

ELECTROMAGNETISM M_{rot}, p_{m}, the lines of force and Permanent magnets have been known 2000 years ago, but only in 1820, H. Oersted (Danish physicist) found that around a conductor with a current creates a magnetic field, which affects the magnetic needle. Later, it was found that the magnetic field is produced by moving bodies, or any charges. The magnetic field, like the electric, is a type of matter. The magnetic field has energy. By means of the magnetic field the interaction between electric currents moving charges. Experience has shown that the effects of the magnetic field on the current varies depending on the shape of the conductor, in which the current flows, the location of the conductor and the direction of the current. Therefore, in order to characterize the magnetic field, it is necessary to consider the effect on a certain current. For the study of the electric field using a test point charge. Similarly, for the study of the magnetic field using a current loop, whose dimensions are small compared with the distance to the currents that form a magnetic field. The orientation of the contour (with a current loop) in space is characterized by the normal to the contour. The positive direction of the normal is determined by the righthand rule: the four fingers of his right hand in the direction of the current position in the loop, deflected at right angles to the thumb indicates the direction of the normal. The magnetic field exerts on the loop with current orienting effect. The current loop is installed in a magnetic field so that it coincides with the normal direction of the magnetic field lines.
Magnetic moment of current loop is a vector equal to the product of the current flowing through the loop on the vector square . Direction coincides with the direction .Direction determined by the righthand rule. Because current loop experiences orienting action of the field, then it in a magnetic field exerts a force couple. Rotating moment forces depends on the properties of the field at a given point and the properties of current loop
 magnetic induction vector is a quantitative measure of force of the magnetic field. . If at a given point of the magnetic field to make a variety of current loop with the magnetic moments of p_{1}, p_{2}, ... p_{n}, then the torque will be different for each current loop M_{1}, M_{2}, ... M_{n}, but the ratio
for all current loops is the same and can serve to characterize the magnetic field. Magnetic induction at a given point of a uniform magnetic field is numerically equal to the maximum torque , acting on the current loop with the magnetic moment of one, when the normal to the to the current loop is perpendicular to direction of the field ( also determined by the Lorentz force or Ampere force). The direction of vector coincides with the direction of in the case when the current loop is in equilibrium and . A magnetic field conveniently represented with lines of force of vector .Force line of vector called a line whose tangent at any point coincides with the direction of at this point. The direction of lines of force of vector determined by the righthand rule. For linear conductor: thumb in the direction of the current, bent four fingers indicate the direction of the field line. For a circular coil with a current: four fingers  on the current direction, the thumb indicates the direction of the field line in the center of the coil. Lines of magnetic induction , unlike force lines of vector , of the electric field is always closed and covered conductor. (The lines of force of vectorbegin on positive charges and end on negative, approach perpendicular to the surface charge density of the lines of force characterizes the field.) In some cases, along with the vector applied vector of intensity of magnetic field ,which is associated with the vector by ratio;
µ_{0} –magnetic constant ; , µ  magnetic permeability of the medium  shows how many times the magnetic field in the medium more (or less) of the magnetic field in the vacuum . , where B  the magnetic field in the material, B_{0}  external magnetizing field. From a comparison of the characteristics of the electric field vector (vector and a vector ) and magnetic field (vector and ) it follows that intensity vector of electric field is similar to the magnetic induction .Both determine the effect of the force fields and depend on the properties of the medium in which the fields are created. Analogue of the electric displacement is the vector of intensity of magnetic field . Vector which describes the magnetic field macrocurrents macrocurrents  currents flowing through a conductor), so do not depend on the properties of the medium (Tesla);
§ 2 he BiotSavartLaplace’s Law
Magnetic induction field, created by the conductor element , in which the current I flows , at some point A, whose position relative to the determined by the radius vector , determined by the BiotSavartLaplace law
 the BiotSavartLaplace law (in vector form) . Because in the BiotSavartLaplace law there is a vector product , then vector must be perpendicular to the plane of the vectors and . The direction of vector � determined on the righthand rule. Modulus (magnitude) of the vector is equal to  the BiotSavartLaplace law (in scalar form)
where α –the angle between the and . 2.The principle of superposition of fields: Magnetic induction of the resulting field, multicurrents (or moving charges), equal to the geometric (vector) sum of the magnetic induction generated by each current separately. 3. Application of the BiotSavartLaplace’s law to the calculation of magnetic fields. a) A magnetic field of the direct current
; ;
Since the induction created by different elementary sections, which we have broken conductor at this point have the same direction, we can sum the geometric vectors replace the scalar summation
 magnetic induction linear conductor of finite length.  intensity of the magnetic field of a conductor of finite length. In the case of an infinitely long conductor ; . b) The magnetic field at the center of a circular currentcarrying conductor
α = 90°; sin α = 1.
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