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Electrostatic Energy (Электростатическая энергия)

The force in electric field:

The work (from mechanics):

Definition of the potential difference:

For infinitely remote point "a":

The work is done by the electric field without any external force. This is insolated system.

Energy conservation law (total energy can't be changed):

(W – potential, A – work).

But what exactly work do? This work in insulated system (where only charges and electric field exist) transformed into kinetic energy if there no other participles of all this event. (честно, я не понял, почему он тут вдруг начал говорить про кинетическую энергию, хотя до этого всё время говорил про потенциальную)

So, we have got:

But if there external force which moves a charge and moves so that velocity of charge is constant (or velocity at the start = velocity at the finish point), so there is no change of kinetic energy. In this case, the external force applied to electric charge look like that (equal but with the opposite sign): . And after all we get the same relation: .

Virtual experiment. (Эксперимент по нахождению энергии системы)

Consider three points P1, P2, and P3 in a charge free space. The point charges Q1 ,Q2 , and Q3 are brought from infinity to those points, respectively and in turn (соответственно и по очереди).

No work is done in bringing point charge Q1 from infinity to point P1 (because there wasn't electric field in the beginning). Then we have

U21 is the potential induced at point P2 due to Q1,

U31 is the potential induced at point P3 due to Q1 ,

U32 is the potential induced at point P3 due to Q2.

If we want to find a potential in any point, we need to summarize the potentials, which induced by all charges.

Now we reverse this experiment and we move at the beginning charge Q3, then Q2, then Q1.

U23 is the potential induced at point P2 due to Q3,

U12 is the potential induced at point P1 due to Q2 ,

U13 is the potential induced at point P1 due to Q3.

And if we add two equation we get:

or

U1 is the potential induced at point P1 due to Q2 and Q3,

U2 is the potential induced at point P2 due to Q1 and Q3 ,

U3 is the potential induced at point P3 due to Q1 and Q2.

Consequences (Следствия)

In general case:

If the charges are distributed over the space:

for the space charges (U – function because it distributed somehow over the space, where we do integrate). These charges really may exist.

for the surface charges (for example – conducting electrode)

for the line charges (it doesn't exist in our world, because we can't compress the charges into infinitely thin line, but in practice we can have ALMOST linear charges (energy transfer lines – wires) and we can approximate it as a thin line? but bad consequences may happen because of approximation – it may give us an infinite WE and we can't to calculate it)

Substituting in the expression for the energy of charges distributed in the volume (now it's not only electrostatic field, but in electric field this consequence work too):

(for any field)

Applying the Gauss theorem (not Gauss law for field! по-русски это формула Остроградского - Гаусса) to the first term:

We have static system, which is limited (not infinitely). So, we have a point, which is very far from system. So far, that system may seemed like a point (may be charge point, may be not). And if we are going to infinity our potential and displacement induced by this point are inversed proportional to the radius.

Area of a spherical surface

Energy:

Finally, we get:

Also, we can conclude something (but it is a kind of a sumption [предположение]). Нельзя говорить, что мы выделим в области объём, и там будет какая-то энергия. Энергия WE=Q*U говорит нам, что на самом деле энергия концентрируется в заряде, а через объёмную плотность энергии формула говорит, что энергия концентрируется вокруг заряда. Что из этого правильно и нет – может быть потом он расскажет, а может и нет.

Energy per unit volume (volume density of electric energy):

For isotropic medium:

Electric currents. (Электрический ток)

Just now we consider only constant currents. But we expand our result on all current.

Variables and units. (Переменные)

Basic definitions (Основные понятия)

Current – is the charge which cross some area over time unit:

Current density: and

How current density induce in the beginning? There should be some current carrier. In our usual material (metals) usual carries part are electrons. So

current density depends on the velocity and density of moving charges:

Conductivity and resistance (Проводимость и сопротивление)

where is the mobility of electrons (electrons often hits ions and they are stopped by them)

Ne – concentration of electrons.

conductivity:

Ohm’s law:

Resistance:

Power and Joule’s Law (Мощность и закон Джоуля)

Consider a charge Q moves at a velocity v by an electric field E to a distance l. In this case, the expression of the work done is:

Power – is the energy, which dissipated (рассеянный) or consumed or generated over time unit:

Total charge:

So Joule’s law in differential form

For a constant cross-section conductor, the expression of the volume is:

Expression for the power: (Joule’s law in integral form)

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