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displays, which can be jarring. In time, presumably MathJax will replace the PNG math display, and then we'll have a whole new bunch of complaints and preferences. For now, the simplest is to stick to making the style consistent within the article. —
992:{\displaystyle \mathrm {d} {\star \mathbf {F} }={\frac {1}{6}}{F^{\alpha \beta }}_{;\alpha }{\sqrt {-g}}\,\varepsilon _{\beta \gamma \delta \alpha }\mathrm {d} x^{\gamma }\wedge \mathrm {d} x^{\delta }\wedge \mathrm {d} x^{\alpha }=\mathbf {J} ,}
829:{\displaystyle \mathrm {d} {\star \mathbf {F} }={\frac {1}{6}}{F^{\alpha \beta }}_{;\alpha }{\sqrt {-g}}\,\varepsilon _{\beta \gamma \delta \eta }\mathrm {d} x^{\gamma }\wedge \mathrm {d} x^{\delta }\wedge \mathrm {d} x^{\eta }=\mathbf {J} ,}
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I think this is one of those instances where preferences differ (I've seen people making changes in both directions). People who have default browser serif and sans-serif fonts that work well together will often prefer the inline
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I don't understand the point of the math template for the inline text - it simply disrupts the font appearance between arial and whatever the math template font is. For things like:
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I think because our dimension is composed of four spacetime, we should use four coordinate indices. But I'm still not sure about converting, especially for the order of
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which is far cleaner and less to write with no loss of continuity... For this article I will change math to hmtl (inline symbols, not displayed formulae).
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is the current per unit area, also a function of time and position. The units used above are the standard
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is the current per unit area, also a function of time and position. The units used above are the standard
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Knowledge. If you would like to participate, please visit the project page, where you can join
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is this a mistake? should it say "and the three components of the magnetic vector potential" ?
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Also the entire section on covariant tensor forms - see the same link.
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I will remove the relativistic material from this article to
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Merge banners to be removed, no favour, one opposition.
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Covariant formulation of classical electromagnetism
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1023::
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