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In addition, any upper bound to will result in a lower bound to.
The parameters themselves were given a zero lower bound to prevent them from becoming negative, and an upper bound to prevent non-physical values.
First, r measurements are simulated at each t j ∈ T by shifting R j from the lower bound to the upper bound on the estimated state bounds.
This could be considered as a lower bound to performance.
In our experiments we select β0 by rounding up the lower bound to the nearest tenth.
A lower bound to the creep rupture time of internally pressurised thick cylinders is derived.
New lower bound to E s2) has been obtained for the extended supersaturated designs.
A lower bound to E χ2) has been obtained for the extended supersaturated designs.
A lower bound to E χ2) has been obtained for the proposed designs.
As it can be seen, this case serves as a lower bound to the IA case.
Obviously this will give us a lower bound to the optimal primal solution.
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