Differences
This shows you the differences between two versions of the page.
Both sides previous revision Previous revision | Next revisionBoth sides next revision | ||
184_notes:examples:week12_force_between_wires [2018/07/19 13:32] – curdemma | 184_notes:examples:week12_force_between_wires [2021/07/08 13:16] – schram45 | ||
---|---|---|---|
Line 39: | Line 39: | ||
When we take the cross product of $d\vec{l}_2$ and $B_1$, this gives | When we take the cross product of $d\vec{l}_2$ and $B_1$, this gives | ||
$$\text{d}\vec{l}_2 \times \vec{B}_1 = \text{d}y \hat{y} \times \frac{\mu_0 I_1}{2 \pi R} \hat{z}$$ | $$\text{d}\vec{l}_2 \times \vec{B}_1 = \text{d}y \hat{y} \times \frac{\mu_0 I_1}{2 \pi R} \hat{z}$$ | ||
- | $$\text{d}\vec{l}_2 \times \vec{B}_1 = \frac{\mu_0 I_1}{2 \pi R}\text{d}y \biggl(\hat{x}\times\hat{z}\biggr)$$ | + | $$\text{d}\vec{l}_2 \times \vec{B}_1 = \frac{\mu_0 I_1}{2 \pi R}\text{d}y \biggl(\hat{y}\times\hat{z}\biggr)$$ |
$$\text{d}\vec{l}_2 \times \vec{B}_1 = \frac{\mu_0 I_1}{2 \pi R}\text{d}y \hat{x}$$ | $$\text{d}\vec{l}_2 \times \vec{B}_1 = \frac{\mu_0 I_1}{2 \pi R}\text{d}y \hat{x}$$ | ||