
$\mathrm{T}=2 \pi \sqrt{\frac{\mathrm{I}}{\mathrm{C}}}=2 \pi \sqrt{\frac{(\mathrm{B}-\mathrm{mg}) \mathrm{L}}{\mathrm{m} \theta \mathrm{L}^{2}}}$
$\mathrm{T}=2 \pi \sqrt{\frac{\rho_{\mathrm{air}} \mathrm{V}_{\mathrm{g}}-\rho_{\mathrm{He}} \mathrm{V}_{\mathrm{g}}}{\rho_{\mathrm{air}} \mathrm{V}_{\mathrm{L}}}}$
$[1]$ The magnetic field strength may have been increased while the particle was travelling in air
$[2]$ The particle lost energy by ionising the air
$[3]$ The particle lost charge by ionising the air



