fixed derivation of EKF propagation equations
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@ -382,29 +382,22 @@
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"\n",
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"$$\\begin{aligned}m &= f'(x=1.5) \\\\&= 2(1.5) - 2 \\\\&= 1\\end{aligned}$$ \n",
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"\n",
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"Linearizing systems of differential equations is similar. We linearize $f(\\mathbf x, \\mathbf u)$, and $h(\\mathbf x)$ by taking the partial derivatives of each to evaluate $\\mathbf A$ and $\\mathbf H$ at the point $\\mathbf x_t$ and $\\mathbf u_t$. We call the partial derivative of a matrix the [*Jacobian*](https://en.wikipedia.org/wiki/Jacobian_matrix_and_determinant). This gives us the the system dynamics matrix and measurement model matrix:\n",
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"Linearizing systems of differential equations is similar. We linearize $f(\\mathbf x, \\mathbf u)$, and $h(\\mathbf x)$ by taking the partial derivatives of each to evaluate $\\mathbf F$ and $\\mathbf H$ at the point $\\mathbf x_t$ and $\\mathbf u_t$. We call the partial derivative of a matrix the [*Jacobian*](https://en.wikipedia.org/wiki/Jacobian_matrix_and_determinant). This gives us the the discrete state transition matrix and measurement model matrix:\n",
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"\n",
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"$$\n",
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"\\begin{aligned}\n",
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"\\mathbf A \n",
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"\\mathbf F \n",
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"&= {\\frac{\\partial{f(\\mathbf x_t, \\mathbf u_t)}}{\\partial{\\mathbf x}}}\\biggr|_{{\\mathbf x_t},{\\mathbf u_t}} \\\\\n",
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"\\mathbf H &= \\frac{\\partial{h(\\bar{\\mathbf x}_t)}}{\\partial{\\bar{\\mathbf x}}}\\biggr|_{\\bar{\\mathbf x}_t} \n",
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"\\end{aligned}\n",
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"$$\n",
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"\n",
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"Finally, we find the discrete state transition matrix $\\mathbf F$ by using the Taylor series expansion of $e^{\\mathbf A \\Delta t}$:\n",
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"\n",
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"$$\\mathbf F = e^{\\mathbf A\\Delta t} = \\mathbf{I} + \\mathbf A\\Delta t + \\frac{(\\mathbf A\\Delta t)^2}{2!} + \\frac{(\\mathbf A\\Delta t)^3}{3!} + ... $$\n",
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"\n",
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"Alternatively, you can use one of the other techniques we learned in the **Kalman Math** chapter. \n",
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"\n",
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"This leads to the following equations for the EKF. I put boxes around the differences from the linear filter:\n",
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"\n",
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"$$\\begin{array}{l|l}\n",
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"\\text{linear Kalman filter} & \\text{EKF} \\\\\n",
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"\\hline \n",
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"& \\boxed{\\mathbf A = {\\frac{\\partial{f(\\mathbf x_t, \\mathbf u_t)}}{\\partial{\\mathbf x}}}\\biggr|_{{\\mathbf x_t},{\\mathbf u_t}}} \\\\\n",
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"& \\boxed{\\mathbf F = e^{\\mathbf A \\Delta t}} \\\\\n",
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"& \\boxed{\\mathbf F = {\\frac{\\partial{f(\\mathbf x_t, \\mathbf u_t)}}{\\partial{\\mathbf x}}}\\biggr|_{{\\mathbf x_t},{\\mathbf u_t}}} \\\\\n",
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"\\mathbf{\\bar x} = \\mathbf{Fx} + \\mathbf{Bu} & \\boxed{\\mathbf{\\bar x} = f(\\mathbf x, \\mathbf u)} \\\\\n",
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"\\mathbf{\\bar P} = \\mathbf{FPF}^\\mathsf{T}+\\mathbf Q & \\mathbf{\\bar P} = \\mathbf{FPF}^\\mathsf{T}+\\mathbf Q \\\\\n",
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"\\hline\n",
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