FOURIER–MOTZKIN ELIMINATION

(Redirected from Fourier-Motzkin elimination)
'Fourier–Motzkin elimination' is a mathematical algorithm for eliminating variables from a system of linear inequalities. It can both look for real and for integer solutions. It is computationally expensive.
Elimination (or exists-elimination) of variables ''V'' from a system of relations (here, linear inequalities) consists in creating another system of the same kind, but without the variables ''V'', such that both systems have the same solutions over the remaining variables.
If one eliminates all variables from a system of linear inequalities, then one obtains a system of constant inequalities, which can be trivially decided to be true or false, such that this system has solutions (is true) if and only if the original system has solutions. As a consequence, elimination of all variables can be used to detect whether a system of inequalities has solutions or not.
Let us consider a system S of n inequalities with r variables xi_1 to xi_r, with xi_r the variable to eliminate. The linear inequalities in the system can be grouped into three classes, depending on the sign (positive, negative or null) of the coefficient for xi_r:

★ those that are equivalent to some inequalities of the form xi_r geq sum_{k=1}^{r-1} a_k xi_k; let us note these as xi_r geq A_i(xi_1, dots, xi_{r-1}), for i ranging from 1 to n_A where n_A is the number of such inequalities;

★ those that are equivalent to some inequalities of the form xi_r leq sum_{k=1}^{r-1} a_k xi_k; let us note these as xi_r leq B_i(xi_1, dots, xi_{r-1}), for i ranging from 1 to n_B where n_B is the number of such inequalities;

★ those in which xi_r plays no role, grouped into a single conjunction phi.
The original system is thus equivalent to max(A_1(xi_1, dots, xi_{r-1}), dots, A_{n_A}(xi_1, dots, xi_{r-1}) leq xi_r leq min(B_1(xi_1, dots, xi_{r-1}), dots, B_{n_A}(xi_1, dots, xi_{r-1}) wedge phi.
Elimination consists in producing a system equivalent to exists xi_r~S. Obviously, the above formula is equivalent to max(A_1(xi_1, dots, xi_{r-1}), dots, A_{n_A}(xi_1, dots, xi_{r-1}) leq min(B_1(xi_1, dots, xi_{r-1}), dots, B_{n_A}(xi_1, dots, xi_{r-1}) wedge phi.
The inequality max(A_1(xi_1, dots, xi_{r-1}), dots, A_{n_A}(xi_1, dots, xi_{r-1}) leq min(B_1(xi_1, dots, xi_{r-1}), dots, B_{n_A}(xi_1, dots, xi_{r-1}) is equivalent to n_A n_B inequalities A_i(xi_1, dots, xi_{r-1}) leq B_j(xi_1, dots, xi_{r-1}), for 1 leq i leq n_A and 1 leq j leq n_B.
We have therefore transformed the original system into another system where xi_r is eliminated. Note that the output system has (n-n_A-n_B)+n_A n_B inequalities. In particular, if n_A = n_B = n/2, then the number of output inequalities is n^2/4.

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See also
References

See also



Real closed field: the cylindrical algebraic decomposition algorithm performs quantifier elimination over ''polynomial'' inequalities, not just linear

References



★ Alexander Schrijver, ''Theory of Linear and Integer Programming''. John Wiley & sons, 1998, ISBN 0-471-98232-6, pp. 155-156

★ Keβler, Christoph W., ''Parallel Fourier–Motzkin Elimination'', Universität Trier Citeseer page
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