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Sunday, May 24, 2020

comet P/2019 LD2 (ATLAS)

In this mpml message, Sam Deen pointed out that this asteroid in not a Jupyter Troian  but probably a 4-8 km size long period comet that in February 2017 achieved a perihelium low enough to start outgassing .
In this simulation, Tony Dunn confirmed that 2019 LD2 is not a Troian, Greek or Hilda but a comet that regulary makes very close passed to Jupiter and Saturn.

In fact, the object has now been given a cometary designation P/2019 LD2 (ATLAS)

For what's worth due to the uncertainty, I also tried a couple of day ago  to see when the comet entered the solar system assuming a conventional distance greater than 100 au .

I simulated 100 clones in the past 280K years (Mercury6 software by John E. Chambers - Bulirsch-Stoer integration, intial timestep 0.05 days).
Clones  Target
mean sd   mean sd
q 4.57802477541 1.671146e-05   4.57801992309 1.6782e-05
e 0.13528015709 9.88572e-06   0.13527811197 9.8665e-06
i 11.55192320685 1.746557e-05   11.55192194572 1.7512e-05
peri 123.44833869054 0.00209362353   123.44893096687 0.0021043
node 179.74537221523 0.00017704315   179.74536895343 0.00017777
tp 2458949.96748775 0.01979864266   2458949.97292011 0.01993
**In the meantime, the nominal parameters have been updated but I hope that this does not radically change the macroscopic behaviour.

The nominal comet entered the solar system about 32K years ago, while the most recent date for a clone to enter the solar system was about 4K years ago.

This is the overall time distribution (being a backward simulation, the clones are "ejected" from the point of view of the simulator...):


At first glance, it seemed to me that some clones entered the solar system on a hyperbolic trajectory (total energy > 0) but this is not the case.

This would be quite strange if real, many thanks to Marshall Eubanks for noting this aspect.

Looking better, we see situations like this, where you can see that the simulation does not end with the clone on a hyperbolic trajectory even if that orbit was apparently achieved in a given moment:

Time

a

e

i

peri

node

long

311100.5

11.10955

0.56037

12.7835

207.0631

179.7592

26.8223

311000.5

12.17985

0.599077

13.1885

206.6135

180.4985

27.112

310900.5

-6.12701

1.813375

2.8379

213.9255

160.4411

14.3666

310800.5

126.90366

0.960378

4.4906

347.4277

20.2166

7.6443

310700.5

58.4381

0.913926

4.4251

347.0157

20.7539

7.7696

310600.5

48.95964

0.897233

4.3941

346.7163

21.1435

7.8598


The reason why this can happen was explained by Jean Meeus:

"When one calculates the HELIOCENTRIC orbit near the time the object is close to Jupiter, one obtains a hyperbolic orbit, that however is meaningless because at that instant the object is attracted more by Jupiter than by the Sun."

So in the following plots, it is safe to ignore the brief moments where the orbit has apparently a total energy > 0 

This is the v_infinity distribution  plot not meaninfgful (it just "captures" a brief close encounter moment):



Mimimum perihelium distribution

Due to the wild uncertainty, the minimum perihelium could have been very low: in fact, about 10% of the clones could have had a close pass with Earth but not sooner than 4K years ago.


Max eccentricity distribution
(dis-regard the points with eccentricity > 1)



Kind Regards,
Alessandro Odasso

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