\mathrm{Q}=\mathrm{n}\mathrm{e}
\mathrm{I}=\frac{\mathrm{Q}}{\mathrm{t}}
\mathrm{V}=\frac{\mathrm{W}}{\mathrm{Q}}
\mathrm{V}_{1}-\mathrm{V}_{2}=\frac{\mathrm{W}}{\mathrm{Q}}
Statement: At constant temperature, the current through an ohmic conductor is directly proportional to the potential difference across it.
\mathrm{V}=\mathrm{I}\mathrm{R}