n → ∞ lim r = 1 ∑ n tan ( 4 × 2 r π ) sec ( 4 × 2 r − 1 π ) = ?
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Very nice! Although the property you prove holds for all A (apart from undefined points of the tangent and secant functions). What you can show is that the sum telescopes for any A , then plug in A = 4 π at the end (at the moment, it looks as though the identity is a special property of A = 4 π )
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Let 4 π = A . Therefore, tan 2 A sec A = cos 2 A cos A sin 2 A = cos 2 A cos A sin A cos 2 A − cos A sin 2 A = tan A − tan 2 A lim n → ∞ ∑ r = 1 n tan ( 4 ∗ 2 r π ) sec ( 4 ∗ 2 r − 1 π ) = lim n → ∞ tan A − tan 2 n + 1 A = tan 4 π = 1