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A particle of charge $\mathit{q}$ and mass $\mathit{m}$ moves in a circular path of radius $\mathit{r}$ in a uniform magnetic field $\mathit{B}$.

The angular momentum of the particle can be described by the expression:

A

$\mathit{eBr}$

B

$\mathit{2eBr}$

C

$\mathit{eBr^2}$

D

$\mathit{eBr m_p}$

E

$\mathit{2eBr m_p}$

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