We investigate the contributions coming from the penguin operators in the nonresonant B − → M M π − (M = π − , K − , K 0 ) decays. The effective Wilson coefficients of the the strong penguin operators O 4,6 are found to be relatively larger. We calculate the contributions arising from the O 4 and O 6 operators in the nonresonant decays B − → M M π − (M = π − , K − , K0 ) using a model combining heavy quark symmetry and the chiral symmetry, developed previously. We find that the forbidden nonresonant B − → K 0 K0 π − decay occurs through the strong penguin operators. These penguin contributions affect the branching ratios for B − → M M π − (M = π − , K − ) by only a few percent. The branching ratio for B − → K 0 K0 π − is estimated to be of the order 10 −6 .