- an axis-aligned square (angle is 0°),
- a diamond shape, which is a square rotated by 45°.
1. Exogenous Angle
| Exogenous Angle Model |
|---|
| \[\begin{align} \max\> & {\color{darkred}s} \\&{\color{darkblue}p}'_{i,x} \le {\color{darkred}x}' + {\color{darkblue}M} {\color{darkred}\delta}_{i,1} && \forall i \\&{\color{darkblue}p}'_{i,x} \ge {\color{darkred}x}' + {\color{darkred}s} - {\color{darkblue}M} {\color{darkred}\delta}_{i,2} && \forall i \\&{\color{darkblue}p}'_{i,y} \le {\color{darkred}y}' + {\color{darkblue}M} {\color{darkred}\delta}_{i,3} && \forall i \\&{\color{darkblue}p}'_{i,y} \ge {\color{darkred}y}' + {\color{darkred}s} - {\color{darkblue}M} {\color{darkred}\delta}_{i,4} && \forall i \\ & \sum_k {\color{darkred}\delta}_{i,k} = 3 && \forall i \\&{\color{darkred}q}_{j,x}' = {\color{darkred}x}' + {\color{darkred}s} {\color{darkblue}\Delta}_{j,x} && \forall j \\&{\color{darkred}q}_{j,y}' = {\color{darkred}y}' + {\color{darkred}s} {\color{darkblue}\Delta}_{j,y} && \forall j \\&{\color{darkred}q}_{j,x} ={\color{darkred}q}_{j,x}' \cos({\color{darkblue}\theta}) - {\color{darkred}q}_{j,y}' \sin({\color{darkblue}\theta}) && \forall j \\&{\color{darkred}q}_{j,y} ={\color{darkred}q}_{j,x}' \sin({\color{darkblue}\theta}) + {\color{darkred}q}_{j,y}' \cos({\color{darkblue}\theta}) && \forall j \\&{\color{darkred}q}_{j,c} \in [0, {\color{darkblue}{\mathit{maxSize}}}] \\&{\color{darkred}s} \in [0,{\color{darkblue}{\mathit{maxSize}}}] \\&{\color{darkred}\delta}_{i,k} \in \{0,1\} \\&{\color{darkblue}p}'_{i,x} := {\color{darkblue}p}_{i,x} \cos({\color{darkblue}\theta}) + {\color{darkblue}p}_{i,y} \sin({\color{darkblue}\theta}) \\&{\color{darkblue}p}'_{i,y} := -{\color{darkblue}p}_{i,x} \sin({\color{darkblue}\theta}) + {\color{darkblue}p}_{i,y} \cos({\color{darkblue}\theta}) \\&{\color{darkblue}\Delta} = \begin{pmatrix} 0 & 0 \\ 0 & 1 \\ 1 & 0 \\ 1 & 1\end{pmatrix} \end{align}\] |
- \(\sin({\color{darkblue}\theta})\) and \(\cos({\color{darkblue}\theta})\) are constants. Unbelievably, this is actually a linear MIP model!
- \({\color{darkred}x}',{\color{darkred}y}'\) denotes the lower-left corner of the axis-aligned square (like in [1]).
- \({\color{darkred}q}_{j,c}', j=1,\dots,4\) are the four corner points (in transformed space). We map them back to \({\color{darkred}q}_{j,c}\), which form a rotated square.
- Below, we plot the solution both in the transformed space and in the original coordinate system.
- This is a very easy MIP:
Proven optimal solution
MIP Solution: 3.085938 (657 iterations, 0 nodes)
Next thing to try: make \(\theta\) endogenous.