To solve the problem, we need to determine the magnitude and direction of the electric field \( \vec{E} \) that will prevent the electron from deflecting in the presence of a magnetic field \( \vec{B} \). When no deflection occurs, the magnetic force equals the electric force.
Step 1: Determine the magnetic force (\( F_B \)) on the electron.
The formula for the magnetic force is given by:
\( F_B = qvB \sin\theta \)
Since \( \vec{B} \) is perpendicular to the velocity of the electron (\( \theta = 90^\circ \)), \( \sin\theta = 1 \). Therefore:
\( F_B = qvB \)
Insert the known values:
- Electron charge (\( q \)) = \( 1.6 \times 10^{-19} \) C
- Speed of electron (\( v \)) = \( \frac{c}{100} = \frac{3 \times 10^8}{100} = 3 \times 10^6 \) m/s
- Magnetic field (\( B \)) = \( 9 \times 10^{-4} \) T
Substitute the values:
\( F_B = (1.6 \times 10^{-19})(3 \times 10^6)(9 \times 10^{-4}) \)
\( F_B = 4.32 \times 10^{-16} \) N
Step 2: Determine the electric field (\( \vec{E} \)) to balance this force.
To ensure no deflection, the electric force \( F_E \) must equal \( F_B \):
\( F_E = qE = F_B \)
\( E = \frac{F_B}{q} \)
Substitute known values:
\( E = \frac{4.32 \times 10^{-16}}{1.6 \times 10^{-19}} \)
\( E = 2.7 \times 10^2 \) V/m
Conclusion:
For the electron not to deflect, the electric field \( \vec{E} \) must be perpendicular to \( \vec{B} \), and its magnitude is \( 2.7 \times 10^2 \) V/m. Hence, the correct choice is: \( \vec{E} \) is perpendicular to \( \vec{B} \) and its magnitude is \( 2.7 \times 10^2 \) V/m.