If a passing star can jostle comets in the Oort Cloud, why doesn't the Moon disrupt the orbits of high-flying satellites?
Or does it? Maybe the satellites need periodic course corrections?
If a passing star can jostle comets in the Oort Cloud, why doesn't the Moon disrupt the orbits of high-flying satellites?
Or does it? Maybe the satellites need periodic course corrections?
The moon absolutely disrupts the orbit of a geostationary satellite. Just as the moon can cause tides on the Earth's surface, the moon's gravitational pull on a satellite will cause it to begin to drift slightly north/south in its orbit. Geostationary satellites must actively counteract this if they wish to remain geostationary.
See this page for more info https://www.satsig.net//satellite/inclined-orbit-operation.htm
The moon will always "perturb" the orbit to some extent, but to "disrupt" an orbit is to kick the satellite out of orbit. And this will only happen if the orbit is very wide, approximately when it reaches the Lagrange point L1, at about 85% the Moon's distance! Here's a drawing clearly showing stable and disrupted orbits: (replace Sun-Earth system with the Earth-Moon)
https://en.wikipedia.org/wiki/Lagrange_point#/media/File:Lagrange_points2.svg
The drawing also shows that things are much less favorable for orbits around the smaller mass, i.e. a satellite around the Moon instead of Earth. More precisely, the region around the Moon where those orbits would still be stable is the so-called Hill sphere: $$ R_H= (e-1) \ a \ \left(\frac{m_2}{m_1+m_2}\right)^{1/3} $$ but with masses $m_1$ and $m_2$ for the Earth-Moon system (and $e$ and $a$ the exentricity and semi-major axis) that gives almost the same result as just using the L1 position.
The highest-flying satellites orbit the earth at a distance of $42000$ km (the geostationary orbit) away from the center of the earth.
Remember the gravitational force is $F\propto \frac{M}{r^2}$.
Thus the force of the moon (mass $M=7.3\cdot 10^{22}$ kg, distance $r=380000$ km) on the satellite is very much smaller than the force of the earth (mass $M=6.0\cdot 10^{24}$ kg, distance $r=42000$ km) on the satellite. Using these numbers you find the force by the moon is around $10^{-4}$ times smaller than the force by the earth. So the effect of the moon is too small to significantly disrupt the satellite orbit around the earth.
The situation is different when a star moves through the Oort cloud. The star and the sun have similar masses, and they are similar distances away from the comets. Hence the forces by star and sun acting on a comet would be of similar size.
The moon bounces around all over the place--it never hits the same apogee or perigee twice. What you see published are only averages, and maxima and minima figures derive from computer simulations that can predict (ahead and backward) about 5ky. In spite of this chaos LLR (lunar laser ranging) purports to measure the rate at which the moon is receding due to tidal drag--this must require considerable averaging and modeling over many years.
The point being, it's a lot easier to simulate lunar attraction on satellites than to measure the rate of lunar recession.