The magnetic force on a charged particle moving through a magnetic field is given by the formula:
\(|\vec{F}| = q|\vec{u} \times \vec{B}|\)
Given:\( \vec{F} = 5e \hat{k} \, \text{N} \), \( q = -e \) (charge of electron), \( \vec{u} = 3\hat{i} + 5\hat{j} \, \text{m/s} \), and \( \vec{B} = B_0 \hat{i} + 2B_0 \hat{j} \, \text{T} \).
Calculate cross product \(\vec{u} \times \vec{B}\):
\(|\vec{u} \times \vec{B}| = \left|\begin{array}{ccc}\hat{i} & \hat{j} & \hat{k} \\ 3 & 5 & 0 \\ B_0 & 2B_0 & 0 \end{array}\right|\)
The determinant results in \(\hat{0}\hat{i} - \hat{0}\hat{j} + (3 \cdot 2B_0 - 5 \cdot B_0) \hat{k}\):
\(|\vec{u} \times \vec{B}| = (6B_0 - 5B_0)\hat{k} = B_0\hat{k}\)
Thus, \(|\vec{F}| = e|\vec{u} \times \vec{B}| = eB_0\)
Since \(|\vec{F}| = 5e\), equating gives:
\(eB_0 = 5e\)
Solving for \(B_0\), we find:
\(B_0 = 5\)
The solution \(B_0 = 5 \, \text{T}\) is within the given range \([5, 5]\).
The magnetic force is given by:
\[ \vec{F} = q (\vec{v} \times \vec{B}) \]
Substituting the values:
\[ 5e \hat{k} = e \left( 3\hat{i} + 5\hat{j} \right) \times \left( B_0 \hat{i} + 2B_0 \hat{j} \right) \]
Calculating the cross product:
\[ 5e \hat{k} = e \left( 6B_0 \hat{k} - 5B_0 \hat{k} \right) \]
Simplifying:
\[ 5e \hat{k} = e B_0 \hat{k} \]
Therefore:
\[ B_0 = 5T \]
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 : \(A_2 \rightleftharpoons 2A\)