Einstein Relatively Easy

Pin It

If you like this content, you can help maintaining this website with a small tip on my tipeee page  


 "You told us how an almost churchlike atmosphere is pervading your desolate house now. And justifiably so, for unusual divine powers are at work in there."
 Besso to Einstein, 30 Oct 1915


In the last two articles, we have derived the Gμν (Einstein tensor) and Tμν (energy-momenum tensor) components of the Einstein equation:

We have yet to determine the constant k.

To achieve this, we need to show that the Einstein equation reduces to Newton’s law of gravity for weak and static gravitational fields (Newtonian limit).

The first step consists in writing  the previous Einstein equation in a slightly different form that is sometimes more practical to use in calculations.

That's actually under this second form that Einstein published it  in his article "The Field Equations of Gravitation" submitted on November 25, 1915 in Königlish Preussiche Akademie der Wissenschaften

Einstein's equation alternative form

Replacing Einstein tensor by its full expression:

Multiplying both sides by gμν yields to:

By definition of the metric contraction, gμνRμν=R and gμνTμν=T so

Because the tensor gμν is the inverse of gνα, their product gives the identity matrix of rank 4 = δμα = I (this can be seen by doing the calculation in a local inertial frame where gμνμν and noting that since it’s a tensor equation, it’s valid in all coordinate systems). By contracting the δνμ tensor we just sum up its diagonal elements and since these are all one, we get



Replacing R by -kT in Einstein original equation gives:


Newtonian limit

In the context of Newtonian limit, we have also already demonstrated from the previous article that the component R00 of the Riemann tensor approximates to

But we can remark that when the metric reduces to the metric η from flat spacetime, we get by the definition of the Ricci tensor:

The Newtonian limit implies also that the only non negligible component of the stress-energy tensor Tμν is T00=ρc2 (Tμν =ρuμuν with ui<<u0=c).

Then we can write

Which yields by developing the 00-th component of Einstein equation to


We can finally formulate the Einstein equation both in its standard and alternative form


Remark 1: When calculated, the value of K is very very small, meaning that the spacetime is very rigid or stiff: a huge value of mass/energy is required to set a 'noticeable' curvature.


Remark 2: Despite the simple appearance of the equations they are actually quite complicated. Given a specified distribution of matter and energy in the form of a stress–energy tensor, the Einstein Equation or Einstein Field Equations (EFE) are understood to be a set of equations for the metric tensor gμν, as both the Ricci tensor and scalar curvature depend on the metric in a complicated nonlinear manner. In fact, when fully written out, the EFE represent a system of 10 coupled, nonlinear second-order partial differential equations for the metric tensor - corresponding to the 10 independant component of the symmetric tensor gμν.

Remark 3: The non-linearity of the EFE has a profund physical meaning. It relates to the auto-referential  role of spacetime in this theory, because it constitutes both the dynamical object and the context within which the dynamics are defined. In other terms, gravitation itself gravites. As stated by Kevin Brown in his Reflections on Relativity, "the self-referential quality of the metric field equations also manifests itself in their non-linearity. Under the laws of general relativity, every form of stress-energy gravitates, including gravitation itself. This is really unavoidable for a theory in which the metrical relations between entities determine the "positions" of those entities, and those positions in turn influence the metric".
This non-lineraity means also, as we will see later, that two gravitons are able to exchange a graviton, which would not be possible in the case of a set of linear equations; for example, electromagnetism's linearity does not allow two photons to exchange another (virtual) photon to interact.

Remark 4: Finally and to be accurate, the EFE do NOT determine completely and uniquely all ten components of the metric. The Einstein equation must place only six independent constraints on the ten gμν(P), leaving four arbitrary functions to be adjusted by man's specialization of the four coordinate functions xα(P). The fact that ten distinct differential equations lead to the setting of only six constraints is precisely due to the null divergence of the Einstein tensor G.




"The essence of my theory is precisely that no independent properties are attributed to space on its own. It can be put jokingly this way. If I allow all things to vanish from the world, then following Newton, the Galilean inertial space remains; following my interpretation, however, nothing remains.."
Letter from A.Einstein to Karl Schwarzschild - Berlin, 9 January 1916

"Quantum mechanics is certainly imposing. But an inner voice tells me that it is not yet the real thing. The theory says a lot, but does not really bring us any closer to the secret of the 'old one'. I, at any rate, am convinced that He is not playing at dice."
Einstein to Max Born, letter 52, 4th december 1926

RSS Feed


Who is online

We have 125 guests and no members online