A long solenoid is fabricated to closely winding wire of radius $0.5\,mm$ over a cylindrical frame so that the successive turns nearly touch each other, the magnetic field at the centre of solenoid if it carries a current of $5\,A$
A$2\pi \, \times \,{10^{ - 2}}\,T$
B$2\pi \, \times \,{10^{ - 3}}\,T$
C$2\pi \, \times \,{10^{ - 4}}\,T$
D$2\pi \, \times \,{10^{ - 5}}\,T$
Medium
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B$2\pi \, \times \,{10^{ - 3}}\,T$
b $\Rightarrow \quad \mathrm{B}=\mu_{0} \frac{\mathrm{N}}{\mathrm{L}} \times \mathrm{I}$
$\mathrm{N} \times 2 \mathrm{r}=\mathrm{L} \quad(\mathrm{r}=\text { radius of wire })$
so $\frac{\mathrm{N}}{\mathrm{L}}=\frac{1}{2 \mathrm{r}}$
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