To maintain the electron's straight trajectory, the magnetic and electric forces must be balanced. The magnetic force is given by \(F_{\text{magnetic}}=qvB\), and the electric force by \(F_{\text{electric}}=qE\). Equating these forces, \(qvB=qE\), yields \(E=vB\).
First, the electron's velocity \(v\) is determined from its kinetic energy:
\(K.E.=\frac{1}{2}mv^2=5 \, \text{eV}=5 \times 1.6 \times 10^{-19} \, \text{J}\).
Rearranging the equation to solve for \(v^2\):
\(v^2=\frac{2 \times 5 \times 1.6 \times 10^{-19}}{9 \times 10^{-31}}\)
The calculated velocity \(v\) is:
\(v=\sqrt{\frac{16 \times 10^{-19}}{9 \times 10^{-31}}}\approx1.32 \times 10^6 \, \text{ms}^{-1}\)
Next, the electric field \(E\) is calculated using \(E=vB\), with \(B=3 \, \mu\text{T}=3 \times 10^{-6} \, \text{T}\):
\(E=1.32 \times 10^6 \times 3 \times 10^{-6}=3.96 \, \text{NC}^{-1}\)
The computed electric field \(E\approx3.96 \, \text{NC}^{-1}\) is within the specified range of 4,4, confirming its validity. The balance of electromagnetic forces ensures the electron's path remains unobstructed.