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Subject:
Gravitation force
Category: Science > Physics Asked by: quantummechanique-ga List Price: $50.00 |
Posted:
03 Dec 2005 03:50 PST
Expires: 06 Dec 2005 02:47 PST Question ID: 600835 |
Greetings I have been thinking about origin of gravitational force for few years and tried to find some reply to my ideas. When I started writing down my ponderings about four dimensional visualisations and infinities, I came across with similarities of random walk theorem and hyperballs or more like possibility dimensions. Like the random walk theorem stated, when the movement is totally random, movement happens around the starting point like a person who is lost goes around circles, because possibility to go a specific direction is equal to going to opposite direction. If there is a presumption that there is a particle in a space that is totally empty excluding the particle, and the particle is making totally random movement in infinitely small perioids of time, the particle would stay at same position even if that particle would be moving with speed of light. That particle would have a hyperball or possibility dimension, which is size of a sphere which radius is speed of light times perioid of time "r=ct". The particle has a possibility to move anywhere inside the hyperball within the time perioid, although it is infinitely improbable to be anywhere else than in starting point. Because time is infinitely continuous factor, hyperball can be infinitely large. When another particle is added to that space, it will also have a hyperball, that will affect to first particle and vice versa. These two hyperballs will have overlapping areas that have higher propabilities than opposite directions. This will cause that these two particles start to move closer each another, since it's most probable direction. This movement is called as gravitation force. -------- My questions about this specific idea are as follows: Is there any logical errors or incomplete definitions? What is your opinion about this idea as an expert of the field? Can it be taken seriously in science world? Other possible objections and comments? |
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There is no answer at this time. |
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Subject:
Re: Gravitation force
From: kottekoe-ga on 03 Dec 2005 08:23 PST |
Quantum Mechanique: To even begin to be taken seriously, you will have to be able to derive quantitatively that the force obeys the inverse square law and is proportional to the mass of both objects. Ultimately, you will have to show that it is consistent with the laws of special and general relativity. If you get that far, people would certainly take note, if it provides an interestingly different perspective on the theory. To be taken really seriously, you will have to predict something that is measurable, but is different from what is already known. Otherwise, you have simply reproduced the existing theory in a different way. For some reason, gravitation attracts an inordinate number of people who have theories. Most of these hope to explain some aspect of gravitation that is important to the inventor, but fail to make quantitative predictions at all, or simply make the same quantitative predictions as Newton's classical theory of gravity, with vague derivations of how we got to Newton's equations. Since your theory is not quantitative, at least as you have stated it, it will never get serious consideration. Also, I cannot follow your speculations about the random walk at the speed of light. You will need to make these arguments quantitative to have it taken seriously. Good luck! |
Subject:
Re: Gravitation force
From: quantummechanique-ga on 03 Dec 2005 10:47 PST |
As far as I understood, going to in depth details would raise the price of the question to 200$, and pointing out too many factors would make it very time-taking. Therefore I tried to keep it as very simple example, and only point out things that are totally necessary to understand the idea. Your comments are very good for my purposes, since hearing what kind of requirements critical people demand, I will be capable to answer them later more thoroughly. To give a better understanding what I meant with random walk, I add a link to page that demostrates it. Check 2d box. http://www.ki.inf.tu-dresden.de/~fritzke/research/TS/example1.html |
Subject:
Re: Gravitation force
From: kottekoe-ga on 03 Dec 2005 15:37 PST |
I am well familiar with random walks, but as I understand your proposal, you have random jumps of length L=c*T, where c is the speed of light and T is an infinitesimal length of time. For a finite value of T, the particle will diffuse with a diffusion constant given by D = L^2/T = c^2*T . Rather than behaving as some "hyperball", if we start the particle at the origin, and look for it at time t, we will find it at a specific location, which in general will be far from the origin, but the size of the "ball" in which we would expect to find it will have a radius of about sqrt(Dt) = c*sqrt(T*t). That is, the ball's radius will be the speed of light times the geometric mean of the elapsed time and the duration of the jump. The particle will always be found at a specific place. What confuses me the most about what you are saying is that if I set the duration of the jump T to zero (since you say infinitely small periods of time), then there are no jumps at all (c*T = 0), the diffusion constant is zero, and nothing happens except that the particle rests at the origin. What also mystifies me is why this helps understand gravity. You have to hypothesize mysterious forces that cause a particle to accelerate this way and that in order to understand a force law that can be stated fairly simply. Why does this help. If you like to understand gravity in terms of interacting particles, rather than potential fields, that is certainly possible without introducing any new physics. Feynman's approach to electrodynamics pictures a world of virtual photons and electrons flitting into and out of existence and the Coulomb attraction or repulsion is accomplished by the point interactions of photons and charged particles. The theory predicts exactly the inverse square law and other features of the classical theory. This can be extended to gravitation as well using the graviton as the particle that mediates the interaction. There are difficulties with a simple field theory of the graviton when relativistic effects are considered and this is still one of the biggest challenges of theoretical physics, finding a fully consistent relativistic quantum field theory for gravity. |
Subject:
Re: Gravitation force
From: quantummechanique-ga on 04 Dec 2005 01:08 PST |
When I mentioned hyperball of the particle, I didn't mean that it would reflect diffusion of the particle. Hyperball was referring to visualisation of four-dimensional space, where the radius of the hyperball was the total length of random jumps. Possibility that a particle would reach the shell of the hyperball would be one to total amount of jumps times possible directions per jump. If even one factor is infinite, that would make the calculation bit difficult. The actual results are seen as you stated. Probability density of the hyperball is the same as bending in the space-time continuum. If hyperball would be thought as a trampoline which radius is the same as radius of the hyperball, and the particle is a marble ball in the center of it. Weight of the marble ball affects how much fabric of the trampoline is being pulled downwards. When there is another particle, they are on the same trampoline fabric. Because the force pulling fabric down is stronger between the marbles than elsewhere, the fabric is lower in between. This makes marbles to roll towards each other. And I try to clarify more about that part when the duration of the jump is zero. As you said length of the jump is speed of light times the perioid of time. You speaked earlier about finite factors, but as far as I understand, it is not disallowed to use infinitesimal factors. Total value would become zero, as anything times zero is zero. This doesn't mean that there wouldn't be any jumps at all. It would mean that there is infinite amount of jumps with infinitesimal duration to certain direction. This would cause diffusion to collapse into zero. Particle is moving at it's origin with the speed of light. This movement that happens at it's place is same as mass of the particle. Thank you again for your comments. I really appreciate it. |
Subject:
Re: Gravitation force
From: kottekoe-ga on 04 Dec 2005 07:14 PST |
You lost me back at the ranch. It is easy to handle the infinities times infinitesimals that you have described. The answer comes back as zero. That is why I described it with a finite T and replaced T with zero at the end. You need to progress from vigorous waving of the hands to equations. That is the only way to compete with Newton's great breakthrough. |
Subject:
Re: Gravitation force
From: kottekoe-ga on 04 Dec 2005 07:17 PST |
P.S. I should have added: But keep at it. There are still mysteries in the theory of gravitation. As I mentioned earlier, one of the greatest challenges of theoretical physics is the union of gravity and quantum mechanics. Revolutions in science are made only by questioning the status quo. |
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