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‫Welcome back.

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‫So let's now quantify the gyroscopic effect for our drone, so this is our drone here and one has a

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‫positive angular rotation.

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‫Also M3 and then M2 has a negative angular rotation and also in four has a negative angular rotation,

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‫Omega four.

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‫So before we quantify the gyroscopic effect, let's define a quantity called total angular velocity

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‫of the propellers and let's just name it Omega.

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‫And then we say that Omega equals omega one, minus Omega two, plus omega three and minus Omega four.

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‫That's how you add the angular velocities of M one and two and three and four, respectively.

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‫Note that you have to put minus signs in front of Omega two and Omega four because according to the

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‫right hand rule, they are negative.

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‫And so since Omega is our total angular velocity of the four murders, then, for example, if all of

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‫them rotate at 50 radians per second in terms of magnitude, then it would be 50 minus 50, plus 50

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‫and minus 50 equals zero radians per second.

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‫So that would be the total quantity of Omega.

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‫And remember, vector magnitudes are always positive.

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‫So, for example, if you have a vector that is, for example, minus three meters per second, then

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‫the magnitude of the vector still would be three meters per second because a magnitude doesn't care

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‫about the direction.

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‫A magnitude just tells you.

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‫The strength of the vector or in other words, the length of this vector of this arrow, next, let's

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‫write down the expression for the moment from the gyroscopic effect for each motor separately.

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‫In the previous example, we had this structure and our disk rotated like this.

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‫And then we rotated the entire structure like this at Alpha Dot radians per second.

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‫In other words, we describe the angular rotation of our entire structure with this angular velocity

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‫vector.

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‫So if you think in terms of a drone now, then how would you describe the rotation of its structure?

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‫Well, you can also use its angular velocities, right?

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‫The drone can rotate about its three body frame, axis X, Y and Z, and the rotation about these axis

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‫has some kind of angular velocity.

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‫And we had a vector to describe that.

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‫We had our angular velocity vector and it looked like this who had P, Q, R, radians per second.

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‫So instead of Alpha Dot, now we're going to have this vector here and instead of a disk rotation,

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‫we're going to have propellor rotations.

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‫So let's call the moment that we get from the gyroscopic effect, thanks to more one, let's call it

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‫like this m sup g r sub M one.

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‫So he stands for the gyroscopic moment for M one more and well, for this structure that we had before

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‫our moment equaled our Alpha Dot Cross H, which is the angular momentum of the disk.

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‫And now we simply have the angular velocity vector in the body frame across the more one angular momentum

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‫h sub M1.

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‫And just to be clear, this vector here, this is the angular velocity vector for the entire drone.

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‫It has P, Q and R radians per second.

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‫It's how the entire drone rotates.

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‫Like this, but this angular momentum vector, this only applies to more one.

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‫So it's this one here, each one you can rewrite this equation like this w in the body frame cross GTP

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‫P times Omega one, GTP is the rodders mass moment of inertia about its rotating axis.

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‫And the major one is the angular velocity of our rotor.

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‫And if you multiply them together, then you get the angular momentum of your M one.

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‫So that was for more one for motor two, it's similar MS up G.R. sub M2 equals the drones angle velocity

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‫in the body frame across H.

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‫Sub M2 or.

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‫W. in the body frame cross minus Jessopp T p times Omega two, and that's because four more to the angular

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‫momentum is negative.

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‫So that's the only difference.

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‫Then for motor three, it would be the following, the angular velocity vector cross the angular momentum

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‫vector for that Mowrer.

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‫And by the way, these are also vectors here.

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‫So I'm going to put arrows on top of the capital H and again W in the body frame cross J sup t p times

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‫Omega three and finally you have M sub, G.R. sub and four equals W in the body frame.

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‫Cross the angular momentum vector four and four equals.

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‫And guess what.

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‫Of course you're going to have minus J subtype times omega four.

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‫And now I'm going to give you an exercise to do you know that this W in the body frame vector is this

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‫one.

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‫You have PK, you are here.

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‫So what I would like you to do now, I would like you to find three by one vectors for each motor here

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‫like this.

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‫So I would like you to take this vector here and here and here and here, substitute them with P, Q,

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‫R and cross them with these things here and let's see what you're going to get as a product.

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‫So try and buy yourself and then I will show you the solution in the next video.

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‫Thank you very much.

