(In practice, I choose the positive direction of and along the direction of toroidal and poloidal magnetic field (i.e., and are always positive in coordinates system). Then, the defined by Eq. (178) is always positive. It follows that should be also positive. Next, let us examine whether this property is correctly preserved by Eq. (183). Case 1: The radial coordinate is chosen as . Then the factor before the integration in Eq. (183) is negative. We can further verify that is always negative for either the case that is pointing inward or outward. Therefore the .r.h.s. of Eq. (183) is always positive for this case. Case 2: The radial coordinate is chosen as . Then the factor before the integration in Eq. (183) is positive. We can further verify that is always positive for either the case that is pointing inward or outward. The above two cases include all possibilities. Therefore, the positivity of is always guaranteed)
a magnetic surface forms a central hole around axis. Using Gauss's
theorem in the volume within the central hole, and noting that no magnetic
field line point-intersects a magnetic surface, we know that the magnetic flux
through any cross section of the hole is equal to each other. Next we
calculate this magnetic flux. To make the calculation easy, we select a plane
cross section perpendicular to the axis, as is shown by the dash line in
Fig. 1. In this case, only contribute to the magnetic flux,
which is written (the positive direction of the cross section is chosen in the
direction of
)
be generalized to any revolution surface that is generated by rotating a curve segment on the poloidal plane around axis. For instance, a curve on the poloidal plane that connects the magnetic axis and a point on a flux surface can form a toroidal surface (e.g., surface in Fig. 53). The magnetic flux through the toroidal surface is given by
i.e.
(531) |
The magnetic surface forms a central hole around axis. The magnetic flux through any cross section of the central hole is equal to each other and is given by , where and are the value of at the axis and the magnetic surface, respectively.
The conclusion in Eq. (530) can be generalized to any revolution surface that is generated by rotating a curve on the poloidal plane about axis. For instance, a curve on the poloidal plane that connects the magnetic axis and a point on a flux surface can form a toroidal surface (e.g., surface in Fig. 53).
Also note the difference between and defined in Sec. 1.4: is the magnetic flux through the central hole of a torus and thus includes the flux in the center transformer, and is the magnetic flux through the ribbon between the magnetic axis and the magnetic surface.
yj 2018-03-09