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‫Welcome back.

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‫And now let's just sum up all these moments together and we will get a total moment that is induced

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‫from the gyroscopic effect.

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‫Well, that's called this moment.

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‫M sup g r like this.

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‫The moment induced from gyroscopic effect.

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‫It equals this moment from and won, so the moment induced from the gyroscopic effect, thanks to more

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‫one.

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‫Plus, the gyroscopic moment from model two, from model three.

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‫And from more for and of course, we can rewrite it like this as well.

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‫This is from model one.

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‫This is this one.

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‫This is from one or two.

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‫So this one here.

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‫This is from Morrisroe, so this one here, and this is from Moore for so it's this one here.

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‫So what we're going to do now, we're going to sum up the first elements of each vector and let's see

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‫what we're going to get from each vector.

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‫We will take the first element and then we're going to sum them up.

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‫So this will be from here.

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‫This comes from here.

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‫This comes from here and this comes from here.

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‫You can factor out queue times GTP, because they are present in every term, then this entire thing

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‫will look like this queue times, GTP Times and in the parentheses you have Omegle one minus Omega two

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‫plus omega three and minus Omega four.

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‫So you have simply factored out queue times GTP and that's what you get.

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‫And now look at this.

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‫What is this?

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‫Well, it's the same thing like this one here.

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‫It's the toll, some of the angle of velocities of all the propellers, so this is your total omega.

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‫So you can actually write it down like this.

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‫Q Times Jay t.P times, the summation sign from K equals one to four and then you're going to have minus

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‫one to the power of K plus one and Omega K.

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‫It makes sense, right?

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‫This part is this part and so when you're K equals one then it would be minus one one plus one and then

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‫Omega one.

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‫So you will have an even power here which is two.

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‫So this minus one becomes a plus one like this and then is just going to be omega one, which is a positive

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‫Omega, which is what you have over here.

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‫However, if your key is to then it would be minus one to plus one and then omega two.

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‫So you will have an odd power here, minus one to the power of three.

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‫Omega two.

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‫And minus one to the power of three will give you minus one and then omega two, and that's what you

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‫have over here.

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‫And the same thing applies when K equals three, then this will become four, so you will have a positive

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‫sign here times omega three, which is this case here.

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‫And of course, if you're case for, then you would have five here.

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‫So you will have an all power.

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‫So you will have minus omega four.

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‫So you can write it down like this, or you can very simply write down this thing like this, Queue

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‫Times, Jessopp, Teep Times or Mega.

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‫And so again, this mega is your total angular velocity vector when you sum up all the angles, velocities

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‫of your propeller's.

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‫So in the code, you can first perform this operation and then what you get here, it will go here,

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‫which is what I did in the code, and now we're going to do the exact same thing for the second elements

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‫of all these four vectors.

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‫So first we take this, which is this one.

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‫Then we take this, which is this one here, then we take this one, which is this element here, and

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‫then we take this element, which is this one here.

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‫And now we're going to factor it out like this, minus P times, Jayce up top.

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‫And again, you will have Omegle one minus Omeonga two plus Omega three and minus Omega four like this.

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‫Again, this entire thing is just an amalgam which we have over here.

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‫And so that will be your final answer for the second elements.

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‫If you sum them all up and if you sum up all the elements in the third element, then it will just be

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‫zero.

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‫And so that means that your total gyroscopic moment m sup g r equals Q Times GTP Times Omega, which

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‫is the total omega, the sum of all the angular velocities of all the propeller's minus P GTP times,

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‫the total Omega and zero.

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‫And the units of course are Knewton meters.

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‫And now the final step that we have to do, we have to put this gyroscopic moment into our force and

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‫moment vector, let's call it Lunda in the body frame and are so gyroscopic force and movement vector.

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‫So why don't you do it yourself?

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‫And then in the next video, I will do it for you.

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‫Thank you very much.

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‫And see you there.

