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So let's have a look at the common of prediction step.

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So this is the first step we need to implement for the common Fiola.

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We begin the estimation step with the initial condition, it's not so this is going to be the best estimate

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of the initial state of the system in this step, we want to propagate the time forward to find the

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best estimate of the time.

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Step one, so we can use the state's best model of the system that we dropped before to predict forward

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what the new state of the system is going to be.

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So this is going to be the best estimate at time, zero multiplied by our state transition matrix,

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plus our control input at TimeStep zero time to control input matrix.

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And this is going to propagate the state forward tompsett one.

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Or in general we can write the equation out like so.

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So the current state estimate is going to be a function of the old state estimate and the old control

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input as well as the two state transition matrixes.

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So this forms of prediction, step of the time update, step of the common fiodor, we use a process

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model of the system we want to estimate to predict state forward.

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So this is basically shifting the main of the Gaussian probably doability distributions forward in time.

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So the equation here shown is the state prediction equation for the common field.

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OK, so now we've looked at the state transition, but we also want to propagate forward the covariance

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of the Gaussian probability distribution.

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So to do this, we begin with the initial estimate pay not so pay is the initial variance of the state

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estimate ignored.

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Now, if we have exact knowledge of the initial state of the system, then we can set pay ought to be

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equal to zero.

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So there's no uncertainty in the estimate.

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We know exactly.

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Exactly.

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If we have no knowledge of X axonal, well, then Peno is going to be turning towards a very large number

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to say that a very large uncertainty.

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But we usually know an approximate value or good assumption of the value of X not so we pay not to be

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the value of the estimated error.

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So now that we have Peno, we can propagate this incredible with time using the linear transformation

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that we've derived before.

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So basically we have our initial covariance.

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Pinart we have our state transmission matrix here and we multiply them out by this equation here to

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propagate the uncertainty forward in time.

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Now, this does not change the amount of uncertainty in the system.

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It just shifts it between the states as the dynamics of the system evolve.

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So the size of pea before and after the magnitude, the amount of uncertainty in between the two stays

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constant.

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So if you look at the process model, we can see that this equation up here is going to account for

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this function.

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This part of the process model is going to take into account the trans state transition, the transition

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of the state between tompsett came on this one and Tompsett K or between zero and one vacancy.

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Can we also have this other uncertainty in the Saudi system?

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So this is where the system process model noise comes in.

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We need to account for this new uncertainty in state due to this process model noise.

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So to account for this in the system, we can add a new covariance term.

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So you can see here this term here now calculates the answer, new uncertainty in the system due to

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the process of noise.

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So our key metrics, if you remember this, is the covariance of the process model noise el is the process,

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model noise, sensitivity matrixes.

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Now, usually we assume that the process model noise is an additive, which basically means that these

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matrices here are just identity.

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If we use this assumption, then we can simplify the equation down to this one chain here.

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So the covariance at times that one is going to be the variance that timestep zero propagated by the

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state transition matrix plus the additive process model noise que.

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So we can sum up the British concept of the common filter by using these equations here.

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So this first equation here looks at this transition.

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So this is the shifting the main of the galaxy in probability distribution of the estimated state.

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This down here is the covariance propagation.

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So this shifts the covariance of the probability distribution of the estimated state.

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So inside the British of the filter, we update the main.

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We update the covariance.

