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| = im a heading =
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| === sub-heading === | | == aaaa == |
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| Test link to svn file <websvn CUSF/README.txt>
| | {{Info|We are currently in the process of finalising the new image for |
| | SolidWorks 2020.}} |
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| = Maths is working! =
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| <math>\LaTeX</math> is the business!
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| This fact is also true in all inertial frames:
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| <math> \begin{bmatrix} c\,t'<br />
| | <math>E=mc^2</math> |
| x'<br />
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| y'<br />
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| z' \end{bmatrix} = \begin{bmatrix} \gamma&-\beta_x\,\gamma&-\beta_y\,\gamma&-\beta_z\,\gamma<br />
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| -\beta_x\,\gamma&1+(\gamma-1)\frac{\beta_{x}^{2}}{\beta^{2}}&(\gamma-1)\frac{\beta_{x}\beta_{y}}{\beta^{2}}&(\gamma-1)\frac{\beta_{x}\beta_{z}}{\beta^{2}}<br />
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| -\beta_y\,\gamma&(\gamma-1)\frac{\beta_{y}\beta_{x}}{\beta^{2}}&1+(\gamma-1)\frac{\beta_{y}^{2}}{\beta^{2}}&(\gamma-1)\frac{\beta_{y}\beta_{z}}{\beta^{2}}<br />
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| -\beta_z\,\gamma&(\gamma-1)\frac{\beta_{z}\beta_{x}}{\beta^{2}}&(\gamma-1)\frac{\beta_{z}\beta_{y}}{\beta^{2}}&1+(\gamma-1)\frac{\beta_{z}^{2}}{\beta^{2}}<br />
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| \end{bmatrix} \begin{bmatrix} c\,t<br />
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| x<br />
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| y<br />
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| z \end{bmatrix}\ </math>
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| And with minimum uncertainty:
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| <math>i\hbar\frac{\partial}{\partial t} \Psi(\mathbf{r},\,t) = \hat H \Psi(\mathbf{r},t)</math>
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Latest revision as of 15:58, 4 January 2022
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We are currently in the process of finalising the new image for
SolidWorks 2020.
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[math]\displaystyle{ E=mc^2 }[/math]
