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====Initial Contact==== Geometrically we appreciate that, as <math>~r_0</math> is increased, the two circles will first touch at a point that lies along the (blue-dashed) line-segment that connects the centers of both circles. More specifically, the initial interception will be at the point identified in Figure 2 by the solid blue dot lying on the surface of the pink torus. The distance between the two centers — which we will denote as <math>~h</math> — is also the hypotenuse of a right triangle whose other two sides are of length (opposite the angle, <math>~\alpha</math>) <math>~\varpi_t - R_0</math> and (adjacent to the angle, <math>~\alpha</math>) <math>~Z_0</math>. We see that the initial interception will occur when <math>~r_0 + r_t = h</math>, that is, when <div align="center"> <table border="0" cellpadding="5" align="center"> <tr> <td align="right"> <math>~r_0 = r_+</math> </td> <td align="center"> <math>~\equiv</math> </td> <td align="left"> <math>~h - r_t</math> </td> </tr> <tr> <td align="right"> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~[(\varpi_t - R_0)^2 + Z_0^2 ]^{1/2} - r_t </math> </td> </tr> <tr> <td align="right"> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~(\varpi_t - R_0)[1 + \Lambda^2 ]^{1/2} - r_t \, ,</math> </td> </tr> </table> </div> where, <div align="center"> <table border="0" cellpadding="5" align="center"> <tr> <td align="right"> <math>~\Lambda</math> </td> <td align="center"> <math>~\equiv</math> </td> <td align="left"> <math>~\frac{Z_0}{\varpi_t - R_0} \, .</math> </td> </tr> </table> </div> For later reference, we note that the cylindrical coordinates associated with this initial point of contact — ''i.e.,'' the point identified in Figure 2 by the solid blue dot lying on the surface of the pink torus — are, <div align="center"> <table border="0" cellpadding="5" align="center"> <tr> <td align="right"> <math>~\varpi_+</math> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~\varpi_t - r_t \sin\alpha</math> </td> </tr> <tr> <td align="right"> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~\varpi_t - \frac{r_t (\varpi_t-R_0)}{[(\varpi_t - R_0)^2 + Z_0^2 ]^{1/2} }</math> </td> </tr> <tr> <td align="right"> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~\varpi_t - \frac{r_t }{[1+\Lambda^2 ]^{1/2} } \, ,</math> </td> </tr> </table> </div> and, <div align="center"> <table border="0" cellpadding="5" align="center"> <tr> <td align="right"> <math>~Z_+</math> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~r_t \cos\alpha</math> </td> </tr> <tr> <td align="right"> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~\frac{r_t Z_0}{[(\varpi_t - R_0)^2 + Z_0^2 ]^{1/2} }</math> </td> </tr> <tr> <td align="right"> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~\frac{r_t \Lambda}{[1+\Lambda^2 ]^{1/2} } \, .</math> </td> </tr> </table> </div>
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