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A solenoid $60 \mathrm{~cm}$ long and of radius, $4.0 \mathrm{~cm}$ has 3 layers of windings of 300 turns each. A $2.0 \mathrm{~cm}$ long wire of mass $2.5 \mathrm{~g}$ lies inside the solenoid (near its centre) normal to its axis; both the wire and the axis of the solenoid are in the horizontal plane. The wire is connected through two leads parallel to the axis of the solenoid to an external battery which supplies a current of $6.0 \mathrm{~A}$ in the wire. What value of current (with an appropriate sense of circulation) in the windings of the solenoid can support the weight of the wire? $\mathrm{g}=9.8 \mathrm{~m} \mathrm{~s}^{-2}$.

Length of the solenoid is given as I $=60 \mathrm{~cm}$

Layers of windings is $3$

Each layer has 300 turns

Number of turns per unit length, $n=(3 \times 300) / 0.6=1500 \mathrm{~m}^{-1}$

Inside the solenoid, magnetic field is given by, $\mathrm{B}=\mu_{0} \mathrm{nl}$

$\mu_{0}=4 \pi \times 10^{-7} \mathrm{~T}$

$B=\left(4 \pi \times 10^{-7}\right) \times 1500 \times 1$

$=6 \pi \times 10^{-4} \mid$

Force due to magnetic field is given by,
$F=\mid$ ‘Bl

$l^{\prime}=$ Current in the wire $=6 \mathrm{~A}$

I $=$ length of the wire $=2 \mathrm{~cm}$

When the force due to the magnetic field within the solenoid balances the weight of the wire, the windings of the solenoid would sustain the weight of the wire.

$\left.\right|^{\prime} B \mid=m g$

$m=$ mass of the wire $=2.5 \mathrm{~g}$

$\mathrm{B}=\mathrm{mg} / \mathrm{l}^{\prime} \mid$

From the previous equation (1) we get,

$6 \pi \times 10^{-4} \mathrm{l}=\mathrm{mg} / \mathrm{l}^{\prime} \mid$

$\Rightarrow \mathrm{I}=\mathrm{mg} /\left(6 \pi \times 10^{-4}\right) \mathrm{l}^{\prime} \mid$

$I=\frac{2.5 \times 10^{-3} \times 9.8}{6 \times 0.02 \times 4 \pi \times 10^{-7} \times 1500}=108.37 \mathrm{~A}$

A current of $108.37 \mathrm{~A}$ will support the wire