Abstract.The multi-scale interaction of self-consistently driven magnetic islands with electromagnetic turbulence is studied within the three dimensional, toroidal gyrokinetic framework. It can be seen that, even in the presence of electromagnetic turbulence the linear structure of the mode is retained. Turbulent fluctuations do not destroy the growing island early in its development, which then maintains a coherent form as it grows.The island is seeded by the electromagnetic turbulence fluctuations, which provide an initial island structure through nonlinear interactions and which grows at a rate significantly faster than the linear tearing growth rate. These island structures saturate at a width that is approximately ρ i in size. In the presence of turbulence the island then grows at the linear rate even though the island is significantly wider than the resonant layer width, a regime where the island is expected to grow at a significantly reduced non-linear rate.A large degree of stochastisation around the separatrix, and an almost complete break down of the X-point is seen. This significantly reduces the effective island width.Magnetic islands in a tokamak can lead to loss of confinement or even major disruptions of the plasma. The tearing mode [1, 2], specifically the neoclassical tearing mode (NTM) [3] is expected to set the beta limit in a reactor [4,5]. The dynamics of magnetic islands is the result of the interplay of variety of processes. On one hand, their instability is widely believed to be due to neoclassical effects, first of all to the non-linear drive caused by the bootstrap-current perturbation due to the island itself and often the polarisation current is invoked as a mechanism for its threshold [6,7]. Within the singular layer, centred around rational surfaces, (Parallel wave-vector of the mode, k || = 0) the assumptions of ideal MHD break down and magnetic reconnection may take place. For a collisionless mode the mechanism of reconnection is the electron inertia, where the singular layer width, and in turn the growth rate, are related closely to the electron skin depth [8]. When collisions become significant, it is plasma resistivity arXiv:1409.0648v2 [physics.plasm-ph]