**Corrected version
**Published: October 30, 2014 by Milutin Marjanov

Revised version: May 12, 2015

Concept of homogeneity (or inhomogeneity) of the gravitational field is rather a specific one. Namely, according to the Newton`s law of gravitation, either intensity or direction, or each of these two characteristics of the gravitational force acting on the body, depend on its position in the gravitational field. So, in fact, for the body as a whole, the gravitational field is always an inhomogeneous one. Such classification makes sense only if it is restricted to the active part of the gravitational field, that is, on the part occupied by the body.

## Homogeneous and Inhomogeneous Gravitational Field

Consider a body of mass *m* moving in the gravitational field of the dominant mass m*. Assume that m/m*‹‹1, so the gravitational field is a stationary one. Gravitational noice, as well as the gravitational anomalies, are excluded.

Motion of the body is composed: while moving in its orbit, it revolves about its principal central axis of inertia *(1)*, which is perpendicular to the orbital plane. The mass center *C* of the body is chosen to be at the origin of two moving frames of reference *xCy* and ξ*C*η. The first one is related to the geometry of the orbit, *Cx* being oriented toward the gravitational center, that is toward its mass center C*. The orbital angle is ψ. The second frame is related to the geometry of mass of the body, Cξ having direction of the principal axis *(3)* and Cη – direction of the axis *(2)* of the ellipsoid of inertia. Position of the second reference frame with respect to the first one is defined by the angle of relative rotation φ *(Fig.1)*.

*Fig. 1 – Body in the gravitational field and two frames of reference*

In a homogeneous gravitational field, intensities and directions of the elementary gravitational forces *dF* acting on the body`s particles *dm* depend on the position

of the mass center in the gravitational field, solely. They are functions neither of the positions of the particles (ξ,η) within the body, nor of the angle of relative rotation φ. All these forces have the same direction, that is, they are parallel to the coordinate axis Cx and their sum, the “weight” of the body, coincides with that line, regardless of the relative position of the body in the frame of reference *xCy*. In a homogeneous gravitational field the resultant of the elementary gravitational forces always passes through the mass center of the body and the gravitational moment does not exist. In fact, the mass center of the body in a homogeneous gravitational field represents the center of gravity, as concieved by Archimedes some 2,5 centuries B.C. (Fig. 2).

Such an interpretation of the gravitational field acting on the body is only posible if the dimensions of the body are negligible compared to the distance between the mass center of the body and of the gravitational center. If the largest dimension of the body is *D*, invariability of intensities and directions of the gravitational forces acting on the body`s particles imply D/R≈0 compared to unity in the approximate calculus of the gravitational load

According to the Newton’s law of gravitation, intensity of the gravitational force is equal

where *G* represents the gravitational constant, while the gravitational moment

*Fig. 2 – Homogeneous gravitational field*

On the other hand, if the gravitational field is inhomogeneous one, at least the second power of the fraction *D/R* has to be retained in the expression containing unity in the course of calculus of the gravitational load. Depending on the retained power of *D/R* it is possible to speak of the second, or the higher order inhomogeneity of the field. In the inhomogeneous gravitational field intensities and directions of the elementary forces depend on the position of the mass center in the gravitational field, but also on the position of the particles within the body, as well as on the relative position of the body.

All these forces converge toward the gravitational center and so does their resultant.

Generally, this resultant doesn’t pass through the mass center of the body, so it has to produce the gravitational moment *(Fig. 3)*.

*Fig. 3 – Inhomogeneous gravitational field*

Within the second order inhomogeneity case, the gravitational force and the gravitational moment are equal

where *I2* and *I3* are the medium and the minimum principal moments of inertia for the mass center of the body. Obviously, both components of the gravitational load are harmonic functions of the angle of relative rotation, with amplitudes that depend on the size of dominant mass, on distance between the body and the dominant mass center and finally, on distribution of masses in the body.

We have to point out the following fact:

*When a small body goes around the large body in the closed orbit its orbital and rotational motions, as a rule, gradually become resonant just because of the gravitational torque existence* (/3/,/4/).

*The first characteristic of inhomogeneity of the gravitational field is the existence of the gravitational moment, in the general case.*

*The second one is the absence of the center of gravity of the body.*

## Body without Center of Gravity

Authors of many of textbooks are not quite precise about that point. Having, probably, in mind the existence of the gravitational moment in such a field, they often claim implicitly, or even explicitly, that in an inhomogeneous gravitational field the center of gravity doesn’t coincide with the mass center of the body. This is definitely wrong, of course, because such an assertion may lead the reader to the false conclusion that there exists something like a “moving center of the gravity” in the rotating body exposed to the inhomogeneous gravitational field. There is no such a point in, or in the vicinity of the body, satisfying the definition of the center of gravity, if the body is exposed to the field of the convergent gravitational forces. The “weight” vector of the body has to pass through the point toward which converge all its components and that is the gravitational center. The relative rotation of the body produces tilting of this vector about this center *(Fig. 4)*.

The angle between the gravitational force and the direction CC* is equal

*Fig. 4 – Oscillation of the gravitational force around the gravitational center*

## Conclusion

We have stressed the distinction between homogeneous and inhomogeneous gravitational fields. A homogeneous gravitational field is marked by the existence of the center of gravity and the absence of the gravitational moment acting on the body. On the other hand, in an inhomogeneous gravitational field the body has no center of gravity and the gravitational moment, generally, exist. Concerning the calculus of the gravitational load, one has to adopt

compared to unity, for the homogeneous and at least

compared to unity, for an inhomogeneous gravitational field.

*References*

1. S. Hawking and W. Israel: 300 Years of Gravitation, Cambridge University Press, 1989;

2. C. W. Misner, K. S. Thorne, J. A. Wheeler: Gravitation, W.H. Freeman and Comp, San Francisco, 1973;

3. Marjanov M. Gravitational Resonances, Bull. Astron., Belgrade, 156, 9 – 19; 1997;

4. Marjanov M. One Solution of the Newton’s Three Body Problem