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 Conductors in electrostatic field § 1 of the The charge distribution in the conductor. The connection between the field intensity at the surface of the conductor and the surface charge density Free charges in the conductor can move under the influence of an arbitrarily small force. Therefore, for the balance of the charges in the conductor must meet the following conditions: Field intensity inside the conductor must be zero , since ie potential within the conductor must be constant. Field intensity on surface of the conductor must be perpendicular to the surface Consequently, the surface charge of the conductor at equilibrium is an equipotential. At equilibrium, the charges in any place inside the conductor can not be excess charges - they are distributed over the surface of a conductor with a density σ. Consider a closed surface in the form of a cylinder whose generators are perpendicular to the surface of the conductor. On the surface of the conductor are free charges with surface density σ. Because inside a conductor there are no charges, the flow through the surface of the cylinder inside the conductor is zero. The flow through the top of the cylinder outside the a conductor on the Gauss theorem is equal    ie electric displacement vector equal to the surface density of free charges of a conductor or  II. In making an uncharged conductor to an external electrostatic field his free charges will move: positive - on the field, negative - against the field. Then on one side of the conductor will accumulate positive and the other negative charges. These charges are said to be induced. The redistribution of the charges will be as long as the intensity in the conductor becomes zero, and the line intensity outside of the conductor will be the perpendicular to the surface. Induced charges appear on the conductor due to the displacement, ie are surface density charges and shifted as is therefore called the electric displacement vector.   § 2 Capacitance conductors. Capacitors I. Secluded called conductors, far from other conductors bodies charges. The potential of such a conductor is directly proportional to the charge on it From experience, it follows that different conductors, being equally charged Q1 = Q2 takes various potentials φ1 ≠φ2 due to the different shapes, sizes, and surrounding environment conductor (ε). Therefore, for an isolated conductor have the formula , where - capacity of secluded conductor. Capacity of the secluded conductor is equal to a charge q, give the conductor that changes its potential by 1 volt. In the SI system capacity is measured in farads Capacity of the ball II. Capacity solitary conductors is very small. For practical purposes it is necessary to create such a device, which allows to store large charges at small sizes and capacities. Capacitor- device for charge storage and electrical power. The simplest capacitor consists of two conductors separated by a gap of air or dielectric (air - is also a dielectric). The conductors are called the plates of the capacitor, and their location in relation to each other are selected such that the electric field is concentrated in the gap between them. Under the capacity of the capacitor understood the physical value of C equal to the ratio of the charge q, accumulated on the plates, to the difference of potentials between the plates.  Calculate the capacity of parallel-plate capacitor with plates of area S, the surface charge density σ, the dielectric constant ε of the dielectric between the plates, the distance between the plates is d. The field intensity is . Using the relation Δφ and E, we find    -   capacity of plate capacitor For a cylindrical capacitor: For a spherical capacitor: Because for some values ??of the voltage in the dielectric breakdown occurs (electrical discharge through the dielectric layer), then there is a breakdown voltage capacitors. Breakdown voltage depends on the shape of facings, dielectric properties and its thickness. III. Capacitance in parallel and series connection of capacitors parallel  According to the law of conservation of charge        b) serial connection  According to the law of conservation of charge        § 3 The energy of the electrostatic field 1. Energy of the system of fixed point charges The electrostatic field is potential. The forces acting between charges - conservative forces. System of fixed point charges should have potential energy. We find the potential energy of two fixed point charges q1 and q2, separated by a distance r from each other. The potential energy of the charge q2 in the field created charge q1, equal to  Similarly, the potential energy of the charge q1 in the field created by a charge q2, equal to It is seen that W1 = W2, then identify potential energy of the system of charges q1 and q2 in W, we can write where φi - potential generated at the point where the charge qi, all charges except the i-th. The energy of secluded charged conductor. The energy of the electric field of a charged secluded conductor can be determined by considering the total work done on the movement of small amounts of charge dq from infinity to this conductor. If the conductor has a charge q, capacitance C and potential φ, is to transfer the charge dq from infinity to conductor the work must be expended To charge conductor from ground potential to a potential φ must do the work The potential energy equal to the work that needs to be performed in order to charge the conductor 4. The energy of a charged capacitor. We express the energy of the capacitor through the values ??characterizing the capacitor    because field is uniform inside the capacitor, you can enter the volume energy density (bulk density - the energy per unit volume)  