Page 44 - Maxwell House
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24                                                                 Chapter 1


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                                                                   9
                       =                            = 8.988 ∙ 10  N
                       
                          4 ∙ 3.1415 ∙ 8.854 1 ∙ 10 −12  ∙ 1000 2
        From a mechanical point of view a force ( =ma) can accelerate a heavy truck of m = 50 tons
                                           
        = 50 000 kg with a = 200 km/s ! So in one second the truck will be 100 km from the traffic
                                  2
        lights and an hour will reach a speed of 720,000 km/hour, if it could survive such powerful
        push.
        Significant charges are not uncommon around us. The Earth bears a negative charge of about
        −4.5 ∙ 10  C [15] and our atmosphere accumulates a roughly equal and opposite charge. It is,
                5
        therefore, no surprise that nature produces so many fireworks, within average 100 lightning
        strikes per second! The immense amount of charge that travels through a lightning bolt can
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        reach up to 350 C or the charge of 2.18 ∙ 10  electrons with a total mass 2 ∙ 10 −12  kg or only
        6 g per year. The age of the Earth is about 4.56 ∙ 10  years. Thus for the whole Earth history
                                                  9
        lightning would deliver 27 360 tons of electrons. Meanwhile, a single commercially produced
        ultracapacitor of 10,000 farads for the wind and the solar power generation system connected
        to a 2.7-volt battery stores 27,000 C or the equivalent of 77 of the most powerful lightning
        strikes! A compact battery of 17 such capacitors is capable of storing more charges than the
        whole Earth.

         1.6.7   Electric Field Reality
        The equation (1.20) and (1.24) proves the quite remarkable fact that electrical charges store
        their  potential energy in their surrounding electrical fields.  That  will bring into play the
        conservation energy law: field potential energy can be released and converted into any other
        form of energy such as radiant and heat, motion and sound, chemical, you name them. The
        electrical fields become quite real: they carry energy and can be measured! For example, the
        existence of electric potential implies the transformation of electric field energy into kinetic
        energy of movable charges. In other words, electrical potential or pure voltage can be the source
        of an electrical current in the material where movable charges such as electrons are not bound
        to atomic nucleus or molecules and are free to respond to outside forces created by electrical
        fields. Subsequently, the greater voltage means more dominant force, the higher electric current
        and more energy to be taken from the electrical sources. However, the movement of a mass of
        charged particles that is too big leads to a high probability of collisions between these particles
        and the crystal lattice of conductive material and thus an increase in energy loss. That is why a
        voltage of 750,000V and higher is  used to  reduce the transposed  mass of charges  while
        transferring  the bulk of electrical  energy  from power stations to remote consumers.  The
        potential of several hundred million volts between earth surface and thunderstorm clouds causes
        powerful lightning. Shuffling  your  feet across synthetic carpets  might  increase  your  body
        electric potential up to 36 000 V. The sparks jumping from your finger are not dangerous but
        annoying and sometimes rather painful!

        1.6.8   Displacement Vector D. 3  Maxwell’s Equation
                                     rd
        Now, we turn to the electric charge conservation law, one of the fundamental laws of physics,
        and will demonstrate its association with Gauss’s Law. First of all, let us rewrite Gauss’s law
                           rd
        as the integral form of 3  Maxwell’s equation (see Table 1.7)
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