A long copper tube of inner radius $R$ carries a current $i$. The magnetic field $B$ inside the tube is
  • A$\frac{{{\mu _0}i}}{{2\pi R}}$
  • B$\frac{{{\mu _0}i}}{{4\pi R}}$
  • C$\frac{{{\mu _0}i}}{{2R}}$
  • D
    Zero
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