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missed spot in cleaning up latex
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examples/case_studies/ssm_hurricane_tracking.ipynb

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@@ -12641,10 +12641,22 @@
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"our state vector (in one dimension) \n",
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"\n",
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"$$\n",
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"x_{t} = \\begin{bmatrix}p(t) \\\\ v(t) \\\\ a(t) \\end{bmatrix} $$ and our ODE system becomes $$\\frac{d}{dt} \\begin{bmatrix}p(t) \\\\ v(t) \\\\a(t) \\end{bmatrix} = \\begin{bmatrix}v(t) \\\\ a(t) \\\\ 0 \\end{bmatrix}\n",
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"x_{t} = \\begin{bmatrix}p(t) \\\\ v(t) \\\\ a(t) \\end{bmatrix}\n",
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"$$ \n",
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"\n",
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"and our ODE system becomes \n",
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"\n",
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"$$\n",
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"\\frac{d}{dt} \\begin{bmatrix}p(t) \\\\ v(t) \\\\a(t) \\end{bmatrix} = \\begin{bmatrix}v(t) \\\\ a(t) \\\\ 0 \\end{bmatrix}\n",
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"$$\n",
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"\n",
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"Now we integrate our system over $\\Delta{t}$ and we have $$p(t + \\Delta{t}) = p(t) + \\int_{t}^{t + \\Delta{t}}v(t')dt'$$ assuming that the change in time is small and that the change in velocity is negligible we can approximate the integrals using the forward Euler method and get \n",
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"Now we integrate our system over $\\Delta{t}$ and we have \n",
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"\n",
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"$$\n",
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"p(t + \\Delta{t}) = p(t) + \\int_{t}^{t + \\Delta{t}}v(t')dt'\n",
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"$$ \n",
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"\n",
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"assuming that the change in time is small and that the change in velocity is negligible we can approximate the integrals using the forward Euler method and get \n",
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"\n",
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"$$\n",
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"p(t + \\Delta{t}) \\approx p(t) + v(t)\\Delta{t}\n",

examples/case_studies/ssm_hurricane_tracking.myst.md

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@@ -770,10 +770,22 @@ We can also derive the Newtonian equations of motion from a system of ordinary d
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our state vector (in one dimension)
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$$
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x_{t} = \begin{bmatrix}p(t) \\ v(t) \\ a(t) \end{bmatrix} $$ and our ODE system becomes $$\frac{d}{dt} \begin{bmatrix}p(t) \\ v(t) \\a(t) \end{bmatrix} = \begin{bmatrix}v(t) \\ a(t) \\ 0 \end{bmatrix}
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x_{t} = \begin{bmatrix}p(t) \\ v(t) \\ a(t) \end{bmatrix}
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$$
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and our ODE system becomes
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$$
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\frac{d}{dt} \begin{bmatrix}p(t) \\ v(t) \\a(t) \end{bmatrix} = \begin{bmatrix}v(t) \\ a(t) \\ 0 \end{bmatrix}
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$$
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Now we integrate our system over $\Delta{t}$ and we have $$p(t + \Delta{t}) = p(t) + \int_{t}^{t + \Delta{t}}v(t')dt'$$ assuming that the change in time is small and that the change in velocity is negligible we can approximate the integrals using the forward Euler method and get
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Now we integrate our system over $\Delta{t}$ and we have
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$$
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p(t + \Delta{t}) = p(t) + \int_{t}^{t + \Delta{t}}v(t')dt'
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$$
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assuming that the change in time is small and that the change in velocity is negligible we can approximate the integrals using the forward Euler method and get
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$$
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p(t + \Delta{t}) \approx p(t) + v(t)\Delta{t}

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