The toroidal magnetic flux through the plasma column is calculated analytically for current-free stellarators of arbitrary geometry without assumptions on the plasma shape, aspect ratio, etc. This is done with accuracy sufficient for extracting the contribution due to the finite plasma pressure from this flux. The final result is a formula relating the measured diamagnetic signal with β, the ratio of the plasma pressure to the magnetic pressure. This formula is obtained assuming small β and the relative depth of the magnetic well. These are natural conditions for stellarators, therefore the final result can be recommended for magnetic diagnostics without practical limitations. Keywords: stellarator, magnetic diagnostics, diamagnetic signal, plasma equilibrium, current-free plasma DOI: 10.1585/pfr.5.S2054
InroductionDiamagnetic measurements are a traditional diagnostics used for determining the plasma energy content in tokamaks and stellarators [1][2][3][4][5]. Interpretation of the measurements are based on a simple formula originally derived for a circular plasma cylinder [6] 2 δΦwhere the measured diamagnetic signal is defined asB is the magnetic field, B v is the vacuum magnetic field, Φ 0 = B 0 S ⊥ with S ⊥ = πb 2 being the transverse crosssection of the plasma column, b is its minor radius, B 0 is the toroidal field, B J is the poloidal field at the plasma boundary due to the net toroidal current,β ≡ 2p/B 2 0 is the ratio of the volume-averaged plasma pressure p to the magnetic field pressure B 2 0 /2. It is known that Eq. (1) can be applied to large-aspectratio tokamaks with a circular plasma [7]. The same or slightly modified formula has been used for conventional stellarators [8][9][10], though the validity of Eq. (1) has been proved for straight stellarators only [11,12]. Strictly speaking, for stellarators with current-carrying plasma (B J 0) Eq. (1) should contain an additional term [11,12]. Here we consider the case when this contribution can be disregarded.The diamagnetic signal for arbitrary shape and aspect ratio current-free plasma in a toroidal conventional stellarator was calculated analytically in [13]. In analytical author's e-mail: pustovit@nfi.kiae.ru * permanent address: Russian Research Centre 'Kurchatov Institute', Pl. Kurchatova, Moscow, 123182, Russia theory, when a cylindrical result is generalized for account of the toroidal effects, this is usually done by large-aspectratio expansion. It was unexpected that the problem considered in [13] turned out to be solvable without this 'natural' simplification and even without any assumption on the plasma shape. The obtained result [13] was ready for practical use. Similar to (1), it directly relates the measured diamagnetic signal δΦ to the value of interest, the integral on the right hand side over the plasma volume. Here the constant F b = 2πrB t describes the vacuum toroidal field B t , r is the radius from the main vertical axis, and δ SH is a small correction related to the Shafranov shift and helical field. Later, numerical calculation...