DLMF:14.5.E20 (Q4732)

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DLMF:14.5.E20
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    Statements

    𝖯 1 2 ( cos θ ) = 2 π ( 2 E ( sin ( 1 2 θ ) ) - K ( sin ( 1 2 θ ) ) ) , shorthand-Ferrers-Legendre-P-first-kind 1 2 𝜃 2 𝜋 2 complete-elliptic-integral-second-kind-E 1 2 𝜃 complete-elliptic-integral-first-kind-K 1 2 𝜃 {\displaystyle{\displaystyle\mathsf{P}_{\frac{1}{2}}\left(\cos\theta\right)=% \frac{2}{\pi}\left(2E\left(\sin\left(\tfrac{1}{2}\theta\right)\right)-K\left(% \sin\left(\tfrac{1}{2}\theta\right)\right)\right),}}
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    DLMF:14.5.E20
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    π {\displaystyle{\displaystyle\pi}}
    C3.S12.E1.m2akdec
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    K ( k ) complete-elliptic-integral-first-kind-K 𝑘 {\displaystyle{\displaystyle K\left(\NVar{k}\right)}}
    C19.S2.E8.m1adec
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    E ( k ) complete-elliptic-integral-second-kind-E 𝑘 {\displaystyle{\displaystyle E\left(\NVar{k}\right)}}
    C19.S2.E8.m2adec
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    cos z 𝑧 {\displaystyle{\displaystyle\cos\NVar{z}}}
    C4.S14.E2.m2afdec
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    𝖯 ν ( x ) = 𝖯 ν 0 ( x ) shorthand-Ferrers-Legendre-P-first-kind 𝜈 𝑥 Ferrers-Legendre-P-first-kind 0 𝜈 𝑥 {\displaystyle{\displaystyle\mathsf{P}_{\NVar{\nu}}\left(\NVar{x}\right)=% \mathsf{P}^{0}_{\nu}\left(x\right)}}
    C14.S2.SS2.p2.m2abdec
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    sin z 𝑧 {\displaystyle{\displaystyle\sin\NVar{z}}}
    C4.S14.E1.m2afdec
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    0 < θ < π 0 𝜃 𝜋 {\displaystyle{\displaystyle 0<\theta<\pi}}
    C14.S5.XMD2.m1edec
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