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Display information for equation id:math.1898.2 on revision:1898

* Page found: Das hamiltonsche Wirkungsprinzip (eq math.1898.2)

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TeX (original user input): 

\begin{align}
  & \delta W=0 \\
 & W:=\int\limits_{{{t}_{1}}}^{{{t}_{2}}}{dt}F=\int\limits_{{{t}_{1}}}^{{{t}_{2}}}{dt}L({{q}_{1}},...{{q}_{f}},{{{\dot{q}}}_{1}},...,{{{\dot{q}}}_{f}},t)=\int\limits_{{{t}_{1}}}^{{{t}_{2}}}{dt}T-V \\
\end{align}

TeX (checked): 

{\begin{aligned}&\delta W=0\\&W:=\int \limits _{{t}_{1}}^{{t}_{2}}{dt}F=\int \limits _{{t}_{1}}^{{t}_{2}}{dt}L({{q}_{1}},...{{q}_{f}},{{\dot {q}}_{1}},...,{{\dot {q}}_{f}},t)=\int \limits _{{t}_{1}}^{{t}_{2}}{dt}T-V\\\end{aligned}}

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MathML (22.889 KB / 2.713 KB) :

δ ⁢ W = 0 W := ∫ t 1 t 2 𝑑 t ⁢ F = ∫ t 1 t 2 𝑑 t ⁢ L ⁢ ( q 1 , … ⁢ q f , q ˙ 1 , … , q ˙ f , t ) = ∫ t 1 t 2 𝑑 t ⁢ T - V missing-subexpression 𝛿 𝑊 0 missing-subexpression assign 𝑊 superscript subscript subscript 𝑡 1 subscript 𝑡 2 differential-d 𝑡 𝐹 superscript subscript subscript 𝑡 1 subscript 𝑡 2 differential-d 𝑡 𝐿 subscript 𝑞 1 … subscript 𝑞 𝑓 subscript ˙ 𝑞 1 … subscript ˙ 𝑞 𝑓 𝑡 superscript subscript subscript 𝑡 1 subscript 𝑡 2 differential-d 𝑡 𝑇 𝑉 {\displaystyle{\displaystyle\begin{aligned} &\displaystyle\delta W=0\\ &\displaystyle W:=\int\limits_{{{t}_{1}}}^{{{t}_{2}}}{dt}F=\int\limits_{{{t}_{% 1}}}^{{{t}_{2}}}{dt}L({{q}_{1}},...{{q}_{f}},{{{\dot{q}}}_{1}},...,{{{\dot{q}}% }_{f}},t)=\int\limits_{{{t}_{1}}}^{{{t}_{2}}}{dt}T-V\\ \end{aligned}}}

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MathML (2.267 KB / 447 B) :

δW=0W:=∫t1t2dtF=∫t1t2dtL(q1,...qf,q˙1,...,q˙f,t)=∫t1t2dtT−V

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Calculated based on the variables occurring on the entire Das hamiltonsche Wirkungsprinzip page

Identifiers

  • δ
  • W
  • W
  • t1
  • t2
  • t
  • F
  • t1
  • t2
  • t
  • L
  • q1
  • qf
  • q˙1
  • q˙f
  • t
  • t1
  • t2
  • t
  • T
  • V

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