The change in electrostatic energy is calculated by the work done by the external electric field on the system. The energy change in a system of charges due to an external electric field \( \vec{E} \) is given by: \[ \Delta U = \sum_i q_i \vec{E} \cdot \vec{r}_i \] where \( \vec{r}_i \) is the position vector of the charge \( q_i \).
The external electric field is radial, directed along the position vectors of the charges, and its magnitude is given by \( E = \frac{A}{r^2} \).
The electric field at each position is: \[ E_1 = \frac{A}{r_1^2} = \frac{3 \times 10^5}{(0.03)^2} \, \text{V/m} = 3.33 \times 10^7 \, \text{V/m} \] and similarly, \[ E_2 = \frac{A}{r_2^2} = 3.33 \times 10^7 \, \text{V/m} \]
The work done by the external electric field is: \[ W_1 = q_1 E_1 r_1 = (5 \times 10^{-6}) \times (3.33 \times 10^7) \times (0.03) \] \[ W_1 = 4.995 \, \text{J} \] Similarly, for \( q_2 \): \[ W_2 = q_2 E_2 r_2 = (-1 \times 10^{-6}) \times (3.33 \times 10^7) \times (0.03) \] \[ W_2 = -0.999 \, \text{J} \]
The total work done by the external electric field on the system is the sum of the individual works: \[ \Delta U = W_1 + W_2 = 4.995 + (-0.999) = 3.996 \, \text{J} \]
The change in the electrostatic energy of the system due to the external electric field is \( \boxed{3.996 \, \text{J}} \).
Two batteries of emf's \(3V \& 6V\) and internal resistances 0.2 Ω \(\&\) 0.4 Ω are connected in parallel. This combination is connected to a 4 Ω resistor. Find:
(i) the equivalent emf of the combination
(ii) the equivalent internal resistance of the combination
(iii) the current drawn from the combination