Would anyone question the zeroth law of thermodynamics? Please visit this link and make your own personal decision. http://en.wikipedia.org/wiki/Zeroth_...thermodynamics
Would anyone question the zeroth law of thermodynamics? Please visit this link and make your own personal decision. http://en.wikipedia.org/wiki/Zeroth_...thermodynamics
Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: ¶a(t)·¶r(t)=c²
Graybeard (01-24-2011)
AntonioLao (01-22-2011)
You still need to clearly state what is it about the zeroth law that you are agreeing to? And it must be supported with your own assertions. It never was straight forward until you understand the second, the third, and the first law, in these order of progressive understanding.
Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: ¶a(t)·¶r(t)=c²
'Blondie says I must hate all Brunettes. I'll try, but if I can't ... I'll love them both'
... graffiti on Tavern wall, Pompeii, circa AD 70.
AntonioLao (01-24-2011)
The question is tantamount to asking can thermal equilibrium truly exist in a universe? My argument is that if thermal equality exists then the universe will never evolve to its present state since any form of motion always requires a temperature gradient such that the absolute difference of two given temperatures remains a finite positive quantity even if this quantity is infinitesimally small amount. Although negative temperature is not effectively defined the absolute zero of temperature is not attainable by any thermal experiment.
Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: ¶a(t)·¶r(t)=c²
Graybeard (01-24-2011)
'Blondie says I must hate all Brunettes. I'll try, but if I can't ... I'll love them both'
... graffiti on Tavern wall, Pompeii, circa AD 70.
AntonioLao (01-25-2011)
I'm hypothesizing that Local Infinitesimal Motion (LIM) can be conserved as the quantum vacuum fluctuations of the squares of zero-point energies such that the infinitesimal thermal gradient is equal to the product of two temperatures. These are equal only if both are zero.
Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: ¶a(t)·¶r(t)=c²
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