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PLAN OF DB SPECIAL RELATIVITY
 dba axioms of special relativity 
 dbb lorentz transformations 
 dbc length contraction and time dilation 
 dbd speed cumulation 
 dbe E=MC**2 
 dbf paradox of langevins traveller 

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DBE.E=MC**2

E=MC**2 has deep ontological and epistemological implications discussed in Postface.

Notations:

Unless they are elementary displacements noted dx,dy..., vectors are usually noted with upper case letters (A,B...) and their components with lower case letters designating indexes (i,j,k...) written as upper or lower, following vector's name: A .i .j B In ASCII context we shall write them with help of brackets and slash, as follows: A(i/), B(/j) Upper indexes designate contravariant components and lower indexes covariant ones. Thus A(i/) designates the i-th covariant component of vector A and B(/j) the j-th contravariant component of vector B. In cases when the variance is not yet defined we shall skip the slash and C(k) will mean the k-th component of C of unknown variance. We shall write derivative of y with respect to x as: d(y)/d(x) and partial derivative of u with respect to v: p(u)/p(v). Let's further introduce Einstein's indexing notation implying summation over each index repeated within a monome as upper and lower one. Thus, for 3D: A(i/)B(/i)=A(1/)B(/1)+A(2/)B(/2)+A(3/)B(/3) This convention applies also to partial derivatives as follows: (px(/i)/py(/j))dy(/j) = (px(/i)/py(/1))dy(/1)+(px(/i)/py(/2))dy(/2) +(px(/i)/py(/3))dy(/3) NOTE: We shall follow Einstein's conventions: lighttime l=Ct, normalized speed v=V/C and lambda=sqrt(1-v**2)

Pre-relativistic Maxwell equations:

p(B(ab/)/p(x(b/))=(1/C)(pe(c/)/p(t)+i(c/)) p(e(a/)/p(x(b/)-p(e(b/)/p(x(a/)=(1/C)p(B(ab/)/p(t) and divergences: p(e(a/))/p(x(a/) = D p(B(ab/)/p(x(c/)) = 0

Tensorial unification

Let's introduce tensor constructs Q(ij/) and J(k/) corresponding to B,e,i,D as follows: Q(23/)__Q(31/)__Q(12/)__Q(14/)__Q(24/)__Q(34/) B(x/)___B(y/)___B(z/)___-je(x/)_-je(y/)_-je(z/) J(1/)____J(2/)____J(3/)____J(4/) i(x/)/c__i(y/)/c__i(z/)/c__jD Note: Q(ab/) = -Q(ab/) due to antisymmetry j = sqrt(-1) Thus, Field representation may be merged into two following forms: p(Q(ab/))/p(x(b/)) = J(a/) p(Q(ab/)/p(x(c/) + p(Q(bc/)/p(x(a/) + p(Q(ca/)/p(x(b/) = 0 Lorentz Transformation for the Electro-Magnetic Field: [v=V/C lambda=sqrt(1-v**2)] E(x/)=e(x/) B(x/)=b(x/) E(y/)=(e(y/)-vb(z/))/lambda B(y/)=(b(y/)+ve(z/))/lambda E(z/)=(e(z/)+vb(y/))/lambda B(z/)=(b(z/)-ve(y/))/lambda Let's consider the force k acting at electricity per volume unit: k=qe + [i,B] where i: speed of electricity with unit as C [i,B]: crossproduct The first component of k is: Q(12/)J(2/)+Q(13/)J(3/)+Q(14/)J(4/) (Q(11/) vanishes due to the antisymmetry) Components of k are given by -3 first components of the 4-Vector K: K(a/)=Q(ab/)J(b/) -4th component of K: K(4/)=Q(41/)J(1/)+Q(42/)J(2/)+Q(43/)J(3/)= j(e(x/)i(x/)+(e(y/)i(y/)+e(z/)i(z/)=jL Let's imagine a Body experiencing along lighttime [l1,l2] the action of E-M Field. The changes of its momentum DelI(x/),DelI(y/),DelI(z/) and energy DelE are given by: DelI(x/)=int[l1,l2]dl(int(k(x/)dxdydz))= =(1/j)intK(1/)dx(1/)dx(2/)dx(3/)dx(4/) DelI(y/)= ... DelI(z/)= ... DelE=int[l1,l2]dl(int(Ldxdydz))= =(1/j)int((1/j)K(4/)dx(1/)dx(2/)dx(3/)dx(4/) As the 4D volume element is invariant, the components of K form a 4-Vector Terms transform in the same way as their differentials so that the terms I(x/),I(y/),I(z/),jE form a 4-Vector describing the momentary state of the Body. Now, this 4-Vector may also be expressed with the Mass M and the speed of the "material point" Body.

"Material" Point

Let's recall that -ds**2 = d(tau) = -(dx(1/)**2+dx(2/)**2+dx(3/)**2 - dx(4/)**2 = = dL**2*lambda**2 is an invariant which describes elementary increment of the 4D line L representing the movement of a "material" point. If we chose the l (lighttime) axis so that its direction is that of the concerned line differentials or, as one says, we transform the "material" point into "rest", we'll get d(tau)=dx(4/)**2. Thus, d(tau) will be measured with a lighttime clock falling freely together. Therefore, tau is called "proper time" of the "material" point and d(tau) is invariant. Consequently, we see that u(s/)=dx(s/)/d(tau) has itself, as the dx(s/), vector character and we shall call u(s/) the "4-Vector of speed". Its components satisfy the condition: sigma(u(s/)**2)=-1 Calling r(a/)=da/dl, the components of u(s/) in the traditional notation are: (1/lambda)(r(x/),r(y/),r(z/),j) u(s/) is the unique 4-Vector which may be formed with speed components of a "material" point. Consequently, we see that u(s/)=dx(s/)/d(tau) has itself, as the dx(s/), vector character and we shall call u(s/) the "4-Vector of speed". Its components satisfy the condition: sigma(u(s/)**2)=-1 Calling r(a/)=da/dl, the components of u(s/) in the traditional notation are: (1/lambda)(r(x/),r(y/),r(z/),j) (u(s/) is the unique 4-Vector which may be formed with speed components of a "material" point. Consequently (M*dx(a/)/d(tau) ist for a "material" point the 4-Vector equivalent to the momentum/energy 4-Vector, which we have derived above. Equating the components we get: Momentum: I(x/)=M*r(x/)/lambda I(y/)=M*r(y/)/lambda I(z/)=M*r(z/)/lambda Energy, E(l/)=M/lambda Back to our original notation: Energy, E(l/)=Mdl/lambda Momentum and energy tend to infinity for V approaching C and for low speeds momentum approximates that of traditional physics. Calling energy and mass of immobile "material" point respectively E(l/)=Eo, Mo and noting that for an immobile "material" point lambda=1 we get: Eo=Modl=Mod(Ct)**2 Choosing second as unit of time and dropping "o" for cosmetic reasons we get: E=MC**2

POSTFACE

E=MC**2 is an impressing illustration of the P(henomenal)-Equivalence. P-Equivalence: A Phenomenon, say "Light" is given exclusively by its observable Aspects. Continuous Field wave and Discrete photons are P-Equivalent aspects of the Phenomenon "Light". Similarly, E=MC**2 illustrates the P-Equivalence of Mass and Energy. This simple statement has surprisingly deep implications. Indeed, Mass and Energy have no phenomenal sense and are just coefficients in formulas representing phenomenal, observable construct "Field". Under the disguise of pure abstractions, E=MC**2 implies P-Equivalence of Electro-Magnetism and the fields constructing subatomic particles. A decaying particle converts involved quantity of a strong field to enormous amount of radiation weaker by factor C**2. Seen from Special Relativity, E=MC**2 appears as anticipation not only of the General Relativity, but also of the Quantum Field Theory.