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© 1999-2008 HEAT
JSPWiki v2.4.104
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| [{ALLOW view xkrumpha}] |
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| [{LTMathDebug}] |
| [{ALLOW view All}] |
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| \forall x \in M \exists y: \nabla x = y }] |
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| \sum_{ x=1}^\infty \frac{1}{x^2} = \frac{ \pi^2}{6} |
| }] |
| [{LTMath |
| \sum_i \vec A \cdot \vec B = -P \! \int \! \textbf{r} \cdot |
| \hat{\mathbf{n}}\, dA = P \! \int \! {\vec \nabla} \cdot \textbf{r}\, dV. |
| }] |
| [{LTMath |
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| [{LTMath |
| \mathbb{ABCDEFGHIJKLMNOPQRSTUVWXYZ} |
| }] |
| [{LTMath |
| \mathrm{I_{k0}^{''}=\frac{\frac{U_V}{\sqrt{3}}}{Z_1\frac{U_V^2}{S_V}}} |
| }] |
| [{LTMath |
| d{\bf{B}} = \frac{{\mu _0 }}{{4\pi }}\frac{{Id\ell \times {\bf{\hat r}}}}{{r^2 }} |
| }] |
| [{LTMath |
| - \frac{{\hbar ^2 }}{{2m}}\frac{{\partial ^2 \psi (x,t)}}{{\partial x^2 }} + U(x)\psi (x,t) = i\hbar \frac{{\partial \psi (x,t)}}{{\partial t}} |
| }] |
| [{LTMath |
| \sin x = \sum\limits_{n = 1}^\infty {\frac{{\left( { - 1} \right)^{n - 1} x^{2n - 1} }}{{\left( {2n - 1} \right)!}}} |
| }] |
| [{LTMath |
| \cos x = \sum\limits_{n = 0}^\infty {\frac{{\left( { - 1} \right)^n x^{2n} }}{{\left( {2n} \right)!}}} |
| }] |
| [{LTMath |
| \sin \theta _1 \pm \sin \theta _2 = 2\sin \left( {\frac{{\theta _1 \pm \theta _2 }}{2}} \right)\cos \left( {\frac{{\theta _1 \mp \theta _2 }}{2}} \right) |
| }] |
| [{LTMath |
| \cos \theta _1 + \cos \theta _2 = 2\cos \left( {\frac{{\theta _1 + \theta _2 }}{2}} \right)\cos \left( {\frac{{\theta _1 - \theta _2 }}{2}} \right) |
| }] |
| [{LTMath |
| \sum_{n=0}^N g_n(x) = \sum\nolimits_{n=0}^N g_n(x) = |
| \int_a^b f(x) \,\mbox{d}x = \int\limits_a^b f(x) \,\mbox{d}x = |
| \oint_c^d F(z) \,\mbox{d}z }] |
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