t^2-1\right)^2}\notag\\[1ex]
&-\frac{\left(e_t^2-3\right) \,\text{e}^{-2 u}}{4 \left(e_t^2-1\right)^2}-\frac{\left(e_t^2-3\right) \,\text{e}^{2 u}}{4 \left(e_t^2-1\right)^2}+\frac{5 e_t^2+1}{2 \left(e_t^2-1\right)^2}\Bigg]\,.
\end{align}
Hence,
\fi
By considering $d\bar{l}=du (\cosh u-\frac{1}{e_t})$, every terms encountered in the Fourier transformation could be written in form of the typical integral,
\begin{align}\label{typicalintegral}
I_t:=\int^{+\infty}_{-\infty} du \,\text{e}^{i\,p\,\sinh u+k \,u-i\,\frac{p}{e_t}\,u}\,.
\end{align}
This is nothing but one of integral representations of Hankel function of the first kind $H^{(1)}_{a}(x)$ (we will call it just the Hankel function henceforth),
\begin{align}
H^{(1)}_{a} (x)=\frac{1}{i\,\,\pi}\int ^{+\infty}_{-\infty}\,\text{e}^{x \sinh u-a u} \,du\,.
\end{align}
Note that the integral on the right hand side is only convergent when the order is in $-1<\text{Re}(a)<1$, which is not our case  ($k$ could be bigger than 1 in $I_t$). It implies that the typical integral $I_t$ is actually divergent in the usual integral sense. But the Hankel function is even analytic outside of $-1<\text{Re}(a)<1$, hence, we will use the Hankel function as a regularized, hence finite value of the typical divergent integral by the argument of analytic continuation resulting in
\begin{align}
I_t=i\,\pi\,H^{(1)}_{i\,\frac{p}{e_t}-k}(i\,p).
\end{align}
After successive uses of the relations
\begin{align}
H^{(1)}_{a-1}(x)+H^{(1)}_{a+1}(x)=\frac{2a}{x}H^{(1)}_{a}(x)\,,
\end{align}
to unify all the orders appearing in the integrands to either $0$ or $1$, we obtain the intermediate results of $|\hat{I}_{ij}(p)|^2$, $|\hat{I}_{ijk}(p)|^2$ and $|\hat{J}_{ij}(p)|^2$ at the leading order.
\iffalse
For instance, $|\hat{I}_{ij}(p)|^2$ at the leading order has the following form,
\begin{widetext}
\begin{align}
|\hat{I}_{ij}(p)|^2&=
G^4\,M^6\,j^8\,\pi^2\,\Bigg[\frac{8 i \left(3\,e_t^2-4\right) H_{\frac{i p}{e_t}}^{(1)}(i p)\, \dot{H}^{(1)}_\frac{i p}{e_t}\left(i p\right)}{e_t^2 \,\left(e_t^2-1\right)^3 p^3}+\left(\frac{8}{\left(e_t^2-1\right)^3 \,p^4}+\frac{8}{e_t^2 \,\left(e_t^2-1\right)^2 p^2}\right) \Big(\dot{H}^{(1)}_\frac{i p}{e_t}\left(i p\right)\Big)^2\notag\\[1ex]
&+\left(\frac{8}{\left(e_t^4-e_t^6\right)\, p^2}-\frac{8 \left(e_t^4-3 e_t^2+3\right)}{3 e_t^2 \left(e_t^2-1\right)^4\, p^4}\right)\, \Big(H_{\frac{i p}{e_t}}^{(1)}(i p)\Big)^2\Bigg]+\mathcal{O}(1/c)\,,
\end{align}
\end{widetext}
where $\dot{H}^{(1)}_a(x)=\frac{\partial}{\partial x}H^{(1)}_a(x)$. Note that by the following relation,
\begin{align}\label{derivHankel}
\dot{H}^{(1)}_a(x)= \frac{a\, H_a^{(1)}(x)}{x}-H_{a+1}^{(1)}(x)\,,
\end{align}
one can express $|\hat{I}_{ij}(p)|$ without $\dot{H}^{(1)}$, which is more desirable for the practical computations (we displayed it with $\dot{H}^{(1)}$ because of the compactness and the future purpose).
\fi
As pointed out in \cite{Bini:2017wfr}, the large-$e_t$ expansion drops the $p$ dependence in the order of the Hankel function, which makes the computation much simpler. After taking the large-$e_t$ expansion, every terms can be dealt by the following master integral (similar expression is reported in Eq.(7.24) of \cite{Bini:2020rzn}),
\begin{widetext}
\begin{align}\label{masterfourier}
\int ^{+\infty}_{-\infty} \,dp\,p^n H^{(1)}_{a}(i\,p)\,H^{(1)}_{b} (i\,p)=& \frac{2^n\,\text{e}^{-i\frac{(1+a+b)\,\pi}{2}}}{i\,\,\pi\,\Gamma(1+n)} \,\Gamma\Big(\frac{1-a-b+n}{2}\Big)\,\Gamma\Big(\frac{1+a-b+n}{2}\Big)\notag\\[1ex]
&\times\Gamma\Big(\frac{1-a+b+n}{2}\Big)\,\Gamma\Big(\frac{1+a+b+n}{2}\Big)\,,
\end{align}
\end{widetext}
Now that all the computation is reduced down to the straightforward but extensive machinery work, we only present the final results with the first 12 terms in the large $e_t$ expansion $\Delta\mathcal{E}^{(l)}_{(0)}$ in Appendix.\ref{sec:partialresult}. (We use the superscript $(l)$ to denote that this is not exact one but expressed in large-$e_t$ (or, large-$j$) expansion.) We have found that the first three terms are coincident to Eq.(4.14) in \cite{Bini:2021qvf}. By the exactly same procedure, we also get the first 12 terms of $\Delta\mathcal{E}_{(2)}$ and $\Delta\mathcal{E}_{(3)}$ presented in Appendix.\ref{sec:partialresult}.
\section{Leading Quadratic tail contribution}\label{sec:tails}
In this section, we are going to obtain analytic expressions of $(\text{tail})^2$ and $\text{tail}(\text{tail})$ contributions. In terms of mulitpole moments, the leading order terms of each pieces \cite{Arun:2007rg} are
\begin{widetext}
\begin{subequations}
\begin{align}
\Delta\mathcal{E}_{(\text{tail})^2}&=\frac{4\,G^3\,\mathcal{M}^2}{c^{11}\,5}\,\frac{1}{G^7\,M^7}\int^{+\infty}_{-\infty}\,dt\,\Bigg(\int^{+\infty}_0\,d\tau\,I^{(5)}_{ij}(t-\tau)\Bigg[\log\Big(\frac{c\,\tau\,G\,M}{2\,r_0}\Big)+\frac{11}{12}\Bigg]\Bigg)^2\,,\\[1ex]
\Delta\mathcal{E}_{\text{tail}(\text{tail})}&=\frac{4\,G^3\,\mathcal{M}^2}{c^{11}\,5}\,\frac{1}{G^7\,M^7}\int^{+\infty}_{-\infty}\, dt\, I^{(3)}_{ij}(t)\int^{+\infty}_{0} \,d\tau\,I^{(6)}_{ij}(t-\tau)\,\Bigg[\log^2\Big(\frac{c\,\tau\,G\,M}{2\,r_0}\Big)+\frac{57}{70}\,\log\Big(\frac{c\,\tau\,G\,M}{2\,r_0}\Big)+\frac{124627}{44100}\Bigg]\,.
\end{align}
\end{subequations}
Similarly, they are rearranged compactly in Fourier domain into
\begin{subequations}
\begin{align}
\Delta\mathcal{E}_{(4)}&=\frac{\mathcal{M}^2}{c^{11}\,G^4\,M^7}\,\frac{2 }{5\,\pi}\,\frac{n^7}{e_t^7}\,\Bigg[\frac{2\,\pi^2}{3}-\frac{214}{105}\Bigg(\,\log \Big(\frac{2\, n \,r_0}{c\,e_t\,G\,M}\Big)+\gamma_E\Bigg)-\frac{116761}{29400}\Bigg]\,\Big( \int^\infty_0 dp\,|\hat{I}_{ij}|^2\,p^8\Big)\,,\\[2ex]
\Delta\mathcal{E}_{(5)}&=-\frac{\mathcal{M}^2}{c^{11}\,G^4\,M^7}\,\frac{428}{525\,\pi}\,\frac{n^7}{e_t^7}\, \int^\infty_0 dp\,|\hat{I}_{ij}|^2\,p^8\,\log p\,,
\end{align}
\end{subequations}
where we use the relations \cite{Arun:2007rg}, Eq.(\ref{log1}) and
\begin{align}\label{log2}
\int^{+\infty}_0 dt\,\text{e}^{i\,\sigma\,t}\log^2 (t)=\frac{i}{\sigma}\,\Bigg\{\frac{\pi^2}{6}-\Bigg[\frac{\pi}{2}\,\text{sign}(\sigma)+i\,\Big(\log\big(|\sigma|\big)+\gamma\Big)\Bigg]^2\Bigg\}\,.
\end{align}
Thanks to even power of $p$ in the integrand, $\Delta\mathcal{E}_{(4)}$ can be integrated in an exact way. Using the elementary integrals $E^i(n)$ defined in Appendix.\ref{elementaryintegral},
\begin{align}
&\int^\infty_0 dp\,|\hat{I}_{ij}|^2\,p^8=8\,\pi^2\,e_t^3\, j^8\,G^4\,M^6\,\nu^2\notag\\[1ex]
&\times\Bigg[\frac{\left(3 \,e_t^2-4\right)\, e_t\, E^{y}(5)}{\left(e_t^2-1\right)^3}+\frac{e_t^2\,E^{z}(4)}{\left(e_t^2-1\right)^3}+\frac{e_t^2\,E^{z}(6)}{\left(e_t^2-1\right)^2}-\frac{E^{x}(6)}{e_t^2-1}-\frac{\left(e_t^4-3\, e_t^2+3\right)\, E^{x}(4)}{3 \,\left(e_t^2-1\right)^4}\Bigg]\,,
\end{align}
where the exact solutions of each elementary integrals are listed in Eqs.(\ref{eleIntegrals}).\end{widetext}
Gathering all pieces, we obtain the exact expression ($\mathcal{M}=M$ at this order) displayed in Eq.(\ref{deltaE4}) of Appendix.\ref{sec:partialresult}. We have checked that the $r_0$ dependence in $\Delta \mathcal{E}_{(4)}$ is canceled with $r_0$ in Eq.(31.d)~ of \cite{thefirst}, so the final result does not depend on $r_0$.\\
In the case of $\Delta\mathcal{E}_{(5)}$, since there is no closed form solution, we use the same strategy of computing the Newtonian tails explained in Sec.~\ref{sec:tail}. The picky $\,\log p$ can be dealt by the derivative with respect to $n$ in the master integral Eq.(\ref{masterfourier}), and hence is reduced down to the machinery work as well. Likewise, we display the first 12 terms of the large-$e_t$ expansion of $\Delta\mathcal{E}_{(5)}$ in Appendix.\ref{sec:partialresult}. And the agreement is found in the first three terms with Eq.(4.14) in Ref.\cite{Bini:2021qvf}.\footnote{Only the second arxiv version of \cite{Bini:2021qvf} for now.}
\section{1PN tail contribution}\label{sec:1PNtail}
Now, we need to tackle down the most tricky computation of $\Delta\mathcal{E}_{(1)}$ in this paper. Since we could not obtain Fourier transform of the quadrupole moment at the 1PN order in general, time domain integration is attempted. Contrary to the way we have computed, we could not find the systematic and simple automatic way of integration \textit{i.e.} master integral method, so the integrations should be treated in a rather heuristic way.  For the first 4 terms, we could find exact values of the coefficients by symbolic integration, but we failed for the other 8 terms. Instead, numerical integration and PSLQ algorithm \cite{PSLQ} are adopted to find analytic form of the coefficients. Since we have encountered more than 10 thousands terms, we will explain the process of computation roughly.  \\
By putting all dynamical variables Eq.(\ref{qk}) in the quadrupole moment Eq.(\ref{moments}a), we construct the integral over $u$ and $v$ which are given via the relations to the time variables
\begin{subequations}
\begin{align}
t&= \frac{1}{n}\big(e_t\sinh u-u\big)\,,\\
t-\tau&=\frac{1}{n}\big(e_t\sinh v-v\big)\,.
\end{align}
\end{subequations}
For the efficient computation, we subsequently choose two dynamical parameters $(\kappa,\,q)$ in the integrand,
\begin{subequations}
\begin{align}
\kappa&=\text{e}^{u}\,,\\
    q&= \frac{\text{e}^{v}}{\kappa}\,.
\end{align}
\end{subequations}
Schematically, the tail radiation in time domain has the following form
\begin{subequations}
\begin{align}
\Delta\mathcal{E}
&\sim\int^{+\infty}_{-\infty}dt \int^{t}_{-\infty}d(t-\tau) \,\mathcal{I}_1(t,t-\tau)\,,\\[1ex]
&\sim\int^{+\infty}_{-\infty}du \int^{u}_{-\infty}dv \,\mathcal{I}_2(u,v)\,,\\[1ex]
&\sim\int^{+\infty}_{0}d\kappa \int^{1}_{0}dq \,\mathcal{I}_3(\kappa,q)\,,
\end{align}
\end{subequations}
where $\mathcal{I}_{1,2,3}$ represent some integrands. One can easily see that the choice of $q$ makes two integrals independent. All terms we encounter is classified into four categories,
\begin{subequations}
\begin{align}
I_1&=\frac{(q\,\kappa^2+1)^n\,\kappa^l}{(q-1)^a\,(q^2\,\kappa^2+1)^b}\,,\\[1ex]
I_2&=\frac{(q\,\kappa^2+1)^n\,\,\kappa^l \,\arctan(\frac{\kappa-1}{\kappa+1})}{(q-1)^a\,(q^2\,\kappa^2+1)^b}\,,\\[1ex]
I_3&=\frac{(q\,\kappa^2+1)^n\,\,\kappa^l\,\log^m(q)}{(q-1)^a\,(q^2\,\kappa^2+1)^c}\,,\\[1ex]
I_4&=\frac{(q\,\kappa^2+1)^n\,\,\kappa^l\,\arctan(\frac{\kappa-1}{\kappa+1})\,\log^m(q)}{(q-1)^a\,(q^2\,\kappa^2+1)^b}\,,
\end{align}
\end{subequations}
where $m,l,a,b,c$ denote some positive integers whereas $n$ is an integer.
To solve them, we have found that
\begin{widetext}
\begin{align}
&\int^1_0\, dq\, \frac{\log ^n(q)\,q^m}{(q+a)(q+b)(q+c)(q+d)}\\[1.5ex]
= &(-1)^{n+m+1}\,n!\,\Bigg[\frac{\,a^m\,\text{Li}_{n+1}(\frac{-1}{a})}{(a-b)(a-c)(a-d)}+\frac{b^m\,\text{Li}_{n+1}(\frac{-1}{b})}{(b-a)(b-c)(b-d)}+\frac{c^m\,\text{Li}_{n+1}(\frac{-1}{c})}{(c-a)(c-b)(c-d)}+\frac{d^m\,\text{Li}_{n+1}(\frac{-1}{d})}{(d-a)(d-b)(d-c)}\Bigg]\,,\notag
\end{align}
\end{widetext}
where $n,m$ are positive integer with $m\leq3$, and $\text{Li}_n$ is poly-logarithm. After taking successive derivatives with respect to $a,b,c,d$, we manage to integrate all types of integrand over $q$.  In the cases of $I_1$, $I_2$ and $I_3$, further integration over $\kappa$ is also possible analytically (hence, every coefficients of $\nu^3$ term are determined exactly). However, in the case of $I_4$, we encounter multi-logarithm terms such as
\begin{align}
\int \,dq\, I_4\sim g(Q)\,\arctan(Q)\,\text{Li}_{n}(f(Q))\,,
\end{align}
where $f(Q), g(Q)$ are some rational function of polynomial of $Q$ with $Q=\frac{\kappa-1}{\kappa+1}$.
Given that $\arctan$ is also a logarithmic function, we need to do integration over two or more logarithm. When $n=2$ (\textit{i.e.} dilogarithm),  we could get rid of $\text{Li}_2$ by integration-by-part, but when $n\geq 3$, because the derivative of $\text{Li}_n$ is still a poly-logarithm,  we could not find an analytic way of integration. Instead, for remaining terms, we integrate $I_4$ type integrals ($q$ is already integrated), numerically with $600\sim1000$ digits, and attempt to find their analytic forms using PSLQ algorithm. Since PSLQ algorithm is used for guessing a relation between integers, we need to make a list of candidates. For even orders $e_t^n$ ($n=8,6,4\cdots$), the candidate list is consist with combinations of even powers of $\pi$, and  $\zeta(m)$ with odd integer $m$, such as
\begin{align}
\{1,\pi^2,\pi^4,\cdots,\zeta(3),\pi^2\zeta(3),\cdots\zeta(5),\pi^2\zeta(5),\cdots\}\,,
\end{align}
and odd powers of $\pi$ for odd powers of $e_t$,
\begin{align}
\{\pi,\pi^3,\pi^5\cdots\}\,.
\end{align}
The higher order of $e_t$ we take, the longer candidate lists are required.
We first guess analytic forms of numerical coefficients using first $400\sim800$ digits, and check if the number of digits used in guessed integers is much smaller than $400\sim800$. For example, if from this 40 digits number, $$46.50941502044973026321447260065209280334\,,$$ PSLQ guesses these two long integers (in each numerator and denominator) in totally 55 digits, $$\frac{4320335101191349704192837044}{291827644122831121457024899}\pi\,,$$ we regard it as a failure, because it just stores 40 digits with 55 digits.
But if PSLQ find two digits such as $\frac{3}{2}\pi^3$, we regard it trustworthy. After meeting this standard, we also check if they can predict the next 200 digits, and if so, we confirm them. Using the coefficients determined in this way, we compute the first 12 terms of $\Delta\mathcal{E}_{(1)}$ which can be found in Appendix.\ref{sec:partialresult}.
\section{Radiation from Parabolic orbits}\label{sec:parab}
In this section, we are going to compute hereditary part of energy radiation $\Delta\mathcal{E}^{(p)}_\text{hered}$ from parabolic orbits and this could be understood as the limit of $e_t\to1$ (or, $E\to0$) in the hyperbolic radiation. As pointed out in \cite{thefirst}, the choice of the parametrization $(e_t, h)$ (or $(e, h)$) of orbits allows us quickly converging large eccentricity expansions even approximating well at $e_t=1$. We check if this works even in the hereditary contribution as well as the validity of our hyperbolic computations.\\
The parabolic version of keplerian parametrization can be derived by changing $u$ to $w$ via $u=(e_t^2-1)^{1/2} \,w$ in Eqs.(\ref{qk}). After taking the limit of $e_t\to1$, one will get
\begin{widetext}
\begin{subequations}
\begin{align}
r&=\frac{j^2 w^2}{2}+\frac{j^2}{2}+\frac{1}{c^2}\, \left(\frac{\nu -6}{2}+(1-\nu ) w^2\right)\,,\\[1ex]
t&=\frac{j^3 w^3}{6}+\frac{j^3 w}{2}+\frac{j}{c^2}\, \left(-\frac{1}{2}  (\nu -1) w^3-\frac{3}{2} (\nu -1) w\right)\,,\\[1ex]
\phi&=2 \arctan(w)+\frac{2 \left(3\, w^2\, \arctan(w)-\nu\,  w+4 \,w+3 \,\arctan(w)\right)}{c^2\,j^2\, \left(1+w^2\right)}\,.
\end{align}
\end{subequations}
\end{widetext}
By these, it is possible to construct every mulipole moments in terms of $w$. In the computation of $\Delta\mathcal{E}^{(p)}_{(0)}$ and $\Delta\mathcal{E}^{(p)}_{(1)}$, the most of the integrations can be done straightforwardly except
\begin{align}
I_p:=\int^{\infty}_{-\infty}dw\,\frac{w \left(w^6+6 w^4-18 w^2+4\right) \arctan(w)}{ \left(w^2+1\right)^7 \left(w^2+4\right)^{7/2}}\,,
\end{align}
which arises in 1PN order of quadrupole tail part. After inserting the integral representation of $$\arctan( w)=\int^{1}_0{dk}\frac{w}{1+w^2\,k^2}\,,$$ the successive integrations over $w$ and $k$ could yield the analytic result. By simplifying the result with the help of the second order of Clausen function, we managed to obtain
\begin{align}
I_p =\frac{385\, \text{Cl}_2\left(\frac{\pi }{3}\right)}{1024\, \sqrt{3}}-\frac{5221}{115200}-\frac{501151 \,\pi }{2799360\, \sqrt{3}}+\frac{77 \,\pi\,  \log (3)}{1024\, \sqrt{3}}\,,
\end{align}
where
\begin{align}
\text{Cl}_2\left(z\right):=-\int^{z}_0\,dx\,\log\Big|2\sin\frac{x}{2}\Big|.
\end{align}
Specially, $\text{Cl}_2\left(\frac{\pi }{3}\right)$ is the maximum value of $\text{Cl}_2\left(z\right)$ when $z$ is real.
\iffalse
which could be computed quite quickly by BBP-type [],
\begin{align}
\text{Cl}_2\left(\frac{\pi }{3}\right)
&=\sqrt{3}\,\sum_{k=0}^{\infty}\Bigg[\frac{1}{(6k+1)^2}+\frac{1}{(6k+2)^2}-\frac{1}{(6k+4)^2}-\frac{1}{(6k+5)^2}\Bigg]\,,\notag\\[1ex]
&=\frac{\sqrt{3}}{9}\,\sum_{k=0}^{\infty}\frac{(-1)^k}{27^k}\Bigg[\frac{18}{(6k+1)^2}-\frac{18}{(6k+2)^2}-\frac{24}{(6k+3)^2}-\frac{6}{(6k+4)^2}+\frac{2}{(6k+5)^2}\Bigg]\,.
\end{align}
\fi
\begin{widetext}
As a result, we obtain the quadrupolar tail piece of energy radiation from parabolic orbits $\Delta\mathcal{E}^{(p)}$\,,
\begin{align}
\Delta\mathcal{E}^{(p)}_{(0,1)}=\frac{M\,\nu^2\,\pi}{c^{8}\,j^{10}}\bBigg@{3}[\frac{169984}{45 \,\sqrt{3} }+\frac{1}{c^2\,j^{2}}  \left(27720  \, \text{Cl}_2\left(\frac{\pi }{3}\right)+\frac{7949344\,\pi}{1215}-\frac{41631152  }{525 \,\sqrt{3}}+5544\, \pi\, \log (3)+\frac{2818048 \, \nu }{63 \sqrt{3}}\right)\bBigg@{3}]\,.
\end{align}
\end{widetext}
In the case of contributions $\Delta\mathcal{E}^{(p)}_{(2)}$, $\Delta\mathcal{E}^{(p)}_{(3)}$, all computation is trivial. And for $\Delta\mathcal{E}^{(p)}_{(4)}$, it is easily obtained by putting 1 in $e_t$ in Eq.(\ref{deltaE4}) because it is exact,
\begin{subequations}
\begin{align}
\Delta\mathcal{E}^{(p)}_{(2)}&=\frac{M\,\nu^2\,(1-4\,\nu)\,\pi}{c^{10}\,j^{12}}\frac{1448960}{63 \,\sqrt{3}}\,,\\
\Delta\mathcal{E}^{(p)}_{(3)}&=\frac{M\,\nu^2\,(1-4\,\nu)\,\pi}{c^{10}\,j^{12}}\,\frac{4096}{9\, \sqrt{3}}\,,
\end{align}
\begin{align}
\Delta\mathcal{E}^{(p)}_{(4)}&=\frac{M\,\nu^2\,\pi}{c^{11}\,j^{13}}\,\Bigg[-\frac{161249 \,  \gamma}{15}  -\frac{161249}{15} \,  \log \left(\frac{2\,r_0\,n}{e_t\,G\,M\,c}\right)\notag\\[1ex]
&+\frac{10549 \,\pi^2}{3}-\frac{175958827  }{8400}\Bigg]\,,
\end{align}
\end{subequations}
where we keep $\log(n)$, because it is divergent at $e_t=1$, which will be canceled by $\Delta\mathcal{E}_{(5)}$. \\
The fifth piece $\Delta\mathcal{E}^{(p)}_{(5)}$ is left. After performing inverse Fourier transform, $\Delta\mathcal{E}_{(5)}$ is re-expressed in time domain as
\begin{align}
&\Delta\mathcal{E}_{(5)}=\frac{428}{525}\Bigg[\Big(\gamma+\log\left(\frac{n}{c^3\,e_t}\right)\Big)\,\int^{+\infty}_{-\infty} dt\,\Big(I_{ij}^{(4)}(t)\Big)^2\,\notag\\[1ex]
&+\int^{+\infty}_{-\infty} dt\,\int^{+\infty}_{t} d\tau\, I_{ij}^{(5)}(t+\tau) I_{ij}^{(4)}(\tau)\log(\tau\,c^3)\Bigg]\,.
\end{align}
As previously computed, almost all term can be dealt by elementary integration methods, but $\arctan$ term should be replaced by its integral representation again. One could get
\begin{align}
&\Delta\mathcal{E}^{(p)}_{(5)}=\frac{M\,\nu^2\,\pi}{c^{11}\,j^{13}}\Bigg[\frac{161249  \, \gamma }{15}+\frac{161249}{15}\,  \log \left(\frac{n}{c^3\,e_t}\right)\\[1ex]
&-\frac{90210202 }{1575}+\frac{161249}{5} \, \log (2\,c\,j)+\frac{161249}{30}\,  \log (3)\Bigg]\,.\notag
\end{align}
Indeed, the $\log(n)$ term in $\Delta\mathcal{E}^{(p)}_{(4)}$ and $\Delta\mathcal{E}^{(p)}_{(5)}$ are canceled. Contrary to $\Delta\mathcal{E}^{(p)}_{(5)}$ having $\log(j)$ dependence, $\Delta\mathcal{E}^{(l)}_{(5)}$ does not have it. This missing $\log(j)$ comes in from $\log(n)=\log\left(\frac{(e_t^2-1)^{3/2}}{j^3}\right)$ in $\Delta\mathcal{E}_{(4)}$ (Eq.(\ref{deltaE4})), which also indicates that $\Delta\mathcal{E}_{(4)}$ and $\Delta\mathcal{E}_{(5)}$ should not be treated independently.\\
Finally, we compare the exact parabolic results $\Delta\mathcal{E}^{(p)}$ and the hyperbolic results in large-$e_t$ expansion $\Delta\mathcal{E}^{(l)}$ at $e_t=1$ in Table.\ref{table:1}. One could find that they have very close values, which shows the robustness of our computations as well as the efficiency of large-$e_t$ expansion.
\begin{table}
\begin{tabular}{|c|c|c|c| }
\hline
&$\Delta\mathcal{E}^{(p)}$& $\Delta\mathcal{E}^{(l)}|_{e_t=1}$  \\
\hline \hline
$\Delta\mathcal{E}_{(0)}$ &107.0544 & 107.0545 \\
$\Delta\mathcal{E}_{(1)}$ &1240.453 & 1240.384 \\
$\Delta\mathcal{E}_{(2)}+\Delta\mathcal{E}_{(3)}$ &332.3571& 332.3535 \\
 $\Delta\mathcal{E}_{(4)}+\Delta\mathcal{E}_{(5)}$&-1114.843 &-1114.842 \\
\hline
\end{tabular}
\caption{7 digits comparisons. $G=M=c=j=r_0=1$ and $\nu=1/8$ are chosen}
\label{table:1}
\end{table}\\
For the completeness, we present the completed result of $\Delta\mathcal{E}^{(p)}=\Delta\mathcal{E}^{(p)}_\text{inst}+\Delta\mathcal{E}^{(p)}_\text{hered}$ from parabolic orbits upto 3PN combined with the instantaneous contribution (Eq.(43) of \cite{thefirst}),
\begin{widetext}
\begin{align}
\Delta\mathcal{E}^{(p)}&=\frac{M\,\nu^2\,\pi}{c^5\,j^7}\,\bBigg@{3}\{\frac{170}{3}+\frac{1}{c^2\,j^2}\,\Bigg(\frac{13447}{20}-\frac{1127 \,\nu }{3}\Bigg)+\frac{1}{c^3\,j^3}\,\frac{169984}{45\sqrt{3}}+\frac{1}{c^4\,j^4}\,\Bigg(\frac{5839651}{1008}-\frac{258051 \,\nu}{40}+\frac{5481 \,\nu ^2}{4}\Bigg)\notag\\[1ex]
&+\frac{1}{c^5\,j^5}\,\Bigg(27720 \,\text{Cl}_2\left(\frac{\,\pi }{3}\right)-\frac{29317552}{525 \sqrt{3}}+\frac{7949344 \,\pi }{1215}+5544 \,\pi  \log (3)-\frac{3092480 \,\nu }{63 \sqrt{3}}\Bigg)\notag\\[1ex]
&+\frac{1}{c^6\,j^6}\,\Bigg[\frac{161249 \log (2\,\sqrt{3}\,c\,j)}{15}+\frac{10549 \,\pi^2}{3}+\frac{16880186749}{241920}+\left(-\frac{3972009943}{30240}+\frac{208813 \,\pi^2}{160}\right) \,\nu\notag\\[1ex]
&\quad+\frac{1157409 \,\nu^2}{32}-\frac{29645 \,\nu^3}{8}\Bigg]\bBigg@{3}\}+\mathcal{O}\Bigg(\frac{1}{c^{12}}\Bigg).
\end{align}
\end{widetext}
\section{Discussion \& Future work}
We have computed the hereditary part of energy radiation from hyperbolic scatterings as well as parabolic scatterings. For hyperbolic computation, we rely on large-$e_t$ (or, large-$j$) expansion while the parabolic result is exact.  As expected, the hyperbolic result in large-$e_t$ is close to the value of the parabolic one numerically. It is also interesting to point out that the irrational values appear in the parabolic case is $\pi$, $\log(2)$, $\log(3)$, $\sqrt{3}$ and $\text{Cl}_2(\frac{\pi}{3})$ whereas $\pi$, $\log(2)$, $\gamma$ and $\zeta(2n+1)$ in the hyperbolic case.  In order to complete 3PN radiation reaction to scattering angle, impact parameter, we need to compute angular momentum radiation. This is going to be done in a subsequent paper using the same techniques elaborated in this paper except the memory effect which will probably require another treatment. We also expect that the practical knowledge on the integrations gained from this work, might be helpful to extend our knowledge specially in non-local in time conservative dynamics, which has the similar structure with hereditary radiation.

\section*{Acknowledgments}
We thank Yannick Boetzel for the setup of the formalism at the beginning phase, Rafael A. Porto for discussion and Hyung-Mok Lee for technical support.  G.C is supported by the ERC Consolidator Grant "Precision Gravity: From the LHC to
LISA," provided by the European Research Council (ERC) under the European Union's H2020 research and innovation
programme (grant No. 817791).
\newpage
\begin{widetext}

redpajama_set_name: RedPajamaArXiv


text:
Popular Game App: The Pokémon Hunt Continues – Berlin
The estimated reading time is 2 minutes
Popular Game App: The Pokémon Hunt Continues - Berlin
May 17, 2019 at 3:18 pm 0
It is Saturday, 17 clock, at the Beuth College in Wedding: About 30 people stand together in a cluster and stare at their cell phones. What are you doing? Fighting – or whatever they call it – doing a raid, and doing a strong Pokémon together in a virtual arena. They play Pokémon Go, the mobile game that triggered a worldwide hype in 2016, turning children and adults alike into a hunt for small, digital fantasy creatures to become modern scavenger hunters.
Not only to collect and trade Pokémon, but also to incubate "eggs" or catch "worms". That went on for about a summer. Today, only the hardcore fans are playing, they are all the more crazy about the Japanese originating animals.
They are called Taubsi or Schiggy, the most famous – small, yellow, black Kulleraugen – is Pikachu. With Poké balls they are shot at and caught. Actually very simple. And maybe that's why the enthusiasm for many quickly disappeared, with many bugs and mistakes at the beginning. It took some time until there were new game histories and updates.
But the game can not be killed and the hard core of the fans is not just made up of young people who are constantly busy with their cell phones. In fact, all ages are represented: parents play with their children, couples run together, singles meet like-minded people, and even retirees are active in the Pokémon Go scene.
Especially in large squares, the groups stand out: at the Gendarmenmarkt, Potsdamer Platz or at Alexanderplatz – they do not have to make an appointment to meet like-minded people. Because in prominent places hunters are attracted by numerous battle arenas.
On sunday, there is again a worldwide "Comunity Day"
In Weddinger Sprengelpark beer benches are set up on this day, on salads, sausages and cakes. What looks like a birthday party is actually an event where players go back and forth for three hours. Again and again somebody shouts euphorically "Shiny!" When a dazzling, especially coveted Pokémon has been caught. Everyone is motivated to catch a lot of catches, because together it just makes it even more fun.
The enthusiasm is fueled by a new movie, "Pokémon master detective Pikachu" is currently in the cinemas. The mobile game itself is teeming with the main characters in the movie right now, and every player hopes for a special Pikachu with a detective hat.
This Sunday is again worldwide "Community Day" from 15 to 18 clock. In other words: On this day, a particularly rare Pokémon occurs frequently, which attracts many fans to the streets. If you still want to join in, do not be late, the "Pokémon Go" app can be downloaded for free for all mobile phone types.
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text:
Willem Beukelszoon, né dans la seconde moitié du  à Biervliet en Flandre zélandaise et mort vraisemblablement vers le milieu du , est un pêcheur néerlandais à qui l'on attribue traditionnellement l'art de préserver les harengs.

Biographie

Sa date de naissance est inconnue. On sait avec certitude qu'il était échevin à Biervliet en 1312. Un vitrail de l' fait état de sa mort en 1397, ce qui est donc impossible. On situe plus vraisemblablement sa mort vers le milieu du siècle, l'année 1347 ayant été proposée.

Conservation du hareng
La méthode de conservation du hareng attribuée à Beukelszoon consiste à vider le hareng en laissant en place le seul pancréas. Celui-ci continue à sécréter des enzymes, qui contribuent à préserver et à rendre plus goûteuse la chair du poisson. Les harengs sont ensuite salés et encaqués.

Le salage des harengs est toutefois mentionné dans des manuscrits néerlandais antérieurs au  et aurait aussi été en usage avant cette période dans les pays scandinaves.

Notoriété
 Le poète néo-latin Jean-Baptiste Camberlyn l'a célébré dans son poème , publié en 1828.
 Le poète néerlandais Jacob Cats lui a rendu hommage dans .
 Nominé dans le cadre du programme télévisé  visant en 2005 à élire le plus grand Hollandais de tous les temps, il a fini en .

Notes et références

Voir aussi

 Hollandse nieuwe
 Jean-Baptiste Camberlyn

Liens externes

Personnalité néerlandaise du XIVe siècle
Date de naissance non renseignée (XIIIe siècle)
Date de décès non renseignée (XIVe siècle)
Pêcheur
Naissance dans la province de Zélande
Inventeur du XIVe siècle

redpajama_set_name: RedPajamaWikipedia


text:
Rob Ford, poverty and Toronto's 2012 budget
On Saturday, many people gathered at Moss Park in the City of Toronto to protest proposed cuts to housing and social services that are expected in the city's upcoming 2012 budget.
The "Stop the Cuts" protest is just one in a series of protests that have dogged the steps of beleaguered Mayor Rob Ford ever since he took over the helm of the City of Toronto. Rob Ford, who took over the mantle of leadership under the banner of stopping the gravy train that operated at City Hall, and cutting costs, has been battled every step of the way by poverty activists who have seen him as the poster child for cuts to programs that benefit the poor. The indictment is not without foundation.
Mayor Ford and his brother Doug, determined to balance the city's budget, have adopted a steam rolling approach that has been seen as insensitive to the needs of the poor of the City of Toronto. Truth be told most politicians who adopt a policy of eliminating financial waste are typically seen as being insensitive to the needs of the poor primarily because their cost cutting measures always hit the poor the hardest.
Tragically, the first targets of cost cutting salvos are always programs that are intended to benefit the poor; ironically, it is those who need the money from whom the money is taken. Why? Because there is a perception that programs such as funding community libraries, women's shelters, and employment programs, are not really needed and are wasteful. These programs then find their way onto the chopping block.
The problem for Rob Ford is that Torontonians apparently saw him as being a different kind of politician; one who could reduce waste without harming services or raising taxes. This has not been the case. Thus, the city's 2012 budget, expected to be released this Monday, the target of the "Stop the Cut" protests, is expected to contain devastating cuts to services that benefit the poor in Toronto. These include libraries, shelters, and programs at community centers.
The perception that programs that benefit the poor are wasteful and not really needed, a perception that is shared only by those who do not really need the services in question, is symptomatic of a pervasive cultural attitude that says that the poor are responsible for their own predicament and that others in society should not be responsible for their upkeep.
It is worth reminding ourselves that the Mosaic Code, the foundation of our moral worldview, included an obligation to help the poor.
2,000 Occupy Toronto protesters march on Yonge to 'Evict Rob Ford'
Toronto Mayor Rob Ford, City Staff launch annual City Toy Drive
49.1 Million People Live in Poverty; New Census Supplemental Poverty Measure
Ford Romances the Rockies with the 2013 Ford Escape
Rick Scott's "Rob Peter To Pay Paul" Budget Pits Public Schools vs. Hospitals
Toronto's forthcoming 2012 operating budget: where the wind blows


> > exit node but what just happened could be a consequence of doing it.
> don't consider that unserious..
I agree. I was about to set up a tor node a few years ago but never got around to it. I send cash to orgs working for human rights in countries with oppressive regimes. I am all for providing anonymized access to help free speech. Perhaps its better with anon access to specific applications like twitter, fb etc and not general internet access. I suspect that the 'free speech' part of the total tor traffic volume is pretty small(?).


The Chillicothe Metropolitan Housing Authority (CMHA) and the U.S. Department of Housing and Urban Development (HUD) welcome you as a property owner to the Section 8 Housing Choice Voucher Program (HCV).
Change or Set-up Direct Deposit. Click here for the Direct Deposit Information form to add, change, or cancel a direct deposit. Please complete the Direct Deposit Authorization form and send it by mail to Housing Choice Voucher Department, 178 W. Fourth Street, Chillicothe, Ohio 45601 or fax to 740-775-7896. All changes must be in writing to the Housing Authority no later than the 21st of the month before the desired month in which the direct deposit is to be processed, i.e. if we receive your direct deposit authorization by May 21, your direct deposit will then be effective June 1.
All funds will be credited no later than the 5th day of each month.
If you have any questions about how to complete these forms, you may telephone our office at 740-775-7881 and ask to speak to Tabitha Cobb Ext. 111.
If you wish to request a rent increase, after the first year of your lease with your tenant. If you have a lease with a tenant who has a Housing Choice Voucher, you must give both the tenant and the Housing Authority a notice, in writing, 60 days prior to the increase. The rent amount requested must be determined by the Housing Authority to be "reasonable" in the current market. Send your request to the attention of the Occupancy Specialist who is working with your tenant.
Check discrepancy. Begin by calling the Occupancy Specialist that is handling your tenant's file.
Please note, your W-9 must be updated annually throughout your participation with the Housing Choice Voucher Program.


text:
Q: retrieving data from hive gives type cast error in flutter I am trying to get the weight data from hive using flutter, however, i am getting a below error:
type 'double' is not a subtype of type 'UserDataModel'

My user data is :
@HiveType(typeId: 2)
class UserDataModel extends HiveObject {
@HiveField(0)
final String lifestyle;
@HiveField(1)
final String sex;
@HiveField(2)
final String photoData;
@HiveField(3)
final int age;
@HiveField(4)
final int height;
@HiveField(5)
final double weight; plus consturctor & adapter.

I am trying to display an amount by calling a userBox:
  body: SafeArea(
    child: ListView.builder(
      itemCount: hiveBox.length,
      itemBuilder: (BuildContext context, int index) {
        ExerciseBox data = hiveBox.getAt(index);
        UserDataModel datas = userBox.getAt(index);
        return Container(
          child: InkWell(
            onTap: () {

                        },
                      ),
                      CupertinoActionSheetAction(
                        child:
   Text(Languages.of(context)!.deleteWorkout),
                        onPressed: () {
                          setState(() {
                            hiveBox.deleteAt(index);
                          });
                          Navigator.pop(context);
                        },
                      )
                    ],
                  ),
                );
              } else {
                showModalBottomSheet(
                  context: context,
                  builder: (context) {
                    return Column(
                      mainAxisSize: MainAxisSize.min,
                      children: <Widget>[
                        ListTile(
                          title: Text(
                            data.date.year.toString() +
                                "/" +
                                data.date.month.toString() +
                                '/' +
                                data.date.day.toString() +
                                ' ' +
                                data.date.hour.toString() +
                                ":" +
                                data.date.minute.toString(),
                            style: const TextStyle(
                                color: Colors.black,
                                fontSize: 15,
                                fontWeight: FontWeight.w500),
                          ),
                        ),
                        ListTile(
                          //leading: new Icon(Icons.photo),
                          title:
  Text(Languages.of(context)!.useThisSettings),
                          onTap: () {
                            if (hiveBox.getAt(index).isCustom == true)
  {
                              ScaffoldMessenger.of(context)
                                ..removeCurrentSnackBar()
                                ..showSnackBar(SnackBar(
                                    content:
   Text(Languages.of(context)!.settingsNoUse)));
                            } else {
                              setState(() {
                                int duration = data.exerciseTime *
                                    data.numberExercise *
                                    data.numberRepetitions +
                                    data.restTime *
                                        data.numberRepetitions *
                                        (data.numberExercise - 1) +
                                    data.changeRepTime *
                                        (data.numberRepetitions - 1);
                                MinutesTotal = (duration ~/ 60)
                                    .toString()
                                    .padLeft(2, '0');
                                SecondsTotal = (duration % 60)
                                    .toString()
                                    .padLeft(2, '0');
                                BurnedCalories =
   (datas.weight*4.5*0.0175*int.parse(MinutesTotal))
   .toString().padLeft(2, '0');
                              hiveBox.put('burnedCalories',
    int.parse(BurnedCalories));
                              });
                            }
                            Navigator.pop(context);
                          },
                        ),
                    );
                  },
                );
              }
            },

how to retrieve the data from the box? As u can see I am using 2 different box data, that should not be a problem, right? I am just learning flutter and very new to hive. help appreciated very much! Thanks!


text:
NYU Appoints Lisa M. Coleman as Chief Diversity Officer
Written by Blacknews.com
New York, NY — New York University President Andrew Hamilton today named Lisa Coleman to be Senior Vice President for Global Inclusion, Diversity, and Strategic Innovation and NYU's inaugural Chief Diversity Officer. Dr. Coleman will start in her position in September 2017.
Dr. Coleman comes to NYU from Harvard, where she has served as the Chief Diversity Officer and Special Assistant to the President since 2010.
Dr. Hamilton said, "Many people on our campus have long worked hard to improve NYU's record on equity, diversity, and inclusion. But this issue is a priority for me, and appointing a senior person – who will report directly to me – in whom we can repose the responsibility, is an important and necessary step to advance our efforts."
He continues, "Among the many candidates the Search Committee reviewed, Lisa Coleman stood out. She has a strong record at her previous posts. She already knew and understood NYU well, having received her doctorate here. And her scholarly background will benefit NYU's efforts. But more even than these important qualities, what distinguished Dr. Coleman was her character: her forthright nature, her wisdom, her ability to connect with students, faculty, administrators, and staff; her energy; and her evident desire and ability to bring people together."
"We are glad to welcome Lisa Coleman back to NYU and have great faith in her ability to help us be the diverse, welcoming, and inclusive university we want to be," he conclude.
Dr. Coleman – who will report directly to the president and be part of the Senior Leadership Team – will, in close collaboration with Provost Katherine E. Fleming, lead the development and implementation of a strategic plan to systematically advance equity, diversity, and inclusion across all NYU schools and units.
Prior to Harvard, Dr. Coleman had worked in a similar capacity at Tufts University from 2007 to 2010. Prior to becoming Tufts' first senior diversity officer, she directed the Africana Studies Program and taught in American Studies, English, and Women's Studies. Before joining Tufts, Dr. Coleman also taught in the City University of New York system and held positions at Merrill Lynch, Inc. and the Association of American Medical Colleges in Washington DC.
Dr. Coleman is an alumna of NYU, where she earned a Ph.D. in the American Studies program. She earned her B.A. from Denison University in Granville, Ohio, and three master's degrees from the Ohio State University.
People On The Move - Kirk Sykes M.Ed.
Published on: 2016-07-03 Reads: 5178 times
Baltimore (BBR) - Education - Kirk Sykes, M.Ed. has been named Executive Director of Secondary Schools...
Howard University Honors Cathy Hughes As New Namesake
Silver Spring, MD — Howard University honored Cathy Hughes, founder and chairperson of Radio One,...
The Average Black Family Would Need 228 Years to Build the Wealth of a White Family Today
(THE NATION) - If current economic trends continue, the average black household will need 228...
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Mareena Robinson Snowden, is the first Black woman to graduate from MIT with a Ph.D. in Nuclear Engineering
(Blacktour.com) - Black girl magic was in full effect earlier this month when Mareena Robinson...
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text:
Q: How to gracefully handle sql injection in Spring data JPA Affected:

*

*Spring Data JPA 1.10.2, 1.9.4

*Other unsupported versions are also affected

Spring:
https://pivotal.io/security/cve-2016-6652
http://cve.circl.lu/cve/CVE-2016-6652
Mitigation:
Users of affected versions should apply the following mitigation:

*

*Users are advised to upgrade to Spring Data JPA in version 1.10.4
(Hopper SR4) or 1.9.6 (Gosling SR6). These versions contain
sanitizing of the Sort instances handed to the data access layer and
only allow referring to domain object fields and aliases used in the
JPQL backing the query method.

*Should users still need to hand complex sort expressions to the data
access layer, they can use the newly introduced JpaSort.unsafe(…) to
reinstantiate the old behavior.
Question:
We are using latest version of Spring data but security assessment tool shows that  Sql injection vulnerability in code , should we start using OWASP ESAPI API on Repo level ?


They say you gotta live every day as if it's your last. I don't recommend that. I tried that one time. It was a Wednesday -- I woke up, quit my job, slapped a cop and hit on my girlfriend's mother. Then, Thursday rolled around. Much to my chagrin, found out they don't have no bumper stickers telling you what to do the day after you lived your previous day as if it was the last day of your life.


text:
You are here: Home1 / The positive branding of Islam
author: Angelic Caroline Alihusain-del Castilho
The positive branding of Islam
Download the PDF file
Qatar and the World: Branding for a Micro-State
There are two factors that have shaped Qatar's integration and place in the international system. The first revolves around the constraints and problems of small states while the second is Qatar's response — a strategy of branding the state for survival. This article discusses Qatar's situation as a micro-state and analyzes the nature and success of its response.
Public diplomacy and nation brand
In a time where interaction with citizens is the key to diplomatic success, Morocco still lags behind other small states and does not yet pursue efficient strategies of public diplomacy and nation brand.
The emergence of international public opinion and the origins of public diplomacy in Japan in the inter-war period
The emergence of international public opinion and the origins of public diplomacy in Japan in the inter-war period.
Australia's Public Diplomacy: Building Our Image
Nation branding and the role of public diplomacy in assisting small island states in developing strong nation brands
The concept of applying branding principles and strategies to nation states has been around for decades. However, in recent years, the concept has occupied prime attention in academia and the business sector.
Branding the Nation – The historical context
Changing Minds, Winning Peace: A New Strategic Direction for US Public Diplomacy in the Arab and Muslim World
A reprint of the historic report of the Advisory Group on Public Diplomacy for the Arab and Muslim World, this document was submitted to the US Congress in 2003 as a first step toward reforming America's dilapidated strategic communication infrastructure. The bipartisan Advisory Group, chaired by Ambassador Edward P. Djerejian, made a series of recommendations in this report that helped re-shape US public diplomacy.
Britain TM: Renewing Our Identity
The rhetoric of public diplomacy and propaganda wars: A view from self-presentation theory
Efforts by governments to affect foreign public opinion through direct communication – and in competition with rival governments – have been a stable and consistent feature of international diplomacy since the turn of the twentieth century.
Public Diplomacy's Branding Trap
Branding India: An Incredible Story
Public Diplomacy and Nation Branding: Conceptual Similarities and Differences
Brands and national image: An exploration of inverse country-of-origin effect
The study explores the relationship between perceptions about products produced in a country and the country's reputation and image. It considers country-of-origin effect (COO) from an inverse perspective; rather than looking at how national reputation affects perceptions of products, it measures how brand image affects country image. It used a method that blends survey and experimental design to test the effects of brand association on country image using 488 subjects. The results indicate support for an inverse COO: knowledge of the country of origin of a brand can enhance the image of the c...
Marketing a Country: Promotion as a Tool for Marketing a Country
It has been ten years since the first occasional paper by the Foreign Investment Advisory Service, Marketing a Country, was published. In that time Marketing a CountrY has become a standard text on the structure and functions of agzncies that promote foreign direct investment. I have seen copies of the paper in ministries and promotion agencies all over the -world. Usually pages are dog-eared, and the text is heavily underlined, indicating intense study of the contents. Marketing a Country created a languagTe for discussing the investment promotion function, and has provided a rationale fo...


After an automobile accident, the party at fault may seem obvious. However, things are not always as clear-cut as they seem. Especially when death or injury is involved, it is helpful to contact an experienced auto accident attorney , who can help to determine whether there is a crash worthiness case associated with the wreck. Crash worthiness refers to design flaws by the auto manufacturer or the component supplier. Several such issues have made the news in recent years, like the Ford Explorer rollover cases, and the Toyota sticking accelerator cases. Auto accident lawyers often spend a lot of time and resources finding the underlying cause in such cases. Frenkel & Frenkel was once involved in a case where a car burst into flames after being rear-ended, and they uncovered a design defect that caused a bolt to pierce the gas tank upon impact. Often, the loss associated with a crash worthiness case can be devastating. Expensive injuries or the even more devastating loss of a loved one can be overwhelming to a family. Insurance is often not enough to cover the costs associated with such a case. Contacting reputable car accident attorneys like Frenkel & Frenkel can help you hold the responsible parties accountable, and ensure that you have the ability to cover your financial losses. They will leave no stone unturned in seeking justice when a manufacturer has been negligent in preventing such loss.