The magnetic shear for a concentric-circular configuration is defined by
| (382) |
where r is the minor radius of a magnetic surface. The above expression can be re-arranged as
| (383) |
Integrating the above equation over r and assuming ŝ is a constant, we obtain
| (384) |
Performing the integration, the above equation is written as
| (385) |
where q0 = q(r0). Equation (385) can be finally written as
| (386) |
This is a profile with a constant magnetic shear s. In Ben’s toroidal ITG simulation, the following q profile is used:
| (387) |
with q′(r0) = ŝq0∕r0. This is a linear profile over r, with the values of q and the shear at r = r0 being q0 and ŝ, respectively.