In a protoplanetary disk around a young star, it is believed
that regions with higher gas densities tend to concentrate solid material. If
these high gas density regions are sufficiently long-lived, the aggregates of
solid material within them can gravitationally collapse to form planets. The
presence of a gas giant planet like Jupiter can create such long-lived, high
gas density regions; especially around the gas giant planet’s leading (L4) and
trailing (L5) Lagrangian points. The high gas density regions around L4 and L5
tend to concentrate solid material in a process known as Lagrangian trapping. A
paper by Lyra et al. (2008) show that Lagrangian trapping can lead to
gravitational collapse of aggregated solid material and form objects with
masses in the regime of terrestrial planets (~ 0.1 to 10 Earth masses).
Figure 1: A contour plot showing the 5 Lagrangian points of
the Sun-Earth system. The same layout of the 5 Lagrangian points also applies
for the Sun-Jupiter system. The regions around the leading (L4) and trailing
(L5) Lagrangian points are “islands of stability”.
As a gas giant planet orbits around its infant star, it
clears out a wide gap in the protoplanetary disk. The environment within the
gap is depleted of gas and other materials. Nevertheless, the regions around L4
and L5 serve as “islands of stability” where high gas densities are retained. The
high gas densities create drag and damp the motion of solid particles. This
allows Lagrangian trapping to occur where solid particles become trapped in the
high gas density regions around L4 and L5. Simulations were conducted by Lyra
et al. (2008) to determine the effectiveness of Lagrangian trapping in forming
terrestrial planets with masses ranging from sub-Earth-mass to
super-Earth-mass. A planet formed at L4 or L5 is known as a Trojan planet or
Trojan Earth (if it has ~ 1 Earth mass). The word “Trojan” comes from the
Trojan asteroids that exist around Jupiter’s L4 and L5 Lagrangian points.
Lyra et al. (2008) investigated the formation of Trojan
planets by running simulations using a gas giant planet with the mass of
Jupiter and solid particles with diameters of 1 cm, 10 cm, 30 cm and 1 m. The
10 cm and 30 cm solid particles readily underwent gravitational collapse at the
Lagrangian points. For the 1 cm solid particles, they were so well coupled to
the gas that gravity is not the main factor driving their collapse. Instead,
the 1 cm solid particles collapse as the high gas density regions around L4 and
L5 gradually shrunk. For the large 1 m solid particles, they remained unbound
because they were too heavy to be captured by gas drag into the high gas
density regions.
Each simulation by Lyra et al. (2008) was run using only one
particle size. Gravitational collapse was more efficient for 10 cm solid particles
than for 30 cm ones. The 10 cm solid particles collapsed to form a 0.6
Earth-mass planet at L4 and a 2.6 Earth-mass planet at L5. For the case
involving 30 cm solid particles, a 0.1 Earth-mass planet was formed at L4, but the
solid particles remained unbound at L5. These planet masses are only applicable
for the particular set of assumptions used in the simulations by Lyra et al.
(2008).
Figure 2: Artist’s conception of an Earth-size planet with
vegetation covering most of the planet’s surface from pole-to-pole. Credit: Goran
Licanin.
Figure 3: Artist’s conception of a habitable Earth-size
planet with a large ice sheet on one of the planet’s poles.
Lagrangian trapping can produce a wide range of planetary
masses depending on many conditions such as mass of gas giant planet, density
of protoplanetary disk, size distribution of solid particles, etc. As a result,
a huge diversity of Trojan planets is expected. Trojan planets formed at the
Lagrangian points of a gas giant planet orbiting within the habitable zone of
its parent star can potentially be Earth-like and habitable. Such “Trojan
Earths” can appear very similar to the Earth. For a gas giant planet orbiting
further from its parent star, Trojan planets formed at its Lagrangian points
can acquire a significant fraction of icy material if temperatures are cool
enough for ices to exist in the protoplanetary disk. Such a Trojan planet is
expected to have a surface ice shell overlying a vast global ocean of liquid
water.
If Trojan objects with masses in the regime of terrestrial
planets can form, it is worth considering why Trojan planets are absent in the
Solar System. One reason could be that the initial Trojan objects that formed
at Jupiter’s L4 and L5 Lagrangian points were de-stabilized when Jupiter and
Saturn crossed the 2:1 mean motion resonance. Following that, Jupiter acquired
a new population of Trojan objects. However, without gas drag, the new
population of Trojan objects could not assembly into planets and hence left
behind what is now observed as the Trojan asteroids at Jupiter’s Lagrangian
points. As a result, Trojan planets are probably more common in planetary
systems with only one gas giant planet or in planetary systems where the gas
giant planets did not undergo resonance crossing.
Reference:
Lyra et al. (2008), “Standing on the shoulders of giants:
Trojan Earths and vortex trapping in low mass self-gravitating protoplanetary
disks of gas and solids”, arXiv:0810.3192 [astro-ph]