Estimate the magnetic field strength required at the $\mathrm{LHC}$ to make $7.0$ -TeV protons travel in a circle of circumference $27 \mathrm{~km}$. Start by deriving an expression, using Newton's second law, for the field strength $B$ in terms of the particle's momentum $p$, its charge $q$, and the radius $r$. Even though derived using classical physics, the expression is relativistically correct. (The estimate will come out much lower than the actual value of $8.33 \mathrm{~T}$. In the $\mathrm{LHC}$, the protons do not travel in a constant magnetic field; they move in straight-line segments between magnets.)