Perhaps instead of  finite sets one should work with *effective divisors*, i.e., formal linear combibinations of the form $\newcommand{\bZ}{\mathbb{Z}}$ $\newcommand{\bR}{\mathbb{R}}$ $\newcommand{\bp}{\boldsymbol{p}}$

$$ D= \sum_{\bp\in\bR^N} m_D(\bp) \bp,  $$

where $m_D:\bR^N\to\bZ_{\geq 0}$ is a function  with finite support. Denote by $\newcommand{\Div}{\mathrm{Div}}$  $\Div_{\geq 0}(\bR^N)$ the space of effective divisors in $\bR^N$.  $\Div_{\ge 0}$ has an obvious semigroup structure. Think of the center of mass as a map $\newcommand{\eC}{\mathscr{C}}$

$$ \eC: \Div_{\geq 0}(\bR^N)\to \Div_{\geq 0}(\bR^N),  $$

with the following properties. 

**1.** For any divisor $D$,  the support of the center of mass $\eC(D)$ consists of a single point.  

**2.** For any divisors $D_1,D_2\in\Div_{\geq 0}(\bR^N)$  we have 

$$ \eC(D_1+D_1) =\eC\Bigl(\; \eC(D_1)+\eC(D_2)\; \Bigr).$$

**3.** For any point $\bp\in \bR^N$ and any $m\in\bZ_{\geq 0}$

$$\eC(m \delta_{\bp})=m\delta_{\bp}, $$

where $\delta_{\bp}$ denotes the Dirac divisor of mass $1$ supported at  $\bp$.

**4.** $\eC$ is continuous with respect to the obvious topology on $\Div_{\geq 0}(\bR^N)$, where supports of divisors converge in the Hausdorff metric and in the limit the total mass is conserved. 

**Claim.** I believe that these properties uniquely determine  $\eC$.  

**Weaker Claim.**  The map $\eC$ is uniquely determined if  besides  **1**,...**4** we assume the following additional condition.

**5.** If the support of $D$ is contained in an affine subspace $V\subset \bR^N$, then  the support of $\eC(D)$ is contained in the same affine subspace.


**Edit.** Strengthened  Condition $3$.