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Electric Charges and Fields

2021, BDS Learning Application

In practice, we deal with charges much greater in magnitude than the charge on an electron, so we can ignore the quantum nature of charges and imagine that the charge is spread in a region in a continuous manner. Such a charge distribution is known as a continuous charge distribution. Calculation of the force on a charge due to a continuous charge distribution As shown in figure consider a point charge q0 lying near a region of continuous charge distribution. This continuous charge distribution can be imagined to consist of a large number of small charges dq. According to Coulomb's law, the force on point charge qo due to small charge dq is Force on a point charge q0 due to a continuous charge distribution.

Electric Charges and Fields CONTINUOUS CHARGE DISTRIBUTION In practice, we deal with charges much greater in magnitude than the charge on an electron, so we can ignore the quantum nature of charges and imagine that the charge is spread in a region in a continuous manner. Such a charge distribution is known as a continuous charge distribution. Calculation of the force on a charge due to a continuous charge distribution As shown in figure consider a point charge q0 lying near a region of continuous charge distribution. This continuous charge distribution can be imagined to consist of a large number of small charges dq. According to Coulomb's law, the force on point charge qo due to small charge dq is Force on a point charge q0 due to a continuous charge distribution. Where = , is a unit vector pointing from the small charge dq towards the point charge qo. By the principle of superposition, the total force on charge qo will be the vector sum of the forces exerted by all such small charges and is given by Or = Different types of continuous charge distributions. There are three types of continuous charge distributions (a) Volume charge distribution. It is a charge distribution spread over a three dimensional volume or region V of space, as shown in Figure. We define the volume charge density at any point in this volume as the charge contained per unit volume at that point, i.e., = Volume charge distribution The SI unit for volume charge distribution is coulomb per cubic meter (Cm-3). For example, if a charge q is distributed over the entire volume of a sphere of radius R, then its volume charge density is C The charge contained in volume dV is dq = p dV Total electrostatic force exerted on charge q0 due to the entire volume V is given by = = dV Electric field due to the volume charge distribution at the location of charge q0 is = = dV (b) Surface charge distribution. It is a charge distribution spread over a two-dimensional surface S in space, as shown in Figure. We define the surface charge density at any point on this surface as the charge per unit area at that point, i.e., = The SI unit for is Cm-2. Surface charge distribution For example, if a charge q is uniformly distributed over the surface of a spherical conductor of radius R, then its surface charge density is = Cm-2 The charge contained in small area dS is dq = dS Total electrostatic force exerted on charge q0 due to the entire surface S is given by = Electric field due to the surface charge distribution at the location of charge q0 is = = (c) Line charge distribution. It is a charge distribution along a one-dimensional curve or line L in space, as shown in Figure. We define the line charge density at any point on this line as the charge per unit length of the line at that point, i.e., = The SI unit for is Cm-1. Line charge distribution. For example, if a charge q is uniformly distributed over a ring of radius R, then its linear charge density is λ = Cm-1 The charge contained in small length dL is dq = λ dL Total electrostatic force exerted on charge q0 due to the entire length L is given by = dL Electric field due to the line charge distribution at the location of charge q0 is = = The total electric field due to a continuous charge distribution is given by = + + = (d) General charge distribution. A general charge distribution consists of continuous as well as discrete charges. Hence total electric field due to a general charge distribution at the location of charge q0 is given by = + = In all the above cases, is a variable unit vector directed from each point of the volume, surface or line charge distribution towards the location of the point charge q0.