<<

46th Lunar and Planetary Science Conference (2015) 2467.pdf

OORT CLOUD ENCOUNTERS WITH MARS, , AND MERCURY. Renu Mal- hotra (Lunar and Planetary Laboratory, The University of Arizona, Tucson, AZ 85721; [email protected])

Introduction: The close encounter of Mars with an comet Siding Spring C/2013 A1 on Oc- tober 19, 2014 was of great interest for its transient and

long term effects on the planet’s atmosphere. What is Mars the frequency of such events in the inner ? 0.03 A rough estimate for the mean time between encoun- Earth ters of parabolic with terrestrial planets – Mars, Venus Earth, Venus and Mercury – is obtained here. 0.02 Parabolic comet encounter frequency: Oort Mercury Cloud comets (also known as ‘long period comets’ or

‘new comets’) in the inner solar system have a nearly 0.01 isotropic distribution of orbital planes, nearly parabolic orbits, and an approximately uniform distribution of perihelion distances; the rate of new parabolic comets (of absolute magnitude brighter than about 10) entering 0 the Earth’s orbit is approximately 3 per 4 years [1]. 0 50 100 encounter velocity (km/s) From these observations, we can estimate that the rate of such comets crossing Mars’ orbit is approximately 1.14 per year. The mean residence time of such para- Figure 1. Distribution of encounter velocities of para- bolic comets within Mars' orbit is about 0.34 years. bolic comets with Mars (red curve), with Earth (green This yields the steady state number of parabolic com- curve), with Venus (magenta) and with Mercury (blue ets within 1.52 AU of the of about 0.39. There- curve). We approximate the orbits of the planets as fore, the steady-state number density of parabolic circular orbits. comets in Mars crossing orbits is about 0.026 per cubic AU; we will denote this by �. The relative velocity during a Mars' encounter of such parabolic comets is approximately in the range of 20-60 km s-1 (see Figure 1000

1). We can estimate the mean time between encounters 100 by imagining that such comets appear randomly in the 10 space near Mars, with a mean speed V = 40 km s-1 rela- tive to Mars. Then the mean time between encounters 1 2 at flyby distances up to d is given by T♂(d) ≈ 1/(�d V�) 0.1 6 5 -2 ≈ 3.3x10 yr (d/10 km) (see Figure 2). For Siding 0.01 Spring C/2013’s flyby distance (d ≈ 140,000 km), the mean time of encounters is ~1.7 myr. 0.001 0.0001 For Earth, Venus and Mercury, a similar calcula- tion finds that the mean time for encounters with para- bolic comets is 2.1 myr x (d/105 km)-2, 1.5 myr x (d/105 0.1 1 10 100 1000 -2 5 -2 km) , 0.8 myr (d/10 km) , respectively (see Figure d / 100,000 km 2).

Figure 2. The mean time of encounters of parabolic Comet tail lengths typically exceed 106 km. Para- comets as a function of encounter distance with Mars bolic comet encounters with the terrestrial planets, (red curve), with Earth (green curve), with Venus (ma- with flyby distances of less than 106 km, occur with a genta) and with Mercury (blue curve). The Mars en- frequency of about one per ten thousand years. counter distance of Siding Spring C/2013 A1 is indi- cated by the vertical dotted line. 46th Lunar and Planetary Science Conference (2015) 2467.pdf

Encounters with periodic, ‘short period’ comets (including the so-called Jupiter-family comets and Hal- ley family comets) require different considerations than presented above: periodic comets are rather more predictable than the random, unpredictable encounters with long period comets.

References: [1] Fernandez, J., Comets - Nature, Dynamics, Origin and their Cosmological Relevance, Astrophysics Space Science Library, volume 328, Springer, Dordrecht (2005).