When a current-carrying coil is placed in a magnetic field, it experiences a magnetic torque. This is the fundamental principle behind electric motors and moving coil galvanometers.
The Physical Setup
Imagine a rectangular coil with N turns, carrying a current I, placed in a uniform magnetic field B
The problem states that the coil is held parallel to the magnetic field.
This phrasing is a classic trap! The angle θ in our torque formula is not the angle between the coil's plane and the field, but rather the angle between the coil's area vector A and the magnetic field B. Since the area vector is always perpendicular to the plane of the coil, a coil parallel to the field means its area vector is perpendicular to the field. Therefore, θ=90∘.
The Master Equation
The magnetic torque
τ acting on the coil is given by the cross product of its magnetic dipole moment
m and the magnetic field
B:
τ=m×B
Since the magnitude of the magnetic moment is
m=NIA, the magnitude of the torque becomes:
τ=NIABsinθ
Because
θ=90∘,
sin90∘=1, and the torque is at its maximum value:
τ=NIAB
The Final Calculation
We are given the following values:
- Torque, τ=1.5 N-m
- Number of turns, N=500
- Current, I=0.5 A
- Area, A=3×10−4 m2
We need to find the magnetic field strength
B. Rearranging our master equation to solve for
B:
B=NIAτ
Substituting the known values into the equation:
B=500×0.5×3×10−41.5
Let's simplify the denominator.
500×0.5=250, and
250×3=750. So we have:
B=750×10−41.5
Bringing the
10−4 to the numerator makes it
104 or
10000:
B=7501.5×10000=75015000
B=20 T
The required magnetic field strength is an astonishing 20 Tesla! In reality, such a strong magnetic field is typically only found in massive superconducting electromagnets, like those used in MRI machines or particle accelerators. A typical galvanometer operates on a fraction of a Tesla.