Moon Center of Mass/ Center of Gravity

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SUMMARY

The discussion clarifies the distinction between the center of mass (CM) and center of gravity (CG) in the context of the Moon. While both coincide for uniform objects under uniform gravitational fields, the Moon's gravitational field is not uniform due to tidal stresses from Earth's gravity. This results in the CG not aligning with the CM, particularly when considering the Moon's size and gravitational variations. The gravitational pull between two uniform spheres can be simplified to point masses at their respective CM, but calculating CG involves more complexity related to torque and rotation.

PREREQUISITES
  • Understanding of gravitational fields and forces
  • Familiarity with the concepts of center of mass and center of gravity
  • Basic knowledge of torque and rotational dynamics
  • Concepts of uniform spheres and gravitational interactions
NEXT STEPS
  • Study the differences between center of mass and center of gravity in non-uniform gravitational fields
  • Explore the implications of tidal forces on celestial bodies
  • Learn about the mathematical formulation of torque in rotational systems
  • Investigate the gravitational interactions between multiple celestial bodies
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Physics students, educators, and anyone interested in gravitational dynamics and celestial mechanics will benefit from this discussion.

schaefera
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Hi,

I was wondering about an issue that we just started in my physics class: we learned that center of mass (CM) and center of gravity (CG) coincide in an object as long as the force of gravity is uniform over that object. So, for something near the Earth's surface we can say that CM and CG coincide because the small change in height means that gravity is essentially uniform over that object; but when you get to the moon, do the CM and CG coincide? It's a very large object, so does gravity have a constant value all along it?

Thanks!
 
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Both the center of gravity and center of mass of a uniform sphere coincide with the geometrical center. The Earth's pull is not uniform from the front of the moon to the back, but the only effect this has on the moon is to cause a tidal stress.
 
Is there any reason why this is true? I'm thinking that even if the moon were thought of as nested, spherical shells, that doesn't mean the force of gravity can't be somewhere other than the center of mass (or can it)?
 
schaefera said:
Is there any reason why this is true? I'm thinking that even if the moon were thought of as nested, spherical shells, that doesn't mean the force of gravity can't be somewhere other than the center of mass (or can it)?

I never heard someone referring to "center of gravity" in space. But, conceptually, moon's center of gravity is definitely not center of mass.
 
Bill_K said:
This is a well-known theorem, but if you don't accept it, by all means tell us where you think it is instead. Or see http://hyperphysics.phy-astr.gsu.edu/hbase/mechanics/sphshell.html.

Yes, the gravitational pull between two uniform spheres can be calculated as if they were two points at their respective center of mass.

But is center of gravity something you need to calculate the magnitude of gravity? No! The "as if gravity exerted on one point" is in the context of torque and rotation!
 
Consider an object consisting of two point masses, m1 and m2, separated by displacement vector r. Suppose they are in presence of gravitational field with vector strength g1 and g2 respectively. Center of mass is trivially located at rCM=rm2/(m1 + m2) from m1.

Finding center of gravity is slightly more complicated. It is a point a combined force from which generates the same amount of torque on the system.

\vec{T} = m_2 \vec{r}_2 \times \vec{g}_2

\vec{F} = m_1 \vec{g}_1 + m_2 \vec{g}_2

To generate torque T, force F must be applied to a point:

\vec{r}_{CG} = \frac{\vec{F} \times \vec{T}}{||F||^2} + \vec{r}_p

Note that the solution is not unique. rp is any vector perpendicular to F. However, for general g1 and g2, there is no solution rCG = rCM.
 

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