We study power corrections to the event shapes in annihilation in the two jets kinematical region, . We argue that for $e \sim \Lambda_{QCD}/Q1/\lr{Qe}^n$ have to be taken into account for an arbitrary . This is achieved by introducing a new universal distribution, the shape function, which describes the energy flow in the final state. The event shape differential distributions are given by a convolution of the shape function with perturbatively resummed cross-sections. Choosing a physically motivated ansatz for the shape function, we observe a good agreement of our predictions with available data on the differential thrust, -parameter and heavy-jet mass distributions and their first few moments.

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