Yo, what's up, boy? Who are you? I'm Jegeeney. Who? I'm Jegeeney. Why are you stuttering? No, I meant I'm Jegeeney. As in ghetto, Jegeeney. Jegeeney? Oh, you're not the actual Jegeeney. No, no, no, I am. I'm just the cheaper version, the less quality one. I wish you were joking. Did you just make a wish? No, it's just an expression. And that's one wish gone. Wait, what? Yeah, I don't make the rules. OK, so what are the rules? Well, there's only one rule. Every time you say I wish, everything after that counts as a wish. So be careful. You have two wishes left. Oh, so I have three. You had three. Why three? It's always been that way. Yeah, but why three? I wish to know that. Oh, wish granted. OK, so what's the answer? You have three wishes, because I said so. One wish left. OK, so what do I really need? I want to find my missing sock to complete my pair. Really? You want that? I can get you an island in the Bahamas, and all you want is a sock. OK, then let me rethink this. I got it. It better be clever. I want a new pair of socks. Hey, if you could have a wish, what would you wish for? To be free, like in Aladdin? Are you shitting me right now? You know how cool this is? I got super-powered motherfuckers. I want a new apartment, one bedroom.  Maybe a little kitchen, but not too big. I'm not asking for much. I don't want to bother. You're super- I really want to fly. Economy plus. If possible. I want to be invisible. Now we're talking. But only when people are asleep. I don't want to bother. I want to be super strong. Lift buses, lift houses, right? No, there's this one jar I can't open in the kitchen. So it would just be for this one jar, and this one time. I'm pretty sure I can open it next time. I really want to travel back in time. To save someone's life? To visit an ancestor? No, there was this promotion on toilet paper that I think I heard about. I just want to go back in time and see if it's true. And look at the deal. I want to talk to animals. Anyone can already talk to animals. Look, I'll talk to this cat. Hello, hello, meow, meow, meow. But I'm shy. I want to control the weather. Creating storms, huh? Providing rain in Africa. No, I bought this umbrella a while ago, and I never got to use it. I want to run fast. So you don't have to use the plane anymore? No, so that I don't miss the plane. I've missed it twice already, and I don't like it. I want to breathe underwater. Oh, nice, so you can explore the vast ocean. No, it's because when I'm showering, I can't breathe well. Hey, can you make me rich? Yeah, I was hoping you wouldn't say that. You don't remember? Ghetto genie? Oh, so I can't get my own Ferrari, right? You know Toyota's are good too, right? I can make a red second hand. But you said you could get me an island in the Bahamas. But I never said what type of island. I was thinking more like a two square meter deserted island, and you can't get out of it. I really want to make the world a better place. Everybody deserves to be equal. So as a regular guy who only wants good for his planet, I wish to make peace around the world. Yeah, what are you saying? Yeah, I didn't hear that. Oh, by the way, you're out of toilet paper. So the wish before would be useful. Why don't you replace it yourself? You used it. Yeah, no, I don't do that. So you were saying, I wish, right, because why would I get three wishes? Time to go to work. Yo, trying to sleep, I don't have a place to stay. What the?


Speaking of that, it's time to get a W. I don't know man.  How many yards? What up, stop? Yeah. But I'm saying that that position. For sure. It's just the way you play.  The game is short. So. What up with it, man? Let's get it, guys. Front check. Yo, don't watch hockey. I'm gonna hockey, man. Is it 2-1 now, man? It's not 2-1. Stop it. 2-1 check. That man wanna go and win that game. If he was up two scores or something, I would be like, okay, we're about to be 14-13. That was a fake. Don't do it. Man, it's this glitcher user in Sean Taylor, man. They need to take safetys out of these positions like this. He's been complaining about that for real.  I just really don't like that. Why is it stupid? It's just, come on, man. Because you got it. It's just. It's supposed to be solid, man. I mean, when you keep it, obviously, when you're defense, you love it, but I hate that you have Sean Taylor right now.   Oh, yeah. Good history. That's why I wish we was on balance. But. Do that. Do that. Fumble. Woo! They said there's fumbles on the surface. I don't know why you would play.  No, it's not happening. Don't do it.   No, the spy was bagging my life right now.   I was just all in a bad spot. I can't believe my safety don't even, like, try to get an animation right there. I got to hit Vernon Davis. He could have got that first. I think you hit the outright right there. You're good.  I got to hit Vernon Davis. I might have got that first on the zigzag. Ah. He'll kill me there. You're serving, boys. Come on, man. I said, no big plays in the run. We'll be all right. We'll get out of here.  That was two. I felt like that was more than that. What are we playing for? I just matched up, so we just decided to play a few. Yeah, that's the third game, technically. Oh, you fumbled. Damn, that looked like the one. I was throwing a pick, too. Kind of instant block shed. Like, what is this game on right now? Man. Watch the cops. Hold on, W. Lay that aggressive, man.   It should have been worse right now. Have a good one, Cypher. See you tomorrow, bro. You know, shots to pack eggs in 100 bits. Appreciate you, bro. It hasn't came close to stopping me lately. Come on, man. What's okay? Ren plays a life right now. Girls call him Nubby? What?  That's right. You work with that Nub, you know what I'm saying? You ain't working with a Nub. You ain't trying hard enough. It's that yellow wall, bro. EJ, he's feeling better, man. Gentlemen. It's a 27-66 in a bill. 34 away from 5-1.  Overthrow, overthrow. Oh, my God, Cam Chancellor. Why are we 7 yards? You want him to guard the seat? I don't know.  That was so bad, Cam.  Jesus Christ. That was a huge play. It's an obvious run from this situation. So he might pass. I was thinking about it, honestly. It's an obvious run from this, especially when you're shot. What's up, Pops? Bye-bye. This is hot right here, boys. This is hot right here. It's green. It's raw. It's hot, boys. It's hot, man. Oh, that's how you feel? Good deal, boy. You don't shoot through a 6, man. I damn sure was rushing one person when you were in 5-1, though. I know. That's why I got to get you. I was like, too. Ain't no quarterback Joe in the same team. Damn, bro. Yeah, it was a good stop, I am. I feel like I get that I'm in really, really good control again. Oh, yeah, that's a good play. You can overcome it, too. Dang, I'm like that? I'm gonna keep living on ads like that. Nothing open here, boys.   I can go get 7. Going for it? Good deal, boys. Why would you go for this? You know what? He said absolutely like this is the car. We got the ball right here. I'm gonna get the ball back for the half. You're not that dumb. How is that? You think that's really dumb? Seriously. You think that's dumb? Yes. I punched you to the 50-yard line. Taking the sack was bad. That's what killed me. He's justifying me.   I think it's pretty smart. Seriously, how is it dumb? You put me on inside the 10-yard line. I put you with the 10-yard line. It's just as easy for you to score from the 10-yard line. Bro, I said 130. You think just going 50 yards is gonna... Listen, I feel like you was gonna get in field goal range. I'm serious. I feel like you was gonna get in field goal range. That puts you in the hardest field goal range for you to score a touchdown. It happened and the toss actually popped. Seriously.  If I stood the 30-yard line, I would have justified that one. We can poll maybe 10 players.  No, seriously, you would have ran the whole clock and took three at the worst. I get what you're saying about the run-clock thing, but that's not in the first half. The end of the game is different. This guy not run a little fast, man. Thank you, man. He caught that. He's not gonna just keep running with balls.  Come on, man.   That's why you're running Morse. I don't know how he's playing Morse. He's faster than Morse. He's gotta be. Morse has 91 speed. My Morse, I don't have that Morse that... He's 90 speed. It's like in regs, that's the easiest touchdown of my life. Fuck, man. It was a debate to give him the ball right there. It's like... The end of the game is different, bruh. End of the game, that's definitely the call.  For sure. I wanted the ball, but I didn't want to go 3-3. I don't know. Damn, you still have a long day. Good hit, Sean. Pick it, pick it.  What's up, pups? I'm in her office. Pups, what you doing? You gotta see his vampire teeth. His vampire teeth? No, I didn't see it. Good day. God damn it, man.  What happened to my aim on that? I moved it all the way to the left last second. Oh, my goodness. Backed off cover, Sue is just a... I see games, I see, I see. I just never, I never throw that ball down. No, two men on the top, too. That's on me. I even backed that dude up right there. I mean, just, I mean, it didn't look great, but just, I put Tyra Gilder in at the time of the game.  Same player, I hate these players. He ran the same defense. Play my supposed to call. Pups, what are you laughing at? What was that? On what, though? Well, Kane's in your culture? Yeah, I'll box him, I'll box him. He's off to save his half, really? I did. Ah, man. Really bad last drive. Same thing that happened last. Two bad drives in the half. I need a fumble, come on, boys. Nah, it had me going plus three at that call. That wasn't because of the call. I just gave up a couple of streaks.  You mean seven here? Oh, yeah. Three's okay with seven. Definitely seven. Makes you feel good here.  Good swat, kid. Let's go champ. Oh, man. That play was going to be open our way. Yeah, number second. They got you.  That was good coverage, though.  Yeah, I didn't go hard right there. I'm going to give it a huge play. Hit the underneath five first. Holding the three here. What up with the DPC? Chilling, chilling, chilling. Other game, we got disconnected. I got disconnected. No, that's not enough to catch. Who's that B? Yeah, that was the feeling. That route would beat me again.  I'll throw it early because I thought you would see it and run over there. Yo, shout out to Marco for Grosso for subbing to the channel.  Sub 27, 67 to the middle. It was good. That's Twitch Prime, too. Anybody with Twitch Prime, Amazon Prime, you can sub for free to anybody on Twitch. What up, BD-Wink? Shout out to my man, Zoom Reads, with the sub, man. Twitch Prime.  I'm going to break it out later in the game. We're probably not ready for it.  That's okay. What? Just one little time, and then girlie went backwards. What's up with it? Chipped Skylark, what's good, bro? Take it easy, Big Mike. Have a good night, dude. I'm just making them take time. No big toss, please. It wasn't worth me turning the ball over there. I really should have used the clock more. We should be in the fourth quarter. Did you, uh, you had dinner? Yeah. You got? Okay. Did you look at the dinners? Yeah. Give me the ball. Some of them are marked like what they are, and then you just... So I think they all have some sort of reps. All right, Chad, we just need points to start. Yeah, we just need points to start. It don't matter what... 7th is beautiful, though. You gotta be able to play football right now. I'll say that the next one is going for 80. Ain't no runs out of my playbook, papa. I know that money drive wouldn't be the love of toss. Yeah, I love you, Philly. This fight wide really is the biggest thing that's really giving me a lot of trouble. Honestly, really fucking... What's up with it, dawg? That's not a play, man. I'll tell you what, yo, Alon. Whoever problem got Alon, tell mommy to get the credit card out because these dudes, I mean, Clowney or what's his name, might as well not even be alive. There we go, Clowney. Eat! It's not GGs because he's on the goal. It might be.  Guard that shit, man. We good, y'all? I'm off, so I can't move. Wow, my clock is running too.  I can't even snap the ball. Can you go offside? I'm trying. Damn, I put... If someone really is on a money... I could snap it. I would have to call time out. That's so bad. You know Huddle, right? No, you try to get 7, but you'll settle for 3 if you need. Man, I'm disappointed in myself. Brought to a year-long dude fight. I don't need to talk to him.  I need to be on this guy because that's the guy that's killing me right now. Thank you.  I ain't mad at it. All I need is a couple of holes. Oh, my dude stopped. I'm glad I didn't throw it anyway. Trying to hit him up, trying, bro. We got to just get in the spot where we need to stop to get the ball back.  We'll settle, folks. We're good, we're good. I almost did it. I need a ball one time, man. That's a job, bro. 7 of the job. Give me a hand. What about me? Did that time Melvin Goren get the best playmaker ever? What is it? Pull the plastic off the box. What are you doing? Mr. You look like he has a knife, though. Oh, we can't let him catch it like that, man. Come on, Cam. Good day, man. Damn, he really sat down right there. What is he, in the hook? I thought I was supposed to be using him, but you caught me off him. Fuck. You got to try for 7 here, guys. It's so big if you can get that. Come on, Clowney.  Just beat him one time. Catch it.  You don't want me to score 7. Yeah, I know, but I want to cloud the run. I feel like this might get tighter if you do score here. Good game. That's the first time I try to throw it right at somebody. Oh, man. I've had this for five while, man. She's giving me trouble because I don't want to give her a big call, man. And not your daddy. No, no, no, no. No, no, no, no, no. What? What? Grandpa was kind of open.  He could have moved at the last second when he went to throw it.  It was right over? Yeah, man. He's open when you're watching. I'll get in the game. Y'all are cock-eyed. The same people that see everybody open are the same cock-eyed playing it. Stop it, bro. I appreciate it, though. Papa? Jesus. Papa? That's the look you have right now. What? What do you do? That was wild. He's trying to get into that.  That's kind of hot right there. What's up, little guy? What are these? What are those? Onside and then Gronk for the cash, boys. I'm getting three. Deeper than them, man. Sharkweed. That's real. I told you I wouldn't lose Superbowl. What'd you say? I told you I wasn't going to lose the Superbowl. I'm not damn sure I wasn't going to lose in Philly. Oh, here we go. I'll be right back, guy.


During the summer of 1942, Lafayette, Indiana, residents experienced a six-week reign of terror in which 50 serious and misdemeanor crimes were committed by one or more individuals. Beginning on June 2, the crime wave included 20 counts of breaking into automobiles, three counts of motor vehicle theft, approximately 20 misdemeanor counts of shoplifting and petty theft, six home and business burglaries, and two counts of aggravated assault occurred during two of those burglaries. This list does not include any affiliated counts of selling stolen property. Around 2.30 in the morning on June 20, Mrs. Mary Soller, 72, and her sister-in-law, Emma Soller, were asleep in separate rooms when they were both awakened by someone turning on the lights in each room. Thinking Emma was awake and needed assistance, 72-year-old Mary had just stood up when a man wearing a mask threw a one-quart glass milk bottle that struck her on the left side of her head, which then corrained off to hit a doorframe where it shattered to pieces. She then collected two $20 bills and headed them over, satisfying the burglar, who then made his escape. Suffering from a head injury and shock, the frail woman spent several days at a local hospital. Lafayette detectives investigating the case concluded her attacker used a common-style skeleton key to enter the home. The next aggravated assault came on June 30, while Mrs. Frances North was ironing clothes in her kitchen as her two young children slept. Since her husband worked the night shift at an industrial plant, she was startled by a noise in the front room. When one of the children made the noise, she left to check on them. As she stepped into the front room, a masked burglar accosted her, screaming.  He then pushed her into another room and beat her. The intruder then ran out the front door, taking the revolver and a Waltham brand watch. Also suffering from shock, Mrs. North sat on the floor for several hours before she summoned the strength to scream for help. Eventually, neighbors arrived and the police were called at 12.50 am. Her attacker's description matched the description the Solar Sisters had given. Local detectives were already piecing together all the separate crimes and looking for connections. Knowing North's attacker would likely try to sell the Waltham watch, they were keen to find where it would show up. Their strategy worked and six days later, they found a man who purchased the watch in good faith for three dollars. From him, they traced the purchase back to the seller. On June 7th, the front page of the Lafayette Journal and Courier announced the crime wave was over with the arrest of Floyd Burton Loveless, 15, and his brother, Robert K. Loveless, 17. When Floyd was just three, his mother Hazel, 29, stepped in front of a train on June 15, 1930. It was written up in the newspaper like it was an accident. Their father worked for the railroad and was often gone. Their grandmother raised the boys in Clarks Hill, a village 15 miles south of Lafayette. On June 2nd, the boys left home for Lafayette and went on a crime spree. No stranger to the law, both boys were already on probation for prior offenses. Seven months earlier, Floyd was placed on probation after serving nine days in jail for the burglary of a rural home near Lafayette. Robert's probation stemmed from a 1939 conviction for motor vehicle theft. He first served time at White's Indiana Manual Labor Institute for that crime, a punitive juvenile facility with a school and working farm. Memories of that institution may have tapered Robert's tolerance for crime to only 15 misdemeanor counts of shoplifting. It was young Floyd who was Lafayette's John Dillinger for June of 1942. Behind bars, Floyd's confessions trickled out of him over the next five to six days.  This included the two assaults, the burglaries, the motor vehicle thefts, and 20 counts of breaking into a parked automobile. Tried in juvenile court first degree burglary, Floyd Burton Loveless was given the maximum sentence allowed, commitment to the Indiana Boys School until he reached the age of 21. Sooner, if the school trustees believed he had reformed, like most juvenile institutions in other states, IBS was a tough place.  However, since it was classed as a school and not a penal institution, the 1300 acre facility did not have an impassable fence or guard towers. The only measure to prevent any boy from escaping was a locked door for their barracks like quarters and a guard or two wandering the grounds. Floyd entered the institution on July 15. 30 days later, he and another boy, David Klein, 15, escaped, and it took six hours before someone noticed they were gone. Situated 30 miles northeast of Indianapolis, the boys stole a car and drove west, most likely taking the US 40, the fastest and easiest road to get there. They financed their trip by burglarizing homes. Floyd found a revolver in one of them and kept it for himself. He should have left it there. Shortly, it would change his life forever. By August 20, the two boys were near Elco, Nevada, where they quarreled and decided it was best to split up. Floyd let Klein keep the Indiana car, but Klein stayed with Floyd until he had commandeered one for himself. It didn't take long before Floyd found a truck with a key still in it. Klein drove behind him as they got back on the Victoria Highway, aka US Highway 40, to continue their journey to California. Stealing the truck was Floyd's second biggest mistake that day. It belonged to Elmer Hill, the popular manager of the horseshoe ranch at nearby Dunphy. Everyone knew Elmer's truck, and when Carlin Constable ate off burning, learned the stolen truck was coming his way, he parked his vehicle along the highway and waited. With Elco 23 miles east of him, burning didn't have long to wait. He had served as the town's constable for 26 years, re-elected by the people each time since 1915. Throughout the county, he was known as a reliable lawman. But on that day, August 20th, shortly before noon, the odds were against him. He spotted Elmer's truck, noticed someone else was driving it, and stood there until it stopped. And about that same time, the stolen car driven by Klein was also preparing to stop, but drove away when the constable waived him off. Burning walked over, opened the door, and told Floyd, he would have to take me in for being in a car I didn't belong in. Loveless, later testified. Not sensing the danger he was in, burning got behind the wheel, forcing Floyd to slide over to the passenger seat. He would later tell officials, I pulled out a gun and said I wouldn't go back with him. He grabbed the gun and I shot him. The gun got jammed and we started finding, and then I pulled the trigger again, and it worked, and I drove off down the road. Burning collapsed on the driver's seat, and Floyd pulled him the rest of the way into the truck. Then, with Burning slumped over on the passenger side, Floyd got behind the wheel and continued driving west. Over the next few miles, Burning moaned in agony. Loveless replied that he was taking him to a hospital. Instead, he caught up with Klein a little further down the highway at Primo Station, a middle of nowhere gas station, and rest stop within natural spring.  Klein later testified that when Loveless got into the car, he asked him what happened, and Floyd said he had shot the officer and left him in the truck. Klein said nothing, drove a little further, and then exclaimed that he saw a pistol lying in the sagebrush by the side of the road. When Floyd went to look for the weapon, he drove off and left him there. The end for Klein came about 90 miles further down the highway, near Winimuka, where a roadblock was waiting for him. Klein took the shoulder and drove around it, forcing him to take a 7-mile dirt road that was a dead end. He was trapped. A cruiser belonging to deputy sheriff George Armstead pursued Klein. Writing shotgun with him was Wallace Van Reed and Arthur C. Sebbis, who were running against each other to be the next sheriff of Humboldt County, trailing behind him a thick cloud of dust. The two opposing candidates put nine bullets in Klein's car, hoping to stop him. None of them did. At the end of the road, they watched as Klein discovered the dead end, turned the car around, and sped towards them. Setting up another roadblock at a narrow point in the road, all three got out and readied themselves. As he had done before, Klein steered for the shoulder in hopes of driving around them. Both candidates saw this and opened up with two shotguns, shredding the windshield. Two of the 12 gauge pellets hit Klein in the cheek, and that was it for him. He was taken into custody and driven back to Elko County. Meanwhile, an Elko County deputy sheriff found loveless walking along the highway a few miles west of here, where he had abandoned the stolen truck and a gravely wounded constable burning, paralyzed from the neck down. On the drive to Elko County jail, loveless confessed to stealing a truck and shooting burning, but when he met up again with Klein behind bars, he recanted his confession and refused to say anything more. Burning died from his wounds 36 hours later. Elko County's case against loveless began in juvenile court, but was soon bumped up to district court, a move that would have him tried as an adult. He was formally charged with murder on September 12th, pleaded innocent on September 22nd, and his trial began on September 28, 39 days after he mortally wounded burning. Jury selection lasted most of the first and second day, and by the end of business on the third day, September 30th, the trial itself was over, and loveless was found, guilty as charged in the information. His defense attorney had, but just one strategy, avoid the death penalty. The high point of the trial was when loveless took the stand and wept as he described shooting constable burning. Explaining himself as best he could, loveless told the jury he didn't know burning was a law enforcement officer, since he was wearing plain clothes. Dale Klein's actions to rid himself of loveless and his willingness to testify against him saved him from being charged as an accomplice. He would later be taken into federal custody for interstate motor vehicle theft, and held until the age of maturity. According to Nevada State law, District Judge James Dysart, who oversaw the case, had no choice but to sentence loveless to death, which he did on October 5th. His execution date was scheduled for December 13th. One Nevada newspaper pointed out that his sentence could later be commuted to life in prison by the State Board of Parton and Perot, or the governor. But it was clear from almost the beginning that was never going to happen. From the time he was bumped from juvenile to district court, to the judge sentencing him to death, Nevada newspapers, including the Reno Gazette and the Nevada State Journal, systematically lied about Floyd being 16 years old. He wasn't. He was 15. He would turn 16 on November 2nd. They had his files. The FBI had his files. They didn't get it wrong on accident. They never got Klein's age wrong. He was always 15. 16 made Floyd loveless more of a man and less of a boy if his true age were published. Several days after his sentencing, loveless was transferred to the Nevada State Prison Carson City, where he resided on death row. On November 30th, two weeks before his execution date, his defense attorney, Taylor Wines, filed an appeal, something he didn't have to do. In his oral argument before the State Supreme Court, Wines rightly pointed out that his client was found guilty of murder, but the kind of murder was left out. According to section 10068 of Nevada Compat Laws 1929, murder is not just murder. First degree or second degree murder must be clearly spelled out in the charges and instructions to the jury. All murder which shall be perpetrated by means of poison or lying in wait, torture or by any other kind of willful, deliberate and premeditated killing or what shall be committed in the perpetration or attempt to perpetrate any arson, rape, robbery or burglary shall be deemed murder of the first degree. And all other kinds of murder shall be deemed murder of the second degree and the jury before whom any person indicted for murder shall be tried shall, if they find such person guilty thereof, designate by their verdict whether it be murder of the first or second degree. On April 21, 1943, the Nevada State Supreme Court ordered the verdict set aside and Floyd Lovelace to receive a new trial. Returning to Alco County District Court, his second trial began on November 15, 1943 and like the first one, he was over on the third day, November 17th. This time the language was clear, guilty of murder in the first degree. Lovelace, now 17, was again sentenced to die in the Nevada Gas Chamber. But fortunately, a second trial also gave him the right to an appeal which his defense filed on February 29, 1944. As he waited for oral arguments and the court's decision, Floyd Lovelace lost his bitterness and became a proper young man. He kept time for prison boxing matches, read books in his cell, wrote letters, embraced the Catholic faith, and played on the prison softball team. His skills as a second baseman even got his name in the sports section of the Nevada State Journal when NSP trounced the 947th Guard Squadron 6-2. Oral arguments were heard on July 10 and the Nevada State Supreme Court published its opinion on August 6. Judgment was affirmed. Execution was scheduled for September 29, 1944. During his last 44 days, the State Board of Partons and Paroles refused to commute his sentence and the governor declined to intervene. His attorney filed a writ of habeas corpus claiming Lovelace was insane. But this only postponed his execution from 5 a.m. to 6 o'clock that evening. At that time, the warden read the death warrant to him and a physician attached a stethoscope to his chest. Lovelace's last request to the warden was for roses to be sent to his grandmother back in Indiana. This was granted. At 6.24 p.m., he was led from his cell and walked his last 13 steps with father Buell by his side. Although no last words were recorded, it is customary for prisoners about to be executed to ask forgiveness from all those in life they had hurt and to forgive all who sinned against them. Lovelace was then strapped into a steel chair and the doctor connected the stethoscope to monitor just outside the small cinder block building.  Floyd took a deep breath as he had been advised to do and by 6.29 p.m., he was pronounced dead.


All right, we're going to get started. Thank you all for being here today. My name is Jesse Suin. I'm a co-founder and CTO of Acuity, and one of the original creators of the Argo project. So we're here at ArgoCon, and you might expect me to be singing the praises of Argo CD and GitOps. But actually, today I'll be spending a little time kind of explaining some of the challenges with GitOps and some of the things that Argo CD isn't great at and why we feel that more tooling needs to be developed to improve that developer experience. A little bit about Acuity. We are a team founded by Argo creators, leads, maintainers of the Argo project. And we help companies implement GitOps with Argo. Acuity offers an easy to manage platform for running a more scalable and secure version of Argo CD. And we also offer solutions and support for the Argo project. So if you think about what GitOps is, it's really more of a philosophy than and not really a solution. Basically, GitOps is just adding additional rules and constraints on how you should be deploying changes to your environments. But it really doesn't provide any guidance on the practices or processes to go about achieving that. So at the end of the day, GitOps just made things harder for everyone. Because a lot of this stuff that we were previously doing before GitOps in our CI pipeline no longer worked after GitOps. And when we built Argo CD, we built it as a tool to help practice GitOps. But it was never enough. It's great at deploying changes from a Git repository to a single environment. But there's a lot of things that it doesn't do. First, it has no understanding of multiple environments or a concept of a pipeline to orchestrate changes across environments. It doesn't even help you write changes to Git because it expects some other tool to do that ahead of time. And finally, once it does sync an app, it doesn't do any verification of that update after the fact, such as running any form of tests or analysis. So over the years, a number of small features and Argo ProjLab projects have cropped up to deal with these limitations. And I call these a spot solutions because each of these tools or these features only solve one piece of the puzzle. And none of these consider the bigger picture or the overall developer experience. And with all these approaches, it just feels like we're kind of trying to brute force Argo CD into something it was really never designed to do. So we set out to kind of build a tool that approaches the challenges of GitOps in CD holistically. We wanted the solution to provide a flexible pipeline to define how changes are promoted between different environments. We wanted an intuitive UI that gives a better understanding about what was or needs to be or about to be promoted. We wanted to hide the GitOps nuances to developers who frankly don't really care about GitOps. And we wanted to provide guardrails ensuring that promotions are happening within defined processes. So Cargo is an open source project that we recently announced to fill in these gaps. And it's a multi-stage GitOps application orchestration tool for promoting changes through multiple environments. And our biggest goal of Cargo is to provide a better, more intuitive layer on top of your GitOps tooling. We want to enable application developers to safely promote their apps through multiple environments. For normal day-to-day operations, we envision app developers to be visiting the Cargo UI more often than the Argo CD UI because to promote their changes day to day. They still go to Argo CD when there's a problem, you see logs, events, but in the happy path, Cargo would be used more often to deploy things. So with Cargo, you'll get better visibility into your promotion process. You're seeing all your environments at a glance, understanding what's running, where, and what's safe to deploy. You'll be able to see history of what was deployed along with links back to your source code repo and commit history. And we built it with the GitOps use case in mind. And one of the unique features about our Cargo is its ability to promote configuration, not just images. And in other words, you're able to promote manifest changes like environment variables from stage to stage. Cargo makes Git writebacks and rollbacks really easy with one click. And finally, you can start practicing progressive delivery by qualifying your artifacts before they're allowed to deploy to other stages. So if you're interested in Cargo, check out our GitHub. And we also have a Discord server where you can ask questions, chat with other users, and also where we host office hours. So the biggest thing you can do is just give us feedback, try it out, and yeah, start the Git repo. Thank you.


Engines for electric cars, magnetic resonance imaging in medicine, electric candles in the kitchen, the charger of your smartphone, radio, Wi-Fi and so on. Any device that exploits electricity or magnetism is fundamentally based on the Maxwell equations. The goal of this video is not to derive the Maxwell equations theoretically or experimentally but to present them as simple and understandable as possible. I will also briefly explain the mathematics that occur in the Maxwell equations. However you should know what a partial derivative is and what an integral is before you continue to watch the video. To understand all Maxwell equations you first need to know what an electric and a magnetic field is.  The electric force between these two spheres, which are the distance r from each other, is given by Coulomb's law. Here 1 over 4 pi epsilon 0 is a constant pre-factor with the electric field constant epsilon 0, which provides the right unit of force, the unit Newton. Now what if you know the value of the big charge and want to know the value of the force that the big charge exerts on the small charge? However you do not know the exact value of this little charge or you intentionally leave that value open and only want to look at the electric force exerted by the big charge. So you have to somehow eliminate the small charge q from Coulomb's law. To do so you simply divide Coulomb's law by q on both sides. This way on the right hand side the small charge drops out and instead lands on the left hand side of the equation. The quotient on the left hand side f over q is defined as the electric field E of the source charge q. By calling it source charge we imply that the charge q is the source of the electric field. The electric field E thus indicates the electric force which would act on a small charge when placed at the distance r to the source charge. So far only the magnitude that is the strength of the electric field has been considered without taking into account the exact direction of the electric field. However the Maxwell equations are general and also include the direction of the electric field. So we have to turn the electric field into a vector. Vectors are shown in boldface. Handwritten mostly with a little arrow above the letter to distinguish it from scalar, poor numbers. I omit the arrows because they make the equations unnecessarily ugly. The electric field E as a vector in three dimensional space has three components EX, EY and EZ. Let's look at the first component. The first component depends on the space coordinates X, Y, Z and it is the magnitude of the electric field in X direction. That is depending on which concrete location is used for X, Y, Z the value EX is different. The same applies to the other two components EY which indicates the magnitude in the Y direction and EZ which indicates the magnitude in the Z direction. The components of the electric field thus indicate which electric force would act on a test charge at a specific location in the first, second or third spatial direction. Another important physical quantity found in the Maxwell equations is the magnetic field B. Experimentally it is found that a particle with electric charge Q moving at the velocity V in an external magnetic field experiences a magnetic force which deflects the particle. The force on the particle increases in proportion to its charge Q and its velocity V that is doubling the charge or the speed doubles the force on the particle. But not only that the force also increases in proportion to the applied magnetic field. The unit of this quantity must be such that the right hand side of the equation gives the unit of force that is Newton or kilogram meter per second squared. By a simple transformation you will find that the unit must be kilogram per ampere second squared. This is what we call the unit of Tesla and we call B magnetic flux density or short magnetic field. The magnetic flux density describes the external magnetic field and thus determines the magnitude of the force on a charged particle. The equation Q times V times B for the magnetic force on a charged particle represents only the magnitude of the force. In order to formulate the magnetic force with vectors analogous to the electric force, the force, the velocity and the magnetic field are expressed in vector form. Now the three quantities are not scalars but three-dimensional vectors with components in the x, y and z direction. Now the question is how should the velocity vector V be vectorially multiplied by the magnetic field vector B? If you look more closely at the deflection of the charge in the magnetic field you will notice that the magnetic force always points in a direction orthogonal to the velocity and to the magnetic field lines. This orthogonality can be easily taken into account with a so-called cross product. The cross product of two vectors V and B is defined so that the result of the cross product V cross B which is a vector is always orthogonal to the two vectors V and B. The first component is VIBZ minus VZBI. The second component is VZBX minus VXBZ and the third component of the cross product is VXBY minus VYBX. For the force to be always orthogonal to V and B we take the cross product of V and B in our equation. So in vector form the magnetic force is generally given by Q times V cross B. The charge is an ordinary scalar factor. As you can see the physical quantity B describes the strength of the magnetic field which leads to a deflection of moving charges. Now you have learned the two important physical ingredients found in the Maxwell equations. The electric field E and the magnetic field B. Both are so-called vector fields. This means that to each location XYZ in space you can assign an electric and a magnetic field vector indicating both magnitude and direction of the electric and magnetic fields.  These four Maxwell equations can be represented in two different ways. There is the so-called integral form which expresses the Maxwell equations with integrals and the differential form which expresses the Maxwell equations with derivatives. While the differential form of Maxwell's equations is useful for calculating the magnetic and electric fields at a single point in space the integral form is there to compute the fields over an entire region in space. The integral form is well suited for the calculation of symmetric problems such as the calculation of the electric field of a charged sphere, a charged cylinder or a charged plane. The differential form is more suitable for the calculation of complicated numerical problems using computers or for example for the derivation of the electromagnetic waves. In addition the differential form looks much more compact than the integral form. Both forms are useful and can be transformed into each other using two mathematical theorems. One theorem is called divergence integral theorem and the other one curl integral theorem. If you understand the two theorems it will be easier for you to understand the Maxwell equations. Let's first look at the divergence integral theorem. This is what the divergence integral theorem looks like in its full splendor. First let's look at the right-hand side of the equation. The A represents a surface enclosing any volume for example the surface of a cube, a sphere or the surface of any three-dimensional body you can think of. The small circle around the integral indicates that this surface must satisfy a condition. The surface must be closed. In other words it must not contain any holes so that the quality is met mathematically. The surface A is thus a closed surface. The F is a vector field and represents either the electric field or the magnetic field when considering the Maxwell equations. So it is a vector with three components. DA is an infinitesimal surface element that is an infinitely small surface element of the considered surface A. As you may have already noticed the A in the DA element is shown in boldface so it is a vector with a magnitude and a direction. The magnitude of the DA element indicates the area of the small piece of the surface. The DA element is orthogonal to the surface and by definition points out of the surface. The dot between the vector field and the DA element represents the so-called scalar product. The scalar product is a way to multiply two vectors. So here the scalar product between the vector field and the DA element is formed. The scalar product is defined as follows. As you can see from the definition the first, second and third components of the two vectors are multiplied and then added up. The result of the scalar product is no longer a vector but an ordinary number as so-called scalar. To understand what this number means you must first know that any vector can be written as the sum of two other vectors.  Another mathematical fact is that the scalar product of two orthogonal vectors always yields zero which means that in our case scalar product between the part F orthogonal and the DA element is zero. However the scalar product between the part F parallel and the DA element is generally not zero. So now you can see what the scalar product on the right hand side of the equation does. It just picks out the part of the vector field that is exactly parallel to the DA element. The remaining part of the vector field that points in the orthogonal direction is eliminated by the scalar product. Subsequently the scalar products for all locations of the considered surface A are added up. That is the task of the integral. The right hand side of the divergence integral theorem thus sums up all the components of the vector field F that flow into or flow out of the surface A. Such an integral in which small pieces of a surface are summed up is called surface integral. If as in this case the integrand is a vector field this surface integral is called the flux phi of the vector field F through the surface A. This description is based on what this surface integral means. It measures how much of the vector field F flows out or flows into a considered surface A. If the vector field F and the surface integral is an electric field E then this surface integral is called electric flux through the surface A. And if the vector field F is a magnetic field B the surface integral is called magnetic flux through the surface A. Now let's look at the left hand side of the theorem. V is a volume but not any volume it is the volume enclosed by the surface A. dv is an infinitesimal volume element in other words an infinitely small volume piece of the considered volume V. The upside down triangle is called nabla operator and it has three components like a vector. Its components however are not numbers but derivatives corresponding to the space coordinates. The first component is the derivative with respect to x the second component is the derivative with respect to y and the third component is the derivative with respect to z. Such an operator like the nabla operator only takes effect when applied to a field and that also happens in this integral. The nabla operator is applied to the vector field by taking the scalar product between the nabla operator and the vector field. As you can see it is the sum of the derivatives of the vector field with respect to the space coordinates x, y and z. Such a scalar product between the nabla operator and a vector field F is called the divergence of the vector field F. The result at the location x, y, z is no longer a vector but a scalar which can be either positive negative or zero. If the divergence at location x, y, z is positive then there is a source of a vector field F at this location. If this location is enclosed by a surface then the flux through the surface is also positive. The vector field so to speak flows out of the surface. If the divergence at location x, y, z is negative then there is a sink of a vector field F at this location. If this location is enclosed by a surface then the flux through the surface is also negative. The vector field flows into the surface. If the divergence at location x, y, z disappears then that location is neither a sink nor a source of the vector field. The vector field does not flow out or into or it flows in as much as out so the two amounts cancel each other out. Subsequently the divergence that is the sources and sinks of the vector field is summed up at each location within the volume using the integral. Such an integral where small pieces of volume are summed up is called volume integral. So let's summarize the statement of the divergence integral theorem. On the left side is the sum of the sources and sinks of the vector field within a volume and on the right side is the total flux of the vector field through the surface of that volume and the two side should be the same. The divergence integral theorem thus states that the sum of the sources and sinks of a vector field within a volume is the same as the flux of the vector field through the surface of that volume. Now consider the second important theorem necessary for understanding the Maxwell equations the curl integral theorem. If you understand the divergence integral theorem then the curl integral theorem should not be totally cryptic to you. You already know the vector field F the scalar product the nabla operator and the DA element should also be familiar to you now. First let's look at the right hand side of the equation the L is a line in space. The circle around the integral sign indicates that this line must be closed that is it should form a loop whose beginning and end are connected. The DL is an infinitesimal line element of the loop so an infinitely small piece of the line. Again you should notice that the DL element is shown in boldface. It's a vector with a magnitude and a direction. The magnitude of the DL element indicates the length of this small line and its direction points along the line L. Now the scalar product between the vector field F and the line element DL is formed. You already know what the task of the scalar product is. First split up the vector field into two parts into F parallel which is parallel to the DL element and into F orthogonal which is orthogonal to the DL element. The scalar product with a DL element eliminates the orthogonal component without touching the part of the vector field parallel to the DL element. Since at each location the DL element points along the line only the part of the vector field that runs along the line L is considered in the scalar product. The other part of the vector field drops out. Then the scalar products for each location on the loop are summed up using the integral. Such an integral in which small line elements are summed up is called line integral. Now you know what happens on the right hand side of the curl integral theorem. The line integral measures how much of the vector field F runs along the line L. Because the line is closed this scalar product returns to the same point where the summation started. The closed line integral thus indicates how much of the vector field F rotates along the loop L. If the vector field F in this line integral is an electric field E then this line integral is referred to as electric voltage along the line L. On the other hand when the vector field F is a magnetic field B the line integral is called magnetic voltage along the line L. The voltage in the case of an electric field is proportional to the energy that a positively charged particle gains as it passes the line L. A negatively charged particle on the other hand loses this energy as it passes the line L. The line integral of the electric field that is the voltage measures the energy gain or energy loss of charged particles as they pass through the line L under consideration. Now you should have understood the right hand side of the curl integral theorem. Let's look at the left hand side now. Here the surface A occurs again. This surface unlike the divergence integral theorem must not be a closed surface but it is simply the surface enclosed by the line L. The A is again an infinitesimal piece of the surface A and at any location it is orthogonal on that surface. In addition here comes the cross product which you have already met when we discussed the magnetic force. Here the cross product is formed between the nubla operator and the vector field F. In addition to the scalar product it is the second way to multiply two vectors. This cross product between the nubla operator and the vector field F is called the curl of the vector field F. The result in contrast to the scalar product is again a vector field. This new vector states how much of the field F rotates around a point within the surface A. Then the scalar product is formed between the new vector field nubla cross F with the infinitesimal surface element DA. Thus as you already know only the part of nubla cross F is picked out which runs parallel to the surface element. Since the surface element is orthogonal to the surface A the scalar product picks out only the part of the vector field nubla cross F which is also orthogonal on the surface A. Subsequently all scalar products within the surface A are summed up by means of the integral. Let's summarize the statement of the curl integral theorem. On the right hand side the vector field F is summed up along a line L. Thus the rotation of the vector field around the enclosed surface is considered. On the left hand side the curl of the vector field F is summed up at each individual point within the surface. Both sides should be equal according to the theorem. The curl integral theorem thus states that the total curl of a vector field F within the surface A corresponds to the rotation of the vector field F along the edge L of that surface. Well it is somehow clear that the rotation of the vector field inside of the surface cancels in the summation in only the rotation of the vector field along the edge L remains. With the acquired knowledge you are now ready to fully understand the Maxwell equations. Here we go. This is the first Maxwell equation in integral form. The left hand side of the Maxwell equation should be familiar to you. It is a surface integral in which the electric field E occurs. This integral measures how much of the electric field comes out of or enters the surface A. The integral thus represents the electric flux through the surface A. On the right hand side is the total charge Q which is enclosed by the surface A divided by the electric field constant which provides the correct unit. The first Maxwell equation states that the electric flux phi through a closed surface A corresponds to the electric charge Q enclosed by the surface. By the way, Coulomb's law is a special case of the first Maxwell equation. With the previously learned divergence integral theorem, which combines a volume integral with the surface integral, the surface integral on the left hand side of the first Maxwell equation can be replaced by a volume integral of the divergence of the electric field. The enclosed charge Q can also be expressed with a volume integral. By definition, charge density rho is charge per volume. Bring the volume to the other side. The volume V can generally be written in the form of a volume integral. That is, the volume integral of the charge density rho over volume V is the charge enclosed in that volume. This turns the right hand side of the Maxwell equation into a volume integral. As you can see, we integrate over the same volume V on both sides. For this equation to be satisfied for an arbitrarily chosen volume V, the integrants on both sides must be equal, the right integrant being multiplied by the constant 1 over epsilon 0. And now you have discovered the differential form of the first Maxwell equation. The divergence of E is equal to rho over epsilon 0. On the left hand side of the differential form, you can see the divergence of the electric field. You know that at a specific point in space, it can be positive, negative or zero. The sign of the divergence determines the type of the charge at the considered point in space. If the divergence is positive, then the charge density rho at this point in space is positive and thus also the charge. In this point of space, there is therefore a positive charge, which is a source of the electric field. If the divergence is negative, then the charge density rho is negative and thus also the charge. At this point of space, there is therefore a negative charge, which is a sink of the electric field. If the divergence is zero, then the charge density rho is zero as well. At this point in space, there is either no charge or there is just as much positive charge as negative, so the total charge at this point is cancelled out. At this point in space, an ideal electric dipole could be located. The first Maxwell equation in differential form states that the electric charges are the sources and sinks of the electric field. Charges generate the electric field. This is the second Maxwell equation in integral form. There is nothing unfamiliar in this equation. Everything should look familiar to you now. On the left hand side, you see a surface integral over A. Now, not an integral of an electric field as in the first Maxwell equation, but an integral of a magnetic field B. According to the equation, the magnetic flux through the closed surface A is always zero. The second Maxwell equation states that there are always just as many magnetic field vectors coming out of a surface as there are vectors entering the surface. With the divergence integral theorem, the surface integral can be transformed into a volume integral. This way, the divergence of the magnetic field comes into play. This integral shall be zero. The integral for any volume V is only always zero if the integral is zero. In this way, the second Maxwell equation emerges in its differential form. Divergence of B is equal to zero. If the divergence is zero, this means that at each point in space, x, y, z, there is either no magnetic charge, also called a magnetic monopole, or there is just as many positive magnetic charge as negative, so the total charge at that point cancels out, such as an ideal magnetic dipole, which always has both a north and a south pole. The north pole corresponds to a positive magnetic charge, and the south pole corresponds to a negative magnetic charge. Since there are no magnetic monopoles, there are no separated sources and sinks of the magnetic field. The second Maxwell equation in differential form states that there are no magnetic monopoles that generate a magnetic field. Only magnetic dipoles can exist. The second Maxwell equation, like the other Maxwell equations, is an experimental result. That is, if someday a magnetic charge should be found, for example a single north pole without a corresponding south pole, then the second Maxwell equation would have to be modified. Then the Maxwell equations would look even more symmetrical, more beautiful. This is what the third Maxwell equation looks like in an integral form. You probably already know the third Maxwell equation under the name of Faraday's law of induction. This right here is the most general form of the law of induction. On the left-hand side is a line integral of the electric field E over a close line L, which borders the surface A. This integral sums up all the parts of the electric field that run along the line L, which means it sums up how much of the electric field rotates along the line. The integral corresponds to the electric voltage U along the line L. On the right side there is a surface integral of the magnetic field B over an arbitrary surface A. This integral corresponds to the magnetic flux phi through the surface A. This magnetic flux is differentiated with respect to time t. How to differentiate a function as, in this case, the magnetic flux with respect to time, you should have a down pad. The time derivative of the magnetic flux indicates how much the magnetic flux changes as time passes. So it's the temporal change of the magnetic flux. The larger the change of the magnetic flux, the greater the rotating electric field. The minus sign takes into account the direction of the rotation. If the change in the magnetic flux is positive, the electric voltage is negative. If the change in the magnetic flux is negative, the electric voltage is positive. The electric voltage and the change of the magnetic flux thus behave opposite to each other. The minus sign ensures energy conservation. Maybe you know that by the name Lenz law. As you can see, according to this Maxwell equation, rotating electric field produces time varying magnetic field and vice versa. The Lenz law now states that the magnetic flux, which is generated by the rotating electric field, counteracts its cause. Because if it was not the case, the rotating electric field would amplify itself and thus generate energy out of nowhere. That is impossible. So let's summarize. The third Maxwell equation states that the electric voltage along a closed line corresponds to the change in magnetic flux through the surface bordered by that line. In other words, a change in the magnetic flux through the surface A creates an electric voltage along the edge of A. Consider another important special case. If the magnetic field does not change in time, the right side of the Maxwell equation will be eliminated. Then the equation states that the electric voltage along a closed line is always zero. So there is no rotating electric field as long as the magnetic field doesn't change over time. If an electron passes the closed line L, it would not change its energy. Because as you learned, electric voltage indicates how much energy a charge gains or loses when it passes a line. In this case, the voltage is zero, therefore no change in energy. With a curl integral theorem, you can transform the integral form into the differential form. This theorem connects a line integral with a surface integral. To do this, simply replace the line integral with the surface integral. This brings the curl of E into play. On the other side, you may pull the time derivative inside the integral. Since the equation applies to any surface A, the integrants on both sides must be equal. And just now, you have discovered the differential form of the third Maxwell equation. Curl of E is equal to the negative time derivative of the magnetic field. The third Maxwell equation in differential form states that the changing magnetic field B causes rotating electric field E and vice versa in such a way that the energy conservation is fulfilled. Let's move on to the fourth, the last Maxwell equation. What kind of an integral is on the left side? Exactly, a line integral of the magnetic field B along the closed line L. This is the definition of the magnetic voltage U. On the right-hand side occurs the electric field constant epsilon 0 and the magnetic field constant mu 0. They ensure that the unit on both sides of the Maxwell equation is the same. In addition, something new occurs here, the electric current I. When electric charges flow along a conductor, they generate a current I. Also, there is another sum end. You know the surface integral of the electric field. This is the electric flux through the surface A. In addition, a time derivative is ahead of the electric flux, so the whole thing is the temporal change of the electric flux. On the right side, there are two summands, one contribution by the current and one contribution by the change of the electric flux. Thus, the fourth Maxwell equation states that the rotating magnetic field is generated first by the electric currents through the surface A and second by the changing electric field. Let us now derive the differential form. With the curl integral theorem, you can transform the line integral into a surface integral, thus bringing the curl of the magnetic field B into play. Now we have to express the current I with the surface integral so that we get a single integrand on the right. We can do that simply by using the current density J. It indicates the current per area through which the current flows. Consequently, the current can also be written as the surface integral of the current density J over the surface A. Note that here in the integral, the scalar product of the current density is taken with the DA element. So we pick only the part of the current density vector that runs parallel to the DA element. Only this parallel part of the current density contributes to the current through the surface A. You can pull the time derivative inside the integral. The two surface integrals can now be combined into one because we integrate over the same surface A. For the equation to be satisfied for any surface A, the integrants on both sides must be equal. And you already have the differential form of the fourth Maxwell equation that you are looking for. Curl of B is equal to mu zero times J plus mu zero epsilon zero times the change of the electric field over time. The differential formulas states that the curl of the magnetic field B at a point in space is caused in two ways. By the current density J and by an electric field changing at this point in space. Let us summarize the four Maxwell equations of electrodynamics in their compact form, in their differential form. The first Maxwell equation, divergence of E is equal to charge density over epsilon zero. Electric charges generate an electric field. The second Maxwell equation, divergence of B is equal to zero. There are no separate magnetic charges, thus no magnetic monopoles. The third Maxwell equation, curl of E is equal to negative temporal change of the magnetic field B. A changing magnetic field creates a rotating electric field and vice versa. The fourth Maxwell equation, curl of B is equal to mu zero times J plus mu zero epsilon zero times the change of the electric field over time. Electric currents and a changing electric field generate a magnetic field. So now you finally learned the foundation of all electrodynamics. Isn't it amazing how much knowledge and how many technical applications are contained in these four equations? By the way, Maxwell equation still hides something interesting that can be revealed by a few steps of transforming the equations. Electromagnetic waves, light. But that's a topic for another video. With this in mind, bye and see you next time.


Welcome to Toffy TV, it's the Everton News Daily, Steve Rotherham, the Liverpool City Region Mayor. If you understand what that means because I don't quite understand what that means. I've spoken, I believe for the first time, about Everton's proposed move to Bramley Mordoch. He was speaking to business leaders in London and he said, we are not looking at a sports stadium in isolation but looking at it as an opportunity to regenerate on a much wider scale. We've all been to sports grounds where it's difficult to get to, certainly in public transport sense, we need to be building in the likes of public transport access to the things we are developing. So for instance at Bramley Mord, it will be a stadium but a regeneration project that includes housing, hotels, retail, leisure and other things. But what we'll do is ensure that we do have public transport links because getting 20 or 30,000 people out of a football stadium along routes that are already congested is about urban planning. He also went on to mention that. He will be getting more powers in 2020 to help move these things along but he said that Everton's planning permission and getting things in place should be well done by 2020 so he doesn't think he will deal with this particular instance but in 2020 projects the size of this will fall under his remit. So he sort of said that it should be all sorted by 2020. Some people have taken that the wrong way and said he's saying that the grounds going to be built in 2020. Now what he's saying is that everything should be in place and maybe the ground is already started to be built or everything will be in place but I think that's the first time I've heard Steve rather than speak about it so that's really good. That's really, again, we've heard the same people, the same noises from the same people for far too long now and it was good to get someone else speaking about it at a national event for property and all that kind of thing. And it's also good this and it's also good that he's speaking about it not just as a stadium but as a thing for Liverpool because we've obviously heard a lot of voices talking about negative things regarding the stadium and what it won't do for the city. What he's saying is it will do lots for the city and we've got to make sure that when that happens we have things in place like transport links and there's been talk in the last couple of weeks about things like trams coming into the city and things like that so or a light railway, something of that nature. I don't know whether that would be connected with Bramley Mordoch but doing the roads at the moment at Bramley Mordoch, the change in the infrastructure of one of the main roads that leads down there. So there are getting things in place, there was pitches this week of the new cruise ship terminal so it's all good, it's all good for the city and hopefully good for ever and moving forward and hopefully all the saying and voices who have been criticising it for whatever reason will start to get on board as it is a brilliant thing for the city of Liverpool and the surrounding areas so hopefully that'll happen soon. Back to the football or get into the football. Richarlison played 25 minutes last night for Brazil, he came on for Brazil. It was Neil Nell at the time and he ended up beating Argentina one Neil in that game and got a big shiny trophy for winning the superclass ago. They scored in the last minute, if they hadn't scored it would have gone to Penalty's because it was a real trophy. Whether Richarlison would have took a Penalty that would have been quite interesting but they won 1-0 and it's great to see him playing for Brazil, obviously it was one of his big dreams and now he's played well four times in the last month also so that's fantastic. Although they took the number nine off him, he's now number seven which I don't mind that but just stick to it so we can get our shades. You know what I mean? I've already ordered me our nine one. We'll have to get our seven one now. So that was good for him. Lucas Dinho and Keat Zuma were both on the bench for France last night and that's where they remained as France came from behind to beat Germany 2-1 in the UEFA League and as I say both of them stayed on the bench so that's great. Dinho played 90 minutes to the night against Iceland and Zuma played 45 minutes so that's that's great. I think that was it from from first team players playing last night. Keat and Dahl scored an absolute wonder strike for the England under 21s in the last minute against Scotland. It was a typical Keat and Dahl goal, got the ball on his left foot and just killed it into the top corner. Absolutely fantastic goal. England have already qualified for the European championships in the summer so it was a much-changed side. He was the only Everton player to start the game. Donna Cavill did come on but it was in the 87th minute just before England got their second goal so Keat and Dahl absolutely absolutely brilliant. Obviously this creates a lot of talk with Evertonings about whether he should play or not. If you're on Patreon we've done a video this week and we talk about Keat and Dahl a little bit in it. You can watch that and see our feelings on it. Maybe another low move is needed. Maybe to Jamie. Somewhere high up you know my feelings. I don't think play should go to the championship if they've already played you know a little bit of Premier League football. Get them to a good level which shows whether they're good enough because I just don't think the championship does show that. Yeah so we scored last night and Andy Robinson came off the bench in 90 plus two minutes for the United States. They drew 1-1 with Peru. He played Mugs again the other night as they were beaten 3-2 by 3-1 or 3-2 by Columbia sorry which he didn't have a great game but it was a good learning exercise playing against really top class players to see whether he will be up for it and again we've done a video over on Patreon talking about Leighton Baines and Phil Jelke and one of the things we discuss is will Leighton Baines get a contract for next season? Andy Robinson will he be up for it if he doesn't. So go and watch that if you're on Patreon or if you're not on Patreon come and join us on Patreon. That's about it. I think we've been linked with Adam Ramsey but again I think we've been linked with them loads of times and I think we'll be linked with them loads more and until there's real meat on the bone I don't really see the point in going into that too much but that's it for the Everett News Daily today. All the internationals have finished and we look forward to the game on Sunday against Crystal Palace. There'll be more coming on that. There will be the match preview and the start 11 show and all those good things so keep your eye out for all those videos here on Toffee TV. We'll see you later.


Upgrade your smart phone with Appalachian Wireless. Get $300 off selected models, capture memories, stream and stay connected with the latest technology. Visit one of our stores or Appalachian Wireless dot com right now. The city of Pikeville will be holding their Jeep show and shine on Friday July 7th. We've done car shows in the past. There's been specialty shows with some really high and hot rides in the past, but around here we're people who like it out in the mountains. We like to get out in the mud, so we're going to have a Jeep show and shine. The Jeep show isn't just for seeing nice looking Jeeps. Awards for Best in Show, Best Vintage Jeep and Best Jeep Truck will be given out to those registered in the event. Maybe you want to see an old school Army Jeep. It'll be here. Maybe you want to see the brand new 2023 Jeep Gladiator truck. It'll be here. The little guys get to look at them. The little gals get to look at them. Everybody just loves it. There are drivers out of the cars all shined up. These Jeeps will just look great in every way, shape and form. Jeep show and shine will begin at 6 p.m. on Friday July 7th. There is no entry fee for the Jeep show and registration will take place on site. For more information about the event, you can email kevinatappwireless.com. For Mountain Top News, I'm Kelsey Dean.


You have probably noticed that this lockdown isn't being taken quite as seriously as the previous one. Now in part, this is inevitable. People are less scared of coronavirus this time around. Now they understand what it's about. It's also down to past mistakes from this government. People saw that Dominic Cummings broke the rules and the government defended him. So they think, why should I follow these rules? But in the short term, I think there are also some very simple failures of this government to sort of get people in the spirit of a lockdown. They haven't really bothered with any messaging at all to tell us to stay at home. They sort of had one announcement, oh, we're in a second lockdown. And that was it. We haven't really heard anything from them after that. Now, if what you're looking for is an effective public messaging campaign, which sort of shows you why staying at home is a good thing, why lockdown is necessary, no one has done it better than the Germans, who for some reason are just better at coronavirus than the rest of us. Well, the rest of us in Western Europe anyway. Let's take a look at this, which puts our government to shame. But fate had other plans with us. When the invisible danger threatened everything we believed in, and fate suddenly ended in our hands. Well, that's how we all gathered our courage and did what was expected of us. The only right thing. We did nothing. Nothing at all. We were as lazy as the washbers.  Our couch was the front. And our patience was our weapon. Sometimes I have to smile a little when I think back to that time. That was our fate. That's how we became heroes back then. In this coronavirus winter 2020. I can't believe I've stayed in all day. Now I get to feel pride. Now I feel civic pride if I have sat on the sofa for 16 hours before going straight back into bed. And I always was a bit surprised that the government weren't really running on this message. Because obviously I don't want to be here downplaying the huge costs, the huge downsides of lockdowns. And I know for so many people it's incredibly difficult. Not everyone can just lie down and be lazy and watch movies all day long. If you've got young children, you've got a difficult living situation. Not everyone can do this. But it does seem to me that the government haven't made or our government haven't made enough of the fact that one of the most important lower cost things we can do.  I think that comparison between, obviously it's silly and it's meant to be light-hearted, but the comparison between what do you have to do to rise up to the challenge in a war, you have to put your life in danger. Whereas this time around, our government at least, by hammering home how a lockdown would be the worst thing to possibly happen, I think partly because it's bad for the economy, they almost overstated the point because given that this is probably the biggest crisis that's going to occur in my first 35 years on this world, I don't know when climate change is going to properly hit, then how lucky are we that the response for us, the way we step up, is we just watch movies and read books and read magazines. Again, I'm not saying this is a universal experience, but as it's the most important thing we can do to get us through this winter without having enormous amounts of coronavirus deaths, it just surprises me that the UK government hasn't gone for this same sort of tactic, this same style of saying, no, stay at home, one, it might not be the end of the world for you, and also this is the number one thing you can do to help us survive this particular wave of the pandemic. Ash, I want to go to you. Am I supposed to levels? I mean, is that attractive to you, what that advert is telling you to do to sort of step up for your country, for your nation, for your people, for the world by lying on your couch for 16 hours a day watching movies and getting takeaway? I mean, I've been a leader in this. Years before the pandemic was even on the horizon.  And where's my medal? You've always been at the cutting edge of global trends, actually. I'm not surprised you're at the forefront of this one as well. As long as they're mostly horizontal. But the reason why that the British government can't speak in that register is because one, it's always been split on the issue of lockdowns. Why we went in late. The, you know, conservative cabinet is written with divides on whether or not the health of the country should be bounced against the health of the economy. It's a false opposition, of course, because, you know, a healthy economy is one where people aren't dying of a deadly disease by the, by the, you know, truckload. But the cabinet is divided. You've also got the problem of internal party management. You've got, you know, back benches who are very, very anti-lockdown. So that's one reason why the government couldn't be convincing and just roll out the advertising campaign and, you know, really try and make that messaging work. The second thing is that they completely emulated their own credibility over the Dominic Cummings affair. So you can't really make the point of, you know, everyone do your bit. Stay at home when the government's chief advisor is raced up to Durham, tested his eyes at Barnard Castle and done a press conference from the Downing Street Rose Garden to tell everyone why it's okay.  So there isn't a figure within the government that can take the lead on this and speak with credibility and with authority. And the third thing, I think, is the specific subversion of the kind of wartime heroism within that advert. And that's why it's so funny and so effective.  Is that this country, this country and its sense of its history, collectively, the nation is high off the smell of its own farts. It really is. And because of the way in which the story of World War II has been turned into a story of British exceptionalism, you know, the sole unique achievement of Great Britain, it means that it's been remarkably flexible and can be bent into whatever the needs of the moment are as long as you emphasise that story of British exceptionalism. So once upon the time, that story of British exceptionalism was an exceptional collective effort. It was something which justified the transformative labour agenda of 1945. But today, it's most frequently invoked with regards to coronavirus as a kind of, you know, I was born in 1958, but don't let that stop, you know, that's not going to stop me telling you how I single-handedly survived the blitz. Therefore, I'm going to throw myself upon the mercy of the pandemic. The logic there, of course, again is faulty. I'm saying, you know, people survived the blitz not by interrupting their day in any way. There were Anderson shelters.  There were really strict rules about this kind of thing. You know, so imagine, I don't know, take some lockdown skeptics.  No, you wouldn't have. So I think it's also about the way in which that sense of British exceptionalism and the story of British exceptionalism and the way in which World War II is invoked has become actually really corrosive to the collective effort which is needed in order to suppress the virus, right? The virus and its ability to infect people is the kind of cumulative product of all of our social behaviors and we don't have a national story for that, which is powerful, which is dominant, which is hegemonic at the moment. And I think that that's why the Germans were able to produce this advert. There are, you know, specific things about the conservative government, this conservative government, but I also think that there are, you know, longer term historical factors at play as well. I imagine the history of the wartime spirit in Germany is pretty goddamn complicated. I don't really know how it works when they play off that particularly historical analogy. But I mean, in a way though, I think the Cummings thing, I don't think we can overstate the importance of that because the wartime analogy, I mean, that was played on quite a lot in the first round of the lockdown. You remember sort of the BBC changed its entire programming to be this is for a lockdown, you know, you had that. Who's that? Joe Bates, is that his name? Joe Wicks, the PE guy. The PE guy with the long hair, sort of like, you know, parents love him. He was doing the sort of exercise on the television for you to do in your living room. There was this whole sort of, all of Britain's cultural industries and political class sort of came together to say, we're doing something exceptional now. We're coming together to solve a societal problem which needs a collective solution. Let's all do it together. Now I think two things happened, which was one, Dominic Cummings broke the rules. So the message had to transform from we know this is hard, but you can do it. Let's make the most of it too. We know this is hard, which means that we can't expect anyone to follow the rules because they're just too difficult. Anyone using their common sense would break them. Which became basically the government's official position. And also I would link back actually to what you said Ash there, which is that the spirit which was generated in the Second World War in this country did lead to a Labour government who sort of invested in the economy, created a more collectivist economy. And I think basically many people in the Conservative Party freaked out that that would happen again. So they saw that in the first wave, in the first lockdown we had, that was sort of encouraging a collective spirit in the population, people being, people suggesting, oh maybe we should pull together, maybe we should pay essential workers more, maybe we should pay nurses and doctors more. Maybe we should all sort of act as a community instead of being forced to act as these sort of atomistic, individualized beings. And they got freaked out by that, which is I think the biggest motivation actually behind this pushback against lockdown from sort of right wing back benches and obviously from people at the top of government as well. Rishi Sunak doesn't seem to like it very much. And as we've discussed Boris Johnson seems to go along with whoever had a conversation with him. Last, there is a sequel to that advert which is just as good actually. So we're going to show you that now that I'm going to go and get some more thoughts from Ash. 2020, that's long ago. We just got to know each other and we were curious about life, about our common future. But then suddenly everything changed and the whole country was looking at us full of hope for young people. We held our hearts and did nothing. We were shivering around the house, carrying as few people as possible and thus prevented the spread of COVID-19, this invisible danger that threatened not only our country but the whole world. Can you ask me today how we young people were able to walk around the house holding out their hands at that time? Maybe it's true when people say that special times need special heroes. I know God, yes, that's what we were. We were special heroes. We're a common hero and fight coronavirus. Every good public information campaign needs a love story, although I can see why they didn't lead with that because you could watch that and think, well, I would be happy for lockdown if I had a beautiful girlfriend. But if you don't have a beautiful partner, maybe you want to go out. Anyway, Ash, your thoughts on that? Maybe we shouldn't go down that rabbit hole. I didn't think you'd be that happy if you were locked down with your beautiful girlfriend. We could modify that video slightly. My primary romantic attachment in that video was in fact a bucket of fried chicken. I don't care who knows it. The thing about that one, in a way which was different from the first one, which was kind of lazy and a bit grotty, and that was why it was funny, is that this kind of leaned into the exceptional joys of lockdown in terms of being liberated from work.  And again, that's hard to cut into when you're a conservative government, which has been invested for the last 10 years of creating as precarious an economy for young people as possible, and also saying you've got to get back into the office. You've got to get back into universities. The entire country depends on you getting a half-priced Nando. What are you doing? Get out of your house. And I think that there is a bit of, it's that strongly conservative instinct within the Conservative Party which is you cannot, under any circumstances, undermine the sense of the inerrant nobility of working till you die. And so nobody wants to touch that, the idea that there are aspects of lockdown, particularly if you have a stable and secure income. If you don't have dependence to look after taking up more of your time, because it is really challenging if you have kids. And there are people who are carers for a family member and when you don't have help from the outside anymore, that's really, really difficult. But if you're in a kind of situation like me and you are in Michael, which is your income's somewhat stable, you've got a stable place to live, kind of all right. We like watching Netflix of takeaways and we're lucky enough to be able to do that for one winter. And there's also the stuff which is fun because you're working from home, which means that you can do your meetings with the camera turned off while you, for instance, try and perfect your recipe for flapjacks, as I've been trying to do.