For some point $p = (p_1,\dots,p_n)$, choose coordinates so that $p = (0,0, \dots, 0)$. Now approximate $f$ and $g$ by Taylor series:
$$ f(x) = f(0) + \left( \sum_i \frac{\partial f}{\partial x_i}(0) \cdot x_i \right) + F(x) $$
$$ g(x) = g(0) + \left( \sum_j \frac{\partial g}{\partial x_j}(0) \cdot x_j \right) + G(x) $$
where $F(x)$ and $G(x)$ are the higher order terms (of degree $\geq 2$).
Now use these expressions to compute $\{f,g\}$. Since $f(0)$ and $g(0)$ are constants, they can be ignored (since constants are Casimirs), and since $\frac{\partial f}{\partial x_i}(0)$ and $\frac{\partial g}{\partial x_j}(0)$ are constants, they can be factored out:
$$ \begin {align*}
\{f,g\}(x) &= \sum_{i,j} \frac{\partial f}{\partial x}_i(0) \frac{\partial g}{\partial x_j}(0) \{x_i, x_j\} \\
&\phantom{=} + \sum_i \frac{\partial f}{\partial x_i}(0) \{x_i, G\} + \sum_j \frac{\partial g}{\partial x_j}(0) \{F, x_j\} \\
&\phantom{=} + \{F,G\}
\end {align*}
$$
Notice that the first line of this equation is exactly what you want. So you need to check that the terms on the second and third line vanish when $(x_1,x_2, \dots, x_n) = (0,0,\dots,0)$. Remember that $F(x)$ and $G(x)$ are power series with all terms of degree $\geq 2$. So when you use the Leibniz rule, every term will have a factor of some $x_k$, so when $x \to 0$, all these terms will be zero.