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sin
θ
=
R
e
(
e
i
θ
)
=
e
i
θ
−
e
−
i
θ
2
i
{\displaystyle \sin \theta =\mathrm {Re} (e^{i\theta })={\frac {e^{i\theta }-e^{-i\theta }}{2i}}}
cos
θ
=
I
m
(
e
i
θ
)
=
e
i
θ
+
e
−
i
θ
2
{\displaystyle \cos \theta =\mathrm {Im} (e^{i\theta })={\frac {e^{i\theta }+e^{-i\theta }}{2}}}
tan
θ
=
sin
θ
cos
θ
=
e
2
i
θ
−
1
i
(
e
2
i
θ
+
1
)
{\displaystyle \tan \theta ={\frac {\sin \theta }{\cos \theta }}={\frac {e^{2i\theta }-1}{i(e^{2i\theta }+1)}}}
csc
θ
=
1
sin
θ
=
2
i
e
i
θ
−
e
−
i
θ
{\displaystyle \csc \theta ={\frac {1}{\sin \theta }}={\frac {2i}{e^{i\theta }-e^{-i\theta }}}}
sec
θ
=
1
cos
θ
=
2
e
i
θ
+
e
−
i
θ
{\displaystyle \sec \theta ={\frac {1}{\cos \theta }}={\frac {2}{e^{i\theta }+e^{-i\theta }}}}
cot
θ
=
1
tan
θ
=
i
(
e
2
i
θ
+
1
)
e
2
i
θ
−
1
{\displaystyle \cot \theta ={\frac {1}{\tan \theta }}={\frac {i(e^{2i\theta }+1)}{e^{2i\theta }-1}}}