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Physics for Geologists, Second edition

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3 Gravity<br />

Universal gravity<br />

When discussing weight, mass and density (page 14) we stated Newton's<br />

Law of Gravitation: that every particle of mass ml attracts every particle<br />

of mass mz with a <strong>for</strong>ce that is directly proportional to the product of their<br />

masses and inversely proportional to the square of the distance between their<br />

centres of mass; and this <strong>for</strong>ce acts along a straight line joining them:<br />

where r is the distance between their centres of mass, and G is the universal<br />

constant of gravitation, and we noted that G is not a true constant because<br />

it has dimensions.<br />

Fields<br />

Fields are difficult to define. Within a body of water there is a pressure field.<br />

If the water is of constant density and is at rest, surfaces of equal pressure<br />

(pgz) are horizontal (that is, normal to the vector -g). When the water flows,<br />

the pressure field changes because the energy of the water changes. Energy is<br />

also a field. Fields may consist of scalars (magnitude), such as temperature,<br />

pressure or energy, or of vectors (magnitude and direction), such as <strong>for</strong>ce;<br />

and they can be mapped.<br />

The space in which terrestrial gravity acts, and the space in which mag-<br />

netism acts, are called gravity fields and magnetic fields, respectively. An<br />

electric current in a wire sets up a magnetic field around the wire. Fields in<br />

physics are spaces (or areas) in which some agent (commonly a <strong>for</strong>ce) oper-<br />

ates. There are fields at various scales, regional and local. The local magnetic<br />

and gravity fields are of interest to geologists because ore bodies may give<br />

rise to anomalies. Take gravity.<br />

On the surface of the Earth the <strong>for</strong>ce due to gravity acting on any object<br />

is, as we saw on page 14,<br />

Copyright 2002 by Richard E. Chapman

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