
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:
\[ \vec{F} = -2iRB \hat{j} \]
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,



What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)