heat physics 3 Laws and Newton Leibniz 3 Law O
source: Newton, leibniz, Clausius, jesus, Clapeyron, Thomson
Newton Leibniz 3 laws
1⃣ Power from universal gravitation FⒶ = GMm / r^2 = GmM / r^2 = F@
2⃣ F = m Σ a
3⃣ In ALL action, energy is preserve.
heat physics 3 Laws
⓪ heat moves within 2 things H & U till H & U become same temperature ... balance of heat
① δU = - δW + δQ
δ means change amount of something ...
U : total internal energy
W : output length ・ Force from system
Q : input heat into system
② Clausius's fundamental
if there is 2 things A & Q
if temperature of A = T(A) and temperature of Q = T(Q)
if T(A) < T(Q), move only heat itself from A to Q is impossible (without quantum physics)
③ Nernst fundamental
temperature of A = T(A) => "absolute" 0 temperature is impossible (without quantum physics)
lets find path
within
1⃣2⃣3⃣ and ⓪①②③
⓪ now we know heat is movement of molecule into 3 axis. (heat energy = 1/2 mvx^2 + mvy^2 + mvz^2)
vx... speed element of x axis
(i think SMALL waving of molecule which can't observe because Hisenberg's uncertainty might become mass ( e = mc^2 ))
now, H and U is confronting.
T(H) < T(U)
1/2 Σm(i)v(i)^2 things H things U 1/2 Σm(i)v(i)^2
h|u
lets zoom up confronting 2 molecules . 1 molecule h of H 1 molecule u of U
if 2 things crush & Force moves to another thing,
slower thing is pushed by faster thing.
◎ slow <= fast (can attack) h 1/2 mv^2 <= (energy) u 1/2 mv^2
✕ slow => fast (can't attack) h 1/2 mv^2 =>/ (energy) u 1/2 mv^2
between 2 molecules, always faster thing push slower thing.
so heat moves from Low temperature to High temperature.
① preservation of energy == infinity energy resource system is possible or not.
(if not think another world)
if heat energy is shown with move of molecule, we may think heat energy can thought as movement of molecules.
we have to prove
heat energy = friction (comes from confliction) = x F
= 1/2 mv^2(before) - 1/2 mv^2(after)
and to think change of mass,
e = mc^2
② ⓪ might be reason why.
③ if ② is true,
if all things have Temperature > "absolute" 0 temp,
its difficult to temperature Tλ to be 0 with move heat of λ into ξ
p pressure
v volume of gas
T temperature
n moll = amount of gas
WE CAN DOWN TEMPERATURE WITH
pv = TnR (Boyle = Charles's Law (of experience))
pressure become softer, T become cooler.
but if pressure of gas never become 0,
temperature never become 0
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