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A straight wire of mass \(200 \mathrm{gm}\) and length \(1.5\) meter carries a current of 2 Amp. It is suspended in mid-air by a uniform horizontal magnetic field B. [take \(\left.\mathrm{g}=10 \mathrm{~m} / \mathrm{s}^{2}\right]\). The \(\mathrm{B}\) is (a) \(\overline{(2 / 3) \text { tes } 1 a}\) (b) \((3 / 2)\) tesla (c) \((20 / 3)\) tesla (d) (3/20) tesla

Short Answer

Expert verified
The magnetic field B required to suspend the wire in mid-air is (a) \(\frac{2}{3} \text{ tesla}\).

Step by step solution

01

Convert the mass of the wire to kg

Since the mass of the wire is given in grams, we need to convert it to kg for our calculations. To do so, divide the mass by 1000. \(m = \frac{200}{1000} kg = 0.2 kg\)
02

Calculate the gravitational force acting on the wire

The gravitational force acting on the wire (its weight) can be found using the formula: \(F_g = m \cdot g\) where m is the mass of the wire and g is the acceleration due to gravity (given as 10 m/s²). \(F_g = (0.2 kg)(10 \frac{m}{s^2}) = 2 N\)
03

Write down the formula for the magnetic force on the wire

The magnetic force F_B acting on a current-carrying wire is given by the formula: \(F_B = B \cdot I \cdot L\) where B is the magnetic field, I is the current passing through the wire, and L is the length of the wire.
04

Equate the magnetic force to the gravitational force

Since the magnetic force is suspending the wire in mid-air, it must be equal to the gravitational force acting on the wire: \(F_B = F_g\)
05

Solve for the magnetic field B

Substitute the known values in the equation: \(B \cdot I \cdot L = F_g\) \(B \cdot (2 A) \cdot (1.5 m) = 2 N\) Now, solve for B: \(B = \frac{2 N}{(2 A)(1.5 m)} = \frac{2}{3} T\) So the magnetic field B required to suspend the wire in mid-air is (a) \(\frac{2}{3} \text{ tesla}\).

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Most popular questions from this chapter

A bar magnet having a magnetic moment of \(2 \times 10^{4} \mathrm{JT}^{-1}\) is free to rotate in a horizontal plane. A horizontal magnetic field \(\mathrm{B}=6 \times 10^{-4}\) Tesla exists in the space. The work done in taking the magnet slowly from a direction parallel to the field to a direction \(60^{\circ}\) from the field is (a) \(0.6 \mathrm{~J}\) (b) \(12 \mathrm{~J}\) (c) \(6 \mathrm{~J}\) (d) \(2 \mathrm{~J}\)

\(\mathrm{A}\) bar magnet of length \(10 \mathrm{~cm}\) and having the pole strength equal \(10^{3} \mathrm{Am}\) to is kept in a magnetic field having magnetic induction (B) equal to \(4 \pi \times 10^{3}\) tesla. It makes an angle of \(30^{\circ}\) with the direction of magnetic induction. The value of the torque acting on the magnet is Joule. (a) \(2 \pi \times 10^{-7}\) (b) \(2 \pi \times 10^{5}\) (c) \(0.5\) (d) \(0.5 \times 10^{2}\)

The magnetic induction at a point \(P\) which is at a distance \(4 \mathrm{~cm}\) from a long current carrying wire is \(10^{-8}\) tesla. The field of induction at a distance \(12 \mathrm{~cm}\) from the same current would be tesla. (a) \(3.33 \times 10^{-9}\) (b) \(1.11 \times 10^{-4}\) (c) \(3 \times 10^{-3}\) (d) \(9 \times 10^{-2}\)

Two thin long parallel wires separated by a distance \(\mathrm{y}\) are carrying a current I Amp each. The magnitude of the force per unit length exerted by one wire on other is (a) \(\left[\left(\mu_{0} I^{2}\right) / y^{2}\right]\) (b) \(\left[\left(\mu_{o} I^{2}\right) /(2 \pi \mathrm{y})\right]\) (c) \(\left[\left(\mu_{0}\right) /(2 \pi)\right](1 / y)\) (d) $\left[\left(\mu_{0}\right) /(2 \pi)\right]\left(1 / \mathrm{y}^{2}\right)$

A He nucleus makes a full rotation in a circle of radius \(0.8\) meter in $2 \mathrm{sec}\(. The value of the mag. field \)\mathrm{B}$ at the centre of the circle will be \(\quad\) Tesla. (a) \(\left(10^{-19} / \mu_{0}\right)\) (b) \(10^{-19} \mu_{0}\) (c) \(2 \times 10^{-10} \mathrm{H}_{0}\) (d) \(\left[\left(2 \times 10^{-10}\right) / \mu_{0}\right]\)

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