The force of interaction of two fixed point electric charges in vacuum is directly proportional to the product of their modules and inversely proportional to the square of the distance between them.
Coulomb's law quantitatively describes the interaction of charged bodies. It is a fundamental law, that is, established by experiment and does not follow from any other law of nature. It is formulated for immobile point charges in vacuum. In reality, point charges do not exist, but such charges can be considered, the dimensions of which are much smaller than the distance between them. The force of interaction in air is almost the same as the force of interaction in vacuum (it is weaker by less than one thousandth).
Electric charge is a physical quantity that characterizes the property of particles or bodies to enter into electromagnetic force interactions.
The law of interaction of fixed charges was first discovered by the French physicist C. Coulomb in 1785. Coulomb's experiments measured the interaction between balls whose dimensions are much smaller than the distance between them. Such charged bodies are called point charges.
Based on numerous experiments, Coulomb established the following law:
The force of interaction of two fixed point electric charges in vacuum is directly proportional to the product of their modules and inversely proportional to the square of the distance between them. It is directed along the straight line connecting the charges, and is an attractive force if the charges are opposite, and a repulsive force if the charges are of the same name.
If we designate charge modules as | q 1 | and | q 2 |, then Coulomb's law can be written in the following form:
\[ F = k \cdot \dfrac(\left|q_1 \right| \cdot \left|q_2 \right|)(r^2) \]
The coefficient of proportionality k in Coulomb's law depends on the choice of the system of units.
\[ k=\frac(1)(4\pi \varepsilon _0) \]
The full formula of Coulomb's law:
\[ F = \dfrac(\left|q_1 \right|\left|q_2 \right|)(4 \pi \varepsilon_0 \varepsilon r^2) \]
\(F\) - Coulomb Strength
\(q_1 q_2 \) - Electric charge of the body
\(r \) - Distance between charges
\(\varepsilon_0 = 8.85*10^(-12) \)- Electrical constant
\(\varepsilon \) - Dielectric constant of the medium
\(k = 9*10^9 \) - Coefficient of proportionality in Coulomb's law
Interaction forces obey Newton's third law: \(\vec(F)_(12)=\vec(F)_(21) \). They are repulsive forces with the same signs of charges and attractive forces with different signs.
Electric charge is usually denoted by the letters q or Q.
The totality of all known experimental facts allows us to draw the following conclusions:
There are two kinds of electric charges, conventionally called positive and negative.
Charges can be transferred (for example, by direct contact) from one body to another. Unlike body mass, electric charge is not an inherent characteristic of a given body. The same body in different conditions may have different charges.
Like charges repel, unlike charges attract. This also shows the fundamental difference between electromagnetic forces and gravitational ones. Gravitational forces are always forces of attraction.
The interaction of fixed electric charges is called electrostatic or Coulomb interaction. The section of electrodynamics that studies the Coulomb interaction is called electrostatics.
Coulomb's law is valid for point charged bodies. In practice, Coulomb's law is well satisfied if the dimensions of the charged bodies are much smaller than the distance between them.
Note that in order for Coulomb's law to be fulfilled, 3 conditions are necessary:
- Point charges- that is, the distance between the charged bodies is much greater than their size.
- Immobility of charges. Otherwise, additional effects come into force: the magnetic field of the moving charge and the corresponding additional Lorentz force acting on another moving charge.
- Interaction of charges in vacuum.
In the International SI system, the coulomb (C) is taken as the unit of charge.
A pendant is a charge that passes in 1 s through the cross section of a conductor at a current strength of 1 A. The unit of current (ampere) in SI is, along with units of length, time and mass, the main unit of measurement.
Javascript is disabled in your browser.ActiveX controls must be enabled in order to make calculations!
In electrostatics, Coulomb's law is one of the fundamental ones. It is used in physics to determine the force of interaction between two fixed point charges or the distance between them. It is a fundamental law of nature that does not depend on any other laws. Then the shape of the real body does not affect the magnitude of the forces. In this article, we will tell plain language Coulomb's law and its application in practice.
Discovery history
Sh.O. Coulomb in 1785 for the first time experimentally proved the interactions described by the law. In his experiments, he used a special torsion balance. However, back in 1773, Cavendish proved, using the example of a spherical capacitor, that there is no electric field. This suggested that electrostatic forces change depending on the distance between the bodies. To be more precise - the square of the distance. Then his research was not published. Historically, this discovery was named after Coulomb, and the quantity in which the charge is measured has a similar name.
Wording
The definition of Coulomb's law is: in a vacuumF interaction of two charged bodies is directly proportional to the product of their modules and inversely proportional to the square of the distance between them.
It sounds short, but it may not be clear to everyone. In simple words: The more charge the bodies have and the closer they are to each other, the greater the force.
And vice versa: If you increase the distance between the charges - the force will become less.
The formula for Coulomb's rule looks like this:
Designation of letters: q - charge value, r - distance between them, k - coefficient, depends on the chosen system of units.
The value of the charge q can be conditionally positive or conditionally negative. This division is very conditional. When bodies come into contact, it can be transmitted from one to another. It follows that the same body can have a charge of different magnitude and sign. A point charge is such a charge or a body whose dimensions are much smaller than the distance of possible interaction.
It should be taken into account that the environment in which the charges are located affects the interaction F. Since it is almost equal in air and in vacuum, Coulomb's discovery is applicable only for these media, this is one of the conditions for applying this type of formula. As already mentioned, in the SI system, the unit of charge is Coulomb, abbreviated as Cl. It characterizes the amount of electricity per unit of time. It is a derivative of the basic SI units.
1 C = 1 A * 1 s
It should be noted that the dimension of 1 C is redundant. Due to the fact that the carriers repel each other, it is difficult to keep them in a small body, although the 1A current itself is small if it flows in a conductor. For example, in the same 100 W incandescent lamp, a current of 0.5 A flows, and in an electric heater and more than 10 A. Such a force (1 C) is approximately equal to the force acting on a body with a mass of 1 t from the side of the globe.
You may have noticed that the formula is almost the same as in the gravitational interaction, only if masses appear in Newtonian mechanics, then charges appear in electrostatics.
Coulomb's formula for a dielectric medium
The coefficient, taking into account the values of the SI system, is determined in N 2 *m 2 /Cl 2. It is equal to:
In many textbooks, this coefficient can be found in the form of a fraction:
Here E 0 \u003d 8.85 * 10-12 C2 / N * m2 is an electrical constant. For a dielectric, E is added - the dielectric constant of the medium, then the Coulomb law can be used to calculate the forces of interaction of charges for vacuum and the medium.
Taking into account the influence of the dielectric, it has the form:
From here we see that the introduction of a dielectric between the bodies reduces the force F.
How are the forces directed?
Charges interact with each other depending on their polarity - the same charges repel, and the opposite (opposite) attract.
By the way, this is the main difference from a similar law of gravitational interaction, where bodies always attract. Forces directed along a line drawn between them is called the radius vector. In physics, it is denoted as r 12 and as a radius vector from the first to the second charge and vice versa. The forces are directed from the center of the charge to the opposite charge along this line if the charges are opposite, and in reverse side, if they are of the same name (two positive or two negative). In vector form:
The force applied to the first charge from the second is denoted as F 12. Then, in vector form, Coulomb's law looks like this:
To determine the force applied to the second charge, the designations F 21 and R 21 are used.
If the body has a complex shape and is large enough that at a given distance it cannot be considered a point, then it is divided into small sections and each section is considered as a point charge. After the geometric addition of all the resulting vectors, the resulting force is obtained. Atoms and molecules interact with each other according to the same law.
Application in practice
Coulomb's works are very important in electrostatics; in practice, they are used in a number of inventions and devices. A striking example is the lightning rod. With its help, they protect buildings and electrical installations from thunderstorms, thereby preventing fire and equipment failure. When it rains with a thunderstorm, an induced charge of large magnitude appears on the earth, they are attracted towards the cloud. It turns out that a large electric field appears on the surface of the earth. Near the tip of the lightning rod, it has a large value, as a result of which a corona discharge is ignited from the tip (from the ground, through the lightning rod to the cloud). The charge from the ground is attracted to the opposite charge of the cloud, according to Coulomb's law. The air is ionized and tension electric field decreases near the end of the lightning rod. Thus, the charges do not accumulate on the building, in which case the probability of a lightning strike is small. If a blow to the building occurs, then through the lightning rod all the energy will go into the ground.
In serious scientific research, the greatest construction of the 21st century is used - the particle accelerator. In it, the electric field does the work of increasing the energy of the particle. Considering these processes from the point of view of the impact on a point charge by a group of charges, then all the relations of the law turn out to be valid.
Useful
Law of conservation of charge
Electric charges can disappear and reappear. However, two elementary charges of opposite signs always appear or disappear. For example, an electron and a positron (positive electron) annihilate when they meet, i.e. turn into neutral gamma photons. In this case, the charges -e and +e disappear. In the course of a process called pair birth, a gamma-ray photon, falling into the field of an atomic nucleus, turns into a pair of particles - an electron and a positron, and charges arise - e and + e.
Thus, the total charge of an electrically isolated system cannot change. This statement is called law of conservation of electric charge.
Note that the law of conservation of electric charge is closely related to the relativistic invariance of charge. Indeed, if the magnitude of the charge depended on its speed, then by setting in motion charges of one sign, we would change the total charge of an isolated system.
Charged bodies interact with each other, with like charges repelling and opposite charges attracting.
The exact mathematical expression of the law of this interaction in 1785 was established by the French physicist Ch. Coulomb. Since then, the law of interaction of motionless electric charges bears his name.
A charged body, whose dimensions can be neglected, in comparison with the distance between the interacting bodies, can be taken as a point charge. Coulomb as a result of his experiments found that:
The force of interaction in vacuum of two fixed point charges is directly proportional to the product of these charges and inversely proportional to the square of the distance between them. The index "" of the force shows that this is the force of the interaction of charges in a vacuum.
It has been established that Coulomb's law is valid at distances from up to several kilometers.
To put an equal sign, it is necessary to introduce some coefficient of proportionality, the value of which depends on the choice of the system of units:
It has already been noted that in SI charge is measured in C. In Coulomb's law, the dimension of the left side is known - the unit of force, the dimension of the right side is known -, therefore, the coefficient k turns out to be dimensional and equal. However, in SI this proportionality factor is usually written in a slightly different form:
hence
where farad ( F) is a unit of electric capacitance (see clause 3.3).
The quantity is called the electrical constant. This is indeed a fundamental constant that appears in many equations of electrodynamics.
Thus, Coulomb's law in scalar form has the form:
Coulomb's law can be expressed in vector form:
where is the radius vector connecting the charge q2 with charge q 1 ,; - the force acting on the charge q 1 charge side q2. per charge q2 charge side q 1 force acts (Fig. 1.1)
Experience shows that the force of interaction of two given charges does not change if any other charges are placed near them.
Electric charge. His discretion. The law of conservation of electric charge. Coulomb's law in vector and scalar form.
Electric charge is a physical quantity that characterizes the property of particles or bodies to enter into electromagnetic force interactions. Electric charge is usually denoted by the letters q or Q. There are two kinds of electric charges, conventionally called positive and negative. Charges can be transferred (for example, by direct contact) from one body to another. Unlike body mass, electric charge is not an inherent characteristic of a given body. The same body in different conditions can have a different charge. Like charges repel, unlike charges attract. An electron and a proton are, respectively, carriers of elementary negative and positive charges. The unit of electric charge is a pendant (C) - an electric charge passing through the cross section of a conductor at a current strength of 1 A in a time of 1 s.
Electric charge is discrete, i.e., the charge of any body is an integer multiple of the elementary electric charge e ().
Law of conservation of charge: algebraic sum of electric charges of any closed system(of a system that does not exchange charges with external bodies) remains unchanged: q1 + q2 + q3 + ... + qn = const.
Coulomb's law: The force of interaction between two point electric charges is proportional to the magnitudes of these charges and inversely proportional to the square of the distance between them.
(in scalar form)
Where F - Coulomb Force, q1 and q2 - Electric charge of the body, r - Distance between charges, e0 = 8.85*10^(-12) - Electrical constant, e- Dielectric constant of the medium, k = 9*10^9 - Proportionality factor.
In order for Coulomb's law to be fulfilled, 3 conditions are necessary:
1 condition: Pointed charges - that is, the distance between charged bodies is much greater than their sizes
Condition 2: Immobility of charges. Otherwise, additional effects come into force: the magnetic field of the moving charge and the corresponding additional Lorentz force acting on another moving charge
3rd condition: Interaction of charges in vacuum
In vector form the law is written as follows:
Where is the force with which charge 1 acts on charge 2; q1, q2 - magnitude of charges; - radius vector (vector directed from charge 1 to charge 2, and equal, in modulus, to the distance between charges - ); k - coefficient of proportionality.
The intensity of the electrostatic field. Expression for the strength of the electrostatic field of a point charge in vector and scalar form. Electric field in vacuum and matter. The dielectric constant.
The strength of the electrostatic field is a vector power characteristic of the field and is numerically equal to the force with which the field acts on a unit test charge applied to a given point of the field:
The unit of tension is 1 N / C - this is the intensity of such an electrostatic field, which acts on a charge of 1 C with a force of 1 N. The tension is also expressed in V / m.
As follows from the formula and Coulomb's law, the field strength of a point charge in vacuum
or 
The direction of the vector E coincides with the direction of the force that acts on the positive charge. If the field is created by a positive charge, then the vector E is directed along the radius vector from the charge to the outer space (repulsion of a test positive charge); if the field is created by a negative charge, then the vector E is directed towards the charge.
That. tension is a power characteristic of the electrostatic field.
For a graphical representation of the electrostatic field, the vector strength lines are used ( lines of force). By the density of the lines of force, one can judge the magnitude of the tension.
If the field is created by a system of charges, then the resulting force acting on the test charge introduced at a given point of the field is equal to the geometric sum of the forces acting on the test charge from each point charge separately. Therefore, the intensity at a given point of the field is equal to:
This ratio expresses principle of superposition of fields: the intensity of the resulting field created by the system of charges is equal to the geometric sum of the field strengths created at a given point by each charge separately.
Electricity in vacuum can be created by the ordered movement of any charged particles (electrons, ions).
The dielectric constant- value characterizing di electrical properties environment - its reaction to an electric field.
In most dielectrics, at not very strong fields, the permittivity does not depend on the field E. In strong electric fields (comparable to intraatomic fields), and in some dielectrics in ordinary fields, the dependence of D on E is nonlinear. The dielectric constant also shows how many times the interaction force F between electric charges in a given medium is less than their interaction force Fo in vacuum
The relative permittivity of a substance can be determined by comparing the capacitance of a test capacitor with a given dielectric (Cx) and the capacitance of the same capacitor in vacuum (Co):
Superposition principle as a fundamental property of fields. General expressions for the strength and potential of the field created at a point with a radius vector by a system of point charges located at points with coordinates. (See item 4)
If we consider the principle of superposition in the most general sense, then according to it, the sum of the impact of external forces acting on a particle will be the sum of the individual values of each of them. This principle applies to various linear systems, i.e. systems whose behavior can be described by linear relations. An example is a simple situation when a linear wave propagates in some particular medium, in which case its properties will be preserved even under the influence of disturbances arising from the wave itself. These properties are defined as a specific sum of the effects of each of the harmonic components.
The superposition principle can also take other formulations that are completely equivalent to the one given above:
· The interaction between two particles does not change when a third particle is introduced, which also interacts with the first two.
· The interaction energy of all particles in a many-particle system is simply the sum of the energies of pair interactions between all possible pairs of particles. There are no multiparticle interactions in the system.
· The equations describing the behavior of a multiparticle system are linear in the number of particles.
6 The circulation of the tension vector is the work that electric forces do when moving a unit positive charge along a closed path L
Since the work of the electrostatic field forces in a closed loop is zero (the work of the potential field forces), therefore, the circulation of the electrostatic field strength in a closed loop is zero.
Field potential. The work of any electrostatic field when moving a charged body in it from one point to another also does not depend on the shape of the trajectory, as well as the work of a uniform field. On a closed trajectory, the work of the electrostatic field is always zero. Fields with this property are called potential fields. In particular, the electrostatic field of a point charge has a potential character.
The work of a potential field can be expressed in terms of a change in potential energy. The formula is valid for any electrostatic field.
7-11 If the lines of force of a uniform electric field of strength penetrate some area S, then the flux of the intensity vector (we used to call the number of lines of force through the area) will be determined by the formula:
where En is the product of the vector and the normal to the given area (Fig. 2.5).
Rice. 2.5
The total number of lines of force passing through the surface S is called the flow of the intensity vector FU through this surface.
In vector form, you can write - the scalar product of two vectors, where the vector .
Thus, the vector flow is a scalar, which, depending on the angle α, can be either positive or negative.
Consider the examples shown in Figures 2.6 and 2.7.
 | |||
| Rice. 2.6 | Rice. 2.7 | ||
For Figure 2.6, surface A1 is surrounded by a positive charge and the flow here is directed outward, i.e. The A2– surface is surrounded by a negative charge, and here it is directed inward. The total flow through surface A is zero.
For Figure 2.7, the flux will be non-zero if the total charge inside the surface is non-zero. For this configuration, the flux through surface A is negative (count the number of field lines).
Thus, the intensity vector flux depends on the charge. This is the meaning of the Ostrogradsky-Gauss theorem.
Gauss theorem
The experimentally established Coulomb's law and the principle of superposition make it possible to completely describe the electrostatic field of a given system of charges in vacuum. However, the properties of the electrostatic field can be expressed in a different, more general form, without resorting to the concept of the Coulomb field of a point charge.
Let us introduce a new physical quantity that characterizes the electric field - the flux Φ of the electric field strength vector. Let some sufficiently small area ΔS be located in the space where the electric field is created. The product of the vector module and the area ΔS and the cosine of the angle α between the vector and the normal to the site is called the elementary flux of the intensity vector through the site ΔS (Fig. 1.3.1):
Let us now consider some arbitrary closed surface S. If we divide this surface into small areas ΔSi, determine the elementary fluxes ΔΦi of the field through these small areas, and then sum them up, then as a result we get the flow Φ of the vector through the closed surface S (Fig. 1.3.2 ):
Gauss' theorem states:
The flow of the electrostatic field strength vector through an arbitrary closed surface is equal to the algebraic sum of the charges located inside this surface, divided by the electric constant ε0.
where R is the radius of the sphere. The flux Φ through the spherical surface will be equal to the product of E and the area of the sphere 4πR2. Hence,
Let us now surround the point charge with an arbitrary closed surface S and consider an auxiliary sphere of radius R0 (Fig. 1.3.3).
Consider a cone with a small solid angle ΔΩ at the vertex. This cone selects a small area ΔS0 on the sphere, and an area ΔS on the surface S. The elementary flows ΔΦ0 and ΔΦ through these areas are the same. Really,
In a similar way, one can show that if the closed surface S does not enclose a point charge q, then the flow Φ = 0. Such a case is shown in fig. 1.3.2. All lines of force of the electric field of a point charge penetrate the closed surface S through and through. There are no charges inside the surface S, therefore, in this region, the lines of force do not break and do not originate.
The generalization of the Gauss theorem to the case of an arbitrary charge distribution follows from the principle of superposition. The field of any charge distribution can be represented as a vector sum of electric fields of point charges. The flow Φ of a system of charges through an arbitrary closed surface S will be the sum of the flows Φi of the electric fields of individual charges. If the charge qi turned out to be inside the surface S, then it makes a contribution to the flow equal to if this charge turned out to be outside the surface, then the contribution of its electric field to the flow will be equal to zero.
Thus, the Gauss theorem is proved.
Gauss's theorem is a consequence of Coulomb's law and the superposition principle. But if we accept the statement contained in this theorem as an initial axiom, then Coulomb's law will turn out to be its consequence. Therefore, Gauss's theorem is sometimes called an alternative formulation of Coulomb's law.
Using the Gauss theorem, in a number of cases it is easy to calculate the electric field strength around a charged body if the given charge distribution has some kind of symmetry and overall structure fields can be guessed.
An example is the problem of calculating the field of a thin-walled, hollow, uniformly charged long cylinder of radius R. This problem has axial symmetry. For reasons of symmetry, the electric field must be directed along the radius. Therefore, to apply the Gauss theorem, it is advisable to choose a closed surface S in the form of a coaxial cylinder of some radius r and length l, closed at both ends (Fig. 1.3.4).
For r ≥ R, the entire flow of the intensity vector will pass through side surface a cylinder whose area is 2πrl, since the flow through both bases is zero. Applying the Gauss theorem gives:
This result does not depend on the radius R of the charged cylinder, so it is also applicable to the field of a long uniformly charged filament.
To determine the field strength inside a charged cylinder, it is necessary to construct a closed surface for the case r< R. В силу симметрии задачи поток вектора напряженности через боковую поверхность гауссова цилиндра должен быть и в этом случае равен Φ = E 2πrl. Согласно теореме Гаусса, этот поток пропорционален заряду, оказавшемуся внутри замкнутой поверхности. Этот заряд равен нулю. Отсюда следует, что электрическое поле внутри однородно заряженного длинного полого цилиндра равно нулю.
Similarly, Gauss's theorem can be applied to determine the electric field in a number of other cases where the charge distribution has some kind of symmetry, for example, symmetry about the center, plane or axis. In each of these cases, it is necessary to choose a closed Gaussian surface of an expedient form. For example, in the case of central symmetry, it is convenient to choose a Gaussian surface in the form of a sphere centered at a point of symmetry. With axial symmetry, a closed surface must be chosen in the form of a coaxial cylinder closed at both ends (as in the example discussed above). If the distribution of charges does not have any symmetry and the general structure of the electric field cannot be guessed, the application of the Gauss theorem cannot simplify the problem of determining the field strength.
Consider another example of a symmetrical distribution of charges - the definition of the field of a uniformly charged plane (Fig. 1.3.5).
In this case, it is advisable to choose the Gaussian surface S in the form of a cylinder of some length, closed at both ends. The axis of the cylinder is directed perpendicular to the charged plane, and its ends are located at the same distance from it. Due to symmetry, the field of a uniformly charged plane must be directed along the normal everywhere. Applying the Gauss theorem gives:
|
where σ is the surface charge density, i.e., the charge per unit area.
The resulting expression for the electric field of a uniformly charged plane is also applicable in the case of flat charged areas of a finite size. In this case, the distance from the point at which the field strength is determined to the charged area must be significantly less than the size of the area.
And schedules for 7 - 11
1. The intensity of the electrostatic field created by a uniformly charged spherical surface.
Let a spherical surface of radius R (Fig. 13.7) bear a uniformly distributed charge q, i.e. the surface charge density at any point on the sphere will be the same.
a. We enclose our spherical surface in a symmetric surface S with radius r>R. The intensity vector flux through the surface S will be equal to
According to the Gauss theorem
Hence
c. Let us draw through the point B, located inside the charged spherical surface, the sphere S with radius r 2. Electrostatic field of the ball. Let we have a ball of radius R, uniformly charged with bulk density. At any point A, lying outside the ball at a distance r from its center (r> R), its field is similar to the field of a point chargelocated at the center of the ball. Then outside the ball and on its surface (r=R) At point B, lying inside the ball at distances r from its center (r>R), the field is determined only by the charge enclosed inside the sphere of radius r. The intensity vector flow through this sphere is equal to on the other hand, according to the Gauss theorem From a comparison of the last expressions it follows where is the permittivity inside the sphere. The dependence of the field strength created by a charged sphere on the distance to the center of the ball is shown in (Fig. 13.10) Let us assume that a hollow cylindrical surface of radius R is charged with a constant linear density . Let us draw a coaxial cylindrical surface of radius The flow of the field strength vector through this surface According to the Gauss theorem From the last two expressions, we determine the field strength created by a uniformly charged thread: Let the plane have an infinite extent and the charge per unit area is equal to σ. From the laws of symmetry it follows that the field is directed everywhere perpendicular to the plane, and if there are no other external charges, then the fields on both sides of the plane must be the same. Let's limit a part of the charged plane to an imaginary cylindrical box, so that the box is cut in half and its generators are perpendicular, and two bases, each having an area S, are parallel to the charged plane (Figure 1.10). total vector flow; tension is equal to the vector times the area S of the first base, plus the vector flow through the opposite base. The flux of tension through the side surface of the cylinder is equal to zero, since the lines of tension do not cross them. Thus, Hence but then the field strength of an infinite uniformly charged plane will be equal to This expression does not include coordinates, therefore the electrostatic field will be uniform, and its strength at any point in the field is the same. 5. The intensity of the field created by two infinite parallel planes, oppositely charged with the same density. As can be seen from Figure 13.13, the field strength between two infinite parallel planes having surface charge densities and , is equal to the sum of the field strengths created by the plates, i.e. Thus, 12. Field of a uniformly charged sphere. Let the electric field be created by the charge Q, uniformly distributed over the surface of a sphere of radius R(Fig. 190). To calculate the field potential at an arbitrary point located at a distance r from the center of the sphere, it is necessary to calculate the work done by the field when moving a unit positive charge from a given point to infinity. Earlier we proved that the field strength of a uniformly charged sphere outside it is equivalent to the field of a point charge located at the center of the sphere. Therefore, outside the sphere, the potential of the field of the sphere will coincide with the potential of the field of a point charge φ
(r)=Q 4πε
0r . (1) In particular, on the surface of a sphere, the potential is equal to φ
0=Q 4πε
0R. There is no electrostatic field inside the sphere, so the work to move a charge from an arbitrary point inside the sphere to its surface is zero A= 0, therefore, the potential difference between these points is also equal to zero Δ φ
= -A= 0. Therefore, all points inside the sphere have the same potential, which coincides with the potential of its surface φ
0=Q 4πε
0R . So, the distribution of the field potential of a uniformly charged sphere has the form (Fig. 191) φ
(r)=⎧⎩⎨Q 4πε
0R, npu r<RQ 4πε
0r, npu r>R . (2) Please note that there is no field inside the sphere, and the potential is different from zero! This example is a vivid illustration of the fact that the potential is determined by the value of the field from a given point to infinity. Dipole. A dielectric (like any substance) consists of atoms and molecules. Since the positive charge of all the nuclei of the molecule is equal to the total charge of the electrons, the molecule as a whole is electrically neutral. The first group of dielectrics(N 2, H 2, O 2, CO 2, CH 4, ...) make up substances, whose molecules have a symmetrical structure, i.e. the centers of "gravity" of positive and negative charges in the absence of an external electric field coincide and, consequently, the dipole moment of the molecule R zero.molecules such dielectrics are called nonpolar. Under the action of an external electric field, the charges of nonpolar molecules are shifted in opposite directions (positive in the field, negative against the field) and the molecule acquires a dipole moment. For example, a hydrogen atom. In the absence of a field, the center of distribution of the negative charge coincides with the position of the positive charge. When the field is turned on, the positive charge is displaced in the direction of the field, the negative one - against the field (Fig. 6): Figure 6 Model of a non-polar dielectric - an elastic dipole (Fig. 7): Figure 7 The dipole moment of this dipole is proportional to the electric field The second group of dielectrics(H 2 O, NH 3, SO 2, CO, ...) are substances whose molecules have asymmetric structure, i.e. centers of "gravity" of positive and negative charges do not coincide. Thus, these molecules in the absence of an external electric field have a dipole moment. molecules such dielectrics are called polar. In the absence of an external field, however, dipole moments of polar molecules due to thermal motion are randomly oriented in space and their resulting moment is zero. If such a dielectric is placed in an external field, then the forces of this field will tend to rotate the dipoles along the field, and a nonzero resulting moment arises. Polar - "+" charge centers and "-" charge centers are displaced, for example, in a water molecule H 2 O. Model of a polar dielectric hard dipole: Figure 8 Dipole moment of the molecule: The third group of dielectrics(NaCl, KCl, KBr, ...) are substances whose molecules have an ionic structure. Ionic crystals are spatial lattices with correct alternation ions of different signs. In these crystals, it is impossible to isolate individual molecules, but they can be considered as a system of two ionic sublattices pushed one into the other. When an electric field is applied to an ionic crystal, some deformation of the crystal lattice or a relative displacement of the sublattices occurs, leading to the appearance of dipole moments. The product of the charge | Q| dipole on his shoulder l called electric dipole moment: p=|Q|l. Dipole field strength Where R is the electric moment of the dipole; r- the module of the radius-vector drawn from the center of the dipole to the point, the field strength in which we are interested; α- angle between the radius-vector r and shoulder l dipole (Fig. 16.1). The dipole field strength at a point lying on the dipole axis (α=0), and at a point lying on the perpendicular to the arm of the dipole, restored from its middle () .
Dipole field potential The potential of the dipole field at a point lying on the dipole axis (α =
0),
and at a point lying on the perpendicular to the arm of the dipole, restored from its middle () ,
φ = 0. Mechanical moment acting on a dipole with an electric moment R, placed in a uniform electric field with intensity E, M=[p;E](vector multiplication), or M=pE sinα ,
where α is the angle between the directions of the vectors R And E. · current strength I
(serves as a quantitative measure of electric current) - a scalar physical quantity determined by the electric charge passing through the cross section of the conductor per unit time: · current density - physical
quantity determined by the strength of the current passing through the unit area of the cross section of the conductor, perpendicular to the direction of the current - vector,
oriented in the direction of the current (i.e. the direction of the vector j coincides with the direction of the ordered movement of positive charges. The unit of current density is ampere per square meter (A / m 2). Current through an arbitrary surface S defined as the vector flow j, i.e. · The expression for the current density through average speed current carriers and their concentration During the time dt, charges will pass through the area dS, separated from it no further than vdt (an expression for the distance between the charges and the area in terms of speed) The charge dq passed after dt through dS where q 0 is the charge of one carrier; n is the number of charges per unit volume (i.e. their concentration): dS v dt - volume. hence, the expression for the current density in terms of the average speed of the current carriers and their concentration has the following form: · D.C.
- current, the strength and direction of which do not change with time. Where q- electric charge passing over time t through the cross section of the conductor. The unit of current strength is ampere (A). · external forces and EMF of the current source third party forces strength non-electrostatic origin, acting on charges from current sources. External forces do work to move electric charges. These forces are electromagnetic in nature: and their work in transferring the test charge q is proportional to q: · The physical quantity determined by the work done by external forces when moving a unit positive charge is calledelectromotive force (emf), operating in the circuit: · Ohm's law for a circuit section · valid only for the interaction of point electric charges, that is, such charged bodies, the linear dimensions of which can be neglected in comparison with the distance between them. · expresses the strength of the interaction between fixed electric charges, that is, this is the electrostatic law. Formulation of Coulomb's Law: The strength of the electrostatic interaction between two point electric charges is directly proportional to the product of the magnitudes of the charges and inversely proportional to the square of the distance between them. Proportionality factor in Coulomb's law depends
1. from the properties of the environment 2. selection of units of measure for the quantities included in the formula. Therefore, it can be represented by the relation Where - coefficient depending only on the choice of system of units; The dimensionless quantity characterizing the electrical properties of the medium is called relative permittivity of the medium
. It does not depend on the choice of the system of units and is equal to one in vacuum. Then Coulomb's law takes the form: for vacuum, Then - the relative permittivity of a medium shows how many times in a given medium the force of interaction between two point electric charges and , located at a distance from each other, is less than in vacuum. In the SI system coefficient , and Coulomb's law has the form: This rationalized notation of the law K oolon. electrical constant, In the GSSE system , . In vector form, Coulomb's law takes the form Where - the vector of the force acting on the charge from the side of the charge , r is the modulus of the radius vector . Any charged body consists of many point electric charges, so the electrostatic force with which one charged body acts on another is equal to the vector sum of the forces applied to all point charges of the second body from each point charge of the first body. 1.3 Electric field. tension.
Space, in which there is an electric charge, has certain physical properties. 1. For everyone another the charge introduced into this space is acted upon by electrostatic Coulomb forces. 2. If a force acts at every point in space, then they say that there is a force field in this space. 3. The field, along with matter, is a form of matter. 4. If the field is stationary, that is, does not change in time, and is created by stationary electric charges, then such a field is called electrostatic.
(13.10)
(13.11)
(13.12)
(13.13)
On the other hand, according to the Gauss theorem
(13.14)
(13.15)
Outside the plate, the vectors from each of them are directed in opposite directions and cancel each other out. Therefore, the field strength in the space surrounding the plates will be equal to zero E=0.
where e is called the electromotive force of the current source. The “+” sign corresponds to the case when, when moving, the source passes in the direction of external forces (from the negative to the positive facing), “-” - to the opposite case
.
.
is the radius vector connecting charge to charge
