# 5.4.1: Field of a Point Mass

Equation 5.3.1, together with the definition of field strength as the force experienced by unit mass, means that the field at a distance \(r\) from a point mass \(M\) is

\[g = \frac{GM}{r^2} \quad \text{N kg}^{-1} \text{ or m s}^{-2} \label{5.4.1} \tag{5.4.1}\]

In vector form, this can be written as

\[\textbf{g} = -\frac{GM}{r^2} \hat{\textbf{r}} \quad \text{N kg}^{-1} \text{ or m s}^{-2} \label{5.4.2} \tag{5.4.2}\]

Here \(\hat{\textbf{r}}\) is a dimensionless *unit* vector in the radial direction.

It can also be written as

\[\textbf{g} = -\frac{GM}{r^3} \textbf{r} \quad \text{N kg}^{-1} \text{ or m s}^{-2} \label{5.4.3} \tag{5.4.3}\]

Here \(\textbf{r}\) is a vector of magnitude \(r\) − hence the \(r^3\) in the denominator.