Magnetic body force on the medium, two ways
The same calculation run twice, side by side. Change anything on either side and the difference is shown output by output. This page is a link: both sets of numbers are in the address bar.
What changed
The two sides are the same. Change something on either.
| Output | A | B | B against A |
|---|---|---|---|
| fm Body force | 18850 N/m³ | 18850 N/m³ | same |
| Δp Pressure across the fringe | 471.2 Pa | 471.2 Pa | same |
Side A, with its numbers
LaTeX
18850\,\mathrm{N/m³} = \mu_0 \cdot 7.5\,\mathrm{kA/m} \cdot 2000000\,\mathrm{A/m²}, \qquad 471.2\,\mathrm{Pa} = 18850\,\mathrm{N/m³} \cdot 25\,\mathrm{mm}
- M itself depends on H inside the gradient (M = χ·H), so this is the force at the stated magnetisation, not a self-consistent one: across the fringe M falls with H and the true mean force is lower.
- Across 2.5 cm of fringe this comes to 471.2 Pa — 48.14 mm of water column. Set that against the loop's pressure drop: a coil end pumps only if it exceeds the loss round the loop.
Side B, with its numbers
LaTeX
18850\,\mathrm{N/m³} = \mu_0 \cdot 7.5\,\mathrm{kA/m} \cdot 2000000\,\mathrm{A/m²}, \qquad 471.2\,\mathrm{Pa} = 18850\,\mathrm{N/m³} \cdot 25\,\mathrm{mm}
- M itself depends on H inside the gradient (M = χ·H), so this is the force at the stated magnetisation, not a self-consistent one: across the fringe M falls with H and the true mean force is lower.
- Across 2.5 cm of fringe this comes to 471.2 Pa — 48.14 mm of water column. Set that against the loop's pressure drop: a coil end pumps only if it exceeds the loss round the loop.