 Solution

A highly conducting solar wind carries the Sun's magnetic field outward by magnetic flux freezing. This can open magnetic field lines that would form closed loops in a static dipole model. Beyond an opening radius $r_o$, approximate the field as radial. Constancy of the magnetic flux in a fixed solid-angle flux tube gives the radial solar-wind magnetic flux lawwhich decays more slowly than the vacuum magnetic dipole field, proportional to $r^{-3}$.

For example, if the field becomes radial already near the solar radius $R_{\odot }$, normalizing both estimates to the same field there givesThus a dipole estimate $10^{-11}\mathrm{T}$ becomes of order $2\times 10^{-9}\mathrm{T}$, comparable to the stated hundredfold enhancement. More generally, matching dipolar decay inside $r_o$ to radial decay outside givesThis is a plausible scaling explanation, not a determination of the actual opening radius. The magnetic field need not be outward everywhere: opposite-polarity sectors can preserve zero net magnetic flux through a closed surface, consistent with Gauss's law for magnetism. The argument concerns the changed geometry of the field in a flowing plasma, rather than changing the dipole exponent by assumption.