Some refactoring
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@ -245,7 +245,7 @@ X(t)=\left\{ R_{0},P_{0}+V_{0}t,V_{0}\right\}
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then the differential equation describing the trajectory is
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then the differential equation describing the trajectory is
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\begin_inset Formula
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\begin_inset Formula
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\[
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\[
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\dot{X}(t)=\left[0_{3x3},V_{0},0_{3x1}\right],\,\,\,\,\,X(0)=\left\{ R_{0},P_{0},V_{0}\right\}
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\dot{X}(t)=\left[0_{3x3},V_{0},0_{3x1}\right],\,\,\,\,\, X(0)=\left\{ R_{0},P_{0},V_{0}\right\}
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\]
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\]
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\end_inset
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\end_inset
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@ -591,7 +591,7 @@ key "Iserles00an"
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,
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,
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\begin_inset Formula
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\begin_inset Formula
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\begin{equation}
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\begin{equation}
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\dot{R}(t)=F(R,t),\,\,\,\,R(0)=R_{0}\label{eq:diffSo3}
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\dot{R}(t)=F(R,t),\,\,\,\, R(0)=R_{0}\label{eq:diffSo3}
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\end{equation}
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\end{equation}
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\end_inset
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\end_inset
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@ -962,20 +962,22 @@ Application: The New IMU Factor
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\end_layout
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\end_layout
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\begin_layout Standard
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\begin_layout Standard
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The above scheme suffers from one problem, which is that
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In the IMU factor, we need to predict the NavState
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\begin_inset Formula $R_{0}$
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\begin_inset Formula $X_{j}$
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\end_inset
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\end_inset
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needs to be known exactly to compensate for the initial velocity
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from the current NavState
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\begin_inset Formula $V_{0}$
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\begin_inset Formula $X_{i}$
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\end_inset
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\end_inset
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and the gravity
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and the IMU measurements in-between.
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\begin_inset Formula $g$
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The above scheme suffers from a problem, which is that
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\begin_inset Formula $X_{i}$
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\end_inset
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\end_inset
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.
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needs to be known in order to compensate properly for the initial velocity
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Hence, we split up
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and rotated gravity vector.
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Hence, the idea of Lupton was to split up
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\begin_inset Formula $v(t)$
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\begin_inset Formula $v(t)$
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\end_inset
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\end_inset
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@ -990,14 +992,14 @@ v(t)=v_{g}(t)+v_{a}(t)
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evolving as
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evolving as
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\begin_inset Formula
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\begin_inset Formula
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\begin{eqnarray*}
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\begin{eqnarray*}
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\dot{v}_{g}(t) & = & R_{0}^{T}\, g\\
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\dot{v}_{g}(t) & = & R_{i}^{T}\, g\\
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\dot{v}_{a}(t) & = & R_{b}^{0}(t)a^{b}(t)
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\dot{v}_{a}(t) & = & R_{b}^{i}(t)a^{b}(t)
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\end{eqnarray*}
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\end{eqnarray*}
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\end_inset
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\end_inset
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The solution for the first equation is simply
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The solution for the first equation is simply
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\begin_inset Formula $v_{g}(t)=R_{0}^{T}gt$
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\begin_inset Formula $v_{g}(t)=R_{i}^{T}gt$
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\end_inset
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\end_inset
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.
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.
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@ -1008,7 +1010,7 @@ The solution for the first equation is simply
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up in three parts
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up in three parts
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\begin_inset Formula
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\begin_inset Formula
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\[
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\[
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p(t)=p_{0}(t)+p_{g}(t)+p_{v}(t)
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p(t)=p_{i}(t)+p_{g}(t)+p_{v}(t)
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\]
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\]
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\end_inset
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\end_inset
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@ -1016,8 +1018,8 @@ p(t)=p_{0}(t)+p_{g}(t)+p_{v}(t)
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evolving as
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evolving as
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\begin_inset Formula
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\begin_inset Formula
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\begin{eqnarray*}
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\begin{eqnarray*}
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\dot{p}_{0}(t) & = & R_{0}^{T}\, V_{0}\\
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\dot{p}_{i}(t) & = & R_{i}^{T}\, V_{i}\\
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\dot{p}_{g}(t) & = & v_{g}(t)=R_{0}^{T}gt\\
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\dot{p}_{g}(t) & = & v_{g}(t)=R_{i}^{T}gt\\
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\dot{p}_{v}(t) & = & v_{a}(t)
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\dot{p}_{v}(t) & = & v_{a}(t)
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\end{eqnarray*}
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\end{eqnarray*}
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@ -1026,8 +1028,8 @@ evolving as
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Here the solutions for the two first equations are simply
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Here the solutions for the two first equations are simply
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\begin_inset Formula
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\begin_inset Formula
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\begin{eqnarray*}
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\begin{eqnarray*}
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p_{0}(t) & = & R_{0}^{T}V_{0}t\\
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p_{i}(t) & = & R_{i}^{T}V_{i}t\\
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p_{g}(t) & = & R_{0}^{T}\frac{gt^{2}}{2}
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p_{g}(t) & = & R_{i}^{T}\frac{gt^{2}}{2}
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\end{eqnarray*}
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\end{eqnarray*}
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\end_inset
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\end_inset
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@ -1038,7 +1040,7 @@ The recipe for the IMU factor is then, in summary.
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\begin{eqnarray*}
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\begin{eqnarray*}
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\dot{\theta}(t) & = & H(\theta(t))^{-1}\,\omega^{b}(t)\\
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\dot{\theta}(t) & = & H(\theta(t))^{-1}\,\omega^{b}(t)\\
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\dot{p}_{v}(t) & = & v_{a}(t)\\
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\dot{p}_{v}(t) & = & v_{a}(t)\\
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\dot{v}_{a}(t) & = & R_{b}^{0}(t)a^{b}(t)
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\dot{v}_{a}(t) & = & R_{b}^{i}(t)a^{b}(t)
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\end{eqnarray*}
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\end{eqnarray*}
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\end_inset
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\end_inset
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@ -1048,14 +1050,14 @@ starting from zero, up to time
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\end_inset
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\end_inset
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, where
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, where
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\begin_inset Formula $R_{b}^{0}(t)=\exp\Skew{\theta(t)}$
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\begin_inset Formula $R_{b}^{i}(t)=\exp\Skew{\theta(t)}$
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\end_inset
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\end_inset
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at all times.
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at all times.
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Form the local coordinate vector as
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Form the local coordinate vector as
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\begin_inset Formula
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\begin_inset Formula
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\[
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\[
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\zeta(t_{ij})=\left[\theta(t_{ij}),p(t_{ij}),v(t_{ij})\right]=\left[\theta(t_{ij}),R_{0}^{T}V_{0}t_{ij}+R_{0}^{T}\frac{gt_{ij}^{2}}{2}+p_{v}(t_{ij}),R_{0}^{T}gt_{ij}+v_{a}(t_{ij})\right]
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\zeta(t_{ij})=\left[\theta(t_{ij}),p(t_{ij}),v(t_{ij})\right]=\left[\theta(t_{ij}),R_{i}^{T}V_{i}t_{ij}+R_{i}^{T}\frac{gt_{ij}^{2}}{2}+p_{v}(t_{ij}),R_{i}^{T}gt_{ij}+v_{a}(t_{ij})\right]
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\]
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\]
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\end_inset
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\end_inset
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@ -1071,7 +1073,7 @@ Predict the NavState
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from
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from
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\begin_inset Formula
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\begin_inset Formula
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\[
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\[
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X_{j}=\mathcal{R}_{X_{j}}(\zeta(t_{ij}))=\left\{ \Phi_{R_{0}}\left(\theta(t_{ij})\right),P_{0}+V_{0}t_{ij}+\frac{gt_{ij}^{2}}{2}+R_{0}\, p_{v}(t_{ij}),V_{0}+gt_{ij}+R_{0}\, v_{a}(t_{ij})\right\}
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X_{j}=\mathcal{R}_{X_{j}}(\zeta(t_{ij}))=\left\{ \Phi_{R_{0}}\left(\theta(t_{ij})\right),P_{i}+V_{i}t_{ij}+\frac{gt_{ij}^{2}}{2}+R_{i}\, p_{v}(t_{ij}),V_{i}+gt_{ij}+R_{i}\, v_{a}(t_{ij})\right\}
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\]
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\]
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\end_inset
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\end_inset
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@ -1079,6 +1081,30 @@ X_{j}=\mathcal{R}_{X_{j}}(\zeta(t_{ij}))=\left\{ \Phi_{R_{0}}\left(\theta(t_{ij}
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\end_layout
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\end_layout
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\begin_layout Standard
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Note that the predicted NavState
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\begin_inset Formula $X_{j}$
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\end_inset
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depends on
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\begin_inset Formula $X_{i}$
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\end_inset
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, but the inrgrated quantities
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\begin_inset Formula $\theta(t)$
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\end_inset
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,
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\begin_inset Formula $p_{i}(t)$
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\end_inset
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, and
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\begin_inset Formula $v_{a}(t)$
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\end_inset
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do not.
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\end_layout
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\begin_layout Subsubsection*
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\begin_layout Subsubsection*
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A Simple Euler Scheme
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A Simple Euler Scheme
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\end_layout
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\end_layout
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@ -1109,6 +1135,27 @@ where
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.
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.
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\end_layout
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\end_layout
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\begin_layout Standard
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In the above, we have to think about how to handle both bias
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\begin_inset Formula $(b_{g},b_{a})$
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\end_inset
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and lever arm
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\begin_inset Formula $T_{s}^{b}$
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\end_inset
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.
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Both of them can be seen as arguments to two functions
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\begin_inset Formula $\omega_{k}^{b}(b_{g})$
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\end_inset
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and
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\begin_inset Formula $a_{k}^{b}(b_{a},T_{s}^{b})$
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\end_inset
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, and hence we have to properly account for their derivatives.
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\end_layout
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\begin_layout Section
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\begin_layout Section
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Old Stuff:
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Old Stuff:
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\end_layout
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\end_layout
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