
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:
\[ \vec{F} = -2iRB \hat{j} \]

Nature of compounds TeO₂ and TeH₂ is___________ and ______________respectively.