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4 Some constructions

1][t]0.71

Construction 4.1   Construct $ y$ so that $ x\, y=1$.

This can be done using the right triangle altitude theorem.
    
1][t]0.28\includegraphics[height=15mm]{figures/altitude}

Construction 4.2   Construct cycles $ \pi_{1}$, $ \pi_{2}$ whose shadows are symmetrical.

From Proposition 2.7, cycles $ \pi_{1}$, $ \pi_{2}$ are reciprocal under the homographic transformation $ \psi\,:\,\psi\left(z\right)=-1/\overline{z}$. When $ \pi_{1}$ is a circle away from $ O$, one can draw a diameter through $ O$, obtaining $ \alpha,\,\beta$ (Fig. 3(a)) and then use Construction 4.1 to obtain $ \gamma=\psi\left(\alpha\right)$ and $ \delta=\psi\left(\beta\right)$ i.e. a diameter of $ \pi_{2}$.

Fig. 3: Circles having opposite apexes
[Original figure]\includegraphics[clip,height=50mm]{figures/pole-plan05} [Meridian figure]\includegraphics[clip,height=50mm]{figures/pole-sphere05}

Construction 4.3   Given a cycle $ \pi_{1}$, construct the points $ \omega_{3},\,\omega_{4}$ whose shadows are the centers on the sphere of $ shadow\left(\pi_{1}\right)$.

Construct $ \pi_{2}$ as in Construction 4.2. Draw a secant circle $ \pi'$ and construct the radical center of $ \pi',\,\pi_{1},\,\pi_{2}$ (dotted lines in Fig. 3(a)). Project orthogonally to $ \left(O\,\omega_{1}\right)$ and obtain $ H$. Use again Construction 4.1 since $ \overline{H\omega_{3}}^{2}=\overline{H\omega_{4}}^{2}=\overline{H\alpha}\,\overline{H\beta}$.

Fig. 3(b) is drawn in the plane that contains the $ \mathbb{S}$-meridian circle through $ \omega_{0}$. The small circle $ shadow\left(\pi_{0}\right)$ stays in a plane perpendicular to the figure, and segment $ \left[S_{\alpha},\, S_{\beta}\right]$ is its diameter. Points $ S_{3},\, S_{4}$ are obtained as $ \mathbb{S}\cap\left(\Omega A_{1}\right)$. A special treatement is required when $ shadow\left(\pi_{1}\right)$ is a great circle. In this case $ \pi_{2}=\pi_{1}$while $ \mathcal{A}_{1}$ is rejected at infinity. One can see directly that $ \omega_{3},\,\omega_{4}=\omega_{1}/\left(1\pm r_{1}\right)$.

In any case, the "poles" cannot be used to characterize a given cycle, since they occur by pair and are not easy to distinguish (when $ O$ is inside $ \pi_{0}$, so is $ \pi_{1}$ and $ \omega_{3}$, $ \pi_{1},$$ \pi_{0}$ are on the same side of $ \Delta$ while $ \omega_{2}$ is on the other side).

Construction 4.4   Construct a circle $ \pi_{1}$ centered on $ \omega_{1}$ and orthogonal to cycle $ \pi_{0}$.

Draw the projective line $ \left(L\right)$ through the south pole $ S_{\infty}$ and either $ S_{1}$ or $ \Omega_{1}=\left(x_{1},y_{1},0\right)$. This line intersects the projective plane $ \left(P\right)$ of $ shadow\left(\pi_{0}\right)$. The intersection $ \left(L\right)\cap\left(P\right)$ is the required $ X_{1}=apex\left(\pi_{1}\right)$.

Proof. [Discussion] When $ A_{1}$ lies strictly inside $ \mathbb{S}$, we have $ r_{1}^{2}<0$ and therefore circle $ \pi_{1}$ is imaginary. When $ \omega_{1}\in\pi_{0}$ and $ \pi_{0}$ is a circle, then $ \pi_{1}$ is the point-circle $ \left\{ \omega_{1}\right\} $. When $ \pi_{0}$ is a line and $ \omega_{1}\in\pi_{0}$, then $ \left(L\right)\subset\left(P\right)$ and all the circles concentric at $ \omega_{1}$ are solutions. When $ \pi_{0}$ is a straight line and $ \omega_{1}\notin\pi_{0}$, then $ \left(L\right)$ intersects $ \left(P\right)$ at $ S_{\infty}$ and $ \pi_{1}$ is the point-circle $ \left\{ \infty\right\} $. The last result is counter-intuitive, but comes from the definition of concentric circles as pencil $ P\left(\left\{ \omega_{1}\right\} ,\left\{ \infty\right\} \right)$ so that $ \left\{ \infty\right\} $ is "centered" everywhere. $ \qedsymbol$

Construction 4.5   Construct the relatives of a given point $ \omega_{0}\neq O$.

Let $ \left(\omega\perp\right)$ and $ \left(O\perp\right)$ be respectively, the straight line drawn in the equatorial plane, through $ \omega_{0}$ orthogonally to $ \left(O\,\omega_{0}\right)$. Additionally, let $ u$ and $ v$ be respectively $ u\doteq apex\left(O\,\omega\right)=\left(y,-x,0,0\right)$ and $ v\doteq apex\left(O,\perp\right)=\left(x,\, y,\,0,\,0\right)$. Then :


Fig. 4: Relatives of a given point
\includegraphics[clip,width=55mm,height=50mm]{figures/related-to-J02}


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Previous: 3 Orthogonality Up: Viewing and Touching the Next: 5 The south plane   Contents


douillet@ensait.fr
2009-03-13