A Laymen's Guide To General Relativity: Part VII

November 30, 2015
Today's article is going to be a short one, because we are nearly at Einstein's equations of general relativity, with only one more minor tool needed to make the final leap.

In the last two articles I gave intuitive definitions of both the Riemann tensor and the Ricci tensor, which are used to define the curvature of spacetime. The third element of this trio of curvature measures is the Ricci scalar, which can be thought of as an average of the Ricci tensor, which itself is an average of the Riemann tensor. The Ricci scalar assigns each point in space and time a number, and that number gives the overall curvature of spacetime at that point.

Using the notation I introduced previously, in which the Ricci tensor is written as Ri(A,V), the Ricci scalar is defined as

Rc =g(x0,x0) Ri(x0,x0) + g(x1,x1) Ri(x1,x1) + g(x2,x2) Ri(x2,x2) + g(x3,x3) Ri(x3,x3

where as before g(x,y) are the metric functions. 

When combined with the definition of the Ricci tensor, the meaning of the Ricci scalar is just a sum over all of the combinations of basis vectors into parallelograms. Take basis vector xi, move it along xi and xj and then again along xj and xi, and then see how much the difference overlaps with vector xj. Now sum over all values of i and j. The end result is an average of the spacetime curvature over all of the possible planes (each plane is defined by two basis vectors).

That is the Ricci scalar, and it is the final piece needed to introduce Einstein's equations. And that is coming up next...
 

A Laymen's Guide To General Relativity: Part VI

November 29, 2015
Having now defined the Riemann tensor, which provides one measure of the curvature of spacetime, the next step towards general relativity is to define two variations on it.

The first object that we can define is called the Ricci Tensor, and it is closely related to the Riemann tensor that we defined last time. Recall that the Riemann tensor was defined as function

B = R(A,U,V)
in which A is the vector being moved, and U and V represent two other vectors that define the two paths along which we a...

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A Laymen's Guide To General Relativity: Part V

November 28, 2015
In the last article I reviewed the problem of having vectors defined in a spacetime where the metric function gives different lengths in different parts of spacetime, and outlined how this could be resolved using connection variables to move vectors around. Although this allows the comparison of two vectors in different parts of spacetime, it creates a new problem.

What happens if we move a vector along two different paths?

Using the covariant derivatives and the connection variables, a vector ...
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A Laymen's Guide To General Relativity: Part IV

November 27, 2015
In the last article we saw how special relativity is really nothing more than a function that gives the distance between two points in a four-dimensional spacetime, and the requirement that this distance be the same for all coordinate systems we might use. We also saw how, in the most general metric function this distance could vary depending on both time and on position within space. And that leads us to a new problem.

If the distance between two points can vary depending on where in spacetim...
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A Laymen's Guide To General Relativity: Part III

November 27, 2015
To me it has always seemed natural to divide the equations of general relativity into five distinct levels, each of which has its own laws and constraints. In my opinion each level must be studied and understood separately before they can be combined into one complete theory.

The foundation of the theory is the spacetime metric, which is the subject of today's article. 

And while the name sounds impressive, it is actually a very simple object. A metric is just a fancy mathematical name for any ...
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A Laymen's Guide to General Relativity: Part II

November 26, 2015
In the previous article, I introduced the Minkowski metric as a generalization of the theorem of Pythagoras and stressed the importance of the distance between two points being invariant under a change of coordinates. In fact the entire special theory of relativity is nothing more complicated than the statement that the distance between two points in four-dimensional spacetime, and given by the Minkowski metric, is the same for all coordinate systems. A few readers have asked me to give a few...

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A Laymen's Guide to General Relativity: Part I

November 25, 2015
This week is a very important anniversary in the scientific community, as it was 100 years ago this week that Albert Einstein submitted an academic paper for peer review, creating the General Theory of Relativity.

In the century that followed, the theory has developed from an obscure mathematical exercise that was famously claimed to be understood by only three people in the world, to a tool so useful that no GPS system would work properly without it. Only one hundred years after it was fi...
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100 Years of General Relativity

November 25, 2015
Exactly one century ago today, Albert Einstein submitted a paper for publication in which he generalized his already successful special theory of relativity. The single paper contained the bulk of the theory of general relativity in a clean finished form, and would forever change not only all of physics, but also our view of nature itself.

It must be said as well that there is some controversy on the authorship, as the brilliant mathematician David Hilbert had submitted a nearly identical theo...
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Card Shuffling Problem

November 3, 2015
A few days ago I was watching an old re-run of the excellent British television program, QI, and the host of the show made an interesting claim regarding a normal deck of playing cards. He took a new deck, which is ordered by number and suit, and gave it a few shuffles. Afterwards he claimed that no deck of cards had ever before been in that order, as the number of possible orderings was so large that statistically it was (almost) impossible that two randomly shuffled decks could ever be in t...
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A Mysterious Star

October 15, 2015
When I opened my e-mail this morning, I was stunned to find a number of messages all regarding the same astronomical oddity. Since it is rare for astronomy to make headlines, this was a most interesting start to the morning.

The topic that everyone is talking about today is the so-called 'most mysterious star in the galaxy' (as several of these e-mails called it). And the reason this star has everyone talking today is that one of the most plausible explanations for it is that it is home to a t...
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About Me


Dr. Chris Bird I am a theoretical physicist & mathematician, with training in electronics, programming, robotics, and a number of other related fields.

   


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