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‫Welcome back.

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‫Let's now substitute our fire and see tangles with zero radiance and see what we get.

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‫So if you have zero radiance here and zero radiance here, you know that you're sign the Zero and Tenjin

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‫zero, they will give you a zero element.

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‫So this entire thing will be zero.

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‫Cosine zero will give you one, but then Tenjin Zero will give you zero.

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‫So you will have one here, but you will have zero here.

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‫So one time zero, it will give you zero.

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‫And here, of course, this was zero and then this was zero.

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‫So you would have zero times zero, which would be zero.

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‫And then here five zero and cosine zero is one.

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‫Here you would have zero and minus sine zero will be zero.

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‫If I make this five zero and then this theta zero, then this numerator will be zero and then this denominator

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‫will be one.

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‫So zero divided by one will give you zero and then five equals zero and theta equals zero.

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‫So the numerator will be one because cosine zero is one and the same thing for the denominator.

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‫So you will have one over one, which means that this entire thing, this entire element will be one.

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‫And so that means that with this small angle assumption, your transfer matrix will become an identity

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‫matrix.

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‫And now something very interesting happens.

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‫This relation that you have here that relates the body frame, angular velocity's with the inertia frame,

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‫angular velocity is this a relationship will become like this.

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‫So you multiply an identity matrix by the body frame, angular velocities.

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‫And so if you write this equation out, then you will find that your Phi Dot, which is here, equals

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‫your P.

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‫Your seat that will equal your Q.

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‫And your side, that will equal or safai, that equals this one theater that equals this one and that

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‫equals this one.

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‫And then it is also logical that your fi double dot equals p dot theater, double dot equals your cute

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‫dot and then side double dot equals your R dot.

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‫And so then you can take these three states based equations here for the attitude.

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‫And you can replace all your PS Qs, R.

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‫S P dots, Q dots and R dots with these values here, and if you do that, then this is what you will

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‫get.

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‫You see, instead of P Q hours, you will have five dots, Seeta dots and side dots, and then instead

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‫of P does Q dots and or dots you will have five double dots, theta double doesn't side double dots.

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‫So just to be clear, these equations here are used only in the NPC controller.

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‫In the plant, you still use these original equations alongside with the transfer matrix where you did

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‫not have that PHI and Theta equals zero radians assumption, where you did not have that small angle

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‫approximation.

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‫So this entire form, these three equations here and then this transfer matrix relationship that would

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‫be in the plant still.

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‫But because in general, the financial tangles will be small throughout the entire maneuver, then because

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‫of this small angle approximation in the controller, in the NPC controller, we will use these equations.

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‫And the performance of the controller because of this assumption will not change significantly because,

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‫see, tangles throughout the maneuver will be small as they should be, because if they are not, then

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‫the U.S. simply won't be able to fly.

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‫Because the propellers of the oveI are not that powerful, that they would be able to produce enough

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‫vertical components thrust in order to counteract the force of gravity when you're fine and FITA angles

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‫are large.

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‫And also, if we think about it logically, then the feedback lionization controller shouldn't really

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‫give big theta reference angles to the NPC because if you're fired, see tangles are large, then you

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‫will have a very huge component in the horizontal direction.

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‫And then if you have some kind of trajectory that you want your you have to follow.

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‫Then with a large horizontal velocity, it will be difficult.

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‫You know, it might drift from the trajectory.

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‫Whenever there is a sharper turn, for example.

