[guided]The test map is designed so that its zeros encode exactly the forbidden Tverberg intersection. Define
\begin{align*}
\Phi: X &\to \mathbb{R}^r \oplus (\mathbb{R}^d)^r
\end{align*}
by
\begin{align*}
\Phi(\lambda_1 x_1 + \cdots + \lambda_r x_r)
= \left((\lambda_1,\dots,\lambda_r),(\lambda_1 f(x_1),\dots,\lambda_r f(x_r))\right).
\end{align*}
This map is continuous because join coordinates vary continuously on the join and $f:K\to\mathbb{R}^d$ is continuous.
The diagonal subspace
\begin{align*}
L = \{((a,\dots,a),(z,\dots,z)) : a \in \mathbb{R}, z \in \mathbb{R}^d\}
\end{align*}
records the situation where all weights are equal and all weighted image points are equal. Let
\begin{align*}
\rho: \mathbb{R}^r \oplus (\mathbb{R}^d)^r &\to L^\perp
\end{align*}
be orthogonal projection. Since the orthogonal complement of the constant vectors in $\mathbb{R}^r$ is
\begin{align*}
W_r = \left\{(a_1,\dots,a_r) \in \mathbb{R}^r : \sum_{i=1}^r a_i = 0\right\},
\end{align*}
the space $L^\perp$ is $S_r$-equivariantly isomorphic to $W_r^{\oplus(d+1)}$, which we denote by $V$.
We verify that $\rho(\Phi(x))$ never vanishes. Take
\begin{align*}
x = \lambda_1 x_1 + \cdots + \lambda_r x_r \in X.
\end{align*}
If $\rho(\Phi(x))=0$, then $\Phi(x)\in L$. The first coordinate of $\Phi(x)$ is $(\lambda_1,\dots,\lambda_r)$, so membership in the diagonal line forces all $\lambda_i$ to be equal. Since their sum is $1$, each equals $1/r$. The second coordinate then gives
\begin{align*}
\frac{1}{r}f(x_1)=\cdots=\frac{1}{r}f(x_r),
\end{align*}
and hence $f(x_1)=\cdots=f(x_r)$. Because every $\lambda_i$ is positive, the deleted-join condition says that the points $x_i$ lie in pairwise disjoint faces $\sigma_i$ of $K$. Thus the common value of the $f(x_i)$ lies in
\begin{align*}
f(\sigma_1) \cap \cdots \cap f(\sigma_r),
\end{align*}
contradicting the assumption.
Thus $\rho(\Phi(x))\ne 0$ for every $x\in X$, and normalization gives
\begin{align*}
\Psi: X &\to S(V)
\end{align*}
by
\begin{align*}
\Psi(x)=\frac{\rho(\Phi(x))}{|\rho(\Phi(x))|}.
\end{align*}
The maps $\Phi$, $\rho$, and the identification $L^\perp\cong V$ are compatible with permutations of the labels, so $\Psi$ is $S_r$-equivariant.[/guided]