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‫Welcome back.

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‫So let's go back to our airfoil here.

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‫Your task was to find the D.H as a function of diesel and in the way you do it is like this.

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‫To get the horizontal component of this vector.

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‫In other words, to get this component here, you simply have to multiply your Deedes times cosine phi

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‫like this.

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‫And to get the horizontal component of the DL vector, well, for that you have to take your DL and

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‫you have to multiply by Sine and Phi and that's when you will get this component here and then you will

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‫add them together and that will be your D.H force vector.

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‫So, again, this is the top few of your blade.

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‫This blade is rotating at an omega radians per second.

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‫This is your differential airfoil element, this is your D.H force factor, which is this one here,

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‫and then the distance from the center of rotation till this D.H vector.

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‫That's what we're going to call an R.

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‫Since we had a small fire angle approximation here, we could say that our sign five would be simply

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‫a fire and then our cosine PHI would be one.

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‫That means that this D.H vector will be DL Times PHY and plus the D, and by the way, the width of

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‫the airfoil is the R and in order to get our differential air resistance moment dequeue, we would have

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‫this formula d.h, which is this one times the distance from the center of rotation to the airfoil.

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‫So times are.

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‫Or you can simply rewrite this equation like this, where this part here, that's this part here.

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‫So that's your differential moment due to air resistance because your blade is rotating at Omega radians

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‫per second.

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‫And now from the previous videos, you know what our differential lift and differential drag was?

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‫Just to be clear, D.H is in Newtons and dequeue is in Newton meters.

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‫And so now we are going to rewrite this dequeue in this way so you can write it out like this.

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‫This portion here.

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‫That would be.

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‫DL Times, Sefi, and this portion here would be your DEEDI and that are here, that's, of course your

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‫aunt here.

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‫That's the distance.

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‫You can do some factoring and you'll end up in this form here.

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‫And note that now I've put this R into the brackets.

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‫So that's why now instead of R squared, you have R cubed here and now in order to get our total q our

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‫total air resistance moment, we have to consider each infinitesimal airfoil on this blade.

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‫So we have to integrate this thing from zero up until Capital R, so this side will be from zero to

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‫Q and this one from zero to R meters.

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‫So as your R goes from zero meters to capital R meters, you take each differential airfoil element

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‫on this blade.

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‫You compute the differential moment for the specific blade and then you move onto the next differential

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‫blade and then as you scan through the blade, you will add them all up continuously or accumulatively,

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‫which is essentially what an integral is.

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‫In other words, if you're D-R was here instead, then you would be computing the area under the curve

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‫of this function here.

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‫And that's integration.

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‫Now, in addition, since Armorer has two blades, then we're going to put two here in order to get

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‫the total air resistance moment for the entire model, taking into account both blades.

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‫So I'm just going to put here and one.

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‫If we do that, we can cancel out these TOS here.

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‫And so the left side will be queues up and one equals and then I'm going to take some stuff out of the

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‫integral, like we talked about before.

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‫So I'm going to take an Omega squared and the air density out of the integral and inside the integral.

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‫You will have everything else.

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‫And so this Kyuss up and one that's your total air resistance moment per motor with two blades.

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‫So simply a cube would be for one blade, but Kyuss up and one would be for one more with two blades.

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‫And now the moment that the drone applies to the motor is then like this.

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‫Ms.

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‫D m equals minus Q, sub M and remember this M sub D.M. and put one because it's four more one.

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‫That's your talk for M one.

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‫So your MS up D.M. one equals and I'm going to put here Omega squared and then I'm going to put here

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‫minus one, the air density.

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‫The integral C times are cubed, and then in the brackets you have the lift coefficient times PHI plus

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‫the drag coefficient and then these are your differential width of your airfoil.

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‫And why did I put this minus one here?

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‫Well, that's just to account for this thing, right?

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‫And now I'm just going to say that this entire thing here, it's C, sub Q and there you go, you now

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‫have an expression for the moment that is applied from the drone to the more.

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‫And you can also write it out like this, Ms.

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‫D.M. One equals CQ Times Omega squared, and since we're dealing with more one than this would be Omega

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‫one squared.

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‫And I should put here on one squared as well.

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‫And also here and even here.

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‫But here we just worked in general variables.

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‫So I'm just going to leave Omega's like this and again you can find this constant C subcu either by

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‫integrating these equations or people also determined it experimentally.

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‫This C subcu can be called a torque factor and this torque factor has a different value from the thrust

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‫factor that we had before C sub T..

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‫So these are two different things, but both total thrust promotor and told moment that is applied to

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‫the more by the drone.

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‫Both of them have Omega squared in it.

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‫So the thrust force was the thrust factor times omegle, one squared, and now the torque applied to

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‫the motor equals C subcu times omegle one squared.

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‫And now we can find our EUFOR and we're going to do that in the next video.

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‫So thank you very much.

