(i) a square coil, where each side of the square is $12a/16$.
(ii) a regular hexagonal coil, where each side of the hexagon is $12a/24$.
The magnetic dipole moments of the coil in each case respectively are:
This problem involves calculating the magnetic dipole moment for a current-carrying wire shaped into two different configurations: a square coil and a regular hexagonal coil. The magnetic dipole moment ($ \vec{m} $) of a current loop is a measure of its magnetic strength and orientation. Its magnitude is given by the formula $ m = NIA $, where $ N $ is the number of turns in the coil, $ I $ is the current flowing through the wire, and $ A $ is the area enclosed by one turn of the coil.
We are given a uniform conducting wire of total length $ L = 12a $ and resistance $ R $, carrying a current $ I $. We need to find the magnetic dipole moment for two cases:
The resistance $ R $ is provided but not needed for calculating the magnetic dipole moment. The key is to determine the number of turns ($ N $) and the area ($ A $) for each shape using the total wire length $ 12a $.
First, let's analyze the square coil.
Simplifying the expression for $ m_1 $: $ m_1 = \frac{4 \times 9}{16} I a^2 = \frac{36}{16} I a^2 = \frac{9}{4} I a^2 $.
Next, let's analyze the regular hexagonal coil.
Calculating the area $ A_2 $: $ A_2 = \frac{3\sqrt{3}}{2} \times \frac{a^2}{4} = \frac{3\sqrt{3}}{8} a^2 $.
Magnetic Dipole Moment ($ m_2 $): Using the formula $ m = NIA $, the magnetic dipole moment for the hexagonal coil is $ m_2 = N_2 I A_2 = 4 \times I \times \frac{3\sqrt{3}}{8} a^2 $.
Simplifying the expression for $ m_2 $: $ m_2 = \frac{4 \times 3\sqrt{3}}{8} I a^2 = \frac{12\sqrt{3}}{8} I a^2 = \frac{3\sqrt{3}}{2} I a^2 $.
The calculated magnetic dipole moments for the square coil and the hexagonal coil are:
Comparing these results with the given options, the correct pair is $ \frac{9}{4} I a^2 $ and $ \frac{3\sqrt{3}}{2} I a^2 $.
Which one of the following statements regarding magnetic field is NOT correct?
A positively charged particle projected towards east is deflected towards north by a magnetic field. The field may be:
The vector potential for an almost point like magnetic dipole located at the origin is \({\rm{A}}\, = \,\frac{{{\rm{\mu }}\,{\rm{sin}}\,{\rm{θ }}}}{{4{\rm{\pi }}{{\rm{r}}^2}}}\widehat ϕ \) , where (r, θ, ϕ) denote the spherical polar coordinates and \(\widehat \phi \) is the unit vector along ϕ . A particle of mass m and charge q, moving in the equatorial plane of the dipole, starts at time = t = 0 with an initial speed ν 0νand an impact parameter b. Its instantaneous speed at the point of closest approach is