| bio | website | |
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| location | ||
| age | ||
| visits | member for | 2 years, 4 months |
| seen | yesterday | |
| stats | profile views | 346 |
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Apr 30 |
comment |
What do I see if I move quickly past a charge surrounded by iron filings? I don't think it's realistic to ignore the electric polarization of the iron filings by the electric field of the charge. This will cause the iron filings and charge to attract one another in their rest frame. |
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Apr 28 |
comment |
Proving the consistency of Faraday's law of electromagnetic induction @Oaoa typo fixed, thanks |
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Apr 28 |
revised |
Proving the consistency of Faraday's law of electromagnetic induction fixed missing d/dt |
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Jan 16 |
comment |
No magnetic field from a static charge - Is there a simple physical argument to show why? @MarkEichenlaub you're right that it doesn't really need the preamble. But I thought it worth putting in to emphasise that the conservation of relativistic energy partly explains the form of the electric Lorentz force created by a static electric change, and perhaps give a clue to the additional physical argument that is needed to show why it mustn't create a magnetic field. |
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Jan 16 |
awarded | Yearling |
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Jan 16 |
revised |
No magnetic field from a static charge - Is there a simple physical argument to show why? improved wording |
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Jan 15 |
asked | No magnetic field from a static charge - Is there a simple physical argument to show why? |
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Jan 9 |
comment |
The Four-Clock Special Relativity Conundrum Could you add an explaination for your notation? |
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Dec 25 |
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The Four-Clock Special Relativity Conundrum @TerryBollinger Thanks. Unfortunately there was a typo in the labelling of the times which no one mentioned, that I've now fixed. |
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Dec 25 |
revised |
The Four-Clock Special Relativity Conundrum typo |
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Dec 23 |
answered | The Four-Clock Special Relativity Conundrum |
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Dec 4 |
awarded | Constituent |
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Nov 26 |
awarded | Caucus |
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Nov 16 |
comment |
Derive $\frac{\mathrm{d}}{\mathrm{d}t}(\gamma m\mathbf{v}) = e\mathbf{E}$ from elementary principles? But now you need to derive the Hamiltonian from elementary principles to answer my question. Still +1 since your answer is very close to my conclusion given the Hamiltonian is the total energy: The Lorentz force law for a static electric field expresses the conservation of energy, with the change in field energy depending only on the change in postion of the charge. |
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Nov 10 |
comment |
Is it possible to recover the old Bohr-Sommerfeld model from the QM description of the atom by turning off some parameters? @RonMaimon and lubos, maybe you're both right? Isn't the Bohr-Sommerfield model to QM what CED is to QED? |
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Nov 9 |
comment |
What was Albert Einstein's proof for $E=mc^2$? A more recent proof by Terence Tao terrytao.wordpress.com/tag/mass-energy-equivalence |
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Nov 9 |
answered | Proving the consistency of Faraday's law of electromagnetic induction |
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Nov 6 |
comment |
What are the challenges to achieving cold fusion? @ron "Pons/Fleisch" you really think so? Don't you think funding of their lab might have had something to do with what they saw? |
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Nov 2 |
comment |
How to publish scientific papers on the internet for free? post them on vixra.org |
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Nov 1 |
comment |
Why do we use Root Mean Square (RMS) values when talking about AC voltage @JohnRennie because it's a "grubby" engineering question, as Gell-Mann would say. |