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@ -26,7 +26,7 @@ Where $l^i(\cdot)$ represents the rate at which satellites are destroyed by coll
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Note that it is reasonable to assume that the loss of satellites to collisions should be
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increasing in the level of debris: $\parder{l^i}{D_t}{} >0$.
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\paragraph{Collision Efficiencies}
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\subsubsection{Collision Efficiencies}
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%TODO: Explain bit about constellation collision efficiencies.
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As demonstrated by \cite{reiland2020}, there are constellation designs by which an operator can
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minimize the risk of intra-constellation collisions.
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@ -41,25 +41,43 @@ are operated for different purposes and require different orbital properties.
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%This could be explained as Coordination across time (time travel doesn't exist yet)
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This coordination is also complicated by the fact that constellations are not
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designed nor launched at the same time.
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Thus although an operator may choos to minimize their total risk when launching
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a constellation, later constellation formation will often add to the total risk.
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It is important to note that satellite-on-satellite collisions are rare\footnote{
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I am only aware of one collision between satellites,
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and one of them was abandon at the time.\cref{ListOfOrbitalIncidents}
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}
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but this is due to the fact that satellites that evasive maneuvers are usually taken
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when collisions appear reasonably possible.
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Consequent to these reasons, I believe the loss function $l^i$ should have the following properties related
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to satellite stocks.
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Consequent to these reasons, I believe the loss function $l^i$ should have the
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following properties related to satellite stocks.
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\begin{align}
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\parder{l^i}{s^k_t}{} > 0 ~~\forall k \in \{1,\dots,N)\\
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\parder{l^i}{s^j_t}{} > \parder{l^i}{s^i_t}{} ~~\forall j\neq i
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\end{align}
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Notably, an additional satellite in any constellation increases the probability of loosing
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a satellite from a given constellation, and this risk is lower
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for the home of the additional satellite.
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\subsection{Debris}
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Debris is generated by various processes, including:
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\begin{itemize}
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\item Naturally occuring debris
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\item Naturally occuring debris is captured from interplanetary space.
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\item Satellite launches, operations, failures, or intentional destruction.
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\item Collisions between two satellites
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\item Collisions between a satellite and debris
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\item Collisions between pieces of debris
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\item Collisions between
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\begin{itemize}
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\item Two satellites
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\item A satellite and debris
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\item Two pieces of debris
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\end{itemize}
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all generate more debris.
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\end{itemize}
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Debris leaves orbit when atmospheric drag slows it down enough to reenter the atmosphere.
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It leaves orbit when atmospheric drag slows it down enough to reenter the atmosphere.
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Because the atmosphere is so negligible for many orbits, reentry can easily take decades
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or centuries.
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These effects can be represented by the following general law of motion.
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\begin{align}
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@ -68,10 +86,11 @@ These effects can be represented by the following general law of motion.
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For simplicity, I formulate this more specifically as:
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\begin{align}
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D_{t+1} = (1-\delta)D_t + g(D_t)
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+ \sum^N_{i=1} \gamma l^i(\{s^j_t\},D_t)
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+ \Gamma \sum^n_{j=1} \{x^j_t\}
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+ \sum^N_{i=1} \vec \gamma l^i(\{s^j_t\},D_t)
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+ \vec \Gamma \sum^n_{j=1} \{x^j_t\}
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\end{align}
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where $\Gamma,\gamma$ represent the debris generated by each launch and collision respectively,
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where $\vec \Gamma,\vec \gamma$ represent the debris generated by each
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launch and collision respectively,
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while $\delta,g(\cdot)$ represent the decay rate of debris and the
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autocatalysis\footnote{
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Using terminology from \cite(RaoRondina2020).
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