(a) The statement "electric charge of a body is quantized" signifies that the charge of any object can only be an integer multiple of the elementary charge carried by electrons or protons. A body can't possess a charge that is a fraction of this elementary charge (like \(\frac{1}{2} e, \frac{3}{2} e\), etc.).
(b) At the macroscopic level, the total number of charges present in an object is extremely large compared to the magnitude of the elementary charge. Therefore, at this scale, we treat the distribution of charge within the object as continuous. This is why the concept of quantization of electric charge can be disregarded when dealing with macroscopic objects.
A dipole of moment \(\overrightarrow{p}\) is placed in uniform electric field \(\overrightarrow{E}\) then torque acting on it is given by : -
Four point charges \(q_A\)\( = 2 µC\), \(q_B\) \(= −5 µC\), \(q_C\) = 2 µC, and \(q_D\) \(= −5 µC\) are located at the corners of a square ABCD of side 10 cm. What is the force on a charge of 1 µC placed at the centre of the square?
Two large, thin metal plates are parallel and close to each other. On their inner faces, the plates have surface charge densities of opposite signs and of magnitude \(17.0 × 10^{−22} Cm^{-2}\). What is E:
(a) in the outer region of the first plate,
(b) in the outer region of the second plate, and (c) between the plates?