Moon Center of Mass/ Center of Gravity

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Discussion Overview

The discussion revolves around the relationship between the center of mass (CM) and center of gravity (CG) of the Moon, particularly in the context of gravitational uniformity and the implications of the Moon's size. Participants explore whether these two points coincide on the Moon and the theoretical underpinnings of their definitions.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant questions whether the CM and CG of the Moon coincide, given its large size and the potential non-uniformity of gravitational force across its surface.
  • Another participant asserts that for a uniform sphere, the CM and CG coincide at the geometrical center, but acknowledges that the Earth's gravitational pull is not uniform across the Moon.
  • Some participants express uncertainty about the validity of the theorem that states CM and CG coincide, suggesting that gravity could act differently than expected in a non-uniform field.
  • There is a discussion about the necessity of calculating CG in the context of torque and rotation, with one participant noting that CG is not needed to determine the magnitude of gravity.
  • A participant introduces a mathematical approach to finding CG and CM for a system of point masses, indicating that the relationship between them is not straightforward in non-uniform fields.

Areas of Agreement / Disagreement

Participants express differing views on whether the center of gravity and center of mass coincide for the Moon, with some supporting the theorem while others challenge its applicability in this context. The discussion remains unresolved with multiple competing perspectives.

Contextual Notes

Participants highlight the complexity of gravitational fields and the implications of non-uniformity, as well as the mathematical distinctions between calculating CG and CM. There are unresolved assumptions regarding the uniformity of gravity over the Moon's surface.

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.

[tex]\vec{T} = m_2 \vec{r}_2 \times \vec{g}_2[/tex]

[tex]\vec{F} = m_1 \vec{g}_1 + m_2 \vec{g}_2[/tex]

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

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

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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