We study the problem of entangling two spins at the distant ends of a spin chain by exploiting the nonequilibrium dynamics of the system after a sudden global quench. As initial states we consider a canted/spiral order product state of the spins, and singlets of neighboring pairs of spins. We find that within the class of canted order initial states, no entanglement is generated at any time except for the special case of the Néel state. While an earlier work had shown that the Néel state is indeed an excellent starting resource for the dynamical generation of long distance entanglement, the curious fact that this is the sole point within a large class of initial product states of the spins was not noted. On the other hand, we find that an initial state which is a series of nearest neighbor Bell states, and well motivated by some physical realizations, is also a good starting resource for end to end entanglement in a similar way to the Néel state. The scheme is shown to be robust to random single spin flip in the initial Néel state as well as randomness of the couplings.PACS numbers: 03.67. Bg, 03.67.Hk, 75.10.Pq Entanglement induced between distinct parts of a many-body system due to the nonequilibrium dynamics following quenches have attracted much attention recently. This has been largely motivated by experimental developments which allow for the realization of long time nonequilibrium dynamics -notably with ultracold atoms in optical lattices [1][2][3][4]. The potential for realizing such dynamics in ion traps has been also pointed out in both theoretical studies [5][6][7], as well as the realization of spin chains [8,9]. Some studies have examined the time development of entanglement between complementary blocks of a one dimensional spin system [6, 10-13] as well as between proximal spins [14,15]. However, in the field of quantum information, it is most desirable to achieve long range entanglement, i.e., the entanglement between two individual spins separated by a significant distance. For example, it is essential for teleportation of a quantum state over a distance [16] and thereby to link well separated quantum registers. Motivated by this point, studies have also been made of the creation of long-range entanglement between the end spins of a spin chain through the nonequilibrium dynamics that follows a quench. The first study in this context considered a chain of harmonic oscillators which were suddenly coupled [17]. For spin chains, the first study in this context considered a sudden quench in the Ising anisotropy parameter of a XXZ model [18]. This was a global quench in the sense that all couplings of the Hamiltonian of a system were changed in the same way by the quench. Such quenches may be easier to realize in systems with limited local addressability such as for ultracold atoms in optical lattices. However, one can also suddenly change a local coupling, as may be easier in gate controlled systems such as quantum dots coupled to leads, and for a spin chain version of such systems, called Kondo sy...