So we have three points on a plane, with coordinates $$ \begin{aligned} \mathbf{r}_A & = \pmatrix{x_A\\y_A\\0} & \mathbf{r}_B & = \pmatrix{x_B\\y_B\\0} & \mathbf{r}_C & = \pmatrix{x_C\\y_C\\0} \end{aligned} $$
A force is acting with a line of action perpendicular to the plane
$$\begin{aligned}
\mathbf{F} & = \pmatrix{0\\0\\F} &
\mathbf{r} & = \pmatrix{x \\ y \\ 0}
\end{aligned}$$
But we don't know the force magnitude or the location. But from any two of the three equipollent moments
$$ \begin{aligned}
\mathbf{M}_A & = \left(\mathbf{r}-\mathbf{r}_A\right) \times \mathbf{F} \\
\mathbf{M}_B & = \left(\mathbf{r}-\mathbf{r}_B\right) \times \mathbf{F} \\
\mathbf{M}_C & = \left(\mathbf{r}-\mathbf{r}_C\right) \times \mathbf{F} \\
\end{aligned}$$ we deduce the force by using the fact that $\mathbf{M}_B - \mathbf{M}_A = \left(\mathbf{r}_A-\mathbf{r}_B \right) \times \mathbf{F}$
$$ \mathbf{F} = \frac{ \left( \mathbf{r}_B-\mathbf{r}_A \right) \times \left(\mathbf{M}_B-\mathbf{M}_A\right) }{ \| \mathbf{r}_B-\mathbf{r}_A \|^2 } $$
provided that $\mathbf{F}$ is perpendicular to the plane of A, B and C.
The location of the force is then recovered from any one of the moments by
$$ \mathbf{r} = \mathbf{r}_A + \frac{ \mathbf{F} \times \mathbf{M}_A}{\| \mathbf{F} \|^2} $$
Quick Proof
Take $\mathbf{M}_B - \mathbf{M}_A = \left(\mathbf{r}_A-\mathbf{r}_B \right) \times \mathbf{F}$ and plug in the solution for $\mathbf{F}$ as follows:
$$\require{cancel}
\begin{aligned}
\mathbf{M}_B - \mathbf{M}_A &= -\left(\mathbf{r}_B-\mathbf{r}_A \right) \times \frac{ \left( \mathbf{r}_B-\mathbf{r}_A \right) \times \left(\mathbf{M}_B-\mathbf{M}_A\right) }{ \| \mathbf{r}_B-\mathbf{r}_A \|^2 } \\
& = -\frac{\left(\mathbf{r}_B-\mathbf{r}_A \right) \cancel{ \left( \left(\mathbf{r}_B-\mathbf{r}_A \right) \cdot\left(\mathbf{M}_B-\mathbf{M}_A\right) \right) } - \left(\mathbf{M}_B-\mathbf{M}_A\right) \| \mathbf{r}_B-\mathbf{r}_A \|^2 }{ \| \mathbf{r}_B-\mathbf{r}_A \|^2 } \\
& \equiv \mathbf{M}_B - \mathbf{M}_A
\end{aligned} $$
Use the vector triple product $a\times(b \times c) = b (a\cdot c) - c (a\cdot b)$
The canceling of $\left(\mathbf{r}_B-\mathbf{r}_A \right) \cdot\left(\mathbf{M}_B-\mathbf{M}_A\right)$ can be proven by the definition of the equipollent moments.
Similarly, take the calculation of $\mathbf{r}$ and expand out the expression $$ \mathbf{F} \times \mathbf{r} = \mathbf{F} \times \mathbf{r}_A + \frac{ \mathbf{F} \times \left( \mathbf{F} \times \mathbf{M}_A \right)}{ \| \mathbf{F} \|^2} = \mathbf{F} \times \mathbf{r}_A + \frac{ \mathbf{F} \cancel{ \left( \mathbf{F} \cdot \mathbf{M}_A \right)}-\mathbf{M}_A \| \mathbf{F} \|^2 }{ \| \mathbf{F} \|^2} = \mathbf{F} \times \mathbf{r}_A - \mathbf{M}_A$$
Example
A force $F=\pmatrix{0\\0\\5}$ acts through the point $\mathbf{r} = \pmatrix{4.2 \\ 2.5 \\ 0}$
We measure the moment $\mathbf{M}_A = \pmatrix{12.5 \\ 29 \\ 0}$ at $\mathbf{r}_A = \pmatrix{10\\0\\0}$
We measure the moment $\mathbf{M}_B = \pmatrix{-12.5 \\ -21 \\ 0}$ at $\mathbf{r}_B = \pmatrix{0\\5\\0}$
Use the following relative quantities $$\begin{aligned} \mathbf{r}_{AB} &= \mathbf{r}_B - \mathbf{r}_A = \pmatrix{-10 \\ 5 \\ 0} & \mathbf{M}_{AB} &= \mathbf{M}_B - \mathbf{M}_A = \pmatrix{-25 \\ -50 \\ 0} \end{aligned}$$
To get the force
$$ \mathbf{F} = \frac{ \pmatrix{-1 \\ 5 \\0} \times \pmatrix{-25 \\ -50 \\ 0} }{ \| \pmatrix{-10 \\ 5 \\0} \|^2} = \pmatrix{0 \\ 0 \\ 5} \; \checkmark $$
$$ \mathbf{r} = \pmatrix{10 \\ 0 \\0} + \frac{ \pmatrix{0\\0\\5} \times \pmatrix{12.5\\29\\0} }{ 5^2 } = \pmatrix{4.2 \\ 2.5 \\ 0} \; \checkmark$$
\times
. $\endgroup$