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‫Welcome back.

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‫So this was our state's basic equation in a very compact form.

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‫Now, of course, we have to dig deeper than that and express this equation in a less compact way in

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‫order to be able to work with that.

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‫However, that's just a matter of representation.

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‫You just expand vectors and matrices and see what's inside.

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‫So, for example, instead of writing this vector like this, we can write it like this where you have

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‫each time derivative of the state equals and then something else.

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‫But before we do that, we have to do something else.

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‫You see this lambda B vector here?

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‫It's a vector that contains the net force and moments.

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‫So you can write it out like this.

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‫You have your F net and then M-Net in the body frame and then transpose.

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‫But these are the net forces and moments that in itself does not tell you much.

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‫The net forces and moments are composed of individual forces.

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‫In moments like this, you have your F one plus F two plus F three plus.

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‫How many forces you have there equals your FNET and then you have your M one plus M two plus M three

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‫plus.

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‫How many moments you have there equals your net moment.

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‫That's why we also call them the sum of the forces and the sum of the moments.

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‫So one thing that we have to do before we express our Newton oilor formulation in the states space form,

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‫we have to identify the individual forces and the individual moments that our drone is exposed to.

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‫So this is your little drone here and you can be exposed to, for example, two F one, and maybe then

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‫later to F to.

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‫And then you can have moment one and then perhaps moment two, so all these forces in moments need to

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‫be added together to get your net force and net moment.

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‫But we have to know the individual forces in moments as well.

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‫So what is our drone exposed to?

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‫Well, first of all, as you can imagine, the drone is exposed to force of gravity, right?

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‫So, again, that's your drone here, and since the drone is mass symmetric, then the equivalent force

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‫of gravity vector acts through the center of mass of the drone.

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‫So this is your force of gravity here.

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‫And the center of mass of the drone is itself aligned with the origin of the body frame, so the origin

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‫of the body frame is also here where you have the center of mass.

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‫See that and dot.

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‫Therefore, you can say that the first lamda and let's call it Lunda one vector B, we can say that

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‫this is for gravity and lets for clarity also call it like this, Lunda G in the body frame.

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‫So G stands for gravity so we can rewrite this lambda G in the body frame in this way here, here this

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‫f g in the body frame is a three by one force vector that has three elements.

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‫So it has effects F, Y, and then F, Z.

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‫And remember, this is in the body frame and now it's important to note that there is no moment of gravity

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‫because the equivalent gravity force vector goes through the center of mass of the wave and the origin

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‫of the body frame is where the center of mass is.

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‫If the body frame origin was somewhere else, like, for example here.

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‫And let's just imagine that this is our body from x axis and then that would be our body frame y axis

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‫and then body frame Z axis.

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‫Then you would have a distance here between the origin of the body frame and the center of mass of the

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‫drone.

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‫And then with respect to this purple body frame, your force of gravity would create a moment.

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‫But we don't want that.

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‫So we do it in a smart way.

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‫And we put the body frame in the best place where its origin matches the center of mass.

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‫So we put the origin here in the center of the drone, that means that no movement is created in our

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‫body frame and what you have is a zero three by one vector.

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‫As your gravity moment elements, so this zero three by one vector looks like this zero zero and zero,

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‫that's how it looks like.

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‫By the way, what do I mean when I say equivalent gravity force vector?

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‫Well, gravity is actually a distributed force.

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‫Imagine that you have a square plate here, then force of gravity acts on every single point on this

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‫object.

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‫Let's say that the mass of the plate is 50 kilograms and let's say that the area of the plate is five

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‫square metres.

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‫You know that the force of gravity equals F G equals mass times G.

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‫Well, that's approximate G to be 10 meters per second squared, even though in reality it's nine point

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‫eight one meters per second squared.

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‫But just to make it easier, let's just say that it's 10 meters per second squared.

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‫Then that means that f some G equals mass times G.

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‫So 50 times 10 equals five hundred Newtons.

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‫In reality, though, this is not a point force, it's a distributed force.

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‫So it would be F g divided by the area of the plate, and that would be five hundred divided by five,

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‫and then that would equal 100 Newton per square meter.

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‫That's how it is in reality.

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‫However, since we assume that the plate is homogeneous, which means uniform in terms of mass distribution.

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‫So you have constant density, constant kilograms per meter cubed, meaning that this part of the plate

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‫is not heavier than this part of the plate, but the mass distribution is equal in all the locations

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‫of the plate.

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‫And this plate has all sides with equal length, then, for example, this side here has length L and

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‫also this side here has length L and the same thing here L and then this one here as well.

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‫L Then for modeling purposes, you take the total F G, which is five hundred Newtons, and you say

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‫that if this force vector acts through the center of mass, which in our case is the middle of the plate,

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‫let's say right here, then if this plate is a rigid body, then it has no difference whether you depict

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‫this case in terms of distributed force of gravity or equivalent force of gravity f g that goes through

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‫the center of mass of this plate.

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‫It makes no difference in terms of what kind of behavior your mathematical model will predict.

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‫No difference whatsoever.

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‫It's just easier to model things with one force going through one specific point, like in this case

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‫here s.m, but it's an equivalent situation.

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‫Hence I'm using the word equivalent force vector going through the center of mass in the case of this

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‫drone and also in the case of this plate, careful, though, these two representations are true for

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‫rigid bodies.

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‫Only if you remove this rigid body assumption or constraint however you want to call it, you are allowing

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‫this plate to bend and it will bend differently when it is subjected to a distributers force compared

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‫to a point force.

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‫But that's more for structural engineers to worry about.

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‫So I just wanted to clarify this point.

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‫If your plate is rigid, then this representation and this representation, they're equivalent.

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‫They will behave in the same way.

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‫However, if they can bend, then they will bend differently.

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‫But in our course, we don't worry about bending.

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‫So that's your lamda gravity here.

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‫So the question is, once the drones force of gravity, well, you know, that force of gravity equals

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‫M times G, right?

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‫So here is your exercise.

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‫How would lamda G in the body frame look like as a six by one vector?

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‫Again, avoid any lengthy calculations?

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‫It is a one minute exercise and that's it.

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‫Try it and I will show you the solution in the next video.

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‫So essentially, if you know that F G equals M times G, right.

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‫And you know that the force of gravity points down in the negative Z direction, then how would you

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‫rewrite this vector as a six by one vector?

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‫How would it look like?

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‫See you in the next video.

