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Display information for equation id:math.1677.35 on revision:1677

* Page found: Kugelsymmetrische Potentiale (eq math.1677.35)

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Hash: 251daca6b826bae8abffc1af60f7feff

TeX (original user input): 

\left( \bar{r}\cdot \bar{p} \right)\left[ \left( \bar{r}\cdot \bar{p} \right)+\frac{\hbar }{i} \right]\Psi (r,\vartheta ,\phi )==-{{\hbar }^{2}}\frac{\partial }{\partial r}\left( {{r}^{2}}\frac{\partial \Psi }{\partial r} \right)

TeX (checked): 

\left({\bar {r}}\cdot {\bar {p}}\right)\left[\left({\bar {r}}\cdot {\bar {p}}\right)+{\frac {\hbar }{i}}\right]\Psi (r,\vartheta ,\phi )==-{{\hbar }^{2}}{\frac {\partial }{\partial r}}\left({{r}^{2}}{\frac {\partial \Psi }{\partial r}}\right)

LaTeXML (experimental; uses MathML) rendering

MathML (10.998 KB / 1.797 KB) :

( r ¯ ⋅ p ¯ ) [ ( r ¯ ⋅ p ¯ ) + ℏ i ] Ψ ( r , ϑ , ϕ ) = = - ℏ 2 ∂ ∂ ⁡ r ( r 2 ∂ ⁡ Ψ ∂ ⁡ r ) fragments fragments ( ¯ 𝑟 ⋅ ¯ 𝑝 ) fragments [ fragments ( ¯ 𝑟 ⋅ ¯ 𝑝 ) Planck-constant-over-2-pi 𝑖 ] Ψ fragments ( r , ϑ , ϕ ) superscript Planck-constant-over-2-pi 2 𝑟 fragments ( superscript 𝑟 2 Ψ 𝑟 ) {\displaystyle{\displaystyle\left(\bar{r}\cdot\bar{p}\right)\left[\left(\bar{r% }\cdot\bar{p}\right)+\frac{\hbar}{i}\right]\Psi(r,\vartheta,\phi)==-{{\hbar}^{% 2}}\frac{\partial}{\partial r}\left({{r}^{2}}\frac{\partial\Psi}{\partial r}% \right)}} 
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(r¯⋅p¯)[(r¯⋅p¯)+ℏi]Ψ(r,ϑ,ϕ)==−ℏ2∂∂r(r2∂Ψ∂r)
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In Maple:

Translation to Mathematica

In Mathematica:

Similar pages

Calculated based on the variables occurring on the entire Kugelsymmetrische Potentiale page

Identifiers

  • r¯
  • p¯
  • r¯
  • p¯
  • i
  • Ψ
  • r
  • ϑ
  • ϕ
  • r
  • r
  • Ψ
  • r

MathML observations

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