Thermo 2nd law Flashcards
what’s the efficiency equation
η = desired output / required input
η = W/Qₕ = (Qₕ - Q꜀) / Qₕ for a heat engine
η = Q꜀/W for a refrigerator
what’s the coefficient of performance
the ‘efficiency’ of a refrigerator/heat engine.
not called efficiency cause a refrigerator has it greater than 1
Kelvin-Planck statement
it’s impossible to make an engine that exclusively extracts heat from a source and produces an equivalent amount of work.
Clausius statement
it’s impossible to make a refrigerator that exclusively transfers heat from a colder to a hotter body
Carnot’s theorem
a reversible engine is the most efficient
all reversible engines operating between two heat baths have the same efficiency (η) depending only on T꜀ and Tₕ
Carnot efficiency equation
η = 1- Q꜀/Qₕ
= 1- T꜀/Tₕ
Clausius inequality
∮1/T đQ ≤ 0
For a system when taken over a cycle
entropy equation
dS =đQ/T
(if T is constant then ΔS=ΔQ/T)
what’s the change in entropy for a reversible process
the total change in entropy (change in entropy of the universe) is 0
this comes from ΔS≥0. if the forward process has ΔS>0 then the reverse process would have ΔS<0 which isn’t possible
how do you find the maximum work extractable when heat is transferred from a finite hot reservoir to an infinite cold one
W= Qₕ - Q꜀
find Qₕ from the equation Qₕ = mcΔT (c: specific heat capacity)
since the cold reservoir is infinite the specific heat is infinite so that equation won’t work. use entropy to find it.
ΔSₕ + ΔS꜀ = 0 (this is the extreme cause which gives the maximum work done)
since T꜀ is constant ΔS꜀= Q꜀/T꜀
ΔSₕ = ∫đQ/T = ∫mc/T dT= mcln(T꜀/Tₕ)
∴ Q꜀ = T꜀mc*ln(T꜀/Tₕ)
then sub in values to get W
if heat is transferred from a hot to a cold reservoir and both are finite in size then derive the formula for the final temperature
ΔS = ΔSₕ + ΔS꜀ = 0 (limiting case)
∫đQₕ/T + ∫đQ꜀/T = 0
mcln(T/Tₕ) + mcln(T/T꜀) = 0
mcln(T/Tₕ) = -mcln(T/T꜀)
ln(T/Tₕ) = ln(T꜀/T)
T/Tₕ = T꜀/T
T= sqrt(Tₕ*T꜀)