
To find the magnetic force on the wire, we need to consider each part of the wire separately: the semicircular portion and the two straight sections.
Thus, the total force on the wire is the force due to the semicircular part alone:
\(\vec{F} = \vec{F}_{\text{semicircle}} + \vec{F}_{\text{straight}} = i (2R) B_0 \hat{k}\)
This force directed in the negative \(\hat{j}\) direction, based on the right-hand rule for a circular loop's magnetic force.
Therefore, the magnetic force on the wire is:
\(-2 i B R \hat{j}\)
The correct answer is:
\( -2 i B R \hat{j} \)
The wire forms a semicircular arc with radius \( R \) and length \( l = 2R \).
Given that the direction of the magnetic field \( \vec{B} \) is in the \( +\hat{k} \) direction.
The magnetic force \( \vec{F} \) is given by:
\[ \vec{F} = i \vec{l} \times \vec{B} \]
Substituting the values:
\[ \vec{F} = -2iRB \hat{j} \]
Three long straight wires carrying current are arranged mutually parallel as shown in the figure. The force experienced by \(15\) cm length of wire \(Q\) is ________. (\( \mu_0 = 4\pi \times 10^{-7}\,\text{T m A}^{-1} \)) 

Let \( \alpha = \dfrac{-1 + i\sqrt{3}}{2} \) and \( \beta = \dfrac{-1 - i\sqrt{3}}{2} \), where \( i = \sqrt{-1} \). If
\[ (7 - 7\alpha + 9\beta)^{20} + (9 + 7\alpha - 7\beta)^{20} + (-7 + 9\alpha + 7\beta)^{20} + (14 + 7\alpha + 7\beta)^{20} = m^{10}, \] then the value of \( m \) is ___________.