This work presents numerical and analytic approaches for calculating the amplitude of edge harmonic oscillations (EHOs) associated with Quiescent H-modes in the presence of symmetry breaking magnetic coils. The analytic approach uses a linear ideal MHD model for EHOs and external kink modes subject to a given boundary condition defined by an externally applied helical field. The imposed 3D field is found to extend the parameter space of unstable external kink modes and EHOs, also providing an amplitude for the MHD perturbation, including the edge corrugation. The saturated states obtained using the linear time-invariant MHD equations are compared with those obtained with the VMEC nonlinear free boundary code, where the error field correction coils (EFCCs) in JET-like geometry were added to obtain a self-consistent equilibrium solution including the plasma response. Quantitative and qualitative agreement is found between the saturated amplitude calculated analytically and with VMEC for the case of the external kink modes. Only qualitative agreement was found for the most complex case of the EHO amplitude, though saturated amplitudes in both approaches are of the same order of magnitude and follow a similar linear trend with applied current to the EFCCs. The results obtained in this paper may help the modelling of the plasma response for external saturated modes, as well as offer an attractive route for scenario development and control in tokamak devices.
This paper explores how external magnetic coils can be used to control and extend the parameter space of edge harmonic oscillations (EHOs) in tokamak devices. The researchers used analytical and numerical models to understand how these external coils can affect the stability and amplitude of EHOs and external kink modes, which are important for achieving stable and high-performance plasma operations.