As shown in the figure, a long straight conductor with semi-circular are of radius \(\frac{\pi}{10} m\) is carrying current \(I =3 A\). The magnitude of the magnetic field at the center \(O\) of the arc is :(The permeability of the vacuum \(=4 \pi \times 10^{-7} NA ^{-2}\) )
Remember the formula for the magnetic field due to a circular arc. Also, consider the direction and contribution of the magnetic field due to straight current carrying wires. Visualizing the magnetic field lines can be helpful.
\(6 \mu T\)
\(4 \mu T\)
\(3 \mu T\)
\(1 \mu T\)
Step 1: Determine the Magnetic Field Due to the Semicircular Arc
The magnetic field at the center of a circular arc of radius R carrying current I is given by:
\( B_c = \frac{\mu_0 I}{4 \pi R} \theta \)
where \( \mu_0 \) is the permeability of free space, and \( \theta \) is the angle subtended by the arc at the center in radians. For a semicircular arc, \( \theta = \pi \).
\( B_c = \frac{\mu_0 I}{4 R} \)
Step 2: Substitute the Given Values
Given \( I = 3 \, \text{A}, \, R = \frac{\pi}{10} \, \text{m}, \, \text{and} \, \mu_0 = 4 \pi \times 10^{-7} \, \text{N A}^{-2} \), we have:
\( B_c = \frac{(4 \pi \times 10^{-7})(3)}{4 \left(\frac{\pi}{10}\right)} \)
\( B_c = \frac{4 \pi \times 10^{-7} \times 3 \times 10}{4 \pi} \)
\( B_c = 3 \times 10^{-6} \, \text{T} = 3 \, \mu \text{T} \)
Step 3: Consider the Magnetic Field Due to the Straight Wires
The straight portions of the wire do not contribute to the magnetic field at point O. This is because the magnetic field lines due to an infinitely long straight wire form concentric circles around the wire. At the center of the semicircle, the straight sections are radial, so the magnetic field produced by them at point O will be perpendicular to the plane of the semicircle and thus won’t affect the field in the plane caused by the semicircular section.
Conclusion: The magnitude of the magnetic field at the center O is \( 3 \, \mu \text{T} \) (Option 3).
Let $ P_n = \alpha^n + \beta^n $, $ n \in \mathbb{N} $. If $ P_{10} = 123,\ P_9 = 76,\ P_8 = 47 $ and $ P_1 = 1 $, then the quadratic equation having roots $ \alpha $ and $ \frac{1}{\beta} $ is:
Moving charges generate an electric field and the rate of flow of charge is known as current. This is the basic concept in Electrostatics. Another important concept related to moving electric charges is the magnetic effect of current. Magnetism is caused by the current.
Region in space around a magnet where the Magnet has its Magnetic effect is called the Magnetic field of the Magnet. Let us suppose that there is a point charge q (moving with a velocity v and, located at r at a given time t) in presence of both the electric field E (r) and the magnetic field B (r). The force on an electric charge q due to both of them can be written as,
F = q [ E (r) + v × B (r)] ≡ EElectric +Fmagnetic
This force was based on the extensive experiments of Ampere and others. It is called the Lorentz force.