Potential energy between the two $+q$ charges: $$U_1 = \frac{1}{4\pi\epsilon_0} \frac{q \cdot q}{2a} = \frac{q^2}{8\pi\epsilon_0 a}$$ Potential energy between the first $+q$ charge and the $-2q$ charge: $$U_2 = \frac{1}{4\pi\epsilon_0} \frac{q \cdot (-2q)}{a} = -\frac{2q^2}{4\pi\epsilon_0 a} = -\frac{4q^2}{8\pi\epsilon_0 a}$$ Potential energy between the second $+q$ charge and the $-2q$ charge: $$U_3 = \frac{1}{4\pi\epsilon_0} \frac{q \cdot (-2q)}{a} = -\frac{2q^2}{4\pi\epsilon_0 a} = -\frac{4q^2}{8\pi\epsilon_0 a}$$
The total potential energy $U$ is the sum of $U_1$, $U_2$, and $U_3$: $$U = U_1 + U_2 + U_3$$ $$U = \frac{q^2}{8\pi\epsilon_0 a} - \frac{4q^2}{8\pi\epsilon_0 a} - \frac{4q^2}{8\pi\epsilon_0 a}$$ $$U = \frac{(1 - 4 - 4)q^2}{8\pi\epsilon_0 a}$$ $$U = -\frac{7q^2}{8\pi\epsilon_0 a}$$ Therefore, the potential energy of the system is $-\frac{7q^2}{8\pi\epsilon_0 a}$.
A point charge $ +q $ is placed at the origin. A second point charge $ +9q $ is placed at $ (d, 0, 0) $ in Cartesian coordinate system. The point in between them where the electric field vanishes is:
A small bob of mass 100 mg and charge +10 µC is connected to an insulating string of length 1 m. It is brought near to an infinitely long non-conducting sheet of charge density \( \sigma \) as shown in figure. If the string subtends an angle of 45° with the sheet at equilibrium, the charge density of sheet will be :
Consider two infinitely large plane parallel conducting plates as shown below. The plates are uniformly charged with a surface charge density \( +\sigma \) and \( -\sigma \). The force experienced by a point charge \( +q \) placed at the mid point between the plates will be:
The correct IUPAC name of \([ \text{Pt}(\text{NH}_3)_2\text{Cl}_2 ]^{2+} \) is: