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| Tags: force, relativistic, schoenfeldeinstein |
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#1
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"And then Schoenfeld-Einstein asked me to entertain his
relatives while he thought of a new name for his force." -The non-credible guy |
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#2
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SCHOENFELD-EINSTEIN RELATIVISTIC FORCE:
F = (m + y^3 B/c m0 v)a This is the relativistic mass-varying force. PROOF: let y = gamma = 1/sqrt(1-v^2/c^2) let B = beta = v/c Consider relativistic mass as a function of v. m(v) = y(v) m0 Since y(v) = 1 / sqrt(1 - v^2/c^2) = 1 / sqrt(u) { where u(v) = 1 - v^2/c^2 } = u^-1/2 Then, dy/dv = -1/2 u^-3/2 (du/dv) = -1/2 u^-3/2 2v/c^2 = v/[c^2 sqrt(u^3)] = v/c^2 y^3 { since 1/sqrt(u^3) = y^3 } = y^3 B/c Consider the relativistic mass rate of change w.r.t velocity, m(v) = y(v) m0 dm/dv = d(y(v) m0)/dv = m0 (dy/dv) = m0 y^3 B/c Since relativistic mass is velocity-dependent, the mass-varying force law is derived as: F = dp/dt = d(m(v) v)/dt = m(v) (dv/dt) + v (dm/dv)(dv/dt) = (m(v) + v dm/dv)a Since the relativistic mass rate of change w.r.t velocity is, dm/dv = m0 y^3 B/c Then the relativistic mass-varying force (SCHOENFELD-EINSTEIN FORCE) is, F = (m(v) + y^3 B/c m0 v)a QED |
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#3
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"John Schoenfeld" wrote in message om... SCHOENFELD-EINSTEIN RELATIVISTIC FORCE: F = (m + y^3 B/c m0 v)a This is the relativistic mass-varying force. PROOF: let y = gamma = 1/sqrt(1-v^2/c^2) let B = beta = v/c Consider relativistic mass as a function of v. m(v) = y(v) m0 Since y(v) = 1 / sqrt(1 - v^2/c^2) = 1 / sqrt(u) { where u(v) = 1 - v^2/c^2 } = u^-1/2 Then, dy/dv = -1/2 u^-3/2 (du/dv) = -1/2 u^-3/2 2v/c^2 = v/[c^2 sqrt(u^3)] = v/c^2 y^3 { since 1/sqrt(u^3) = y^3 } = y^3 B/c Consider the relativistic mass rate of change w.r.t velocity, m(v) = y(v) m0 dm/dv = d(y(v) m0)/dv = m0 (dy/dv) = m0 y^3 B/c Since relativistic mass is velocity-dependent, the mass-varying force law is derived as: F = dp/dt = d(m(v) v)/dt = m(v) (dv/dt) + v (dm/dv)(dv/dt) = (m(v) + v dm/dv)a Since the relativistic mass rate of change w.r.t velocity is, dm/dv = m0 y^3 B/c Then the relativistic mass-varying force (SCHOENFELD-EINSTEIN FORCE) is, F = (m(v) + y^3 B/c m0 v)a QED I thought you said you were leaving this group. Why the about face? Bill |
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#4
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Dear Bill Hobba:
"Bill Hobba" wrote in message ... "John Schoenfeld" wrote in message om... SCHOENFELD-EINSTEIN RELATIVISTIC FORCE: .... QED I thought you said you were leaving this group. Why the about face? Asperger's syndrome. He can't help it. David A. Smith |
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#5
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John Schoenfeld wrote:
SCHOENFELD-EINSTEIN RELATIVISTIC FORCE: F = (m + y^3 B/c m0 v)a Oh man, you broke my bull**** meter! Special Relativity http://scienceworld.wolfram.com/phys...elativity.html What is the experimental basis of Special Relativity? http://math.ucr.edu/home/baez/physic...periments.html Crank Information http://www.google.com/search?q=Schoe...ers.pandora.be |
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#6
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John Schoenfeld wrote:
SCHOENFELD-EINSTEIN RELATIVISTIC FORCE: F = (m + y^3 B/c m0 v)a This is the relativistic mass-varying force. PROOF: let y = gamma = 1/sqrt(1-v^2/c^2) let B = beta = v/c Consider relativistic mass as a function of v. m(v) = y(v) m0 Since y(v) = 1 / sqrt(1 - v^2/c^2) = 1 / sqrt(u) { where u(v) = 1 - v^2/c^2 } = u^-1/2 Then, dy/dv = -1/2 u^-3/2 (du/dv) = -1/2 u^-3/2 2v/c^2 = v/[c^2 sqrt(u^3)] = v/c^2 y^3 { since 1/sqrt(u^3) = y^3 } = y^3 B/c Consider the relativistic mass rate of change w.r.t velocity, m(v) = y(v) m0 dm/dv = d(y(v) m0)/dv = m0 (dy/dv) = m0 y^3 B/c Since relativistic mass is velocity-dependent, the mass-varying force law is derived as: F = dp/dt = d(m(v) v)/dt = m(v) (dv/dt) + v (dm/dv)(dv/dt) = (m(v) + v dm/dv)a Since the relativistic mass rate of change w.r.t velocity is, dm/dv = m0 y^3 B/c Then the relativistic mass-varying force (SCHOENFELD-EINSTEIN FORCE) is, F = (m(v) + y^3 B/c m0 v)a QED Nice. And why do you think this formula is useful for anything? Bye, Bjoern |
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#7
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John Schoenfeld wrote:
SCHOENFELD-EINSTEIN RELATIVISTIC FORCE: [snip] http://www.freefarts.com/farts.html Move cursor over blinkers to hear Schoenfeld's lecture. -- Uncle Al http://www.mazepath.com/uncleal/qz.pdf http://www.mazepath.com/uncleal/eotvos.htm (Do something naughty to physics) |
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#8
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"John Schoenfeld" wrote in message om... SCHOENFELD-EINSTEIN RELATIVISTIC FORCE: You are an ignorant, arrogant jackass Schoenfeld. Go play with Cesar. |
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#9
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"John Schoenfeld" wrote in message om... SCHOENFELD-EINSTEIN RELATIVISTIC FORCE: F = (m + y^3 B/c m0 v)a This is the relativistic mass-varying force. PROOF: let y = gamma = 1/sqrt(1-v^2/c^2) let B = beta = v/c Consider relativistic mass as a function of v. m(v) = y(v) m0 Since y(v) = 1 / sqrt(1 - v^2/c^2) = 1 / sqrt(u) { where u(v) = 1 - v^2/c^2 } = u^-1/2 Then, dy/dv = -1/2 u^-3/2 (du/dv) = -1/2 u^-3/2 2v/c^2 = v/[c^2 sqrt(u^3)] = v/c^2 y^3 { since 1/sqrt(u^3) = y^3 } = y^3 B/c Consider the relativistic mass rate of change w.r.t velocity, m(v) = y(v) m0 dm/dv = d(y(v) m0)/dv = m0 (dy/dv) = m0 y^3 B/c Since relativistic mass is velocity-dependent, the mass-varying force law is derived as: F = dp/dt = d(m(v) v)/dt = m(v) (dv/dt) + v (dm/dv)(dv/dt) = (m(v) + v dm/dv)a Since the relativistic mass rate of change w.r.t velocity is, dm/dv = m0 y^3 B/c Then the relativistic mass-varying force (SCHOENFELD-EINSTEIN FORCE) is, F = (m(v) + y^3 B/c m0 v)a All of that is pure horse dung. All particle accelerators were designed by utilising only one equation, namely dp/dt = e(E + v x B) No particle accelerator has ever been built which has not worked acording to specifications anywhere in the world. Accelerators have been built in which the particles move a speeds of approximately {1-10^-11) c. The design of the ISR was based on this equation. It was possible to keep two proton beams on track to within a couple of millimetres for a distance of 6 light months in that machine. So, not to be too polite about it, to hell with your nonsense. Franz |
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#10
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"Michael Varney" escribió en el mensaje ... "John Schoenfeld" wrote in message om... SCHOENFELD-EINSTEIN RELATIVISTIC FORCE: You are an ignorant, arrogant jackass Schoenfeld. Go play with Cesar. Mike, go play with the other psychos... |
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