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Archive for the ‘particle physics’ category: Page 570

Dec 24, 2014

If c-global can save the World: Why is it being shunned? An Xmas Carol

Posted by in categories: existential risks, particle physics

Imagine there existed a proof that the most reluctantly accepted feature of Einstein’s gravitation theory – that c is no longer a global but only a local constant – was unnecessary: Would that not be wonderful?

The proof was greeted with planet-wide neglect: c-global exists in the Schwarzschild metric of general relativity since 2008 and so in the more fundamental equivalence principle since 2012. It hence also holds true for the full Einstein equation – only the pertinent transform has yet be written down to enable direct unification with quantum mechanics: a holy grail.

Hence most everyone is bound to be working on this in physics? The answer is no given the embarrassment of riches that is implicit. This professional modesty is a sympathetic human trait when you look at it in a detached mood. However, the result in question has also an applied side to it. In light of the latter, a prestigious collective activity has ceased to be safe.

Such collisions of interest do usually sort themselves out spontaneously with time. Here, bad luck for once wills that the unsafe collective activity – the re-ignition of a Nobel-decorated experiment at twice its former world-record energy – has been scheduled to start in only ten weeks’ time.

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Sep 28, 2014

DETAILS DO NOT EVER SUFFICE. FOCUS AND FOCUS! [GRAPHIC]

Posted by in categories: business, chemistry, complex systems, disruptive technology, economics, education, engineering, finance, futurism, general relativity, information science, nanotechnology, particle physics, science, scientific freedom

DETAILS DO NOT EVER SUFFICE. FOCUS AND FOCUS! [GRAPHIC]

0   GRANULARS
“… Practice makes perfect …”

Authored By Copyright Mr. Andres Agostini

White Swan Book Author (Source of this Article)

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Sep 1, 2014

Two numerical Sinai-type Theorems

Posted by in category: particle physics

T1: A numerical instability applies to time-inverted trajectories in deterministic statistical thermodynamics.

T2: A numerical instability applies to non-time inverted trajectories in deterministic statistical cryodynamics.

Cryodynamics in contrast to thermodynamics is based on inter-particle attraction rather than inter-particle repulsion. T2 implies that in numerical simulations of attraction-based gases, markedly deviating trajectories are necessarily generated. Since this fact went unrecognized, a whole new time’s arrow got overlooked numerically.

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Jul 31, 2014

CERN AND THE EARLY EINSTEIN

Posted by in categories: existential risks, particle physics

CERN bets the planet on the early Einstein having been wrong. Let me explain.

After having founded special relativity in mid-1905, the early Einstein held fast to the speed of light c being a global constant of nature for another 2 ½ years. Only in December of 1907 did Einstein switch to the view that c was only an everywhere locally, but not globally, valid constant of nature.

In 2008, results proving that the early Einstein of 1905 was right started to appear in the scientific literature. For example, quantum electrodynamics combined with the equivalence principle (Schwinger) shows this. Up until now, no counterproof is in the literature.

In light of this renaissance of the early Einstein, a previously noncontroversial policy of the famous CERN consortium turns out to be problematical: their refusal to update the outdated Safety Report of mid-2008. Demanding this update has become a priority issue for everyone who learns about its lack.

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Jul 15, 2014

A minor new Result can change the World (c-global)

Posted by in categories: existential risks, particle physics

It is a nice game: Pretend that c, the speed of light in the vacuum, were a global constant of nature. Then the Einstein equation assumes a more compact form. And black holes acquire radically new properties. One should not try to produce them down on earth, for example.

Fortunately, this simple game is pure fiction. Presently, Stephen Hawking’s safety guarantee to the planet – the rapid “evaporation” he described – renders miniature black holes innocuous, his recent modifications notwithstanding.

There are some voices that c is indeed globally constant (http://eujournal.org/index.php/esj/article/view/2608/2469 ). Would this be a reason to look at the issue anew for Hawking and others?

Jul 9, 2014

The global-c “Catastrophe” in Physics

Posted by in categories: existential risks, particle physics

To elder children and young adults, it is a bonanza since everything becomes transparent. The “ugly” dependency of the speed of light on the local pull of gravity – that it is slowed in the vicinity of the sun (Shapiro) and comes to a standstill at the horizon of a black hole (Oppenheiumer) – is gone since the distances travelled are proportionally enlarged. Simultaneously, the so far assumed to be added-on expansion speed of the universe ceases to be an option so that the “Big Bang” is no longer a physical reality. A new freedom – a vast new spatial reality to roam – opened itself up.

The same liberation has almost the opposite effect on slightly older young people – those who have to pass an exam or defend a thesis in a physical discipline. They are at a loss as to what still to believe and defend. Most textbooks have become obsolete. How discuss the new situation with Stephen Hawking, for example, or with CERN? Most importantly: How reconcile it with Einstein’s own work?

The latter job is a joy. A renaissance of the young Einstein – of the three years of his miraculous period ranging from 1905 until late 1907 – follows. These years were fueled by the universal constancy of the speed of light c in the vacuum as is well known.

What about the famous “Einstein equation” of late 1915, however: Has it become obsolete since its c is not a global but only a local constant? The equation only needs a re-scaling. The “too short” spatial distances for the elongated light travelling times just get proportionally stretched. The “Shapiro time delay” is now accompanied by a space dilation (“Shapiro-Cook space dilation”) and the infinite temporal distance to the horizon of a black hole is accompanied by an equally infinite spatial distance valid from outside.

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Jul 5, 2014

Löw – the Lion – demonstrates to the World that Perseverance can win a Palm

Posted by in categories: existential risks, particle physics

My repair of the global constancy of the speed of light c – the loss of which had stopped Einstein from publishing on gravitation for 4 years – has revived Einstein’s early greatest strength.

If c is globally constant, black holes are radically different – nonevaporating – in contradistinction to Hawking. And the by definition superluminal expansion speed of the “Big Bang” is likewise exploded.

Two canonized postulates gone: So it is no wonder that CERN refuses to defend its six years old safety report?

Suppose the young Einstein was indeed stronger: Would it not be worthy to check on this fact, especially so if it could save the planet from a catastrophe?

The world needs a voice capable of defending the older Einstein against the younger one. Anyone able to hit that goal?

May 6, 2014

Affirmation / ES Technical Note on LHC Collider Safety (p-p/MBH)

Posted by in categories: engineering, environmental, ethics, existential risks, particle physics

Although I have already mentioned a recent technical note on the application of Astronomical Observation to LHC/Collider Safety in comments to other posts here and there, I have not posted specifically about it until now. So finally, a short mention:

The technical note follows on from a modest paper I wrote in 2012 (Discussions on the Hypothesis that Cosmic Ray Exposure on Sirius B Negates Terrestrial MBH Concerns from Colliders), which concerned micro-black hole (MBH) production and the white dwarf safety assurance. There I demonstrated that not only are most white dwarf stars not suitable as a safety assurance, but that those hand-picked for the 2008 safety report had magnetic field strength measured to just 99% confidence within the range for safety assurance. That is not to say that the LHC safety argument was only 99% reliable — just that one of the cornerstone assurances was. The affirmation of these measurements was needed for a safety assurance to LHC p-p collisions based on astronomical observations – as a safety assurance that is not based on Hawking Radiation theory — but based on verifiable measurement. The technical note captures the official LSAG (CERN) response on the matter after internal review at CERN in late 2012, which had remained archived from email discussions until recently, when those conclusions were formalised into this technical note:

Link to the technical note: http://environmental-safety.webs.com/TechnicalNote-EnvSA01.pdf

mostly harmless

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May 6, 2014

The Outrageous Questions

Posted by in categories: general relativity, particle physics, physics, science

The May 2014 Scientific American article, “Super Symmetry, A Crisis in Physics”, got me thinking. If the proton mass is substantially greater that the sum of the masses of the quarks & gluons in the proton then there is an outrageous question regarding the Standard Model.

Before I attempt to answer that question we need to understand the concept of falsifiability.

The reason why I am qualified to ask this outrageous question is because I solved the physics of gravity modification, and falsifiability opens up more avenues for research, more questions and the finally the reasons for the outrageous question.

May 5, 2014

An Encounter with a Famous Physicist

Posted by in categories: disruptive technology, innovation, particle physics, physics, science, space, space travel

In April 2012 I met Lisa Randall while book signing at the National Space Symposium, held every April at the Broadmoor Hotel, Colorado Springs, Colorado. She is the Frank B. Baird, Jr., Professor of Science at Harvard University.

She autograph my copy of her book “Warped Passages” and I showed her the proof copy of my book “An Introduction to Gravity Modification, 2nd Edition” with the g=tau.c^2 massless formula for gravitational acceleration, solving the gravity modification physics.

More in the video …