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Fig. 5

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Position vectors of dust source rM and spacecraft r (in spherical coordinates (rM, αM, ωM) and (r, α, ω), respectively), defined in the Suncentered system S (compare to Fig. 1). The particle velocity vector at the time of ejection (u, ψ, λM) is defined in the coordinate system S~$\[\tilde{S}\]$ with the z-axis aligned with the asteroid heliocentric radius-vector and the x-axis pointing toward the local north of the system S. The axes of the source-centered system A are co-directed with the axes of the system S~$\[\tilde{S}\]$. The inclined system A~$\[\tilde{A}\]$ is the system in which the distributions of the ejection direction can be described mathematically in a simple way.

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