Dynamic Viscosity of Spacetime

Okay, so, time for a new idea! :-) A few days ago, while pondering over a biological experiment, a friend of mine mentioned fluid dynamics, particularly viscosity. For those of you are are not familiar with the term, viscosity is the property of a fluid to resist motion between its layers. It can be understood bluntly to be like the friction between two surfaces. Interesting property indeed!

Now flashback to about four months ago, where I was trying to figure out how much force will a body need to be applied to, in order to reach a certain acceleration, in a relativistic world. The formula I could derive was very different of what we know of through the Newtonian laws of Physics. The interesting thing, though, was the fact that force required in order to reach a certain acceleration in a relativistic world is always greater than that required in a classical world.

Thus, this difference in magnitudes of forces in relativistic world and classical world can be seen as a resistance that a body has to overcome in the relativistic world in order to reach a certain acceleration, while no such resistance is faced if we go by the Newtonian laws. Moreover, this resistance increases as our speed increases.

Here, γ = 1/sqrt(1-v²/c²) and is called the Lorentz factor, m is the absolute mass or rest mass of the body, a is the constant acceleration it possesses, v is its instantaneous speed, subscript c refers to classical and subscript R refers to relativistic, P refers to momentum and F refers to force.

This gave me an idea. I had read that research is going on in the area where they consider spacetime to be a superfluid, i.e. a fluid without viscosity. What if spacetime is a viscous fluid, because if it is, then I can easily relate Stoke's Law of Fluid Mechanics to my drag force! But, wait a minute, what is Stoke's Law?

Stoke's Law in fluid mechanics gives the formula for the force that will be experienced by a spherical object of radius R when it tries to move forward in a viscous liquid with a speed v. They call this resistive force as drag force. So, my idea here is to equate this drag force with the difference between relativistic force and classical force in order to find µ , i.e. the dynamic viscosity of spacetime, or in order to make you understand, the measure of stiffness of spacetime.

Here, E=mc^2. We all know where that came from! ;-) So, if my calculations are right (believe me they are, I rechecked like 20 times), then that is the formula for the dynamic viscosity of spacetime. But what is the significance of this dynamic viscosity? 

Well, it is not difficult to imagine that if the density of the fluid increases, its viscosity or stiffness will increase. Let us go the other way round, if viscosity if increasing, and no ther factor is affected, then density of the fluid must be increasing. Hence, as a body moves with faster velocity, viscosity of spacetime around it increases and so does the density. Spacetime becoming denser, if you visualize, is similar to warping of spacetime around the body, which is rightfully predicted by General Relativity. So, the theory explains why the spacetime is getting warped around a moving body! 

You would say that its relativistic mass is increasing as its speed increases, so the warping. But tell me this then, why is the mass increasing in the first place? I think that due to the movement of the body, viscosity of spacetime around it increases, resulting in denser spacetime, which indirectly means warping of spacetime around the body, which results in its increased gravitational effect! Well, something to think about! :-)

Report on Mathematical Explanations of the Spring Theory

The theory proposes that the spacetime fabric has spring-like characteristics and examines the outcomes of the assumption. The spacetime fabric’s spring-like nature results in it executing Simple Harmonic Motion (SHM) just like a compressed spring. Mathematically,

Symbol	For SHM by spacetime fabric	For SHM by particle attached to the spring
x	Present radius of observable universe	Position of particle attached to spring
A	Maximum radius that the observable universe can attain	Amplitude or Maximum displacement of the particle about mean point
ω	2*π*f (where f=frequency)	2*π*f (where f=frequency)
t	Age of the observable universe	The time that has passed since start of the SHM
φ	Phase difference	Phase difference

              

                             

·        Outcomes-

• Big Bang and the fate of the Universe- The hypothesis explains how initially the entire universe was compressed into a small particle (singularity) just like a compressed spring. After the bang, the space time fabric expanded with increasing acceleration in all directions and it still is expanding. Once the natural length of the fabric is reached, it will still expand but with decreasing acceleration, eventually coming to a stop with radius as A (defined above) same as the maximum displacement of a particle at the end of a spring. From there, the fabric will begin deceleration finally converging back to a singularity creating the same conditions as were before the Big Bang.
• Dark Energy- Just like the potential energy stored in a spring, dark energy might be nothing else but just the potential energy stored in the spacetime fabric due to its spring-like nature.
• On solving the given equations,

1. ω = 2.16 x 10^(-78) rad/s
2. A = 5.36 x 10^(86) m = 5.65 x 10^(70) light years
3. T = 9.29 x 10^(70) years

Results-

If the theory holds true,

• The maximum radius of the observable universe is 5.65 x 10^(70) light years.
• Total life of the observable universe is 9.29 x 10^(70) years.