We present a new kind of monogamous relations based on concurrence and concurrence of assistance. For N -qubit systems ABC1...CN−2, the monogamy relations satisfied by the concurrence of N -qubit pure states under the partition AB and C1...CN−2, as well as under the partition ABC1 and C2...CN−2 are established, which give rise to a kind of restrictions on the entanglement distribution and trade off among the subsystems.PACS numbers: 03.67.Mn,03.65.UdQuantum entanglement [1][2][3][4][5][6] is an essential feature of quantum mechanics, which distinguishes the quantum from classical world. As one of the fundamental differences between quantum entanglement and classical correlations, a key property of entanglement is that a quantum system entangled with one of other systems limits its entanglement with the remaining others. In multipartite quantum systems, there can be several inequivalent types entanglement among the subsystems and the amount of entanglement with different types might not be directly comparable to each other. The monogamy relation of entanglement is a way to characterize the different types of entanglement distribution. The monogamy relations give rise to the structures of entanglement in the multipartite setting. Monogamy is also an essential feature allowing for security in quantum key distribution [7]. Monogamy relations are not always satisfied by entanglement measures. Although the concurrence and entanglement of formation do not satisfy such monogamy inequality, it has been shown that the αth (α ≥ 2) power of concurrence and αth (α ≥ √ 2) power entanglement of formation for N -qubit states do satisfy the monogamy relations [8].In this paper, we study the general monogamy inequalities satisfied by the concurrence and concurrence of assistance. We show that the concurrence of multi-qubit pure states satisfies some generalized monogamy inequalities.The concurrence for a bipartite pure state |ψ AB is given by [10][11][12] where ρ A is the reduced density matrix by tracing over the subsystem B, ρ A = T r B (|ψ AB ψ|). The concurrence is extended to mixed states ρ = i p i |ψ i ψ i |, 0 ≤ p i ≤ 1, i p i = 1, by the convex roof extension,where the minimum is taken over all possible pure state decompositions of ρ AB . For a tripartite state |ψ ABC , the concurrence of assistance is defined by [13] C a (|ψ ABC ) ≡ C a (ρ AB ) = max {pi,|ψi } ifor all possible ensemble realizations of ρ AB = T r C (|ψ ABC ψ|) = i p i |ψ i AB ψ i |. When ρ AB = |ψ AB ψ| is a pure state, then one has C(|ψ AB