All Figures

$\begin{figure} \par\includegraphics[width=7cm,clip]{9848fig1.eps} \end{figure}$ Figure 1: The function $\Theta ^{2}_{*}(x)$ with $x=\cos\theta$ against the polar angle $\theta$ with projections on the vertical and horizontal axes $\Theta^2_{*}(x)\cos\theta$ and $\Theta^2_{*}(x)\sin\theta$ respectively, indicating an integrable singularity of finite flux at x=+1 for a jet structure.
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In the text

$\begin{figure} \par\includegraphics[width=7cm,clip]{9848fig2.eps} \end{figure}$ Figure 2: The function $\Theta _{r}(x)$ with $x=\cos\theta$ in a polar plot indicating an integrable singularity at x=+1 for a jet structure.
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In the text

$\begin{figure} \par\includegraphics[width=7cm,clip]{9848fig3.eps} \end{figure}$ Figure 3: The function $\Theta (x)$ with $x=\cos\theta$ indicating integrable singularities at x=+1 and at x=-1 for knot structures.
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In the text

$\begin{figure} \par\includegraphics[width=7cm,clip]{9848fig4.eps} \end{figure}$ Figure 4: The function $\Theta ^{2}_{p}(x)$ with $x=\cos\theta$ indicating a plasma pressure jet in a very narrow cone about x=+1.
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In the text

$\begin{figure} \par\includegraphics[width=7cm,clip]{9848fig5.eps} \end{figure}$ Figure 5: The function $\tilde\rho(x)$ with $x=\cos\theta$ indicating a mass density jet in a very narrow cone about x=+1.
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In the text

$\begin{figure} \par\includegraphics[width=7cm,clip]{9848fig6.eps} \end{figure}$ Figure 6: The magnetic field line $a\eta -\theta$ dependence.
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In the text

$\begin{figure} \par\includegraphics[width=7cm,clip]{9848fig7.eps} \end{figure}$ Figure 7: The magnetic field line $\phi -\theta$ dependence.
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In the text

$\begin{figure} \par\includegraphics[width=7cm,clip]{9848fig8.eps} \end{figure}$ Figure 8: The three-dimensional magnetic field lines, wound on the surface of revolution of Fig. 6, viewed parallel to the x-y plane at about 45 degrees.
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In the text

$\begin{figure} \par\includegraphics[width=7cm,clip]{9848fig9.eps} \end{figure}$ Figure 9: The three-dimensional magnetic field lines, wound on the surface of revolution of Fig. 6, viewed down the z axis.
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In the text

$\begin{figure} \par\includegraphics[width=5.6cm,clip]{9848fg10.eps} \end{figure}$ Figure 10: The three-dimensional magnetic field lines, wounded on the surface of revolution of Fig. 6, viewed along the x axis.
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In the text

$\begin{figure} \par\includegraphics[width=7cm,clip]{9848fg11.eps} \end{figure}$ Figure 11: The function $\Theta _{r}(x)$ , with n=3, indicating an integrable singularity at x=+1 for a jet structure.
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In the text

$\begin{figure} \par\includegraphics[width=7cm,clip]{9848fg12.eps} \end{figure}$ Figure 12: The function $\Theta (x)$ , with n=3, indicating a more symmetric structure.
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In the text

$\begin{figure} \par\includegraphics[width=7cm,clip]{9848fg13.eps} \end{figure}$ Figure 13: The function $\Theta ^{2}_{p}(x)$ , with n=3, indicating a plasma pressure jet in a very narrow cone about x=+1.
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In the text

$\begin{figure} \par\includegraphics[width=7cm,clip]{9848fg14.eps} \end{figure}$ Figure 14: The function $\tilde\rho(x)$ with n=3 indicating a mass density jet in a very narrow cone about x=+1.
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In the text

$\begin{figure} \par\includegraphics[width=7cm,clip]{9848fg15.eps} \end{figure}$ Figure 15: The magnetic field line $a\eta -\theta$ dependence, with n=3, showing a symmetric structure.
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In the text

$\begin{figure} \par\includegraphics[width=6.7cm,clip]{9848fg16.eps} \end{figure}$ Figure 16: The three-dimensional magnetic field lines, with n=3, viewed parallel to the x-y plane at about 45 degrees.
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In the text

$\begin{figure} \par\includegraphics[width=7cm,clip]{9848fg17.eps} \end{figure}$ Figure 17: The three-dimensional magnetic field lines, with n=3, viewed down the z axis.
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In the text

$\begin{figure} \par\includegraphics[width=5.6cm,clip]{9848fg18.eps} \end{figure}$ Figure 18: The three-dimensional magnetic field lines, with n=3, viewed along the x axis.
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In the text