Given: Two infinite line charges moving with velocity \( v \) in the same direction, separated by a distance \( d \). We are to find the condition when magnetic attraction balances electric repulsion. Let \( e \) be the speed of light in free space.
Concepts involved: - A moving line charge produces both electric and magnetic fields.
- Electric field causes repulsion between like charges.
- Magnetic field due to current causes attraction (since currents are in same direction).
- At equilibrium: Electric force = Magnetic force Electric Force per unit length: If linear charge density is \( \lambda \), then: \[ F_E = \frac{1}{2\pi \varepsilon_0} \cdot \frac{\lambda^2}{d} \]
Magnetic Force per unit length: Moving line charges act like current-carrying wires with current \( I = \lambda v \), so: \[ F_B = \frac{\mu_0}{2\pi} \cdot \frac{I^2}{d} = \frac{\mu_0}{2\pi} \cdot \frac{\lambda^2 v^2}{d} \]
Equating: \[ F_E = F_B \Rightarrow \frac{1}{2\pi \varepsilon_0} \cdot \frac{\lambda^2}{d} = \frac{\mu_0}{2\pi} \cdot \frac{\lambda^2 v^2}{d} \] Cancel \( \lambda^2 \), \( d \), \( 2\pi \): \[ \frac{1}{\varepsilon_0} = \mu_0 v^2 \Rightarrow v^2 = \frac{1}{\mu_0 \varepsilon_0} \Rightarrow v = \frac{1}{\sqrt{\mu_0 \varepsilon_0}} = e \]
Final Answer: \( v = e \)
A quantity \( X \) is given by: \[ X = \frac{\epsilon_0 L \Delta V}{\Delta t} \] where:
- \( \epsilon_0 \) is the permittivity of free space,
- \( L \) is the length,
- \( \Delta V \) is the potential difference,
- \( \Delta t \) is the time interval.
The dimension of \( X \) is the same as that of: