Craft presents the Great Gilder Sleeve. Yeah. These company makers of parquet margarine and a complete line of famous quality food products presents Harold Perry as the Great Gilder Sleeve. Craft brings you the Great Gilder Sleeve every week at this time, written by John Whedon and Sam Moore, music by Claude Swaton. Here from the Great Gilder Sleeve in just a moment. When you ladies finish baking those light, fluffy biscuits and those crust brown dinner rolls the whole family loves, here's how to serve them in grand style. While they're still fresh and piping hot, pop them open and spread with delicious parquet margarine. Man, oh man, what flavor. Yes, parquet's fresh, delicate flavor adds a crowning touch that's sure to make any baking treat downright delicious eating. Parquet is a favorite spread for bread, hot toast and rolls, for pancakes and waffles, too, and millions of American homes. And it's a fine energy food, too, that's the best you can serve. What's more, craft fortifies parquet so that every pound contains 9,000 units of important vitamin A. So for delicious, satisfying flavor and for good nutrition, too, serve parquet as often as you can. Tomorrow, ask your dealer for parquet, P-A-R-K-A-Y. Parquet margarine made by craft. Yes, craft makes parquet. It's three weeks since his dismissal as Summerfield's water commissioner. The development of his friend, Pivro McGee's plastic mousetrap has been stymied temporarily for lack of catapult, and Gilder Sleeves affairs appear to be at a standstill. However, he still likes to eat as we see now, joining him at breakfast with his family. Pass the syrup, will you please, my boy? Here, more hotcakes, Miss Gilles, please. Yeah, but not too many birdies. Say, three or four, huh? How about you, Marjorie? No thanks. I think you and Lee Roy are disgusting. Disgusting? We're just healthy, my dear. Well, I'll take one more batch and that'll have to hold you. All right, Brittany. Oh, Mr. Gilles Sleeves, I wonder could you give me some money for the grocery bill? The man asked for it yesterday, but you was out. What does he want money now for? Tell him I'll pay him the bill in the usual way. I told him that, but he wants it now. Why? Why in the name of why? Well, I'll tell you how it was, Mr. Gilles Sleeves. The man came in yesterday afternoon and he says to me, hi, he says, is the boss home? No, he ain't, I says. And he says, well, when he gets home you ask him for this 1843, this due on the groceries, he says. Yes, Brittany. So I says to him, how come I says? And he says, Mr. Gilles Sleeves ain't working now, he says. And I can't afford to take no chances, he says. Chances, I said. Look here, man, you ain't taking no chances on Mr. Gilles Sleeves, I says. Why, he ain't paid me my salary for two weeks, I says. And I ain't one bit worried. Oh, my goodness. I sure told him dinner, Mr. Gilles. You sure told him, buddy. But he still wants his money. Well, I'm sorry about your salary, Bernie. It's strictly an oversight. Here. Oh. Little short. Well, here's one week anyway, Bernie. Oh, thank you, sir. If that's one of your friends, Leroy, have him wait outside and we finish breakfast. I won't have him watching every fourth full I put in my mouth. Oh, it might be piggy. I'll go see it. Darn kids, why don't they stay home? Maybe it's the grocery man. If it is, he can go right back and who is it, Leroy? This is her card. Oh, Miss Gladys Wheeler. Real estate. What does she want? How should I know? Well, ask her to come in. Okay. Isn't Leroy horrible? No, he's not. Well, he's growing up anyway. Come in, Miss Wheeler. Come in. Sit down. Have some hotcakes. Have some coffee. Oh, no, thank you, Mr. Gilles. I'm an awful pest interrupting your breakfast. I'd be glad to wait outside until you're through. Now, sit down. This is my niece, Marjorie. How do you do? How do you do? And my nephew, Leroy. How do you do, Leroy? Say, how do you do, Leroy? Okay, how do you do? Gosh, I'll let her in. Great kid. What can I do for you, Miss Wheeler? Well, Mr. Gildersleeve, I wonder if you've ever considered selling your house. Selling my house? No, I never had. I don't think I'd be interested. I must say, such a lovely home. Still, I have a client who's authorized me to offer you $12,000 for it. $12,000? Leroy. But Uncle Morton only cost $7,000. You children, leave the room, please. Miss Wheeler and I are talking business. And you don't know anything about it. I know the house cost $7,000 originally, Mr. Gildersleeve. Still, my client is willing to pay $12,000. Uh, cash? Cash. Grab an uncle. Leroy. Miss Wheeler, I wonder if you'd like to see the rest of our house. The dining room is no place to discuss business. I guess you've seen everything in our humble abode. Oh, it's all so nice and homey. Oh, yes, but I've been thinking of making a change. Man ought to move once in a while. Then you'll be dropping in at my office this afternoon to sign the contract. Oh, yes, I'll be there. Honestly, Mr. Gildersleeve, it's a pleasure for the man who knows his own mind. Ha, ha, ha. Well, I've always like to make decisions quickly. Bingo, that's me.  Oh, you think so? Well, most men would have to consult their wives. Haven't got one. Mm-hmm. No, sir. Put loose and fancy-free, full of beans, and will I make my own decisions? Well, at least most men would have to consult lawyers and goodness knows who. Why should I pay my lawyer a fee on such a simple deal as this? The old goat, he'll be surprised. Mr. Gildersleeve, as I said before, it's a pleasure to do business with you.  Say, did you ever like to... Do I like to what? Let it go. I'll be in your office this afternoon. Oh, that's fine. Thanks, Miss Gildersleeve. Oh, thank you. Goodbye, Miss Wheeler. Goodbye. Yeah. Bye, George. She's so cute, it's a shame to take advantage of her. Still, it's not her money. What's that? Agree to sell it, my boy. I'll sign the papers this afternoon. Leeroy! Leeroy! Leeroy! Subside, please, Leeroy. Of course, you understand your children will have to give your consent. I'm only the trustee. Well, I'll okay the deal. The house, buddy, we're going to move, isn't that swell? My, my. Are you really going to sell it? If you approve, my dear, the house really belongs to you and Leeroy. Oh, sell it. Sell it and buy a new one. I know just the house. Well, maybe we ought to talk about it a little. I hope you realize your uncle is making a pretty smart deal. Oh, sure. You know, I ought to go into the real estate business myself. It's a lot easier than I thought. Yeah, all you do is you buy a house for $7,000 and sell it for 12. Well, the whole trick, my boy, is to know values. Know values and make decisions quickly. If I'd been the kind of a man that fools around, can't make up his mind, she might have bought some other house. I told you to grab it, Uncle. Sure, but what do you know? I know how much a 7 from 12. Are you sure? No, children. Uncle Mort, it could be by the western's house. It's not very big, but it's cute. Oh, yes, it's a nice house. Very nice. It has two bathrooms. What about me hanging around where you take those bubble baths? I do not take bubble baths. You took one last week. You left a lot of bubbles in the tub, too. I did not. You did so. If that will do, children, the western house might be very nice, Marjorie. Probably get it for $6,000, maybe $5,000. How about something out in that new subdivision? Oh, I'd love to live in shady oaks. The houses are all new out there. The kitchens are nice out there, too. There's a lovely English cottage out there. Two bedrooms and three bathrooms. Only two bedrooms? Oh, Bertie would love the kitchen. Yeah, I'd love it, but I wouldn't want to sleep in it. We'll need something a little bigger than two bedrooms, Marjorie. But don't worry, there are dozens of houses in town that will be fine for us. Let's get a great big house. We don't need a mansion, my boy. As long as there's plenty of bathrooms, it'll be wonderful to have a house with a powder room. A powder room? Every house in Hollywood has a powder room for Uncle Mort. Why not? Yeah, let's have a rumpus room. If I'm going to clean all these rooms, I hope there's a restroom. Don't worry, Bertie. Good times are coming. You know, ever since that real estate woman walked in here this morning, I felt that everything was going to be fine. I'll take this money, we'll buy a new house, then I'll put the rest of it in mousetraps, and pretty soon I'll be a millionaire. And when I'm a millionaire, Marjorie will have two bathrooms all herself. Lee Roy will have a baseball diamond and you will have an assistant. Mr. Gilt! Don't laugh, Bertie. It could happen. This is just a standard form-sale contract, Mr. Gilt receive. It provides that you vacate your house within 30 days. 30 days? Well, that's customary. Oh, but of course I don't have to tell you I can see you've had real estate dealings before. Oh, yes, plenty of them. Would you care to use my pen or...? I'd just glance through the rest of this. Oh, by all means, take your time. Oh, thank you.  Not like an ordinary agent rushing a follow-in to something. Where do I sign? Right here. Oh, yes. Rock, Morton, P. Gilder, please. And the duplicate copy. That's the one I keep. That's right. Rock. Oh, pens don't dry. Oh, sorry, here's another one. Oh, pens. Rock, Morton, P. Gilder, please. Thank you. That does it. Yes, sir. Well, I have a feeling we ought to celebrate a little.  Oh, I'd love to, Mr. Gillespie, but I've got a customer waiting over on the other side of town. Some other time. All right, some other time.  I'd like to throw a little business your way. Oh, really? Well, you'll call me. Something around $5,000 or $6,000. Oh, well, I'm sorry, Mr. Gilder, please. What do you mean? Don't you want my business? Well, yes, but... Well, the fact is, there isn't a single house available in Somerfield. Well, what? Unless you'd be interested in something around 20 or 25,000. Give me back that contract. Now, Mr. Gilder, please. That would hardly be fair to my clients, would it? Fair. What's being fair about it to me? You swindled me out of my house for half what it's worth. And all the time you know I own a house. And all the time you know I won't have anywhere to go. You know where you can go, Mr. Gilder. Oh, my, George, if you... We'll be with us again in just a few seconds. If you like piping hot toast, pancakes, or waffles, try spreading them with delicious parquet margarine. And see what appetizing goodness the delicate, satisfying flavor of parquet adds to these tempting breakfast treats. If you carry a lunch to work at a school, you'll be glad to know that parquet margarine is one of the finest energy foods you can spread on bread or in sandwiches. And a few Mrs. Homemaker are concerned about good family nutrition as we know you are. You, especially, will want to know this important fact. Craft fortifies parquet margarine so that every pound contains 9,000 units of vitamin A. Yes, it's good to know that there is such an economical nourishing spread for bread with such delicious flavor and such dependable craft quality. So be sure to ask for parquet margarine because it's the best way to get the best quality. So be sure to ask for parquet P-A-R-K-A-Y parquet margarine made by craft only two ration points a pound. And remember, craft makes parquet. Now let's get back to the great gilder sleeve who's really painted himself into a corner. Having sold his own house for a good price, he can't find another to move into at any price. He's tried every real estate agent in town examined the classified ads and it's time out to get a haircut and think it over.  Well, Mr. Gilder sleeve, who's going to win the election? Hard to say, Floyd. Hard to say. You don't know anybody who has a house he wants to sell, do you? Why, are you in the market, commissioner? I may be shortly. Well, his fellow in here the other day and my family live in an old's mobile, Floyd. What I need is a house. Why, are you getting thrown out of yours? I'm not getting thrown out, I've sold it. Is that a fact? Funny, I didn't hear about it. I just told you. Bet you got a pretty good price for it, huh? A fair price. Yes, good solid house you got there, well built. Bet you got an easy 8,000 for it. 9,000, maybe. With a garage and all, maybe 10,000. I got a fair price. My problem now is to find a place to live. Yeah. Well, I got a nice little place there. Nothing fancy, you know what I mean? We could do with another bathroom. Wife's always hollering at me. Well, it's a roof over our heads. I'm not worrying about you, Floyd. It's me. Say, now you mention it, I hear where Otto Slesnik and his wife ain't getting along so good again. What's that to me? If I was passing that place here the night, they would carry on something fierce. I heard her call him a bum mechanic. That ain't good. Well, if you don't mind, Floyd, I haven't seen any local gossip at the moment. Now, wait. Supposing it was to go from bad to worse. Supposing they would have bussed up. Well, there'd be a house. Sure, you gotta think of those things. Wife happens to pass a remark. Man reaches for a piece of crockery. First thing you know, there's a house on the market. Floyd, you've given me an idea. Finish me up, will you? Practically done now. Of course, if you're thinking of that house of Otto's, it's only got five rooms. Tell me about it. I need at least seven. It's only an idea.  After all, life's no better roses. Otto and his wife, they're not the only lovebirds in town. If there was only some way... Just because a man opens the door for his wife or carries the groceries home for her, you don't know how he treats her when he gets her there. Floyd, how are the Thompson's getting along these days? Oh, I pray that's all straightened out.  Of course, maybe I ought to say this. No? Why? Well, I don't know this. I only heard. But it seems where Doc Pettybone came home at 4.30 the other morning and she put the bolt on the door and wouldn't let him in. Doc Pettybone always wondered how he stood it. Not a bad house, either. Well, that's only what I heard. Where there's smoke, there must be fire. You know what I mean? By George, I know where I can find out, too. Let me out of this chair, Floyd. They are commissioning. Thanks, Floyd. Thank you very much. Well, if it ain't Fred Kelly. What happened, Fred? No cracks, please. Where'd you get the black eye, Fred? Right into a door in the dark. Oh, that's too bad. Too bad. Uh, let me know if you hear anything, Floyd. Uh-huh. Dr. Pettybone? Well, yes, I do most of this perception work. I know that, Petey, but have you seen it? Yes, I have. As a matter of fact, Mrs. Petty and I played bridge with the doctor and his wife last night. You did, really? Well, how did they seem? Well, they seemed fine. Why? You, uh, didn't notice anything? Notice anything? I mean, you didn't feel any undercurrent there. They seemed to be getting along, all right. Why, yes. No kicking each other under the bridge table or anything? No, why? Nuts. Why do you ask, Mr. Galaxy? I've got to find the house, Petey. I've got to find one right away. Is, uh, this for yourself or for a friend? For myself, naturally. For my family. They'll be out on the street in 30 days if I don't find one. Yeah, yeah. I don't like to pry, Mr. Gillespie, but, uh, was it trouble with the mortgage? No, it was trouble with a woman. Oh, that again. The woman deceived me, Petey. They'll do it every time. Well, I wouldn't say that. Not every time. This one was a real estate agent. I thought if I sold my house for $12,000, bought another for five or six, I'd make a fair profit on the exchange. But she didn't tell me there aren't any other houses. She didn't tell me that. Have you thought of renting a house? Yeah, and so has everybody else. I've even thought of stealing a house, Petey. That's why I asked you about Doc Pettybone. Third things weren't so rosy there, and I thought maybe, say, how many rooms you got in your house, Petey? Mrs. Petey and I are very happy where we are, Mr. Gillespie. Yeah, I didn't think so. You don't know anybody who's leaving town or anything. No, I'm afraid I don't. The doctor hasn't happened to mention anybody who's on the anxious list. Not that I can recall. Perhaps if you waited till the winter season. I can't, Petey. I've got to have a house right away. I can't find one for love or money. You know, speaking of love... Yes? It's too bad you and Mrs. Ransom didn't hit it off there a while back. Why do you say that? Well, I always thought Miss Goodwin very attractive, but that place where she lives is a little small. Petey, I told you I'm all through with that stuff. No more of it. I'll never have anything to do with a woman again as long as I... Still, that's a nice house Lila's got there. Copper plumbing throughout. Nice shade of trees too. Yeah. Petey, I wonder... What? I wonder if Mrs. Ransom wouldn't like to go back to Savannah. After all, she's a long way from home up here, Petey.  Enjoy some of that southern comfort. Get some of that old cornpone. Hear those old banjos ringing. Man, I'd almost go with her. Glad you dropped in, Frogmore. I'll tell you, Lila. I've been a little worried about you lately. Oh, have you really had a nice... Yeah. When I think of you all alone in this great big house here, day after day... Well, I'm not completely alone. I have friends, you know. Oh, yes, of course. Of course you have. But I sometimes ask myself, Lila, if we really know who our truest friends are. Well, I always think of you as my friend Frogmore. I hope you don't mind. Oh, I am very much so. Yes, indeed. You must always think of me that way, Lila. Yes. But what I mean is... Well, everybody knows that a boy's best friend is his mother. A girl's, too. I suppose. Yes. People should stick to their mother and their family, Lila. We mustn't forget the old folks at home. Don't you ever miss them? Well, I think about them. I think about them a lot. But sometimes I feel I'd rather think about them than be with them. Oh, that's the wrong attitude, Lila. Frogmore, why are you suddenly so interested in my folks?  Well, it's not your folks so much, Lila. It's not that. I'm thinking of you. I... Uh, certainly.  You were born in the south. It's in your blood. Don't you hear it calling? Not at the moment. Lila, think of it. Moonlight and honey suckle. Soft summer breezes. Those old banjos ringing. I haven't heard a banjo in the south in 15 years. Well, you could take that one down with you. Think of that Southern cooking, Lila. Think of it. I am thinking of it. And you're thinking of something, too. Yeah, I wonder what it is. I don't know what you mean. Oh, yes, you are. I'm thinking of you, Lila. So far from home. Living all alone up here in this great big house. By the way, how many rooms has it got? Seven. Ever have any water in the cellar? Not a drop. Remarkable. Just the same I worry about you here, Lila. That's very sweet of you, Throckmorton, to worry about me. But I don't worry. Well, you should.  Seven rooms, you say? I never worry because I know that if anything should happen, if I should ever need protection, you're right next door. That's just Italy. Lila, I may not be next door. Throckmorton, you're not leaving town. Well, that depends. Depends on what? It depends on you. Oh, gracious. I mean, here you are, living all alone in a great big house. Here I am. I don't know how to say it.  Why don't you just come right out and say it? Well... That shithead ambushed me first. There. You got me all wrong, Lila. Times is on that now. What is it you wanted to say to me? Uh...  Well, I don't... I'd pay you a good price for your place, Lila. I'd pay you as much as it cost. You see, I gotta have a house. I sold mine. Lila, you're not gonna cry, are you? Lila, don't cry. It was only an offer, Lila. No harm in an offer. I didn't mean to hurt you. I'd take it all back. Keep your house, Lila. I just thought you'd like to go back home and get some of that fried chicken. Smell some of those oleanders again. Hear those old banjoos ringing. I'll make yourself at home, Gildy. You always do. There's an ashtray beside you. I was just enjoying my usual after-dinner K-lack water. Care for a glass? No, thank you. Judge? Yes, Gildy? I dropped over here tonight and let you in on a good thing. It has anything to do with mouse traps. Let me out. No. As a matter of fact, it has to do with this rat trap you're living in here. This what? Your house. I think I may have a prospective purchaser for it. That is, if the price is right. Sorry, I wouldn't be interested.  This is a bona fide offer. No, not interested.  What do you want to wallow around in a nine-room house for? I like it here. May not be beautiful, but it's comfortable, and I like it. I hope and expect to remain here till the day I die. But that may be years. Look, Judge, this man is no piker. He's prepared to offer $5,000 spot-catch for the whole shebang just as she stands. I might possibly consider $14,000. $14,000? That's $2,000 more than I got. If you think your house is worth more than mine... Wait a minute, Gilly. Do you mean to tell me you sold your house? Well, I didn't mean to tell you, Judge, but that's about the size of it. But, Gilly, that house isn't yours to sell. You're only the executor. It's held in trust for Marjorie and Leroy. No, I consulted them before I did it. Oh, you did? Well, why didn't you consult me? Well, dog gone at horse. Every time I consult you about anything, you send me a bill. Well, that's it. What am I going to do, Horace? I've sold the house and I can't find another one. Are you asking me what to do? Well, I'm asking you. I'll bill you, so help me. I'll bill you. Well, go ahead and bill me. All right. As your lawyer, I advise you to get that contract canceled. But how, Judge? How can I do it? Well, it'll take a good lawyer. Fortunately, you've got one. Yes. As your lawyer, I'll refer the contract to the probate judge in charge of the estate to whom it should have been referred for approval in the first place. Good. Do that. And as the probate judge in charge of the estate, I shall declare the contract null and void. Yep. Horace, can you do that? Watch me. By George, the law is a wonderful thing. Just a minute, please. Speaking again as your attorney, the fee for that will be $100. Marked up from 50. $100? Well, I guess it's cheap at that. $100? Or a chicken's frequency dinner cooked by the inimitable birdie. Yeah. It's dead frequency to include dumplings. By George, Horace. Hi, golly, gilly. You old son of a gun. You old horse, please.  You old stick in the mud. Be it ever so humble. Daddy's like all... By George, I'm glad we didn't sell it. Listen to that. Rain on the roof. And here I am, snug as a bug in the rug. Hey, old man. It is? Yes. Remind me, Roy, these days a man is lucky to have a leak over his head. You go to bed. Good night, everybody. It may even surprise some of you good cooks, and it's sure to surprise your family and guests to discover what marvelous new flavor interest you can add to foods with delicious craft-prepared mustard. First, get hefty tangy golden craft-salad mustard. It's something really quite special in a salad mustard. Creamy smooth, mild, yet so zestfully spiced, craft-salad mustard has just put it takes to pep up a golden sauce for hot-cooked vegetables, and it adds a delightful flavor tang to egg and cheese dishes. It puts new sparkle into relishes, appetizers, and sandwich spreads. And here's another great favorite, craft mustard with nippy horseradish added to sharpen your appetite for frankfritters and cold meat cuts and to zip up the flavor of sauces for fish. Buy both kinds for lively flavor variety. Tomorrow, ask your dealer for craft mustard, the nippy horseradish variety, and the tangy golden craft-salad mustard.


So it's our Chromebook 314. It comes either with an HD or full HD panel, touch or non-touch. And same as the previous one, it comes with the Gemina Lake CPU with the refresh version, either dual core or quad core. In terms of ports, you would have two USB Type-C ports. Can I see the ports there? Yeah. So Type-C? Type-C as well. Full USB? And microSD. Exactly. Over here is another Type-C? Yes. Another USB? So what kind of price is this? So this one would be on the full HD non-touch $399. So is it a lot for the education market or? No, this is more aimed for a retail market. The advantage Acer has is that we have a real retail lineup completely differentiated from our education lineup. So if those ones are coming with pure silver, we have it as well in due silver as an option. But those are really aimed for retail markets, as you see from the chassis. If you want to go on education, then that would be more ruggedized devices. Are you one of the most popular Chromebook manufacturers? Yeah, we are. We are number one. Number one in Chromebooks. So this is the, is it this one, the 315? So the 315 would be this one? No, this one there. So it's a 15 inch Chromebook. The difference from the 14 inch, of course, would be that you have the numeric keypad. So you again have, sorry, I need to remove that. And it's pretty. It's a little bit strong. OK, that's OK. It's for security, maybe. Yeah, I think so. Yeah. So there's again in terms of ports, you have two USB type C, USB type A, and a connector. Battery life would be 10 hours. And then, geminalic refresh. Something is strong about it. Good in that. Yeah, great. So this comes with the? This comes again with the geminalic refresh.


the pitch of a softball into the air, free to experience only gravity as it moves, the strike of the bat and the return of the ball to gravity's embrace, the leap of the basketball player into the air in anticipation of dunking the ball. This is a kind of poetry written in the air by gravity, the satisfaction of launching a football into the hands of gravity to have it delivered exactly to the place where it needed to be. All of these are examples of projectile motion, here written out in a kind of concocted perfection as a ball is launched from a moving cart and the ball returns to the cart because the horizontal component of its motion is not affected by the fact that it has been granted a vertical component of motion. Let us explore this kind of motion and all of the benefits and mathematical beauty that it reveals in nature. Let's begin to look more deeply at projectile motion and build a toolkit based on our previous explorations of motion in more than one dimension to describe this motion. First, let's lay out some of the key ideas that we're going to cover in this lecture. First of all, we will find that projectile motion is a special kind of motion that happens when motion in one dimension is unaffected by motion in any other dimension. The motion of airborne objects near the surface of the earth is an excellent example of projectile motion. We can describe that kind of motion using the ideas we have already developed. And in cases of projectile motion where there is constant acceleration along only one of the coordinate directions, the observed trajectory in space will be a parabola. These are the ideas that we will develop more fully in this lecture. Now there are, as you've seen, many common examples of projectile motion that we experience every day. Consider the cartoon over on the right, which show silhouetted figures in various games of sports involving catching, throwing, or deflecting a ball. A ball flying through the air, moving only under the force of gravity, or a person, after pushing off the ground in a jumping maneuver, now unable to contact any other surface to exert any other forces and thus subjected only to gravity. These are examples of projectile motion that are very common in everyday life. Let's consider a very specific situation which will illustrate all the features that we need to explore in projectile motion. Consider the situation that is depicted on the right hand side of this slide. We have some kind of projectile launching device. In this case it's a tube that can allow air to force a projectile out of one end of the tube. This is a blowgun or an air gun and it has been aimed so that the barrel points straight at this metal can which is hanging here from a stand. When the ball leaves the barrel of the gun, the can is simultaneously dropped from the stand. Both the can and the steel ball are now executing projectile motion. The question that we would like to explore is will the steel ball hit the can or will it miss the can? We can analyze the situations, for instance such as firing a steel ball with an initial velocity and dropping a can from rest simultaneously using the equations of motion that we have been playing with and developing so far and try to answer this question. But before we do that in a mathematical sense, let's take a look experimentally at what would be required to set up exactly the situation that I have just described. The essence of this demonstration are three pieces. One is a metal tube that is capable of holding a small ball bearing. This metal ball bearing is like a bullet that one can load into the barrel of the tube in the front here. The tube is connected at the back to a hose that goes to a supply of air that's provided in the classroom workbench environment. So I'm able to turn the handle on the air nozzle and get it to force air through the tube and push on the ball bearing eventually shoving it out of the end of the tube. So we can already see that there is a force that's present to accelerate and launch the ball and that is the force of the air pushing on the ball inside the tube. But once the ball exits the tube the air is really no longer acting on it. That force was only present to accelerate the ball inside the tube and it diminishes quite rapidly once the ball leaves the tube. So out here there is no air pressure pushing from one direction only on the ball and so we would expect that there would be no forces acting on the ball. But of course that's not true. There is a force that will act on the ball. It's acting on the ball constantly throughout this and it really begins to take over once the ball exits the tube and that is gravity. Gravity will tend to want to accelerate the ball down at a rate of about 9.8 meters per second squared. So once the ball exits the tube we can think of at least one force that's definitely acting all the time on this ball and that is gravity and it should be exerting a force in the downward direction yielding an acceleration of 9.8 meters per second squared. Now this ball is made of metal and as a result of that it has some inertia that prevents it from falling prey easily to small forces that would tend to accelerate it. Now as we know in the real world there's air and if we wave our hands around we can feel the resistance of air and in fact air resistance is a force that always tends to sap motion out of an object because it always resists the motion of an object in its direction of motion against that direction. So certainly air resistance will be acting on this ball but it turns out to be a relatively minor force compared to gravity and so we will neglect it in this particular experiment. Let's look at some of the other elements of this. Over here I have a small electromagnet. This is a device that only produces a magnetic field when an electric current is run through the device and if you look closely here you'll see that there is a white pair of wires that goes up and into the electromagnet. Now I can power it using this device over here which is a power supply. It's simply connected into the wall and it converts the voltage from the wall into something that's a bit more friendly for this electromagnet and so with the flick of the dial here and a gentle turn I can start running a current through this by exerting a voltage of about six volts on the wire. So now that I have a voltage and that's the potential for a current inside of this device there should be a magnetic field and I can verify this by switching off the power supply and showing you that I'm unable to get this metal can to stick to the electromagnet. On the other hand if I switch on the voltage and now I attempt to stick the can to the magnet, bingo! It easily remains there in place neither moving up nor down nor left nor right nor forward nor backward there are no net forces acting on this can and it is now in an equilibrium state it cannot move at all. So let's think about what we've done. We have a device that can accelerate a small metal projectile a small metal ball bearing that projectile conveniently is aimed when it leaves this barrel at the can. I took the effort to line up the barrel of this to point like a little rifle at the can. Now here's the last ingredient in this exercise and that is that the current that's powering that electromagnet is controlled by a little switch right here the current is on the metal can is clearly attached to the electromagnet but if I push the switch and I break the electric circuit I interrupt the flow of current to the electromagnet and what happens? Well an electromagnet is only magnetic when there's a current flowing through there. If I interrupt the electric current there will be no magnetic field. Without the counter balancing magnetic force from the electromagnet gravity is now free to act solely and only on this can pulling it closer to the center of the earth. So here's our experiment. Now that we've had a chance to see how such an experiment could be conducted let's begin to analyze this using the principles of motion and physics that we have developed so far. We should begin by describing the situation using a coordinate system with an x and a y axis and I have denoted the units of distance along each of those axes to be meters. We're going to use this to represent and describe the steel ball the can and the features of the motion. We can then place a mark in the coordinate system indicating the initial location of the steel ball the moment that it exits the blowgun and is no longer being acted upon by the compressed air inside the tube and we mark this location using a blue dot shown over here on the left in the graph. Note that I have placed the blue dot at one meter above the horizontal and along the horizontal axis it actually sits at zero meters. This point one indicates the leftmost extent of the x axis here. This location under the blue dot is actually zero meters in the coordinate system. Let us then also mark the initial location of the can just at the moment that it is released from the stand that it is dropped. And remember the exiting of the steel ball from the gun and the dropping of the can occur simultaneously and the moment in time that we will state where those events both occur is t zero t equals zero seconds that's our initial time for the motions to begin. We mark the location of the can with a red dot please note that I have placed the can at a height of three meters above the floor and two meters from where the steel ball exits the gun. And as we are going to see the motion of the steel ball will look like the black path the curve that I've now drawn here shown in the graph. Before we begin to actually explore the motion where this path emerges from in a mathematical sense let us explore key points of the motion accepting this curve as the correct mathematical description before we dive into the details I just mentioned. There are a few key and interesting points along the motion curve of the steel ball projectile. The blue dot already marks one of them it's the initial location of the steel ball in x and y we can denote that location x zero comma y zero it is here that the steel ball leaves the blowgun with an initial velocity and I have represented the arrow of that velocity vector and written out mathematically here it has a horizontal component it has a vertical component and one of the key features of this velocity is that the barrel of the gun and thus the steel ball when it exits the barrel are initially aimed at where the can begins its motion so where the can is hanging from the stand in the experiment. So note that the ball begins at zero comma one meters the can is at two comma three meters and so if we turn off gravity for a moment if we want the steel ball to hit the can its velocity vector has to point along a line that executes equal motion in the x direction as in the y direction in the same amount of time so after some amount of time we want the steel ball to be here if there's no gravity and thus the can can't fall it just sits where it's parked when we initially fire the ball and then in the next unit of time we want the steel ball to traverse this distance continuing along the diagonal between these grid points to strike the can the initial velocity of the ball must be aimed directly at the can even though gravity will act on both of these objects once they are released from either the stand in the case of the can or from the tube in the case of the steel ball so we will need a velocity vector in this depiction of the situation whose horizontal component is the same as its vertical component regardless of what the total magnitude of the velocity is we just based on this picture need the components to be equal now in a different situation where the coordinates of the can or not what I've shown here we might need a different kind of breakdown of the components of velocity and these are things that we can explore in homework and in class so this is one interesting point in the motion the initial location of the steel ball with its initial velocity v0 the apex of the motion that is the highest point along the motion curve in y that the steel ball manages to reach is another interesting key point in the motion since gravity accelerates the steel ball downward toward the surface of the earth there will come a point where the ball no longer moves up or down its vertical motion appears to pause for a moment and then after that point it reverses its vertical motion and begins to fall from rest at the top of the motion curve at this point the ball is only moving horizontally there are no forces acting along the horizontal direction the ball continues to move horizontally the whole time but its vertical motion is more complex because at first it's going against the direction of acceleration due to gravity but eventually gravity wins and it reverses the direction vertically of motion of the ball the horizontal component however is independent from the vertical component this will allow us to analyze this motion this purple arrow indicates the velocity of the ball which only has a horizontal component at the apex of the motion as you can see the motion has two halves before the apex and after the apex before the apex the combination of horizontal and vertical motion for the steel ball points up and to the right but after the apex the combination of horizontal and vertical motion points down and to the right and this combination is ultimately what produces this curve whose actual mathematical shape is a parabola let's begin to analyze the motion of the steel ball and consider what's happening but for now only in the horizontal direction the initial velocity in the horizontal direction is given by the x component of the velocity v0x and it points in the i hat direction in the positive x direction and this i have written here as a unit vector indicating just the direction of the horizontal component along x because there is no source of acceleration in the horizontal direction the steel ball has left the blowgun it's no longer being pushed on by the air inside the gun there is no force acting horizontally if we neglect air resistance and we are doing that in this problem as an aside for a small steel ball neglecting air resistance is a reasonable assumption it has a fairly aerodynamic shape it's also heavy and not so subject to the whims of air air resistance as it moves through the air so we can approximate that there is no source of acceleration or deceleration in the horizontal direction and so after it exits the blowgun and the blowgun can no longer act on the steel ball there is no force that can speed up or slow down the component of velocity in the x direction remember the equation of motion that the velocity at a later time is equal to the velocity at an earlier time plus the acceleration along that direction times the time but since the component of the acceleration in the x direction is zero we see that only in the horizontal direction the velocity remains constant throughout the entire motion and in fact at every point in the motion until an external force acts on the ball for instance the steel ball strikes the floor and the carpet and the floor change what the ball is doing the horizontal velocity will always be the same so we actually now have an equation of motion that gives the x coordinate at any time t after the steel ball is fired from the barrel of the blowgun and again to remind you it begins its journey at zero comma one meters and the can begins its journey although we're not talking about the can right now at two comma three meters and here is the equation of motion for the steel ball in the x direction this will tell you the x coordinate of the steel ball at any time t after being launched from x zero with a velocity v zero x so this isn't so bad it's nice not to have acceleration in one of the directions it makes the equation fairly simple now let's consider what's happening in the vertical direction the initial velocity in the vertical direction has a magnitude v zero y and it points originally in the positive y direction the steel ball is moving to the right and up initially it's being fired upward toward the can so its initial velocity is to the right and up and so it must be that the vertical component of its overall velocity vector points upward with some initial length v zero y at time zero and that's denoted by the blue arrow in the graph now gravity of course is acting in the vertical direction it exerts a constant downward acceleration of 9.8 meters per second squared in magnitude and thus the acceleration component in the y direction is negative g where g is 9.81 meters per second squared this will cause the vertical velocity to change with time again remember the equation of motion relating velocity acceleration and time the velocity at any time t is given by the initial velocity plus the acceleration times time but in the vertical direction the acceleration is negative g times time so we have this equation which tells us that the velocity will while first being positive eventually be overtaken by the acceleration due to gravity reversed and point downward more and more and more as gravity accelerates the ball downward toward the floor now after the apex and remember that the apex is where the vertical velocity is exactly zero meters per second in the vertical direction the steel ball is neither moving upward nor downward at the apex after that point acceleration reverses the direction of velocity and the velocity vector points down and its magnitude will grow larger and larger as gravity continues to act on the ball so we can write an equation of motion that gives the y coordinate at any time t and that's shown here the y coordinate at any time t will be its initial y coordinate plus its initial velocity in the y direction times time minus one half gt squared and the minus sign is because the acceleration is in the negative direction so a in the y direction is replaced by negative g so let us now write the two equations one for the horizontal location and one for the vertical location at any time t i've written those out here on the slide and i've now indicated here this expected trajectory for the motion and we'll see again where this arises from the moment although we already have a kind of qualitative understanding of why this motion should be curved as the horizontal component moves with constant velocity and no acceleration whereas the vertical component has a changing velocity due to the constant acceleration due to gravity now these are the equations that tell us position in space given velocity and acceleration and we can similarly write the components of the velocity itself at any time t and again we have a horizontal component that is constant with all time because no acceleration acts on the horizontal component or neglecting air resistance in the vertical direction however the velocity components magnitude does change with time and in fact at at some point given the acceleration it will reverse and point downward now using the equations on the previous slide we can return to the original question that motivated all of this mathematical and physical activity will the steel ball so fired strike the can to hit the can the steel ball must reach the same coordinates as the can at the same moment in time t now we know what the x coordinate of the can will be at any time t because the can is dropped from rest it's not moving to the left it's not moving to the right when it's dropped and so its x coordinate is the same throughout all of its motion x sub can and we'll use the subscript can to denote quantities for the can is the same as x zero can the initial position of the can along the x axis so we can ask a question at what time does the steel ball reach an x value of x sub can now again taking a look at this picture the x location of the can is two meters from where the steel ball started which is considered to be zero meters along the x axis so we can actually use algebra to answer the question we have an equation of motion for the x coordinate of the steel ball at any time t after it's launched we know that we want to find out at what time t x becomes x sub can which is two meters so we plug in x sub can set that equal to the initial position of the steel ball plus v zero x times t well we know all of these quantities except the time we know x can it's two meters we know x zero for the steel ball it's zero meters we know v zero x for the steel ball it's three meters per second which was written on a previous slide we're assuming that the steel ball is fired with an x initial velocity of three meters per second and a y component of velocity that's also three meters per second in the upward direction so v zero x is three meters per second and if we plug all these numbers in and rearrange and solve for time we find out that the time at which the steel ball reaches an x coordinate of two meters along the x axis which is where the can is is two thirds of a second or point six six six dot dot seconds after the steel ball is launched now using that time we can take the t value of two thirds of a second and we can plug it back into the equation for the y coordinate and find out what the y coordinate of the steel ball will be when it reaches that x coordinate and we find when we do this and I encourage you to try this yourself go back a slide get those equations of motion for x and y v zero x v zero y g and t we now know the time from the x equation we can substitute that into the y equation and solve for the y coordinate at t equals two thirds seconds when x equals x can two meters and when we do that we found out that the y coordinate is point eight two meters when t equals two thirds of a second so we know where the steel ball is supposed to be when it reaches the x coordinate of the can it will be at a height of point eight two meters at two thirds of a second after its initial launch so let's think about the can where will the can be at t equals two thirds of a second well the can is merely being dropped at the very same moment that the steel ball leaves the blowgun we call that time t zero and in our problem that's zero seconds at first as gravity begins to act with constant acceleration on the can its initial velocity is zero it has no velocity in the x direction it is no velocity in the y direction but as gravity continues to act with constant acceleration on the can and since gravity is the only force that acts on the can the can begins to accelerate straight down along the vertical axis toward the ground and that acceleration in the y direction is negative g there is no acceleration in the x direction so there will never be any velocity in the x direction now this is the same constant acceleration that the steel ball is experiencing the can's velocity continues to increase more and more but it only ever has a vertical component since no forces act in the horizontal direction and there was no initial velocity imparted by any force to the can when it was released in that direction the position and velocity of the can are then given by these equations of motion the horizontal position of the can is the same at any time t it's always x zero can which is two meters the y position of the can however is a bit more complicated it is the initial position in y of the can which is three meters above the ground plus the initial velocity of the can times t well the initial velocity is zero it starts from rest so in fact this term goes away because zero times t is zero and then we have to add to that one half a t squared well the acceleration is negative g so we have negative one half g t squared and by throwing out this middle term because it's zero we can simplify this equation to y zero can minus one half g t squared and the velocity of the can is given only by a y term there is no x term because it has no velocity in the x direction to begin with there are no accelerating forces in the x direction so there is never any x component of the velocity there's only a y component of the velocity and it's given by v zero y can minus g t because the can is accelerated down from rest and in fact since v zero y can is zero this is just negative g t in the j hat direction so will the steel ball hit the can in other words after t equals two thirds of a second so two thirds of a second after the can is dropped where will the can be in height well we know where it will be in the horizontal direction it will be exactly where it started it will be at two meters what will its y coordinate be well it started at three meters and if we plug in two thirds of a second and solve given its initial height the acceleration and the time which is two thirds of a second we find that the y coordinate the height of the can above the ground after two thirds of a second is 0.82 meters and if this looks familiar there's a reason why the steel balls coordinates at t equals two thirds of a second are x equals two meters and y equals 0.82 meters and the can's coordinates at the same time two thirds of a second are also two meters and 0.82 meters in the x and y directions respectively so we conclude that the steel ball hits the can but how can this be if we think about the initial situations of the steel ball being fired upward toward the can and the can being dropped from rest it seems amazing that in fact the ball hits the can but the reason for this is because the steel ball was initially aimed at where the can started and after they both enter projectile motion they both experience the same constant acceleration and so projectile motion is extremely powerful it is motivated simply by the fact that we have independent motion in these two directions x and y we could easily extend this to a third direction z if we wanted to and in the special case of objects in projectile motion near the surface of the earth we have this constant downward acceleration from gravity and so we find that we have these situations where we can not only describe very well the motion using the mathematics we've already developed but for this specific situation where a projectiles aimed at a target and the target and the projectile both enter projectile motion in the gravitational field of the earth with no other forces acting on them at the same time that in fact they meet at some point in space later it's really remarkable now there are many examples of projectile motion in the universe a basketball free throw where you carefully aim and then throw a basketball up above a hoop in the hopes of getting it to come down and enter the hoop and make a basket throwing any ball in fact into the air in such a way the the ball will observe projectile motion once it leaves your hand because it will have no forces again neglecting air resistance it will have no forces acting in a direction perpendicular to gravity so along the horizontal and it will feel only the constant acceleration due to gravity in the vertical direction another example another example is jumping while moving if you are running and then jump into the air you now no longer have any surfaces to touch you can't change your motion and you will be in projectile motion in the gravitational field of the earth so think about track and field long jumping things like that jumping over hurdles those kinds of events involve ideally projectile motion where the body makes no contact with another surface until the motion is completed archery riflery any activity where an object is launched into the air and cannot provide its own acceleration rockets don't count rockets carry fuel the fuel is burned this exerts a force on the rocket and so this can affect its motion but any projectile that has no way of exerting a force say by using chemical energy or some other form of energy to convert that into a into motion these will experience projectile motion so think about just how useful it can be to know that when you meet the conditions required for projectile motion it is extremely predictable that motion can be extremely well described now i'm not going to show you the punchline to the steel ball and can demonstration in here we're going to do that in class but you will see that if you set the situation up correctly as i said aiming the steel ball at the can having them release as shown in the experiment earlier at the same time that in fact the steel ball will hit the can now the caveat on all of this is of course there's this thing called the real world and in the real world things are more complex than what i've laid out here you had better account for things for instance like air resistance and also when you fire a projectile off the surface of the earth and it's no longer making contact with the surface of the earth and because we live on a planet that's rotating we go through one day night cycle every 24 hours that motion of the earth the ground moving and the air resistance this adds real complexity to the problem of course in real situations in artillery calculations in thinking about designing something like a baseball stadium at various altitudes or where air atmospheric conditions are slightly different than they would be say at sea level or in another park you need to take these things into account when you're thinking about how many home runs might get hit where the artillery shell might land and so forth but over short distances with appropriately aerodynamic projectiles at low altitudes with weak air resistance all of this works remarkably well and these conditions while they sound very limiting and and yes they do take you away from the most realistic calculations they are nonetheless good enough assumptions that you can make a lot of progress with this subject let's talk about the path of projectile motion i said earlier that the path is a parabola and in fact i'm going to reinforce that and show you that now so again the path of a projectile in this kind of motion with a constant acceleration in one direction no acceleration in the other it has this common shape the parabola now the details of the parabola its height its width these things can vary based on the initial conditions of the situation how fast you fire the projectile how strongly acceleration is and so forth but in general this shape will be preserved assuming you can neglect things like air resistance and so forth the equation for a parabola whose apex or as is shown over here on the right whose minimum point is located at some point in space and i've denoted that x apex and y apex and with a focus a distance f from the apex so the apex would be here and the the focus might be somewhere up here again review the definitions of parabolas that you might have learned in in high school for instance to refresh your memory of all of this stuff the equation for a parabola with these conditions is as follows the y coordinate of the parabola is given by one over four times the focus distance times the quantity x minus x apex all squared plus y apex so this allows you to define a parabola that's offset from the origin and raised above the origin for instance with because it has this apex location that isn't zero comma zero but if we set the apex to be zero comma zero we recover a much simpler and perhaps more familiar equation for the parabola that you would have seen in high school y equals a constant times x squared and that constant is one over four times the focus this is another way of representing a parabola this equation over here is perfectly valid it's a slightly more general form of this equation with the focus and and other pieces like the displacement from the origin and the x-axis and the height above the x-axis that the parabola starts etc that's that's shown over here on the right in this equation these are all equations for parabolas of various kinds generalized or otherwise what about motion well if we take the equations for x and y those coordinates for the steel ball at any time t after it's fired and if we rearrange them so that we can solve for t from one of them and plug that equation for time into the second equation we then find this eliminating time from these equations we only have y x x not y not v zero x v zero y and g and what do we see well we have the the height of the parabola above its initial starting point or below its apex is given by a term that is linear in x multiplied by the the y component of velocity and that looks very similar to the b term over here in the parabola equation and another term that is quadratic in x and that looks very similar to the a term over here in the equation so we see in fact that the relationship between the y coordinate of the steel ball and the x coordinate of the steel ball at any time t after it's launched is given by a parabolic equation so this is just the equation for a parabola in a slightly expanded form over the generic equation specific to our projectile motion situation so again neglecting things like air resistance the rotation of the earth under the projectile etc the motion of a projectile under these conditions is completely predictable before we close out the lecture let's play around a little bit with projectile motion in a computer based simulation a sort of game like environment i have here a cannon that's capable of firing various projectiles and you can see that it's initially set to fire at an angle of 80 degrees above the horizontal there's a target that i'm supposed to hit by shooting projectiles out of the cannon i'm going to move the target over to about 20 meters from where the cannon is located so right about here so i can start by firing a projectile from the cannon i've selected pumpkins with a mass of five kilograms a diameter of just a little over a third of a meter i'm going to fire them from the cannon and watch as they execute projectile motion and see if i can hit the target so let's fire a pumpkin here goes a pumpkin up into the air and we see that it leaves a beautiful parabolic trajectory as simulated by the computer in the air the pumpkin smashes here on the ground we are far from our target we clearly missed the target but i can adjust the firing angle of this let me try firing a little lower maybe 56 degrees and fire well that was terrible this clearly overshot the target but you can see again we have this parabolic arc albeit wider the pumpkin flies further along the horizontal direction although it doesn't go as high in the vertical direction because of the firing angle of the pumpkin and the effects of gravity during the motion it's clear i need to split the difference and do something in between here so let's try something more like 65 degrees and fire the pumpkin one more time ah so close but again you can see that i've increased the firing angle relative to the ground of the pumpkin and so the pumpkin goes a little bit higher but not as far as it did before and you can begin to see these trade-offs in the motion of the pumpkin in projectile motion if i aim the pumpkin higher into the air when i fire it indeed it will go high up into the air but it won't go as far horizontally if i aim too low it'll go far horizontally but it won't go as high as it otherwise would and so hitting the target is a careful balancing act of firing up into the air and firing too low let's try one more firing angle let's try 68 degrees and see what happens so now i fire so close let's try one more time we'll try 70 degrees you can try this game on your own these simulators are available aha i got into the outer ring of the target not too bad these simulations are available from a group called vet vet.colorado.edu i'll make sure to put a link in the slides are on the course website and we can probably improve our game a little bit more by maybe switching this to 72 degrees and firing let's see if we can get dead center on the target not too bad clearly the magic number here is going to be 71 and if i fire one more time indeed boom i'm in the sweet spot of the target so this will give you a little little opportunity to play around with projectile motion without hurting anybody or yourself and you can try various projectiles you can also do things like turning on air resistance so as a last test of this let's try air resistance we're going to add resistance due to air now so the pumpkin is going to feel a drag force as it moves through the air i'm going to fire at the same angle 71 degrees let's watch what happens ooh indeed we see that adding in a bit more realistic aspect that is resistance to motion from air greatly alters the trajectory of the pumpkin it still looks parabolic but it's not a perfect parabola anymore and in fact we fall short of the target because our motion is being resisted by the air through which the pumpkin is moving so feel free to play around with this this is an excellent way to get some intuition and a game-like environment for physics and it will give you a more hands-on feel for projectile motion when you can neglect air resistance and think about trying to hit a target by balancing how much horizontal velocity and how much vertical velocity you present in the presence of gravity let's review the key ideas that we have been exposed to in this lecture on projectile motion we've seen that projectile motion is a special kind of motion that happens when motion in one dimension is unaffected by motion in any other dimension the motion of airborne objects near the surface of the earth is a really excellent example of projectile motion think back to the beginning of the video with the basketball player jumping into the air to dunk the ball or the pitch of a softball toward the batter or the throwing of a football to aim at some distant target make that shot as best you can these are all examples of projectile motion gravity gives us an outstanding laboratory near the surface of the earth to explore this kind of motion and we have seen that we can describe such motion using ideas that we have already developed regarding position and time and velocity and constant acceleration in cases of projectile motion where there is a constant acceleration along only one of the coordinate directions we have seen that the observed trajectory of motion in space will be a parabola we have seen how to make approximations for instance the removal of air resistance from consideration the removal of the rotation of the earth underneath a projectile that's been launched from the surface of the earth and we've seen that for certain limiting cases and assumptions that's it's not a bad thing to do we do need to be cautious in the real world these forces can play major roles especially over large distances or with projectiles that are not very aerodynamic projectile motion is seen to be a beautiful kind of motion a predictable kind of motion one that we can not only describe with the mathematical tools that we've developed so far but whose outcomes we can predict quite reliably as long as we have made a valid set of assumptions


Well, hey, hi everybody. How are you doing? Russell Moore. Welcome to Dedicated to Financial Literacy. It's good to see everyone. Good morning. Welcome to my bedroom. Hey, hey, look, you know, I'm real and I'm raw. So I'm just welcome, welcome. Packing and moving, getting ready for, yeah, our new home. Yeah, we bought a brand new construction. It's still being built. They're finishing up the fence. And so we're excited. We're excited. But our current house, it looks crazy. It's just wild here. So I'm just finding anywhere to just tape and video for my channel. So anyway, I'm just going to make this pretty quick today. I sent one of my favorite YouTubers, meet Kevin. By the way, I want to plug his channel. Check him out. He's really, really good. But he's been saying, along with Kathy Wood, how inflation, a current inflation was going to be transitory. And that deflation was going to be on the rise, so to speak. And I sent him before the jobs report came out. We have, by the way, 194,000 jobs added. We missed expectations by so much. I mean, it was really bad. I know that Biden is trying to make it seem like it wasn't a big deal. I'm sorry. They know that is not where they wanted the numbers to be. They have some administration. But anyway, I left Kevin, meet Kevin, a comment, and I said, listen, please stop telling people that inflation is transitory. It's not. It's not going to be transitory. In fact, inflation is going to go up. It may drop for a moment, but it's going to go back. It's going to go up. Inflation is going to be here for a while, you guys. We're going to be in this inflation bubble for a while. And the reason why I'm saying this, and one of the things I wanted to talk about today is, number one, I want to say, I'm not coming against data. I believe that we have to read data. We have to do our research. Okay, so I am not coming against data. But let's, let's, hey, you guys, let's not fool ourselves to think that the government would not skew numbers, that they won't exaggerate numbers. That's just come on. There's no way that the Biden administration, especially with his polls, his numbers right now are so low. I'm sorry. He is not going to allow anything to get out that's going to make things worse. So they're going to, they're going to pump up the numbers. If they, if it's going to be to their favor, and they're going to drop numbers, if it's going to be to their favor, you guys get that. So for example, unemployment, what did they say probably around 4.9? It's probably more about 5.9. And so I'm just saying that don't just go buy data. Don't just go buy the numbers. Okay. Read them. Read them as a gauge. But let me tell you something. This is why I think a lot of people are getting it wrong. As far as this inflation thing is because they're only going by numbers and data and statistics. You know what, here's why I told meet Kevin. This is why I told him that, and I'm telling this to Kathy Wood as well. She's a great mind. And I'm saying a lot of things she says is right on point. But I just disagree with, I really, I really agree with Peter shift on this. As far as inflation is concerned, as far as the market crashing to the degree that he's saying, I believe eventually that will happen. But for different reasons on why it's going to happen. But here's the thing that I'm saying. Use common sense as well, you guys, when it comes to inflation, use common sense, practical wisdom here. And here's what I told Kevin afterwards after those job numbers came out. I said, look, and then the inflation numbers. And so he and he was looking like shocked. And I'm like, listen, here's what we've done. We've replaced numbers and social media and websites for people for just talking to people. If you want to find out where inflation is going, just start talking to people. When you go to the restaurant, talk to that restaurant owner. Talk to the gas station attendant. Talk to the supermarket clerk. Talk to your friends. Talk to your family. That's how you can find out where inflation is going. Talk to your auto your auto mechanic. Talk to the Jiffy Lou guy. Talk to your UPS man. No, really, just start striking up conversations. Getting to know people. And here's what and this is why I'm saying we have replaced just talking to people and having social outlet. And I get it with the pandemic. I get it. We got to have social distancing. I get it. I get that. I'm not saying break protocols. All I'm saying is we got to get back to just talking to people. If you want to find out about inflation, talk to your aunt. Talk to your uncle. Talk to your retired grandparents. And they'll tell you where they'll tell you they have the answer to inflation, whether it's going to be transitory or not. That's all I did. I just started talking to people. And guess what? The restaurant owner are paying more for buns. They're paying more for cups. Silverware. They're paying more for their meat. They're paying more for their fruit. They're produce. Well, let's talk to the gas station attendant under gas station owner. They're paying more for that. They're gas. We're paying more for gas. Talk to your grandparents that are on fixed income. Are they paying more for when they go to the store? They're getting the same. They're a good gauge. They're getting that same amount every month, that fixed income. Now, is their money getting more or less? Are their bags at the end of the week or at the end of the month whenever they shop? Are the bags more full or less full? Are they getting more for the money that they're putting out? And the answer is no. Haven't you noticed something?  I bought toothpaste, a couple of frozen dinners, some ketchup, a pint of ice cream, a two liter soda, some cereal and you're telling me it's $120 when about six months ago, I got the same, I bought the same thing and I paid 80. Inflation is here, gang. Inflation is here. Here's what you need to do. Here's what I did.   Lumber's back up again. I don't know if you guys knew that. That's gonna affect the housing market. That means the developers are gonna be paying more. Lumber's back up. Copper. It's here, gang. Gold. Gold. That's what we wanna do. This is my disclaimer.  I'm just saying think about it as a hedge against inflation. Gold and silver, actually. I would throw Bitcoin in there, but Bitcoin usually goes where the market goes. I see Bitcoin, Bitcoin in the future, but I think it's gonna still be volatile up and down, up and down, up and down and all around. Start preparing. If you can, property. If you can, get some property. If you can, invest in REITs. Another thing is billboards. Nobody ever thinks about buying billboards or buying the easement on the land and renting out billboards. Yeah, big billboards. Boat slips. Boating where you own, where people keep their boats. Did you know that you can purchase that and rent it out? You gotta start thinking outside the box, you guys. There's so many other ways to invest your money where you can get a return and keep cash flow coming in. But remember, the dollar is going to be, it's gonna go down. It's devaluing. It's gonna get lower and lower. The worth, the dollar's worth is going to diminish. Anyway, prepare for inflation. It's not, it's not done. It's not over. Have a wonderful, wonderful day. And I'm out of here.


Hi everyone, Joe for jazby'scasebreaks.com. Happy Wednesday. Coming at you with a really nice one here. 21-22, Panini Immaculate Basketball, five box full case, pick your team number five. A lot of awesome stuff here. Very big thanks to everybody here for getting in on it. Thanks to the people who bought their team straight up. A lot of people did. Thank you.  You can see that we pulled some teams for that random number block randomizer. We did that, the randomizing in a separate video, but there are the results. So serial number break just for those teams right there. Keep this to my side over here. All right, and there is full case of Immaculate Hoops. Got another one in the store and we have a fun one box break. All random number block style, one box break in the store too. Check it out. I think Jason Jaspy might even have some personal boxes left for this, for a mac of the basketball as well. If you want to get greedy, get the entire box to yourself. You sure can. That's at Jaspy's Rakes on Instagram live only. Live right now. And got another full case in the store. Jaspy's casebreaks.com. If you want to get your team straight up, please do so. Especially if you miss out this time. Don't miss out next time. Use this blank card right here to slow play some of the hits here. Moses Moody leads us off. 16 out of 99.  If you're new to the number block format, we go by that digit right there. So that goes to Daniel and the number six. That means he has six out of whatever, 16 out of whatever, 26, 36, 46, 56, 76, 196, et cetera, et cetera. There's Alperin Sengun, 38 out of 99. Goes to Rockets eight. It's for Brian S. Got Davion Mitchell, 22 out of 25. Nice three color rookie patch. Kings, Kevin with the Kings. Got him straight up, nice. Good looking patch. Modern Marks and Nikhil Alexander Walker, 17 out of 49. Cousin of Shay Gilgis Alexander. Kihoon with the Jazz. We got a one of one, Dehunta Murray. Immaculate Inc. San Antonio Spurs, that's gonna be for Justin Weber. There you go, Justin. Nice, Justin. All aboard the Big Hit Express. Woo-hoo. Are we gonna get any open anymore at Baseball Immaculate? Yeah, whenever we get some back in the shop, we'll definitely post it and we'll break it. 39 out of 49. Nice two color patch in auto. Colin Sexton. Cavs are a number block team. That goes to Cleveland nine. That'll be for Daniel Lois Deelo. Cleveland, this is for you. All right, nice start. Next box. Let's do the one box break of this too. The one box random number block break. It's a really good deal actually. And a lot of fun too. Just going by serial number. That's available right now, jaspeaskrakes.com. Always gotta make sure like a card or something isn't stuck in there. It's happened. There's Donovan Mitchell, 48. Can't read, 46 out of 49. That's still jazz edition for Kihoon. There you go, Tyrese Maxi. 22 out of 99. Piece of his jersey for the Sixers. Robert from Philadelphia. LeBron James, seven out of 99.  Going to the Lakers number block. So Lakers seven. Deelo with the spot that he won in the filler. Aaron Wiggins, 90 out of 99.  RJ Hampton, eight out of 10. Two color patch. On-card autograph, Orlando. Orlando's a number block team. So that goes to Orlando, eight. That's for Brian S. Last spot mojo as well. Brian, 70% of the time. It's 100% of the time. The one on the bottom here is another one for Orlando. Nice Jalen Suggs, RPA. Great patch. Nice on-card autograph, 90 out of 99. So that goes to the Orlando number block. That goes to Orlando, zero. And that is for Deelo. There you go, Daniel. Nice. Yeah, Justin was talking about that one-of-one a little bit earlier and got himself a one-of-one. See, that's how you'll do some reason. We talked about how to research one-of-one, see how to price them out. There's different strategies. All right, another box. Good luck. This one's a shallower box. Maybe there's, yeah, there is a redemption on the bottom. So that could be for number zero, could be for someone on this list. Good luck. Drew Holiday, holiday three out of 25. Milwaukee Bucks three, Sean Mattick. 86 out of 99. Dorian Finney-Smith, Dallas. That will be for Oren. Dallas straight up. We got 71 out of 75. James Harden, dual relic. Nets, Nicholas, the Nets. Like the nice 75th anniversary sort of design there. There's a little dent in that number right there. See how much that happened during some point during the manufacturing, but nice dual relic. We got Kendrick Parkins, big part. O.K.C. Sean Mattick, 60 out of 99. Harold at Signature's Autograph. And we've got Wendell Carter Jr., three color patch in autograph, 11 out of 25.  They could have had a nice break here. So Wendell Carter Jr., 11 out of 25, goes to Orlando I. That'll be for Brian Frank. Nice, Brian. And the redemption. Good luck, everybody. Wow, triple autographs. That's Jaylin Green. Jaylin Suggs, Josh Giddy. Wow. All right, Jaylin Green is a rocket. So that's for zero. Jaylin Suggs is a magic. That's for number, that's a number block team. That goes to zero.  So it's a randomizer between those three teams. All right, we'll do that at the end. Good luck. All right, next box. Got more immaculate in the store, ladies and gentlemen. All right, good luck, folks. Who do you think's holding up that auto? Who's not signing that card right there? It's Jaylin Suggs, 23 out of 99. Orlando III, Sean Mattick. Cameron Thomas, 11 out of 99. Nicholas and the Nets. The Nets straight up. Ooh, nice patch here. One out of seven, Dorian Finney-Smith for the Mavs. Oren got the Mavs straight up. It's a cool jersey number patch. There's Jared Butler, two color, on-car, 29 out of 99, Kihun with the Jazz. Dilo's not sure.  John Collins, two out of 10 for the ATL. Walter with the Hawks. And then we've got a Pelican. We've got Jose Alvarado, 33 out of 50, RPA for the Pels.  All right, final box coming up. Hang on, Rocket, I'm in the middle of something right now. Only we can talk NASCAR after this break. All right, final box, immaculate basketball. Pick your team five. Pick your team six in the store right now, jaskyscasebreaks.com, if you wanna run this back. We also have fun little one box breaks as well, random number blocks. All right, another shallow box, might mean another redemption. Maybe in the middle, looks like a redemption in the middle there. Got Luka Dončić, 15 out of 25. That's for Oren and Dallas. Got Jalen Johnson, 34 out of 99 for the Hawks. That's gonna go to Walter in Atlanta. Grab the redemption here. Let's flip that upside down. 17 out of 25, Jimmy Butler for the Heat. Miami's a number block team. Miami seven is gonna be for Daniel. So the redemption was in the middle. The redemption is gonna be an RPA, rookie patch autographs. That's right, Walter Lutz. There's a Walter Summers in this break. Two Walters. Need more Walter, we don't have a lot of Walters. G, Greg, we got Greg Brown III is your RPA. Greg Brown III, is he a Pelican? No, different P, Portland is a trailblazer. Blazing trails. Robert Runkle got Portland straight up, nice. All right, couple more and then that's that happy time, sad time randomizer. We got Kobe White, 39 out of 49, three color patch and autograph. Chicago is a number block team. 29 out of 49. Chicago nine, that's gonna be Daniel Lewis. Last one is gonna be signature moves. The mailman, Carl Malone, 19 out of 25. That is for Kihoon, picked up the jazz straight up. Nice. All right, nice break, that was Immaculate Five. Now we gotta make one person happy and another person real sad. It's just part of it ladies and gentlemen, it's part of it. All right, we got Jalen Green, Houston. We got Jalen Suggs, Orlando and Josh Giddy, OKC. No other randomized to do right, yeah. All right, well, Sean or Daniel, good luck. Let's roll it and randomize it. Six and a two, eight times team on top after eight gets the card, gets the triple. One, two, three, four, five, six, seven and eighth and final time goes to Houston. Houston is a random number block team. So my apologies to Sean Maddock and OKC, but congrats to Houston is a number block team that goes, any and all redemptions go to zero and that'll be for Daniel Day-Lewis. There you go Dilo, triple auto going your way. If you end up redeeming this, snap a picture of it, tag us on Twitter at Jasper's Breaks. We'd love to see it, we'll hit you with a retweet. All right, thanks everybody. I'm Joe for Jasper's Case Breaks.com and I'll see you next time for the next break, bye bye.


Hi everybody, Joe for Jaspy's casebreaks.com coming at you with 2017 Donner's Optic Football Fat Pack Random Team Break number 35. Just one pack. At the end of the break, we'll re-randomize your names and the top seven names will get mixer spots. The eighth name will get $75 a break credit. So we'll take your name once your names are assigned to a team right here. We'll take your names again new dice roll separate list. There you go. Top seven will get mixer spots and that eighth spot, the first consolation, first sad times person will get $75 a break credit, which is not too bad. Not too shabby at all. So let's do the break itself first, the pack break itself first. So let's roll it, randomize it two into two, four times for each list. One, two, after four times, Brandon down to John and then four times for the teams and fourth and final time. So we've got the Jaguars after the Browns after a hard four. Alright, so here's the first kind of almost half of the list right there. There's the second half of the list right there. A couple other teams. 2017, so is this Mahomes? Possibilities? It was 2017, right? There you go. So Ross. I mean it's just this little guy right here, but possible. Even a rookie card. Alright, so let's print, rip. No trade windows in these little short breaks here. There it is. So good luck to everybody here of course. Here's the final print out. Alright, so nothing earth shattering at all there, but let's go back. Let's grab everybody's names. Get everybody's names in here and let's see who's going to win those mixer spots and that break credit. So everybody's names there again. Let's roll it. Let's randomize it. Six out of three, nine times. One, two, ninth and final time. So after nine, big thanks to this crew right here. Appreciate you getting in. And congrats to Stephen, $75 break credit going your way. Brandon, Mike, Brandon, Zach, Tice, Robert and Stephen will also get spots in the mixer. So congrats to this group right here. Thanks very much for getting in and giving it a shot. Folks, there's one more of these packs that we have to do to not only give away the final mixer spots, but give away some more break credit. If you're watching live, there's a six o'clock Pacific, nine o'clock Eastern deadline on break credit being given away. Otherwise, it just goes back to just the normal seven spots being given away. But one more pack sells out that mixer too, and we can make that happen as well. Check it out on jaspyscasebreaks.com. I'm Joe and I'll break more of you next time. Bye-bye.


So here we have a new Canon camcorder so hi so who are you I'm Paul Atkinson I'm the product specialist for Canada Europe for the pro video camcorder range of the Cinemareos range And this is a very anticipated very exciting camcorder for their pros. Yep This is the long-awaited replacement for the XF 305. This is the XF 705 Yeah, a bit of a world-first for us. This is the first pro level camera It actually uses H.265 HEVC compressions. It's recording format or main recording format So that saves bit rate. Yeah, absolutely. There's lots of advantages to this We're still recording 160 makes per second Onto SD card at 4 to 2 10 bit 4 to 2 10 bits. Yeah 4k 60 and 50 right? Yeah, and you can switch Yes, you can yeah, you can switch this one Go to a service center. So 4 to 2 10 bit internally to dual SD UHS 2 cards. Yes, and then How's the sensor is it one inch? It's a one inch sensor We can do some other things with this as well. We can also record direct HDR and we can do both flavors We can do PQ and HLG. We can also by fitting an external recorder We can record simultaneous HDR and SDR streams Even more clever we can also add on to that the ability to adjust the exposure to one or the other So if you expose correctly for HDR the camera will automatically Reset for the SDR Plus or minus up to 7.5 decibels, but it doesn't let you do both at 4k 60, right? Yes, it will be both really you can do HDR and SDR two streams at 4k 60 at the same time It's one into the SDR will always be external the HDR internal. Oh, wow cool, but We need to HLG format is kind of Compatible with both with SDR displays and HDR, right? That's correct in one file Yeah, that's the beauty of the HLG system So for broadcast in particular where you can't guarantee that people are going to have a full PQ capable monitor The HLG is the one to use. We can also on the back. We've put a 12 G SDI output Which means we only need one cable And again, that's 42 10 bit in HEVC and we can do a full HD in the same as well So there's all the ports you want down here. Yep So we have said we have 12 G SDI for a single connection to external use You can take the same amount of HDMI as well also IP streaming at 16 makes per second So we can open up all these little caps for you. You'll see you have a gigabit ethernet right there Yep, so that'll do 16 makes per second live IP streaming in 4k HDR H265 4 2 2 10 bit streaming that's pretty awesome. Yeah, I mean it's 60 only or 160 16 makes per second 60 makes 60 megabit 1 6 Ah 1 6 so it's not 4k 60 and all that stuff. It's still 4k So it's still 60p, but the data transfer rate is 16 makes per second 16. Yeah, so it's very compressed, right? Yes, but it's kind of like what they do a Netflix Netflix is that kind of bit rate It's H265 is 15 megabit. So that means it has a very strong compression right there Maybe it does but it's also if you think of this being used in documentary or news gathering It's a deficient way to get stuff back to your studio to use room You could also stream it over LTE and stuff like that If you use one of those external things again, that's the beauty of the connectivity of the camera and lots of XLR Yeah, we've got two XLRs one at the front and one at the back and the reason behind this is If you put a radio mic here, you've got four-channel audio You've got a radio mic here that connects in that helps with the balance of the camera And then a wired one or another wireless at the front So you could you could also perhaps The interviewer can have a label correct and then to have the other one as a shotgun Yeah, absolutely, and that's kind of like the perfect combination But it is a kind of big right is that the 305 was smaller or this is slightly smaller than the 305 Slightly lighter We've got the multi-position screen as well So we can have it this way up Let's turn it on for you and get an idea of what the screen looks like I can have this through on this side as well If I was self shooting I can turn it that way It looks like there's two displays, but it's not. No, it's not. It's just the one the other feature that we've put on this is We've incorporated dual-pixel CMOS autofocus And as a benefit of that for those that want to manually focus you've got the focus assist system on there as well And that uses the dual pixel AF technology to give you manual focus confirmation So you can use the dual pixel just to make sure your manual is well made So if you look at zebra kind of stuff if you look on the screen here You see this little GUI here and that tells me whether I need to move the lens the focus left or right And as soon as everything goes green, I'm in focus The importance of that is because you are filming 4k. It's absolutely imperative that your focus is exactly accurate There is no room for error in 4k filming Yeah, and it's the fastest dual pixel implementation in Canon's history. I mean you have different kinds of dual pixels I mean this this is comparable to the C700 C200 speed and Is it like tap to focus also Yeah, absolutely when you tap to focus do you have to tap something to tap something else? You can just tap the GH10 Seems that the UI has something where you have to exit and come back to the next now All I need to do is need to make sure that I'm in autofocus I can press that one as well, but I don't mean one for you that I can go towards the focus I now have my cursor here I can make that a small area or large area I don't want to choose my point of focus if I go on to the stand I can say, okay, I want to focus here a touch It focuses touch And it's instant And What's the price? The price on launch is going to be around about 7,000 euros plus tax Which again for this kind of level of camcorder, I think it's fairly competitive There's been a massive amount of interest from right across different speeds of the industry and it's already Buried in mind. We only announced it two weeks ago But some people in the professional areas think that the H265 is a little bit harder to do post-processing on right? By the time this goes on sale. We are working with partners creating editing systems We know that Avid will be available as a plug-in on launch. I'm unconfident the other providers of NLE will be following very closely behind and There's 160 but can you even tune it down? You said that the live stream was 16 only Yeah I mean you have options to go lower if you want to do 50 or when you it's all variable bit rate But when you are recording you if you record to full HD H264 Then you can bring it down to about 45 makes per second Nice, so that's very exciting to see some H265 happening So it starts here, but perhaps it might go in the more consumer-oriented cameras later I think I think it would be a Good thing to do because it gives you the ability to record a 4k file But to relatively low cost and very easily available recorded media And that's the big attraction that we can go we can buy an SD card pretty much anywhere these days Even the newer specification ones There's no need to use the v90 right? It's just a Little bit more for what SD card would be fine because it's only in a hundred and sixty megabit Yeah, I mean Be fine for it. Yeah, and it's got all the manual controls people want. Yep So you have three ring control at the front for focus zoom and iris The zoom rocker on the side here is the same as we find in our broadcast lenses So this is much stronger much more durable All the controls are logically placed again controls to the left of the camera connections to the right and it's little things it's little things like being able to find out What your audio status is and instead of having to go into a status menu and go find audio You just press the button you discovered there and your audio status is projected straight onto the screen And it's got a long battery day for yep around about 80 minutes of continuous recording is the best information I have at the moment and but until we start getting this out and using it and Get those fingers square away. There's no chance that this nice big beautiful screen is a 4k. No No, it's a that would be cool. Yeah, it would be cool But it's a very bright screen allows you to look at something if you record in HDR It allows you to get a good representation all that footage is going to look like If you didn't want to use the direct HDR recording You've also got the ability and this is a first on a non-cinema camera We've put Canon log 3 onto this as well So you can record in Canon log 3 and then to follow traditional workflow instead of going through the Direct system So I'm excited about the h265 I think is very cool But there there's no option for h264 for people who want that there is an h264 option That's xfavc and that will be the 4208 bit 428 so if you want 422 10 bit you go hivc hivc and it's 160 but did you say there was a lower in xfavc in 4208 bit? Yes But if you want to do the you can't tune the bit rate is fixed at the 150 So that's I think you can come down to 110 actually so what we'll do is we can go out of this one We go into our menu You can see all the menus is all very Logically based This is the cp so this is the preset And you can see the options we have in here So we have wine DR As we have with the other cameras PQ and HLG You can choose rec 709 or 20 20 straight in so these are all three sets You have the 110 option which still gonna be focused 60 nice and if you get if you can go back And there you have a Xf hivc and that's the one way you can choose the h2 6 4 there as well, right? Still on 50 But then then it would be external through the hdmi if you do the two streams or 12 gs di or the sdi Cool, so available Say I'll start is anticipated for early December and What are the customers a broadcast Broadcast independent filmmakers Anybody that's using Xf 305 and there are a lot of those people out there. It's been a really good workhorse camera It's been around a long time the 300 is already Discontinued the 305 will be discontinued fairly soon So, yeah, that was just a 1080p Yeah, that was four two two eight bit and pick two 1080p. Yep, and so there's a big jump big jump And I think so have manageable size for this kind of product I think hEBC is actually the logical thing to do Everybody's been waiting a long time for this. I really do believe that we've got it very right with this camera The the 405 was kind of like a different thing a little bit. It was smaller different markets. It's different. It's for It's perfectly fine for news gathering as a small news gathering camera. It meets The the required criteria 4208 bit, which is perfectly acceptable But this one gives customers About 4 to 2 10 bit option All right, so there it is hEBC focus 60 10 bit 422 hLg all this stuff to dual sd right here very exciting that That this comes out for this kind of market, but potentially could come out and you know for all the other kind of stuff I mean, obviously, I don't talk about future plans, but we've got this technology with the first Major manufacturer to have a camera at this level. Obviously. There are other cameras that record each 265 But by incorporating the MXF wrapper, hence the XF XF HEVC We're able to have all the metadata as well


Y cwestiwn yw Llywodraeth 3.019 yn y ffordd Caerthorff yw Llywodraeth Rhywodraeth Cymraeg yng Nghymru yw 2022-23, yn ymgyrch i'r ffordd Caerthorff yw Llywodraeth yw Llywodraeth yw Llywodraeth yw Llywodraeth yw Llywodraeth? Y rheswlad ar y ffordd Gweithreit 3.019 yn y ffordd Caerthorff yw 89 a 100 sydd yn 29. The motion is therefore agreed. The next item of business is consideration of business motion 3.033 in the name of George Adam on behalf of the parliamentary bureau setting out a business programme. I call on George Adam to move the motion. Thank you very much, Presiding Officer, and moved. No member has asked to speak on the motion. The question is that motion 3033 be agreed. Are we all agreed? The motion is therefore agreed. The next item of business is consideration of three parliamentary bureau motions. I asked George Adam on behalf of the parliamentary bureau to move motions 3034 on approval of an SSI. And 3035 and 3036 on designation of lead committees. Thank you, Presiding Officer, and once again, all moved. Minister, the question on these motions will be put at decision time, and there are four questions to be put as a result of today's business. The first is that amendment 3018.2, in the name of Miles Briggs, which seeks to amend motion 3018 in the name of Shona Robison on prevention of homelessness duties, be agreed. Are we all agreed? No. The Parliament is not agreed, therefore we will move to a vote, and members should cast their votes now. The vote is now closed. I call Craig Hoy for a point of order. Thank you, Presiding Officer, and my app froze, and I would have voted yes. Thank you, Mr Hoy will ensure that's recorded. I call Angus Robertson for a point of order. Thank you very much, Presiding Officer. My voting app is still not functioning. I would have voted no. Thank you, Mr Robertson will ensure that's recorded. I call Rachel Hamilton for a point of order. I had an issue with my app, and I would have voted yes. Thank you, Ms Hamilton will ensure that's recorded. The result of the vote on amendment number 3018.2, in the name of Miles Briggs, is yes, 51, no, 68. There were no abstentions, the amendment is therefore not agreed. The next question is that amendment 3018.1, in the name of Mark Griffin, which seeks to amend motion 3018, in the name of Shona Robison, on prevention of homelessness duties, be agreed. Are we all agreed? No. The Parliament is not agreed, therefore we will move to a vote, and members should cast their votes now. The vote is now closed. Point of order, Ross Greer. If I lost the connectivity, I would have voted no. Thank you, Mr Greer, we'll ensure that's recorded. I call Brian Whittle for a point of order. Thank you, Presiding Officer. My app disconnected, I would have voted yes. Thank you, Mr Whittle, we'll ensure that's recorded. I call Angus Robertson for a point of order. Thank you very much Presiding Officer. My voting app is still not functioning. I would have voted no. Thank you, Mr Robertson, we'll ensure that's recorded. The result of the vote on amendment number 3018.1, in the name of Mark Griffin, is yes, 51, no, 68. There were no abstentions, the amendment is therefore not agreed. The next question is that motion 3018, in the name of Shona Robison, on prevention of homelessness duties, be agreed. Are we all agreed? Can I just check again? Thank you. The motion is therefore agreed. I propose to ask a single question on three parliamentary bureau motions. Does any member object? No member objects, therefore the final question is that motions 3034 to 3036, in the name of George Adam, on approval of an SSI, designation of lead committees be agreed. Are we all agreed? The motion is therefore agreed. That concludes decision time and will now move to members' business.


The driver was swerving, kind of like tried to run away from it, but it wasn't, of course, fast enough. So he ended up getting hit and passed away a few hours later. That's really what motivates me, like seeing it happen. Just wanting to avoid that for any other families, if possible. I don't think I've ever come across a person like this. I mean, not yet in the Air Force, at least. She's motivated. I'm motivated. We make an amazing team. No matter what happens, if I'm helping people throughout the day, that makes me feel good about myself. I'm at work. I'm helping people. I'm doing ADDD. I'm helping people. If I see the numbers of the DUIs on base, or the bases around us, that, you know, I would like to see those numbers go down. It makes me feel like the program is doing what it's supposed to do. I feel like I always have had a heart to help people. So that's why I serve.