This 2021 Toyota Highlander Hybrid XLE in Ruby Flare Red is stock number 11298A. We are here at Summit Automotive in Fond du Lac, Wisconsin. You're new and used SUV headquarters. This one has the 2.5 liter four cylinder motor and it's paired up with the hybrid system combined that puts out 243 horsepower. This vehicle has been fully safety and inspected by our service shop as a fresh oil and filter change. And this vehicle is 100% ready to go. Only 1900 miles on this vehicle. And we shoot all of our videos in 1080p, 60 frames per second. So if you have HD capabilities on your computer, tablet, smartphone, or television turn them on right now because it is definitely your best way to check out the look, styling, quality, and condition of the vehicle before seeing it in person. And if you'd like to check out all the photos on this Highlander in the upper right-hand corner screen is a link to our website. Click that and check us out there. This is an all-wheel drive. Comes with the painted and polished aluminum rims. Has Bridgestone Alenza 23565R18 tires with just about all the tread left on them. Once again, only 1900 miles on here. Ruby Flare Metallic is the color. LED running lights, factory fog lights. I think those are LEDs as well. Front bumper is in excellent shape. It does have the projector lamp headlamps. And I didn't see any dense dings or scuffs on the hood. Very clean as you'd expect with a vehicle with only 1900 miles. Passengers side front fender is in excellent condition as well. And the passenger side rim, no scuffs or scrapes on there. As you go down this side of the vehicle, take note of how clean the body is, how reflective, and mirror-like that paint is. We take these HD videos so if you are far away or even if you're close by and you just cannot make the trip down but you're still interested in purchasing the vehicle, you can see the vehicle, hear the vehicle, and have confidence in what you're looking at before you even get here. So you can make a smart buying decision from the comfort of your own home. And that's why we offer the Summit Auto Fast Pass option in the upper right-hand part of the screen, another link to our website where you can apply for financing, get approved, see a payment quote, even appraise the trade-off from the comfort of your own home. So when you get here all you got to do is drive the vehicle, love it, you'll have everything set and ready to go. Back tires, just as much tread as the front tires, and of course it does have full-wheel disc brakes. As we come around to the back of the vehicle, rear bumper is in excellent shape, no dents, stings, or scuffs on that. And the tailgate is in excellent condition as well. This is a power liftgate. You do get a little bit of a storage area back here. You also get the all-weather covering, which goes on the back of the seats. So when those seats are down, you get a nice all-weather floor mat there. There is storage and jack tools back here. And now these seats go down manually. You can see they go down like so. And normally the strap is supposed to be there, but you can get them like that. To get this gate down, there's a button right here. Press that and it'll come on down. And down the driver's side, just as clean as that passenger's side, no dents, stings, scuffs, or scrapes on that rear quarter. And for full disclosure, this back rim is in excellent condition as well. Down the rest of this side, looks really good. I didn't see any chips or anything on the edges of the doors. You do get blind spot monitoring, heated mirrors, and directional signals. Inside the XLE package gives you the gray leather interior. There are no rips or tears on the seats. Both of these front seats are heated and you do get a power driver seat. Highlander all-weather floor mats throughout. And it does have auto headlamps, tilt and telescopic steering wheel, power windows, power locks, and power mirrors. As we hop inside the vehicle, you can see that this one has 1,971 miles. We'll turn all the ignition stuff on so you can see everything. You get the nice LCD display, outside temperature display. Seat belt status, a whole bunch of really neat information. You have the lane departure warning stuff there too. Instrument cluster is nice and clean. Comes with the leather-wrapped steering wheel. Here's your forward collision warning, lane departure, cruise controls, Bluetooth and information center controls, and audio controls there. This one has the touchscreen radio with the factory navigation system. You also get your heated seat buttons there.  And then you have your different menu options, including projection manager, where you can project your cell phone to the screen via Android Auto or Apple CarPlay, AM, FM, and Sirius XM radio capabilities on here. You do get a USB hookup right there, as well as some charging USBs. Then you get your keyless entry right here. You have different drive modes, sport mode, normal mode, eco mode, stability control. You have EV mode and trail mode. All-weather format on that side, and the passenger seat is in excellent shape as well. This vehicle has never been smoked in, smells very clean inside, and it does have the power sunroof as well. SOS buttons, map lights up there. You do get home link buttons on the bottom of this review mirror for your garage door security systems and lighting systems. And we'll take a quick look at the back seats, and then we'll start it up and take a look under the hood. The back seats are just as clean as the front seats.  You may want to put back here. It does have the side window shades, so those go up like so, which is a really nice feature. If you've got people sitting in back, being burnt by the sun there. You get some rear air controls and then two more USB charging points down there. All-weather format back here as well. And these seats do fold down. Actually, they slide forward to get to that third row. Notice there are three seat belts back there, so you could fit three smaller individuals back there. These seats slide like that. And I think they just slide forward. I don't think they actually fold down. Child safety locks on the back doors. We will start it up and check out under the hood. And it's basically started right now. We might get the engine to start up while we're looking at it. And those are HID headlamps on there. Under the hood, we have the 2.5-liter four-cylinder motor. Engine bay is very clean. Once again, this vehicle has been fully-safetyed and inspected by our service shop. It has a fresh oil and filter change. All the fluids have been checked and topped off. And this vehicle is 100% ready to go. I am just going to turn the lights on so that you can see how nice and bright they are. I don't think we'll get it to start up, but there are those HID, or maybe they're LED projector lamps. Anyways, LED fog lights, but either way, they're super bright. And this vehicle is 100% ready to go. Pretty much like new. I would highly recommend it from a quality and condition standpoint. And to see more pictures of this Toyota Highlander, one of our other 450 new and used cars, trucks, SUVs, minivans, Wranglers, you name it, we got it, go to our website. Right there, www.SummitAuto.com Full pictures and descriptions of every single vehicle from two locations, all at SummitAuto.com. And if you'd like to check out more HD videos, you can go to YouTube.com slash SummitAuto. Remember to like, subscribe, and share on this video and all the videos that you see there. In fact, in a second, we will see a link to subscribe to our YouTube channel in the upper left. A link to more Highlander videos like this one in the upper right. A link to this vehicle on our website in the lower left. And a link to our latest YouTube video in the lower right. Click those check us out. And we're super excited to be offering this like new 2021 Toyota Highlander Hybrid XLE in ruby red. Thanks again for checking out the video.


My name is Kenabushi Chris. I'm here in Sonny and Stone in Las Vegas, Nevada. Filming a video today for Dynavap Devices. We're going to show you how to use the AVB or Orty Vaped Bud that's left over from your Dynavap device and use it in a fun little recipe for sushi. Take our no-bake cookie recipe that we have and chose one great from Betty Crocker. Make it fun and simple and easy just for all of you. All right, we're just going to go ahead and put that right in there. We're going to grab our Philly Cream Cheese, one-third cup just so you know and add that to our mix. And then what I have here is I already have some AVB butter that I created using my magical butter machine. Thank you guys for having it and it just makes everything nice, simple and easy. All right, now what we're going to do is take it to the microwave and we're going to go ahead and go microwave it. So if you follow me we'll get started. What we're going to do is we're going to take and we're going to put those at 15 second intervals. All right, make sure the bowl will be hot whenever you get done so be careful. And here we go. So once we've taken all our AVB butter, our cream cheese, we're just going to take and mix it up to create a nice little dough. So as of right now everything is totally infused and depending on how you made your AVB butter depends on how strong your actual dessert is going to be. All right, just so you know one of the guys, one of the things about the Dynabab device is actually called a TED device or a thermal extraction device, right? Where you take the process of decarboxylation and it takes and removes a carboxyl atom chain to create it from THCA to THC, which we all love. Now that we've got this dough going, we're just going to take it, get this bad boy out of the bowl and put it into the one right here. We've got our no bake cookie recipe chilling in the freezer just to kind of give it a little firmness to it. Don't worry, the power of the punch will still be there. And just so you know that a Dynabab device is so easy to use that if you can roast a marshmallow, you can use a Dynabab device and enjoy its beautiful flavors, okay? And just so you know that is also made in the USA, something I really like. Now what we're going to do is we're going to work this foam dough to create a nice skin, all right? Kind of like a nori or the seaweed for sushi to hold the no bake infused recipe. Work this foam dough. If you're familiar with some foam dough, you can get some in sheets, different colors, flavors, but we're going to do something really cool with this one today. Now you want to take and you're going to flatten out this foam dough to about an eighth to a quarter inch in thickness. And we're working for just a little bit, around eight to 10 inches in length. It's going to be a little sticky, so you're just going to want to work it, but you wet that, you're going to want to wet that cutting board just a little bit. And if you have a buttercream, you could use buttercream, but for this, we're just going to use just a little bit of water to make sure everything is perfect. And you want to take a stretch just a little bit, maybe put it over your hand like that and work it, okay? As you turn it. So here we go. And don't worry about if you rip just a little bit of the edge because we just need to make a sheet. So what we're going to do, take this a little extra off. Don't worry, you can save that for later. That is our fondant nori sheet. Just wanted to bring back our already chilled cookie dough that's infused with our AVB. All right, we've got our fondant nori, which we can infuse that too. We're just going to do it on another day. And I've already prepared a plate for us that we're going to have. We're going to set this bad boy up, all right? I hope you're excited like I am. And just like this, it's easy to clean. So we're going to take our fondant sheet and we're going to take and pretty much put the filling like we would with sushi into it. Hope you're ready.  I didn't want it to sweat too much.  So I put on a little bit of wax paper, which I recommend that you do because in just in case out there, if you are using a fondant sheet, it will come in a nice wax paper as well. All right. So what we're going to do is we're just going to work this all right, which is nice and ready now. Oh, God, I smell that. And it's going to give me stoned a little bit. Oh, this is a sweet treat right here. And just so you know, look for this recipe in the next issue, which is going to be the Thanksgiving special for Vegas Cannabis Magazine because it will definitely be in there. Okay, guys, we're going to save that for later. Okay. And what we're going to do is we're pretty much going to run it the same length as this, but we're going to make this side a little shorter and I'll show you why here in a little bit. So what we're going to do is you're going to take with your thumbs, we're going to take, we're going to pull up on the makisu. Now I could do this by hand, but for us, and just to show you that you can use it, but it's not necessary. We're going to take and roll over and encapsulate all our ingredients, making sure just look down in here. Okay. You see that? Now we've got that full encapsulation just like that from edge to edge. Okay. Because we don't want it to overlap and things like that. It makes a little, a little different. So what we're going to do is we'll take that and whoop, there it is. Run that. Okay. Let's see what we got. Ooh, very nice. So we're going to take this bad boy, go ahead and take this makisu away. It's done its job. And now look at that. We've got a nice, beautiful and fused with AVV sushi roll or dizzato maki because it is for dessert. Make one more time, make sure everything is in there proper. Okay. We're co-sure.  I'm going to take like this. And we want to keep our seam side down. Okay. Just like in sushi, you want to keep your seam side down. And we're just going to take and do a little formation once more. Okay. Now what we're doing today, we're definitely going to make this look like a Dynabap device. Okay. So get ready, the exciting part's coming up. So now that we've done that, what we're going to do is we've got a little bit in the edge here. And that's going to be for a mouthpiece. Okay. Now what we're going to do is we're just going to work it. We're going to work it. All right. Work that phone doll. Add a little slip into your hands so you can take. Boom. All right. And just we're going to work it like we're going to work putty to turn our water on real low.  You ready? Now what I've got here is a nice white steel blade, Japanese. All right. Recommend. You don't need to use it. It's not the cost of the blade. It's the cut it makes. So what we do is we add a little wetness here. Okay. So what we're going to do is we're going to make eight pieces equal pieces, just like this little sushi, but this one we're going to do a little different. Gonna add a little flair to it and you'll see why in just a moment. And like I said, the Dynabap device is actually a very clean, efficient, very inexpensive device. Easy to clean, made in the USA. And hey, if you're out camping, it's probably one of the best ways to go. One more roll around just to make sure everything's nice and beautiful. Right here. We're going to keep this one just a little bigger. And that's a surprise. We're going to work these pieces together nice and straight and end up looking great. We're going to take this, move it off the side. I am going to change the papers. A little technique. Rollie pollie. Wow. Look at that. I hope you saved the pieces that we cut off from creating the Nori sheet because we're going to use that right now. You know what? Let's do it like this. We're going to take and separate it. You've got to keep them separated. So we're going to take, roll this bag away out. Okay. We are going to create a nice little cap for the VapGap actually. VapGap, if you make sure to listen for the double click, that's when you know it's ready. And that's going to have beautiful and beautiful flavor. You can enjoy your AV, you can enjoy your marijuana correctly. So what we're doing is we're going to take and pull this bad boy out to create that VapGap specific to the DynaVap device. What we're going to do is we're just going to take and give her a little love. A little love goes a long way, guys. We're looking for that cylindrical effect. Don't worry. You can play with your food. Okay. It makes it fun. It's okay to play with your food, especially when you get stung off it, guys. Don't worry about that. Okay. Oh, look at that. You guys see that little surprise gift in there? So what we're going to do is the patented VapGap double click, like I said. Take this Vap away and work it. Work this bad boy to make it special. We're just going to take that, just like that, and make sure that whenever you guys are checking out the DynaVap devices on dynavap.com that you use my code Kanabushi and check out for a great discount. Now, let's do something special. I'm going to take and create the patented Titanium device. Let's make this bad boy really cool. Love. Okay. Take your finger and ring it. Call a ringer. Fold this bad boy up so we know it looks like our piece. Okay. All right. Now these things made in the USA are also made out of Titanium. So let's make it Titanium. Gotta make sure to load it up proper, huh? Almost forgot about that. Short-term memory loss, guys. So let's get this beautiful green. Just so you know, Titanium is not safe to eat, guys, but this is food safety. Patented VapGap. Finish it off. Here we have it, guys. Our own little DynaVap device deserves sushi roll. Thank you guys so much for watching this with me. Make sure to check out www.dynavap.com. Use my code Kanabushi and check out. And now you've got a recipe to use your AVV for. Make sure that you know that this is a high-efficiency heat source independent device. Extremely durable, easy to clean, and you can get at a great rate. Thank you so much, Kanabushi Chris. All you Stoners and Stoners. Thank you. Las Vegas, Nevada.


Because you get a great explanation. Everybody there? Read along with me, boys and girls. A force with which you have had some experience is the force of gravity between you and the Earth. This force is also known as weight. How much do you weigh? The answer should not be in kilograms. The answer should be in newtons. Weight is mg. It's measured in newtons. Or in the imperial system, it's measured in pounds. Found where we are? OK. Because it's not like I haven't had it up there for about 15 minutes or so. Let's just keep going. We'll ignore that on the internet. I think we're on the front page still, aren't we? Like the first page? We're there now? OK. So as I was saying, force of gravity is also called weight. Force of gravity is not the same thing as mass, although they are related. Mass is the amount of matter in an object, which we measure in kilograms. Or on the imperial system that was measured in slugs, believe it or not. To relate mass to force, we need to know the number of newtons of force per kilogram of matter. This quantity is known as, here's the term I want you to highlight or underline. This is the new term, gravitational field strength. Gravitational field strength. Find it? Ze? Find it? Hunt. I think you're here. So let me say this again. The number of newtons of force per kilogram is gravitational field strength. Near the Earth's surface, the gravity field strength is 9.8 newtons per kilogram. Now we've seen that 9.8 before, but what were the units that we attached to 9.8 previously? When I said to you 9.8, what was that number last year all the time? It's meters per second squared. It's the acceleration due to gravity. As it turns out, it's also the Earth's gravitational field strength measured in newtons per kilogram. And newtons per kilogram, if you muck around with the units, and we will in a second, is meters per second squared. Usually, if I'm dropping an object and I'm calculating its velocity, I'll say 9.8 meters per second squared. Usually, if I'm calculating a force on an object, I'll often say 9.8 newtons per kilogram, because it's the gravitational field strength. Moon's gravitational field is about 1.6 newtons per kilogram, which means if you dropped an object on the moon, it would fall at an acceleration of 1.6 meter per second squared. Here's the equation. Assuming the pen decides to write, let's try that again. Here's the equation. Fg equals mg, where g is 9.8 newtons per kilogram or meters per second squared. Basic example, example two. Find the weight of a 10-kilogram object on Earth and on the moon. So both of these are asking you to find the weight, which is fg. And in both of these, it's going to be mg. It's going to be mg. Only on the moon, I'll make sure I use g on the moon. And on the Earth, I'll make sure I use g, the gravitational field strength, on the Earth. The mass is 10, g is 9.8. A 10-kilogram mass exerts a force of 98 newtons. That's why when I had the two people pushing on the scale, I said, you know what? If you look at kilograms and multiply by 10, that's roughly the force in newtons. How much force would a 10-kilogram mass on the moon exert? Well, right here it says the moon's gravitational field is 1.6, so that's where the 1.6 came from, 16 newtons. You'd feel about 1.6 to your weight on the moon, which would take some getting used to. Your timing would be way off if you tried to play catch on the moon. Even your jumping would feel weird. Now in a space suit, you can't jump very well. But suppose we built a dome on the moon that had oxygen and a regular atmosphere in it, and so you didn't need to wear a space suit. I suspect the tricky part would be timing your landings because everything would be happening so much slower, you'd overreact and probably trip because you overreacted the land. Now turn the page. Emily, that means you can turn the page now. Example three says, example three says, select the best answer. Here's another one of those using principles of physics right to explain questions. If the force of gravity acts on an object, then the object A remains at rest, B moves at a constant speed, C accelerates in the direction of the force, D, all of the above. Once again, we're going to vote. Once again, how high you hold your hand is how certain you are of the answer. I'm positive. I'm pretty sure I'm only voting because Mr. Dewick is going to remember which people I haven't voted and he'll make fun of me, okay? So if the force of gravity acts on an object, then the object A remains at rest, B moves at a constant speed, C accelerates in the direction of the force, one, two, three, four, five, six, D, all of the above. All right, if you voted C convince me that D is wrong or if you voted D convince me that C is wrong. Can you remain at rest? Can A be true? Well, are all of you being pulled down by gravity right now? Yes, are all of you at rest right now? Yes, some of you more than others apparently Mitchell. B, can you move at a constant speed while under the force of gravity? Yeah, I did that when I jumped out of an airplane in free fall. Have I showed the free fall video yet? I haven't, have I? I'll just show that in a bit then. When I jumped out of my airplane, eventually I hit terminal velocity, which meant that air resistance up and gravity down were equal. So my net acceleration was zero even though gravity was pulling me down, I was moving at a constant speed. Certainly when I opened the parachute, I was moving at a constant speed. C, can you accelerate in the direction of the force? Well, yeah, that's true whenever you drop an object. So the answer is D, all of the above. And where it says explain your answer, I would give the three examples that I just gave an object on a table is at a constant speed even though it's under gravity, we're not gonna write it out. B, constant speed, terminal velocity, C, free fall when you first start to fall. That's how I would explain that one. We're not gonna write all that one out. Instead, we're gonna move to Newton's second law. So Newton's second law says that if we have balanced forces, then objects at rest remain at rest and objects in motion remain in motion. If we have unbalanced forces, actually crossed out Newton's second law, Newton's first law says that if we have balanced forces, then objects remain at rest and objects at rest remain at rest and objects in motion remain in motion. If we have unbalanced forces and the object accelerates in the direction of the net force. We write it this way. F net equals ma where F net is the total sum of all the forces, except writing out total sum is too much work. Does anybody know what's the symbol that we use in chemistry and in physics for the sum of or add them all up? So here's a great shorthand for you. You can reuse it often during this year. If you ever want to write the total or the sum of, it's that, a capital M on its side. It's a Greek letter sigma. It's where we get our letter S from. There's our S, there's the sigma. We just stopped doing that last little bit and curved it. And it stands for, well, here's what it looks like. That there means the total sum of the force, which is the net force in Newton's. Now, F net will never appear on our vector diagrams. It'll never appear on our free body diagrams. It's not a real force because it's not based on an interaction. It's the vector sum of all of the actual real forces. By the way, back here, I said that Newton's per kilogram were the same as meters per second squared. Here's the proof. One Newton per kilogram is the same as a meter per second squared because a Newton meter per second, sorry, kilogram meter per second squared is the same as a Newton. Why? Force is what times what, Conor? Mass, which is measured in kilograms and acceleration, which measured in. Okay, so here's what I'm gonna say. Kilogram meters per second squared. That's force, that's MA. And another way to write force is, another way to write acceleration is force divided by the mass. So if I take the force, kilogram meters per second squared, and I divide it by the mass, kilograms. Kayla, what happens to the kilograms if there's one on top and one on the bottom? So here's what I'm saying is it turns out force divided by mass is meters per second squared is acceleration, but what do I measure force in? Newton's, what do I measure mass in? What we're really saying is, Newton's per kilograms is the same as meters per second squared. There's your little proof. I shouldn't have done that big loopy thing because that's gonna be in the way. Another term for acceleration due to gravity is gravitational field strength. Measured in Newton's per kilogram. So often in a question, instead of saying, the acceleration is five meters per second squared, they'll say the acceleration is five Newton's per kilogram. That is meters per second squared, it's an acceleration. Or they'll say the gravitational field strength is five Newton's per kilogram, that's acceleration. Example four says find the unbalanced or the net force in each case, including direction. What's my net force in diagram A? How big? Two Newton's, what direction? You know what, let's go north, east, south, and west. Let's pretend we're looking down at an object. So this would be two Newton's east. My at symbol doesn't look very good. What's my net force in B? What's my net force in B? 3.7, direction, due south. What's my net force in C? What's my net force in C? One Newton, and this is why I put the at symbol in, so if otherwise there would be one N, then you wouldn't know what the heck it was going on. So one Newton at north. What's my net force in D? Brett, I heard you, thought I heard you. Oh, no, I didn't, okay, five Newton's east. And you can write out the word east so you can go at and put an E for east. E, first of all, what's my net north-south force in E? Zero, that's convenient. What's my net east-west force in E? Seven Newton's direction, west. If Y is greater than, is bigger than X, what's my net force here? Matt, louder.  Which is the approach that I use with my students. I turn every single force question into a great big tug of war. The reason is, in the unit we just finished, we always let down be negative and up be positive, so we always put in negative 9.8 meters second squared. In this unit, because we're often gonna have things moving up and something else moving down, we're just gonna decide the winning direction is positive, and that will take care of the negatives. We're not gonna put in negative 9.8. The math will take care of that for me. To solve force problems, first thing you're gonna hear me do is we're gonna draw a free body diagram. We draw one arrow for each force that acts on the object. We never ever, we never ever, we never ever, we never ever, we never ever put the net force on a free body diagram. It doesn't exist really. It's the mathematical combination of all of them, and we use it to solve things, but it's not an actual force per se. Label all the arrows, put the tail of the arrow at the center of each object, and if you want to, acceleration and velocity vectors can be drawn differently, for example, using wiggly lines. I usually don't put acceleration and velocity on my free body diagram, and a free body diagram, we represent all of the mass of an object with a dot, and then we label the forces. Then you're gonna use the free body diagram to write an algebraic net force equation, solve for any unknowns. Our force equation will be solved by using a tug of war analogy. We will ask ourselves, which force is winning? We can almost always figure that out just by looking at the diagram and scratching our brain.    This allows us to avoid having to decide which directions are positive and which directions are negative. Do I put in a negative 9.8? Never in this unit. We will decide the positive and the negative and it'll take care of itself. Example five, turn the page, no? Nothing, guys a little tired it seems. Yeah, a long weekend, should be awake. Not, absolutely. So, example five, a 2000 Newton rock, hanging from a rope accelerates upwards at three meters per second squared. A says draw a free body diagram. I'm gonna draw the free body diagram right there. I'm gonna represent the forces on the rock with a dot. The mass of the rock I represent as a dot. So put a dot right there. Apparently I have to be really clear this morning. Okay. What are the forces acting on that rock? Get the obvious ones. Okay, gravity is always pulling down. Is the rock in free fall? No, then there must be another force in the opposite direction. What? Well, I notice it's a rope. What did we traditionally call a force exerted by a rope? Tension. Why did I draw my tension arrow so much bigger than my gravity arrow? Who's winning? You know how I know? That's why. That's how I know. And I'll always exaggerate my arrows to remind myself tension is winning and gravity in this case is losing. What's my equation? Well, we'll write this down the first few times. Write this down. Winner, take away loser is equal to the net force, which is just MA. Who's winning? Tension. So anything in the tension direction, anything pointing up is going to be positive. Winner, minus. Who's losing? Loser, that equals MA. So A said draw a free body diagram. B said compare the forces that act on the object. We actually did that in our free body diagram with our arrow lengths. C says write a net force equation. There's our answer to part C. There's our net force equation. Trevor, what does D want us to find? Get the tension by itself, huh? Turns out tension is gonna be MA plus FG. Now let's see here. Do I know the mass? I saw one person nod and one person say no. I think I do, but not blatantly. I can figure out the mass. How can I figure out the mass from this? Emily? Divided by 9.8. You know what I'm gonna do? I'm actually just gonna write in for the mass, 2000 over 9.8, and that way I don't have to worry about sig figs or decimal places or anything. I'll just do that, because I'm gonna do it no matter what. Why not do it in the equation? So there's the mass. Do I know A? Do I know my net acceleration? I do. How big, Kara? Three, minus, or sorry, not minus, plus. Do I know the force of gravity? Yeah, how big? Ooh, maybe I don't know the force of gravity. They blatantly told it to me very, very easily. What's the force of gravity on this rock? Come on, folks, what's the force of gravity on this rock? What's the weight of this rock? I just spent 10 minutes talking about how gravitational fields, we said that weight was the same as MG, that force of gravity is measured in newtons. Boys and girls, what's the force of gravity on this rock? 2,000 people. Really? 2,000 newtons, yes? I don't need to do nine point, they did that for me. I don't need to go through all that garbage. They gave me the weight in newtons. Good, now crunch the numbers. Please, wake yourselves out of these doldrums. I hope that was tiredness and not not knowing. If it was not knowing, you in trouble. Because I just spent five minutes talking about it. Turn your brains on. Find the answer, please. I'm gonna freeze my screen and not tell you the answer because some of you right now are so out of it. John, what'd you get? John, what'd you get? 2,612? Why is that wrong? Because it is. Why is that still wrong? Because it is. Oh, you guys know you got a test on Thursday, right? What do I want every single answer to be this year? Two or three sig figs. Why is this wrong? Four sig figs. How about 2.61 times 10 to the third newtons? Example six. Boy, wake up, people. Example six. Is it correct to say that if the rock in example five is moving upwards, then the string tension must always be greater than the weight of the rock. If the rock in example five is moving upwards, if the rock in example five is moving upwards, will tension always be bigger than FG? Convince me. I hear yes, convince me. Or do I hear no, convince me? Yes or no? If the rock is moving upwards, is tension always bigger than FG? Here's my rock. Right here, see it? What can you tell me about the speed that I just moved at? Constant, so what was my net acceleration? Zero, so if that's zero, how big is this number right here? Zero, what could you tell me about tension and FG? Would tension have to be bigger? In fact, it would be the, if A equals zero, constant speed, tension minus FG equals zero, there's my winner minus loser equation that we started out with, where the zero come from. Well, if acceleration is zero, what's zero times the mass? Zero, tension equals FG. If they're equal, are they greater? No, there's a mathematical explanation with a tiny bit of English, but there's a mathematical answer using principles of physics. For a rock moving upwards, is it ever possible for the chord tension to be less than the weight of the rock? Is it ever possible for this to be smaller than that? Yes or no? Katie said yes, convince me. Katie's right, it's something to do with acceleration, but she's wrong, she doesn't know what. Watch, was the rock moving upwards for a while? Did you see slack in the chord? Would that suggest that, what? I don't even think tension existed at all. In fact, I think tension was zero, but gravity hadn't vanished, had it? So this is really, I think Katie, what you were trying to visualize is this. For a split second, give it a big tug. So my answer to here would be, is it possible? Yes, if mass is in free fall, but still traveling up. You know what, instead of traveling, let's just say still moving, let's use their word, moving up. If your initial velocity upwards is enough that it stays in free fall for a few seconds before coming to a stop, once it starts to come back down and tension yanks up, okay, then tension, but on the way up for a split second in free fall, you all saw the string went limp there, yes? So yeah, it can be an interesting equation to try and draw. A little technical comment here on force equations and vectors. If the mass, in example five, is accelerating down, say at two meters second squared, we have two choices. We could always let down be positive and always let up, sorry, down be negative and always let up be positive. So up and right could be positive, down and left are negative, and we would say that, I don't like that approach. Caitlyn, it works great for small one-dimensional problems, but for two-dimensional problems, we have a problem. For example, here, this mass is moving down negative, but this mass is moving to the right, which last unit was positive.  We will decide to let winner be positive.  What's your homework? Well, your homework is really study for the test on Thursday, but then I don't see you for a week. Like your test is Thursday, next Tuesday, number one, number two, three is great. So one, two, three, four is good, parachute, yay. By the way, on question four, part C is on the next page just so that you know, I don't know it's saying which of the following is true, A, B, and C. Five is good, six, seven, and nine. Nine is a nice challenging one, but it's a great combination of last unit and this unit. That would be a great example of if I was wanting to give you a B-level written question. Okay?


Hello Columbia. Welcome to City Talk. I'm Faye Daniels, Education Coordinator with Columbia Housing Authority and I'm here today to talk about the Columbia Housing Authority Developments Fourth Annual Scholarship Golf Tournament. The tournament is scheduled for Friday, May 4th to begin at 11 o'clock as the shotgun start is going to be held at Cobblestone Park Golf Club in Blythewood. This is our fourth year. First three years were fantastic and we're anticipating another great participation from the community. We've got sponsorship levels for persons who just want to support our scholarship program. We have plenty of room for additional golfers, so if you're interested we're inviting all to come out and support our scholarship program. The Columbia Housing Authority Scholarship Program was established to support high school graduating seniors who are planning to continue their education in higher colleges or universities, tech schools. We do this because we recognize that there was an increasing demand being placed on families due to tuition rise and a decrease in amount of scholarship funds that were available. So to support our families and our youth, we decided to begin holding the tournament to raise monies to support the scholarship fund. Each year we award anywhere from five hundred to a thousand dollars to each student who's planning to enter college. If you're interested in supporting our golf tournament this year, please go to our website at www.chasc.org. All the information is on our website. For general information, if you want to attend and participate, if you want to participate as a golfer, our entry-level fee is a hundred dollars per individual and four hundred dollars for a team, but we have additional sponsorship levels. If you want to participate at any level higher than four hundred dollars, we welcome that and we encourage that. Each scholarship is tremendously invaluable to our students. Every year we have our students come back to us and they visit us even on the day of the tournament. To let the Housing Authority and golfers and other supporters and sponsors know how much they appreciate the scholarships that they receive. For many of them, it's a matter of buying additional books that are needed or money used to help them relocate to a campus and even money to help them with housing that scholarships or financial other financial aid proves not to be adequate for. Our parents as well are greatly appreciative of the support that they get through the scholarship program. If you've not registered, it's not too late. Our registration deadline is Monday, April 30th, but we invite you to come out and join the other many supporters that we have of our scholarship program. We've got bankers, local bankings, we have local banks, physician offices, other businesses, realtors, you name it. We've got the support. We just need more and we invite the community to come out and support. Thank you again for joining us on City Talk. Again, we encourage you to go to our website www.chasc.org and register to come out and play golf with us and have fun and also do good for some students who are well deserving.


Now, you can go further into abstract notation which is called generalized orthogonal groups ok. So, let me write that also just like the way I wrote S o n, I want to do a generalized one. So, now 3 plus 1 space time is gone. These meanings are gone. What I will do is I will have x mu with x 1, x 2, x n then you have y 1, y 2, y m ok. What I am going to see is I am going to write a eta matrix, I am going to write an eta matrix with identity plus identity as n cross n minus identity as m cross k ok. Earlier I had I put this as minus and this as plus, but you can do the. So, I will take such a matrix as eta. So, in our earlier case we had n to be 3 and m to be 1 right. 3 were positive elements, 1 was negative element. How I write is not important. You can juggle around, but totally in the diagonal entries n of them are positive entries, m of them are negative entries ok. So, in the earlier notation which I did for space time 3 plus 1 dimensional space time, C t the one entry was negative, 3 were positive ok. So, in this case 1 is negative, 3 is positive ok. Here n is positive, n of them are positive, m of them are negative. So, now I can write a lambda transpose what will be the dimension in this vector space n plus m cross n plus m and this eta matrix, this is what I am calling it as eta lambda should be eta where n of them are m of them are negative, n of them are positive just keeping track of it. So, m of them are negative, n of them are positive. So, the set of these matrices is what I am going to call that set of these matrices are belonging to the set forms of group which I am going to denote it as S o ok, S o n comma m where n is the number of positive entries and m is the number of negative entries, but it is interchangeable. You can overall negative sign you can put and do things, but this is the way I am going to define that it forms a generalized orthogonal group which satisfies this condition and now what happens to your Lorentz group in this notation? Lorentz group in this generalized orthogonal group notation can be written as number of generators of S o 3 comma 1 is same as number of generators for S o 4 ok. So, S o m comma n what is the number of generators you find out? S o m plus n this is very different from this group why? S o m plus n this group will have all of them plus this one is m of them is different from n of them ok. So, there is a difference here ok sorry I should have put n comma m, n is positive. So, I am just saying that these two are not isomorphic groups, but number of parameters for defining these matrices will be how many? How many parameters you need for this?  This is not different from the number of parameters for S o m plus n, but as a group they are different, if you find the number of generators and number of parameters it is still n plus m C 2 for the generalized groups clear. So, I took you from physical space and physical space time and I put you in a abstract situation of how to look at a group of rotations in an n dimensional real vector space or a vector space which is quote and quote like space time where n of them will be like time and the remaining m of them is like space, but it is not to be viewed as something which you can see in your day to day life. Some of the systems may have such symmetries and you can exploit the symmetries and the algebra of it. O of n comma m will be just a, it is a direct product with the CS group, you can do that also. Just in instead of doing only inversion in space which you would have done in S o n, you will have a time translation, sorry time reversal and space inversion both are possible clear. So, this is what I slowly took you off from on the slide from rotations on S o 3. As I said there physically we saw the parameters here and in the abstract way I taught you today how to see the parameters ok. So, physically when we saw we said you have to fix a direction which is hat n and with respect to the direction you have to do a rotation by some magnitude psi about this direction and that we compactly write it is what I said, but then I took you on to a generalized situation. And there was some confusion at the end of the class that some of you were unclear about this issue. Only thing is I wanted to try and redraw this parameter space in a compact fashion that is what I wanted to do. Only you remember that if you do a rotation by an angle pi using a unit vector let us say along z axis, you could have also done it positive z axis, you can invert it and make it negative z axis it does not really matter as long as you do an angle pi. If you do arbitrary angle other than pi then there is no such equality. It happens this equality happens only for angle pi that the diametrically opposite points on a sphere on a solid sphere of radius pi those two have to be identified is that clear? So, I took a solid sphere this is solid ok. So, solid sphere the maximum radius it can have the radius can be only pi. So, the radial vector when you are doing spherical polar coordinate you will say 0 to infinity. The one which defines for us the parameter space in a compact fashion is a solid sphere with unit vectors like your theta phi, but the radial vector is taken by the magnitude of rotation which you do about such an axis and that rotation also should go from 0 to 2 pi or minus pi to plus pi. So, this is the manifold parameter space which defines the space for defining your rotation in three dimensional space. Any point here if you choose find the radius value suppose it is phi units and let us take it to be making an angle theta with respect to z axis and then on the projection let it make phi and phi with respect to x axis and then you can define this point as someone at particular point you can write it as phi for r and then whatever is the theta and phi as r theta coordinates ok. Phi is not a good number it should always be between minus pi to plus pi maybe I could call it as some 1 in radians ok. So, this is a meaning of saying that I am going to take this point refers to rotation by angle in radians I have taken it to be 1 and then direction is chosen to be making an angle theta with respect to z axis and phi in the x y plane clear. So, that is the parameter space which is drawn after I drawn it I am only trying to use that property that if you take it on the boundary this corresponds to pi right any point here the radial coordinate is pi and you can choose your axis which is also n hat axis along this. What will happen is that whether I do a rotation by pi with angle n hat I can still do it with minus n hat ok. So, this is minus n hat. So, which means that this point is same as this point clear these two points are rotation described by this point is same as rotation described by this point that is not true for interior points only on the boundary. So, the parameter is space not only defines this whole space, but there are some identification which you have to keep in mind ok. It is not just every point on the boundary is independent that is it. And then as a topologist or looking at the topology of this parameter space. Suppose I take close curves in some space which has a hole then there are different ways of taking close curves. Only thing is given this topology which is the parameter space for SO 3. Now, you do not associate rotation matrix with every point. If you ask are there only one type of close curves or more than one type of close curves which you can draw on such a manifold which I have drawn for you. You have to remember in this manifold diametrically opposite points on the radius equal to pi r identified. If you use that information then the group manifold two types of possible close curves. One which does not even go to the boundary ok. So, if you see these curves this is one type of curve. Other close curve can go from here to the boundary, diagonally opposite point is here and you get back. Similarly, this wavy line diametrically opposite point is same as this. So, each of these curves which I have drawn this one curve by any deformation I cannot make it look like this one. By deformation of this I can make it look like this ok. So, in that sense there is two types of non-trivial close curves which I can draw on this group manifold associated with SO 3 where only two types somebody came and said I could intersect the boundary twice, but you can nullify it and bring it inside ok. You can try that out also. Only two independent non-trivial close curves can be drawn for the SO 3 group manifold ok. It is nothing to do with seeing rotations where you know every point is a rotation matrix associated with every point you can write rotation matrix with that psi theta phi, but then once you draw close curve it is just to look at the topology of the group manifold. Is that clear? So, this also we went through. So, let me not get into this and this is left as an exercise for you to do the algebra of generators and this I have already explained to you that set of n cross n matrix with determinant plus 1 forms a group S o n and these will leave the magnitude of the vector invariant which you can formally write it as x i squared and so on ok. I have not introduced the eta here, but you can introduce an eta so that that minus sign is automatically taken care of. So, SO 3 comma 1 is the Lorentz group and the reason is that C t has a sign different from x y z ok. So, now, I am going to introduce the formal abstract Lie algebra. So, a Lie algebra is also a vector space on which you define an operation which you call it as this Lie bracket. This bracket with comma which we call in quantum mechanics has committed a bracket in Lie group's context it is called Lie bracket ok. So, you have a set inside this Lie group just like rotation group had L x L y L z, your Lorentz group had L x L y L z and the boost transformation 6 of them. So, these x y are the generators of that Lie algebra or the generators of the transformation which will constitute to define the commutator brackets ok. For all x n y n g x y commutator should also be in g that is what you see L x L y commutator can be 0, but it can also be the remaining generators. And any scalars multiplying them that is why it is a vector space you can rewrite that commutator as lambda times this, these are known to you from your quantum mechanics commutator bracket it is exactly the same properties.  Jacobi identity is just cyclic permutation of the 3 elements of the Lie algebra ok. So, this vector space which has elements x y z the set if it satisfies all the 4 properties you call that to be that vector space to be a Lie algebra under operation which is the Lie bracket. Suppose the Lie bracket is 0 for all x y when does this happen in our case? Translation group it happened translation generators of translation we found that p x p y p z forms a is constitute a Lie algebra, but it also be a abelian Lie algebra because p x p y is 0 and so on. So, in general if all the elements of this vector space commute with each other then you call it as an abelian Lie algebra. Now, I am looking at Lie algebra not the group if you want to get the group you have to exponentiate the generators of the Lie algebra clear no? So, as a formal definition of a Lie algebra x x x t commutator if you had a set of all the x's x is now an abstract notation and for an abstract transformation what is the Lie algebra and so on. So, in the abstract notation you will have x x x t should give you a linear combination of x k and what is the requirement because this is a commutator kind of Lie bracket with anti-symmetry property whenever you interchange s and t these coefficients should become negative of itself, but also you have seen L x L y will give you L z L y L x will give you a minus L z. So, this is this k is summed up that is the assumption here the repeated index is summed up and then s and t are anti-symmetric this coefficient should be such that s and t are anti-symmetric C s t k are called the structure constants. Is that clear? What is the structure constants in the case of your orbital angular momentum algebra? So, I can write this as L i L j is let me suppress the h cross i times epsilon i j k L k right. So, your epsilon i j k is your C. So, these are the structure constants for your algebra and this algebra is what I will denote it as s o 3 small s small o because this is the algebra of generators for rotations and it is satisfying all the axioms. So, it is definitely a Lie algebra and is it a abelian or non abelian? It is non abelian because it is not going to communicate. You can also have a subset of elements of the Lie algebra G such that elements obey all the rules of a Lie algebra. So, if you do your Lorentz transformation. So, s o 3 1 the algebra will be s o 3 1. So, this o and all is capital so that is the group this is the algebra and the algebra will involve your L l 3 i j L k L. You can also have algebra which involves L 0 i with L i j or anyway let me put this to be j k. You can have L 0 i with L 0 k. You understand what I am writing? The 0 denotes the time coordinate which is of a different minus sign or plus sign in your eta matrix i j k are like your positive coordinates and amongst the positive coordinates if you try to write this bracket what will it give me? Will it give anything which involves the time coordinate? These are the generators of rotation in your physical space or space time. So, if you try to write this out it will turn out to be some linear combination with some L i prime j prime I am not writing what it is with some coefficients. You agree? I am putting a double index because each one is a double index you will have an i j and a k l. Will this have a 0 j prime? 0 j is for boosting. Two consecutive rotations whatever you do are you going to generate something that is if one frame is moving with other frame with velocity v x can you generate by that? No, you can never do that. So, in that sense there is a subset there is a subset or S o 3 which I have written here is a subset of S o 3 1 clear. S o 3 are pure rotations in space even in c square t square minus x square minus y square minus z square you have a subset of rotations x, y, z and when you do such a transformation of x, y, z it is going to only give you this it is not going to take you to the other three generators which are like boosting of one frame with respect to the other. And if you have a subset which satisfies a closed form among that set itself amongst that subset you call it as a sub algebra just like sub groups if you have a subset of a group with product giving you elements which belongs only to that subset you call it as a subgroup. So, this implies that these are elements of S o 3 because any bracket if I write it is going to be only with respect to the spatial components.  The next definition is just like we have we did invariant sub groups you also have an invariant sub algebra H should be a sub algebra of to start with. And if you take any element of the Lie algebra with any element of the sub algebra the Lie bracket if you find it to be inside the sub algebra then you call it as an invariant sub algebra. Can you think of an example for this where you can get this? So, let us take our Lorentz transformation to that let us add translations also space time translation because I am doing Lorentz translation.  If I say that I want to look at the group transformation which is not just Lorentz transformation, but also space time translation. So, how many generators will be there? Lorentz transformation will have 6 generators and space time translation will have 3 translation p x p y p z and the corresponding time translation whose corresponding generator is the Hamiltonian. When you have to write a Lie algebra for this complete set which is what we call it as a Poincare group. Poincare group allows space time translation symmetry, rotation symmetry and boost symmetry together that forms a Poincare group. If you look at this what will be the algebra between p x p y p z and Hamiltonian that will be an Abelian algebra it is a sub algebra. And if you take p x with any of these rotation generators what is that going to be? You all know what happens when you take a Lie with p j will it be a Lie or will it be p? It will be p right. So, you can write it as apart from this i factor. So, I said that p i p j commutator is 0 it is an Abelian sub algebra over on top of it the elements of this Abelian sub algebra with the other rotation generators for example, is giving me back the generators in the Abelian sub algebra.  It is not obvious from here how the group elements will satisfy the properties which we learnt in the discrete groups right. What did we learn in the discrete groups? If it is an invariant sub algebra sub group what is the requirement? Is that right?  Now, I am trying to tell you that an invariant sub algebra is 1 where G with H is an element of that invariant sub algebra. How does this imply that? How do you do that? So, let me take a G 1 element with a H 1 element let me call it to be H 2 suppose corresponding to the element in the Lie algebra you can write group elements. How will you write that? E to the power of i G 1 will be the group element. E to the power of i H 1 is the group element and I need to show this piece is going to be an element of E to the power of i H. This I will give it as an exercise and we will discuss at some point, but these two are equivalent ok. So, when I say that the sub algebra is an invariant sub algebra its commutator or Lie bracket with all the elements of the Lie algebra this is not group element Lie algebra elements which is like generators they have to belong to that sub algebra. How this reflects to what you learnt is to redo the whole thing explicitly and see that it gives me this condition automatically gives me this condition.


Let's get healthy this is featured on freedom where we take your videos and feature them on this show Today, I want to see videos about health from you. Look behind me This is my new juicer that I bought just a few days ago It lets us take carrots and make juice separating the pulp from the juice to get very fresh carrot juice I'll play a clip But for you to win the next featured on freedom spotlight Send us links to your videos down there in the comments below or make a video if you don't have one yet about health That is the theme of today's featured on freedom being healthy exercising eating healthy anything in that area So here is my entry as an example I can't win of the featured on freedom healthy roll it so this is our juicer We'll assemble it and we'll convert all of these carrots into juice It's a very healthy drink and we're going to enjoy it as soon as we assemble it one moment and Here is the juicer fully assembled and now we are ready to make the juice. Let's go Okay, we're starting So now Inside okay ready and that is how we make carrot juice and here I am taking a sip of what we made Now that's fresh carrot juice If you make this at home send us a video we'd love to see how you make juice at your home with your juicer Normally, we don't do healthy things. How many of you get a lot of exercise? How many of you choose to eat healthy? I hope to encourage and inspire you through this featured on freedom contest To think about health at least for one video. I hope this helps. Who am I? I am George CEO and founder of freedom and you've been watching Grow together as a family because this is the freedom family You are part of it. We are all part of it and we're all growing together so grow with us and Partner with freedom that play now button right there on the video bar is all you need to click to get started


Wutabara March Tawa, bana danyash Is he your March? Ya Okay step part Give her the flower Come for it Pili Ya pili And I choose I go for the goal By me? No No Anaka kulke Anakakula Iquna ya jyutu knakalpa Ya manzai, ya manzai Tugud, Tugud Tugud, Tugud Yo yo yo yo, they call me honey moz But ladies call me honey The best MC in Eastern Central Africa Ida na manza marketing, when you, when you Advert Bro, who the meme is that? Uje, Uje ni pata Uje ni pata So, who the meme is that? Who the honey moz? So, who the honey moz? What one who hey? Hey Mkofi, Tmkofain Maze, Valentine's in Mifika Muna tukam, tukam tukia pana ma' dem Yes what do you expect? Ah, ya ya ya Mambo m'ichemuka Mambo m'ichemuka Watcha quanzai, let me introduce my surez Introduce your surez How surez in the building, he? Ya ya Pretty surez Uh huh Pretty chillz I introduce bro Let me talk to Avril Talk to Avril Avril and Niktikering Ya ya ya Wanaume Avril yae Ya ya ya Asha la Sawa, wana wana Avril Avril Avril Ya ya I'm fine Niktikering, how you? I'm fine Muna skia kuna Niktikering Ya ya ya Wana se maju he Introduce watu hako Introduce watu hako What's up and intro? What's up and intro? So, this is what we do Because at the video Ya ya These are truly do my brother In this building So let me call Mr. Dangoche Mr. Dangoche Mr. Dangoche o Kenya Kuelika Bisa Kuelika Bisa Kama Kawa Dangoche Yes All the way from Tanzania Ya ya Let's just say wana nita Ya ubo Ya hubo ya hubo Ya hubo ya hubo Yes, what's up in guys? Yes Yes, and we are chilling with D.I. Adi wama Wait, wait, wait Adi when do you want some man home and away? Home and away Kwani umesinda nani?  Yes Animals Umojiwa ma boy Ya Ya Ya, that's brother starving Ya How is he? They can't Lakin he dem Lazi ma kwa choosi Kwa choosi Umojiwa umojiwa Umojiwa umojiwa Umojiwa umojiwa Umojiwa umojiwa Umojiwa umojiwa Ue, ma wanima Ma wanima run Sawa So stories are never as a must Sawa Dema at break Animal Choosing random shorty from this side Minta na na wu yu Nani Uya kon address Ya ya Umesema unanza na vera sidika Vera sidika Vera sidika Ya Chagwa Chagwa kiziya na modya na patia ma uwa bana Find your match from my right side Na wuyo na umojiwa We are here for fun and also not only for fun but finding someone that you really true love and also you can engage with us. Thank you that's all. Thank you that's all. Yes. You want to come and play a game? Yes. Where is Chagua? Where is Siddika? Choose from this side. Who is your match? It's actually Tau. It's Tau. Who is your match from my right side? It's Tau. Let's go. Who is your match? It's Tau. Who is your match? It's Tau. You can actually look at the outfit. The outfit is Tau. Let's continue. It's actually fine but... Compose your lats. Compose your shoes. Shida ni kiyatu. Kiyamu tu kiyatu shida. Tau. Tau. Una mixaji red na blue. Tau aviyatu. Tau aviyatu. Let's continue. Apovipi? No. Anaga kulkida. Umiha chwa jwani kulkida. Yani kuna jya juna kapoata? Ya maza. Tugudu. Apovipi, Apovipi. I don't like shorts. We don't like shorts. We don't like shorts. We don't like shorts. It's actually fine. It's fine. The height is the problem. It's okay. It's okay. Lukuzi. Lukuzi. Mombasa. Kijana mombasa. Kijana mombasa. Una kwa galeskinu si. Una kwa galeskinu si. Tiliwa na babyface? Babyface. Tiliwa na babyface. Tiliwa na babyface. Tiliwa na babyface. Kuna different. Hansam na babyface.  No, who is your match from this side? Ume kata kila matu? Ume kata kila matu ya match Who is your match?  Saksesa wama go Who is your match? Who is your match? Okay, between these two, who is your match? Who is your match? Who is your match? My brother, do you think she is your match? Absolutely So, my brother, give him the flower See you next time Thank you very much So ladies and gentlemen, tuna kujaterna, nikama tunanzahupe Nikama tunanzahupe mai brother Hanimos, choose the lady mai brother Nikicheki hapa, na cheki hapa, na cheki hapa Nadia ya saye Na ni? Tuwanziapa Naskuiro? Komedian East and Central Africa Best Komedian Awards Pulse Awards Tuwanziapa Naskuiro in a road, no competition In a where's I was? Kwa microphone?  Chain Pazangafu Stop the cow Elupele Wait wait wait Chain eluptan Chain amestemani 5,000 tanzanyan mani Tanzanyan mani Yonitu mbao ya kenya Fimu apartment palekaren Palekaren?  Aa My brother My brother Iya Iya Tuliya Tuliya Romantikali Tuliya Is she your match? She's fine Is she your match? My brother If she's fine Is she your match? Everything fine Yes no Everything fine Yes Everything fine Yes no Everything fine Iya Iya Iya Give him the flower Give him the flower romantikali No no no Romantikali Romantikali Iya Iya Iya Iya Iya Iya Iya Iya How are you guys? you guys... your not dead well Iya My team I'll make war That time To say Hi, I'm Jareen. My Instagram handle is at Konran. I'm here to find my march, Valentine's Day. We are coming to the building. I love the fact that I'm wearing a microphone. You put a microphone on. Chaguwa, chaguwa. Nadia, I'm coming. It's your turn. Let's see. Choose your march from my right side. Apun, yes or no? Yes, no. Mboana. He's short. Short? He's short. He's short for me. He's a dwarf. He's definitely a dwarf. He's a dwarf. He's a dwarf. He's a dwarf. He's a dwarf. He's a dwarf. He's a dwarf. You choose your march? Yes. You choose your march? Yes. Round face. Round face. Kwen, look. He's coming. You're wearing a uniform. Asa hui ni hulawa? Haaa, wetulia hui cha wu liwe?  Kwanini, umesama ditish. Intish, ita kwanini. Kwanini. Just use the mic. Atari kwanini. Yes. Didye kamutu. Uyu, nididye wa willipol naba hati. Anaitu adi hitamutu. Didye kamutu. Mixed jacket is kwaikila una spotify. Nga na na mix palipola willipol. Yes. Why? Ya, why? Ya, why? Ya, why? Ya, why? Ya, why? Ya, why? Ya, why? Ya, why? Ya, why? Ya, why? Ya, why? Anakustua. Anakustua. Anakustua? Anakustua. Kha mutubole una ututu kwa kwanadi. Ya, k們utu. Komedi and Eastern Central Africa, West Limpopo. Uyu anitu wa skwiro. Didye skwiro. Kwanini. Small Ice, Dakshot. Uyuh, nii hiyo yung ii owele fanya grama palipraimera, nii ui kwa good. Small Ice, Dakshot. Ayah, kwa muna kwa muna? Sawa, ayutu re-consider, wul kwa re-consider na nani apat? Uta-consider, bada wa maa bada uta e re-consider Dan goti?  Ati The nyash is bigger than the forehead The nyash is bigger than the forehead What have you said, my brother? I'm saying ngem tukua lakini The void is bigger than the nyash The nyash is bigger than the forehead The void is bigger than the nyash The nyash is bigger than the forehead Take it Animals Usitua kambak haji umepua kambak Yes Ay, ay, ay, ay, ay So gentlemen So many Gentlemen Gentlemen We have three Yeah Three more ladies Yes And how many men are we remaining with, seven? Yes So how three more ladies have to go and now we are talking? Sign an elimination stage We want to remain with three boys With three boys Yes So, I want to eliminate according to appearance Where we to tumtun on? Tumtun on, the words are kwa luku Okay Kwa luku Kwa luku According to outfit appearance Wechagua Yes Hi, my name is Haven And you can find me on Instagram at Nelihaven And on TikTok at Nelami And you can find me in all other social media platforms that haven't majestewan Who are you? Give her the mic Choose Who? He's fine but it's not giving Valentine's Squiro He's not giving Valentine's I am Squiro We'll talk later, my brother And him too No, he has said Wait first, you only one chance Oh, one chance Eliminate one person I'll hold it to outfit appearance Kamutu Kamutu Tonga badae kamutu I'll have Valentine's but Viyatu Viyatu I'll have Valentine's but Viyatu I'll have Eliminate one person I'll hold it to outfit Outfit I'll eliminate one person Outfit Yes, one person Doja, doja We'll have Valentine's And I'll kick it out 30 Sawa, sawa So, what is your name? Tulafanya Tulafanya Bizuri So, easy mawa Napaiawa naume sasa Ima sayawana kute What's your name? Chukawa mawaeako Aina Shida Aina Shida Chukawa mawaeako Let's go mawae Uina mawae Bring me that mawa Doi mawa, doi Nice, nice, nice Thank you So guys We're doing it simple Step forward If you think anyone Klinnia Graca Get in hiding Step forward Right here If you think there's a Step forward Choose anyone from this side That you think will make a Valentine's with success my brother So you want me to wash why don't you situation what will be Lightning, show me why are you not looking at realmente Is it you who likes to speak Ili seima na nili seima na tasi mache na godi ma bidi Piga shuguru Mani stops nonsense Who is your match from this side? Let me start from this side Yes, start my brother The smile is beautiful The smile is beautiful But I'll give a comment like the one they gave it to my brother What's your comment my brother? Round face Continue So no match Denyash What's your comment? What's your comment? Denyash What's your comment? Let's first pause Let's pause When you see the smile man When you see the smile man God yes, God yes, God yes smile man God yes I love the beauty But I think I'm still confused by the true But let me go for Denyash Denyash So she is your match Okay Is he your match? Yeah Okay Give her the flower my brother Beautiful Enjoy your valentines Enjoy your valentines my brother Okay There you have her So kabel, so kabel, yes sir In avril na nikitakeri Na nikitakeri I have avril and nikitakeri Yes So muast, step forward Muast, step forward Who is your match on my left side?  Kamia. We only have one lady remaining. So Averil. And two gentlemen. Averil. Whats up? Whats up. Whats up Averil? Go ja trukit. Yes. Jutu kona wanomu owila mbaki? Yes. Wachadem dachagu? Actually that's what she's doing, my brother. Wachadem machagu e. Wachadem perrezon. Ya ya ya. So Averil. Ya. Uga Fuliza? My brother? We need to work hard in this life. You got to save in account. Save in account? Are you working... What have you even offered to the pedikas? Come on, I am not doing same. Come on, I will pay the same amount. Do you guys want money? Ya. Do you want money? Ya. Are you guys broke? Me, I am not broke. Are you broke? Ya, ya Fuliza. Ya Fuliza. Animals, say 1, say 1. What are you to assume we are gonna pay some? To assume or not do. We are going according to what you love. Choose one person I'm choosing And I choose Choose I go for the gold Buy my brother Buy Buy my brother So what you can tell our brother Yes Brother Nunu wa nini Nunu wa remis Nunu wa remis Enjoy yourself Yes Danoti Yes How do you feel getting a mati? I feel great Kudeni karibu So how do you feel you found your mati And you're going to enjoy your valentines? I'm loving for this valentine This guy is rich So ladies and gentlemen Thank you so much for watching Ya It's been me, Hanimuz It's a good mati We want to talk on enda We want to talk on enda We want to talk on enda I'm a delivery man Maybe you can tell me on enda You Black Black I can't tell you on enda I can't smile on enda I can't smile on enda I can't smile on enda So Hanimuz Yes So Kenyans na kwa mbia We are coming manze So I want to get to a video With your valentines I'll give you a free flower That is your S.P.M.Buzz in a show Natu transponsor debt We're sponsoring a debt For all these people who are at their matches Ya So ladies and gentlemen Thank you so much for watching us Subscribe pala Subscribe pala man Share Share everything We are here Comments Natu taku wa apakamu kuna Pesuna na natu Ya cover anything that you wanted Ya We are here to cover everything And my name is Hanimuz And ladies call me Hanimuz Next time Adios


The United Kingdom Court has granted four-man Nigerian Deputy Senate President, Ike Ikwere Madhu's wife, Beatrice Bale. Ikwere Madhu and his wife were accused of trafficking a young Nigerian to the UK for the purpose of investing his kidney to transplant his organ to their daughter who suffers from kidney failure. While the court denied Ikwere Madhu Bale, that of his wife was granted the common sergeant of London, George Richard Marks, granted Beatrice Bale under stringent conditions.