Question
Question: A straight wire of mass 200 g and length 1.5 m carries a current of 2 A. It is suspended in mid-air ...
A straight wire of mass 200 g and length 1.5 m carries a current of 2 A. It is suspended in mid-air by a uniform horizontal magnetic field B. The magnitude of B (in tesla) is:
Solution
As we all can see that the force acting on a current-carrying wire under a uniform magnetic field is equal to the weight of the wire because the wire is in equilibrium and has no acceleration so it is not moving.
Complete step by step answer:
Refer to the figure given below:
In this figure, ‘i’ is the current flowing in the conductor and the rest are the two forces acting on it.
The force on a current-carrying wire under uniform magnetic field is given by:
F=BiLsinθ
Where F is the force, B is the magnetic field, L is the length of the wire, and θ is the angle between the current direction and magnetic field direction.
Here, we can see that the direction of current is perpendicular to the magnetic field B horizontally, hence the angle θ=90∘.
Hence the above equation becomes,
F=BiL
As we know that, in the position of suspension, the magnetic force becomes equal to the weight of the wire. Therefore, the new equilibrium condition becomes
BiL=mg………………...… (i)
Here m is the mass of the wire, and g is the acceleration due to gravity.
We will now substitute m=200g, L=1.5m, i=2A and g=9.8m/s2 in equation (i) to find the value of B.
⇒B×2A×1.5m=200g×9.8m/s2
⇒B×2A×1.5m=200×10−3kg×9.8m/s2
⇒B=0.65T
Therefore, the magnitude of the magnetic field B in tesla is 0.65T.
Note:
- We must be aware that the force on a current-carrying conductor can also be found out using the formula F=BQv. Here F is the force, B is the magnetic field, Q is the charge in motion and v is the velocity of the charge and this is also known as Lenz law.
- We all have studied that Fleming’s left-hand rule is used to describe the force on a current-carrying conductor placed at right angles to a magnetic field. The current-carrying conductor should be of ferromagnetic material.