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184_notes:b_current [2020/08/23 21:42] – dmcpadden | 184_notes:b_current [2021/06/16 18:53] – [Magnetic field from Many Charges] bartonmo | ||
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We can now use the definition of [[184_notes: | We can now use the definition of [[184_notes: | ||
$$\vec{B}_{tot}= \int \frac{\mu_0}{4 \pi}\frac{I \cdot d\vec{l}\times \hat{r}}{r^2}$$ | $$\vec{B}_{tot}= \int \frac{\mu_0}{4 \pi}\frac{I \cdot d\vec{l}\times \hat{r}}{r^2}$$ | ||
- | **Note that $I$ here is the //conventional// current**, not the electron current. Otherwise many of the pieces of this equation would be what you expected: | + | **Note that $I$ here is the conventional current, not the electron current**. Otherwise many of the pieces of this equation would be what you expected: |
[{{ 184_notes: | [{{ 184_notes: |