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- 1. The electric field in vacuum

Lecture



Это окончание невероятной информации про электрическое поле в вакууме.

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symmetry. Functions of this kind appear whenever we deal with fields of spherical or axial symmetry, with the difference that in the first case 1. The electric field in vacuum is the distance to the center of symmetry of the field, with which the origin of coordinates is made to coincide, while in the second 1. The electric field in vacuum is the distance to the axis of symmetry of the field, along which the axis 1. The electric field in vacuum of the coordinate system is directed. Both of these cases can be treated in a uniform way.

To begin with, let us calculate 1. The electric field in vacuum.

Performing the differentiation, we obtain

1. The electric field in vacuum

Now let us multiply each partial derivative by the unit vector of the corresponding axis and add the results

1. The electric field in vacuum

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Let us now calculate the gradient of an arbitrary scalar function depending only on the magnitude of the position vector 1. The electric field in vacuum. In both cases 1. The electric field in vacuum is a composite function of the coordinates 1. The electric field in vacuum of the point: the function 1. The electric field in vacuum does not depend on them directly and independently, but through the mediation of the inner function 1. The electric field in vacuum. According to the rule for differentiating composite functions

1. The electric field in vacuum

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Comparison shows that this is simply a particular case for 1. The electric field in vacuum, when 1. The electric field in vacuum.

Thus, the general formula for the gradient of a scalar function depending only on the magnitude of the position vector has the form:

1. The electric field in vacuum

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In the particular case of the potential of the field 1. The electric field in vacuum of a point charge located at the origin of coordinates, as it should be, we obtain

1. The electric field in vacuum

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We suggest deriving on your own the following useful relations:

1. The electric field in vacuum

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In the operator 1. The electric field in vacuum in the first relation, the differentiation is carried out with respect to the coordinates 1. The electric field in vacuum of the point with position vector 1. The electric field in vacuum, while in the operator 1. The electric field in vacuum in the second relation — with respect to the coordinates of the point 1. The electric field in vacuum with position vector 1. The electric field in vacuum. To simplify the derivation, it is recommended to make the substitution 1. The electric field in vacuum.

Продолжение:


Часть 1 1. The electric field in vacuum
Часть 2 1.4. Flux of a vector. The Ostrogradsky–Gauss theorem for a
Часть 3 1.5. Application of Gauss's theorem for calculating the electric field
Часть 4 Appendices - 1. The electric field in vacuum
Часть 5 - 1. The electric field in vacuum

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Lectures and tutorial on "Basic Physics"

Terms: Basic Physics