Circular Cross Sections: Difference between revisions

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[[VanWasshenova_Thesis#Determining_wire-theta_correspondence|<math>\vartriangleleft </math>]]
[[VanWasshenova_Thesis#Determining_wire-theta_correspondence|<math>\vartriangleleft </math>]]
[[VanWasshenova_Thesis#Determining_wire-theta_correspondence|<math>\triangle </math>]]
[[VanWasshenova_Thesis#Determining_wire-theta_correspondence|<math>\triangle </math>]]
[[CED_Verification_of_DC_Angle_Theta_and_Wire_Correspondance|<math>\vartriangleright </math>]]
[[Elliptical_Cross_Sections|<math>\vartriangleright </math>]]


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Revision as of 17:37, 15 May 2017

[math]\displaystyle{ \textbf{\underline{Navigation}} }[/math]

[math]\displaystyle{ \vartriangleleft }[/math] [math]\displaystyle{ \triangle }[/math] [math]\displaystyle{ \vartriangleright }[/math]

Circular Conic Section

If the conic is an circle, e=0. This implies

[math]\displaystyle{ e=\frac{\sin (\beta)}{\sin (\alpha)}=\frac{\sin (25^{\circ})}{\sin (90-\theta)}=0 }[/math]


Using the relation

[math]\displaystyle{ sin(90^{\circ}-\theta)=cos(\theta) }[/math]
[math]\displaystyle{ \frac{sin (25^{\circ})}{0}=cos( \theta) =\infty }[/math]


The sector angle will never be perpendicular to the plane of the light cone, so this is not a physical possibility.


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