relative local times, e.g. Texas time and London time or New York Time.
relative local times, e.g. Texas time and London time or New York Time.
Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: ¶a(t)·¶r(t)=c²
Summarized in this song
http://www.healingeagle.net/Eng/Quotes/GreenLeaves.html
Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: ¶a(t)·¶r(t)=c²
You are welcome. Glad you like it. This was the theme song of the 1960 movie 'The Alamo' starring the iconic John Wayne as Davy Crockett.
Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: ¶a(t)·¶r(t)=c²
hi, AntoinoLao
what do you think about spirit being everywhere at once? transending the concepts of time and space.
always present. then would it be stronger where there is more energy? and the opposite, weaker where there is less energy?
thank you,
gunnar
Unfortunately, all differential equations of physics, whether ordinary or partial, are formulated with respect to space, time, or spacetime and the product is square of energy.Originally Posted by gunnar
Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: ¶a(t)·¶r(t)=c²
This world
A fading
Mountain echo
Void and
Unreal
Within
A light snow
Three Thousand Realms
Within those realms
Light snow falls
As the snow
Engulfs my hut
At dusk
My heart, too
Is completely consumed
~Ryokan
hi,
what about an equation for ever present energy forces like earths gravity?
i would think that an always present spirit that is stronger where there is more energy (any environment of energy mass) and is weaker where there is less energy (outside any atmosphere of environment that has energy mass) could have a calculated formula.
thank you,
gunnar
Since spirits lack only directional invariance their energy can be different as strong or weak in different directions but their squares of energy is the same everywhere and everywhen.Originally Posted by gunnar
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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