parent
31bf4b38ca
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@ -1,5 +1,5 @@
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#LyX 2.1 created this file. For more info see http://www.lyx.org/
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\lyxformat 474
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#LyX 2.0 created this file. For more info see http://www.lyx.org/
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\lyxformat 413
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\begin_document
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\begin_header
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\textclass article
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@ -12,13 +12,13 @@
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\font_roman default
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\font_sans default
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\font_typewriter default
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\font_math auto
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\font_default_family default
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\use_non_tex_fonts false
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\font_sc false
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\font_osf false
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\font_sf_scale 100
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\font_tt_scale 100
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\graphics default
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\default_output_format default
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\output_sync 0
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@ -29,24 +29,15 @@
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\use_hyperref false
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\papersize default
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\use_geometry true
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\use_package amsmath 1
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\use_package amssymb 1
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\use_package cancel 1
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\use_package esint 1
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\use_package mathdots 1
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\use_package mathtools 1
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\use_package mhchem 1
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\use_package stackrel 1
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\use_package stmaryrd 1
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\use_package undertilde 1
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\use_amsmath 1
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\use_esint 1
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\use_mhchem 1
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\use_mathdots 1
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\cite_engine basic
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\cite_engine_type default
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\biblio_style plain
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\use_bibtopic false
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\use_indices false
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\paperorientation portrait
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\suppress_date false
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\justification true
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\use_refstyle 1
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\index Index
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\shortcut idx
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@ -253,7 +244,7 @@ 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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\begin_inset Formula
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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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\end_inset
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@ -611,7 +602,7 @@ key "Iserles00an"
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,
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\begin_inset Formula
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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_inset
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@ -956,8 +947,8 @@ Or, as another way to state this, if we solve the differential equations
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\begin_inset Formula
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\begin{eqnarray*}
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\dot{\theta}(t) & = & H(\theta)^{-1}\,\omega^{b}(t)\\
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\dot{p}(t) & = & R_{0}^{T}\,V_{0}+v(t)\\
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\dot{v}(t) & = & R_{0}^{T}\,g+R_{b}^{0}(t)a^{b}(t)
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\dot{p}(t) & = & R_{0}^{T}\, V_{0}+v(t)\\
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\dot{v}(t) & = & R_{0}^{T}\, g+R_{b}^{0}(t)a^{b}(t)
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\end{eqnarray*}
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\end_inset
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@ -1024,7 +1015,7 @@ v(t)=v_{g}(t)+v_{a}(t)
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evolving as
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\begin_inset Formula
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\begin{eqnarray*}
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\dot{v}_{g}(t) & = & R_{i}^{T}\,g\\
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\dot{v}_{g}(t) & = & R_{i}^{T}\, g\\
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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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@ -1050,7 +1041,7 @@ p(t)=p_{i}(t)+p_{g}(t)+p_{v}(t)
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evolving as
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\begin_inset Formula
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\begin{eqnarray*}
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\dot{p}_{i}(t) & = & R_{i}^{T}\,V_{i}\\
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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_{i}^{T}gt\\
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\dot{p}_{v}(t) & = & v_{a}(t)
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\end{eqnarray*}
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@ -1105,7 +1096,7 @@ Predict the NavState
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from
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\begin_inset Formula
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\[
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X_{j}=\mathcal{R}_{X_{i}}(\zeta(t_{ij}))=\left\{ \Phi_{R_{0}}\left(\theta(t_{ij})\right),P_{i}+V_{i}t_{ij}+\frac{gt_{ij}^{2}}{2}+R_{i}\,p_{v}(t_{ij}),V_{i}+gt_{ij}+R_{i}\,v_{a}(t_{ij})\right\}
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X_{j}=\mathcal{R}_{X_{i}}(\zeta(t_{ij}))=\left\{ \Phi_{R_{0}}\left(\theta(t_{ij})\right),P_{i}+V_{i}t_{ij}+\frac{gt_{ij}^{2}}{2}+R_{i}\, p_{v}(t_{ij}),V_{i}+gt_{ij}+R_{i}\, v_{a}(t_{ij})\right\}
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\]
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\end_inset
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@ -1381,7 +1372,7 @@ B_{k}=\left[\begin{array}{c}
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0_{3\times3}\\
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R_{k}\frac{\Delta_{t}}{2}^{2}\\
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R_{k}\Delta_{t}
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\end{array}\right],\,\,\,\,C_{k}=\left[\begin{array}{c}
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\end{array}\right],\,\,\,\, C_{k}=\left[\begin{array}{c}
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H(\theta_{k})^{-1}\Delta_{t}\\
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0_{3\times3}\\
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0_{3\times3}
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@ -1391,147 +1382,6 @@ H(\theta_{k})^{-1}\Delta_{t}\\
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\end_inset
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\end_layout
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\begin_layout Subsubsection*
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Units
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\end_layout
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\begin_layout Standard
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The units of the IMU are as follows:
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\end_layout
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\begin_layout Standard
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\begin_inset Tabular
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<lyxtabular version="3" rows="5" columns="2">
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<features rotate="0" tabularvalignment="middle">
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<column alignment="center" valignment="top">
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<column alignment="center" valignment="top">
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<row>
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<cell alignment="center" valignment="top" topline="true" bottomline="true" leftline="true" usebox="none">
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\begin_inset Text
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\begin_layout Plain Layout
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Parameter
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\end_layout
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\end_inset
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</cell>
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<cell alignment="center" valignment="top" topline="true" bottomline="true" leftline="true" rightline="true" usebox="none">
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\begin_inset Text
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\begin_layout Plain Layout
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Units
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\end_layout
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\end_inset
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</cell>
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</row>
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<row>
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<cell alignment="center" valignment="top" topline="true" leftline="true" usebox="none">
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\begin_inset Text
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\begin_layout Plain Layout
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gyro_noise_sigma
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\end_layout
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\end_inset
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</cell>
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<cell alignment="center" valignment="top" topline="true" leftline="true" rightline="true" usebox="none">
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\begin_inset Text
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\begin_layout Plain Layout
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\begin_inset Formula $rad/s/\sqrt{Hz}$
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\end_inset
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\end_layout
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\end_inset
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</cell>
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</row>
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<row>
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<cell alignment="center" valignment="top" topline="true" leftline="true" usebox="none">
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\begin_inset Text
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\begin_layout Plain Layout
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accel_noise_sigma
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\end_layout
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\end_inset
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</cell>
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<cell alignment="center" valignment="top" topline="true" leftline="true" rightline="true" usebox="none">
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\begin_inset Text
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\begin_layout Plain Layout
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\begin_inset Formula $m/s^{2}/\sqrt{Hz}$
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\end_inset
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\end_layout
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\end_inset
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</cell>
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</row>
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<row>
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<cell alignment="center" valignment="top" topline="true" leftline="true" usebox="none">
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\begin_inset Text
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\begin_layout Plain Layout
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gyro_bias_rw_sigma
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\end_layout
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\end_inset
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</cell>
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<cell alignment="center" valignment="top" topline="true" leftline="true" rightline="true" usebox="none">
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\begin_inset Text
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\begin_layout Plain Layout
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\begin_inset Formula $rad/s$
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\end_inset
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or
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\begin_inset Formula $rad\sqrt{Hz}/s$
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\end_inset
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\end_layout
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\end_inset
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</cell>
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</row>
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<row>
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<cell alignment="center" valignment="top" topline="true" bottomline="true" leftline="true" usebox="none">
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\begin_inset Text
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\begin_layout Plain Layout
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accel_bias_rw_sigma
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\end_layout
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\end_inset
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</cell>
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<cell alignment="center" valignment="top" topline="true" bottomline="true" leftline="true" rightline="true" usebox="none">
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\begin_inset Text
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\begin_layout Plain Layout
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\begin_inset Formula $m/s^{2}$
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\end_inset
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or
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\begin_inset Formula $m\sqrt{Hz}/s^{2}$
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\end_inset
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\end_layout
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\end_inset
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</cell>
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</row>
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</lyxtabular>
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\end_inset
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\end_layout
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\begin_layout Standard
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