Translation for "sivukvanttiluku" to english

Sivukvanttiluku

• azimuthal quantum number
• side quantum number

Translation examples

azimuthal quantum number

Yhtälön ratkaisut ovat: ψ n ℓ m ( r , θ , ϕ ) = ( 2 n a 0 ) 3 ( n − ℓ − 1 ) ! 2 n 3 e − r / n a 0 ( 2 r n a 0 ) ℓ L n − ℓ − 1 2 ℓ + 1 ( 2 r n a 0 ) ⋅ Y ℓ m ( θ , ϕ ) {\displaystyle \psi _{n\ell m}(r,\theta ,\phi )={\sqrt {{\left({\frac {2}{na_{0}}}\right)}^{3}{\frac {(n-\ell -1)!}{2n^{3}}}}}e^{-r/na_{0}}\left({\frac {2r}{na_{0}}}\right)^{\ell }L_{n-\ell -1}^{2\ell +1}\left({\frac {2r}{na_{0}}}\right)\cdot Y_{\ell }^{m}(\theta ,\phi )} missä: a 0 = 4 π ε 0 ℏ 2 m e e 2 {\displaystyle a_{0}={\frac {4\pi \varepsilon _{0}\hbar ^{2}}{m_{e}e^{2}}}} on Bohrin säde, L n − ℓ − 1 2 ℓ + 1 ( ⋯ ) {\displaystyle L_{n-\ell -1}^{2\ell +1}(\cdots )} ovat yleistetyt (n - ℓ − 1):nnen asteen Laguerren polynomit n, ℓ, m ovat kokonaislukuja, jotka tunnetaan nimillä pääkvanttiluku, sivukvanttiluku ja magneettinen kvanttiluku.
The family of solutions is: Ψ n ℓ m ( r , θ , ϕ ) = ( 2 n a 0 ) 3 ( n − ℓ − 1 ) ! 2 n e − r / n a 0 ( 2 r n a 0 ) ℓ L n − ℓ − 1 2 ℓ + 1 ( 2 r n a 0 ) ⋅ Y ℓ m ( θ , ϕ ) {\displaystyle \Psi _{n\ell m}(r,\theta ,\phi )={\sqrt {{\left({\frac {2}{na_{0}}}\right)}^{3}{\frac {(n-\ell -1)!}{2n}}}}e^{-r/na_{0}}\left({\frac {2r}{na_{0}}}\right)^{\ell }L_{n-\ell -1}^{2\ell +1}\left({\frac {2r}{na_{0}}}\right)\cdot Y_{\ell }^{m}(\theta ,\phi )} where a0 = 4πε0ħ2/mee2 is the Bohr radius, L2ℓ + 1 n − ℓ − 1 are the generalized Laguerre polynomials of degree n − ℓ − 1, n = 1, 2, ... is the principal quantum number, ℓ = 0, 1, ... n − 1 the azimuthal quantum number, m = −ℓ, −ℓ + 1, ..., ℓ − 1, ℓ the magnetic quantum number.