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The Roche Limit The Roche limit is the minimum orbital radius which is necessary for dust or particles to grow forming a moon, or necessary for an existing moon to remain internally stable. It is named after Édouard Roche (1820 – 1883).
Determining the Roche limit
Two
particles (mass m, radius r) orbiting the planet
(mass M) will be bound, if their mutual
gravitational force F =
G*m*m/(2r)2 is
greater than the difference of the gravitational
forces ((tidal force) exerted
by the body of mass M on the
particles at R-r and R+r ΔF = F2 - F1 = G*m*M/(R-r)2 - G*m*M/(R+r)2 ΔF =
(G*m*M/R2)*[1/(1-r/R)2 -
1/(1+r/R)2]
For
m<<M (or r/R<<1):
1/(1-r/R)2 - 1/(1+r/R)2
≈ 1/(1-2r/R) - 1/(1+2r/R)
≈ 1+2r/R - (1-2r/R) =
4r/RThe
Roche limit is given by the condition:
ΔF =
F
(G*m*M/R2)*4r/R = G*m*m/(4r2) M*4r/R3 = m/(4r2) R = r*(16*M/m)1/3 ≈ 2.5*r*(M/m)1/3 Using the densities of the bodies m=ρm*4π*r3/3 and M=ρM*4π*rM3/3: R =
r*(16*M/m)1/3 = rM*(16*ρM/ρm)1/3 In case
of equal densities, ρM
= ρm R ≈ 2.5*rM
In the solar system the orbits of the Earth's moon and of the Earth are in a region of stability. The Hill
Sphere
An
astronomical body's Hill sphere is the region in
which it dominates the attraction of satellites.
It is named after John William Hill (1812–1879).
![]() Determining the Hill Sphere radius The satellite or moon (mass μ) is orbiting the star (mass M) with the same angular velocity ω at the distance R+r as the planet (mass m) at the distance R (permanent full moon position). The equilibrum condition for the planet is: m ω2
R = G m M/R2
ω2 = GM/R3 The satellite
is dragged by the combined gravitational
forces exerted by the star and the planet:
μ ω2 (R+r) = G μ M/(R+r)2 + G μ m/r2
Inserting
ω2:
G μ M (R+r)/R3 = G μ M/(R+r)2 + G μ m/r2 M (R+r)/R3 = M/(R+r)2 + G m/r2 M (R+r)3 r2 = M R3 r2 + m R3 (R+r)2 m R3 (R+r)2 = M r2 (R3+3R2r+3Rr2+r3) - M R3 r2 m R3 (R+r)2 = M r3 (3R2+3Rr+r2) For
r<<R: (R+r)2
≈ R2, and 3Rr+r2 ≈ 0.
The equation simplifies:
m R5 = 3 M r3 R2
m R3 = 3 M r3 r = R [m/(3M)]1/3
Last update 2015, Jun 18 |