Problem Analysis:
Key Concept:
The density of electric field lines (number of lines per unit area perpendicular to the lines) is proportional to the magnitude of the electric field strength. Therefore, where the lines are closer together, the field is stronger, and where they are farther apart, the field is weaker. Specifically, the electric field strength $E$ is inversely proportional to the separation $d$ between the lines (assuming a uniform distribution in the perpendicular dimension shown):
$E \propto \frac{1}{d}$
This implies that the ratio of electric fields at two points is inversely proportional to the ratio of the separations at those points:
$\frac{E_B}{E_A} = \frac{d_A}{d_B}$
Calculations:
$\frac{E_B}{E_A} = \frac{d_A}{d_B}$
Substitute $d_B = 2 d_A$:
$\frac{E_B}{E_A} = \frac{d_A}{2 d_A} = \frac{1}{2}$
$E_B = \frac{1}{2} E_A$
Given $E_A = 40 \, \text{Vm}^{-1}$:
$E_B = \frac{1}{2} \times 40 \, \text{Vm}^{-1} = 20 \, \text{Vm}^{-1}$
$F_B = q \times E_B$
Substitute $q = 20 \, \mu\text{C} = 20 \times 10^{-6} \, \text{C}$ and $E_B = 20 \, \text{Vm}^{-1}$ (Note: $1 \, \text{Vm}^{-1} = 1 \, \text{N/C}$):
$F_B = (20 \times 10^{-6} \, \text{C}) \times (20 \, \text{N/C})$
$F_B = 400 \times 10^{-6} \, \text{N}$
$F_B = 4 \times 10^2 \times 10^{-6} \, \text{N}$
$F_B = 4 \times 10^{-4} \, \text{N}$
The final answer is (A): \(4 \times 10^{-4} N\).
Electric Field is the electric force experienced by a unit charge.
The electric force is calculated using the coulomb's law, whose formula is:
\(F=k\dfrac{|q_{1}q_{2}|}{r^{2}}\)
While substituting q2 as 1, electric field becomes:
\(E=k\dfrac{|q_{1}|}{r^{2}}\)
SI unit of Electric Field is V/m (Volt per meter).