1996Birkhäuser Boston eBooksRequires access

Central Forces

Nathaniel Grossman

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Abstract

A central force field is one whose action is always directed toward a fixed point. If that fixed point is taken to be the origin, and if i is taken to be a unit vector directed from the origin to the position r of a particle acted upon by the central force, then the force field can be written 83 $$F(r)=-mP(r)i,$$ where P is a scalar function and m is the mass of the particle. The equation of motion for a particle of constant mass can be written down using Newton’s Second Law; it is 84 $$\ddot{r}=-Pi.$$

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A central force field is one whose action is always directed toward a fixed point. If that fixed point is taken to be the origin, and if i is taken to be a unit vector directed from the origin to the position r of a particle acted upon by the central force, then the force field can be written 83 $$F(r)=-mP(r)i,$$ where P is a scalar function and m is the mass of the particle. The equation of motion for a particle of constant mass can be written down using Newton’s Second Law; it is 84 $$\ddot{r}=-Pi.$$

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Available abstract

A central force field is one whose action is always directed toward a fixed point. If that fixed point is taken to be the origin, and if i is taken to be a unit vector directed from the origin to the position r of a particle acted upon by the central force, then the force field can be written 83 $$F(r)=-mP(r)i,$$ where P is a scalar function and m is the mass of the particle. The equation of motion for a particle of constant mass can be written down using Newton’s Second Law; it is 84 $$\ddot{r}=-Pi.$$

Key concepts: Geology

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