The magnetic force on a charged particle in a magnetic field is described by \(|\vec{F}| = q|\vec{u} \times \vec{B}|\).
Given: \( \vec{F} = 5e \hat{k} \, \text{N} \), \( q = -e \) (electron charge), \( \vec{u} = 3\hat{i} + 5\hat{j} \, \text{m/s} \), and \( \vec{B} = B_0 \hat{i} + 2B_0 \hat{j} \, \text{T} \).
The cross product \(\vec{u} \times \vec{B}\) is calculated as:
\[|\vec{u} \times \vec{B}| = \left|\begin{array}{ccc}\hat{i} & \hat{j} & \hat{k} \\ 3 & 5 & 0 \\ B_0 & 2B_0 & 0 \end{array}\right|\]
Evaluating the determinant yields \(\hat{0}\hat{i} - \hat{0}\hat{j} + (3 \cdot 2B_0 - 5 \cdot B_0) \hat{k}\):
\[|\vec{u} \times \vec{B}| = (6B_0 - 5B_0)\hat{k} = B_0\hat{k}\]
Therefore, \(|\vec{F}| = e|\vec{u} \times \vec{B}| = eB_0\).
Since \(|\vec{F}| = 5e\), we have:
\[eB_0 = 5e\]
Solving for \(B_0\):
\[B_0 = 5\]
The calculated value \(B_0 = 5 \, \text{T}\) is consistent with the given range \([5, 5]\).