(first) eccentricity | e {\displaystyle e} | a 2 − b 2 a {\displaystyle {\frac {\sqrt {a^{2}-b^{2}}}{a}}} | sin α {\displaystyle \sin \alpha } | |
second eccentricity | e ′ {\displaystyle e'} | a 2 − b 2 b {\displaystyle {\frac {\sqrt {a^{2}-b^{2}}}{b}}} | tan α {\displaystyle \tan \alpha } | |
third eccentricity | e ″ {\displaystyle e''} | a 2 − b 2 a 2 + b 2 {\displaystyle {\sqrt {\frac {a^{2}-b^{2}}{a^{2}+b^{2}}}}} | sin α 2 − sin 2 α {\displaystyle {\frac {\sin \alpha }{\sqrt {2-\sin ^{2}\alpha }}}} | |
(first) flattening | f {\displaystyle f} | a − b a {\displaystyle {\frac {a-b}{a}}} | 1 − cos α {\displaystyle 1-\cos \alpha } | = 2 sin 2 ( α 2 ) {\displaystyle =2\sin ^{2}\left({\frac {\alpha }{2}}\right)} |
second flattening | f ′ {\displaystyle f'} | a − b b {\displaystyle {\frac {a-b}{b}}} | sec α − 1 {\displaystyle \sec \alpha -1} | = 2 sin 2 ( α 2 ) 1 − 2 sin 2 ( α 2 ) {\displaystyle ={\frac {2\sin ^{2}({\frac {\alpha }{2}})}{1-2\sin ^{2}({\frac {\alpha }{2}})}}} |
third flattening | n {\displaystyle n} | a − b a + b {\displaystyle {\frac {a-b}{a+b}}} | 1 − cos α 1 + cos α {\displaystyle {\frac {1-\cos \alpha }{1+\cos \alpha }}} | = tan 2 ( α 2 ) {\displaystyle =\tan ^{2}\left({\frac {\alpha }{2}}\right)} |